WO2004030056A1 - Method for correcting astigmatism, method for determining astigmatic sensitivity and method for exposure in charged particle beam aligner - Google Patents

Method for correcting astigmatism, method for determining astigmatic sensitivity and method for exposure in charged particle beam aligner Download PDF

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Publication number
WO2004030056A1
WO2004030056A1 PCT/JP2003/011879 JP0311879W WO2004030056A1 WO 2004030056 A1 WO2004030056 A1 WO 2004030056A1 JP 0311879 W JP0311879 W JP 0311879W WO 2004030056 A1 WO2004030056 A1 WO 2004030056A1
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Prior art keywords
astigmatism
blur
coil
electrode
sensitivity
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PCT/JP2003/011879
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French (fr)
Japanese (ja)
Inventor
Hiroyasu Shimizu
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Nikon Corporation
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Application filed by Nikon Corporation filed Critical Nikon Corporation
Priority to JP2004539469A priority Critical patent/JPWO2004030056A1/en
Priority to AU2003264482A priority patent/AU2003264482A1/en
Publication of WO2004030056A1 publication Critical patent/WO2004030056A1/en

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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/02Details
    • H01J37/04Arrangements of electrodes and associated parts for generating or controlling the discharge, e.g. electron-optical arrangement or ion-optical arrangement
    • H01J37/153Electron-optical or ion-optical arrangements for the correction of image defects, e.g. stigmators
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J2237/00Discharge tubes exposing object to beam, e.g. for analysis treatment, etching, imaging
    • H01J2237/30Electron or ion beam tubes for processing objects
    • H01J2237/317Processing objects on a microscale
    • H01J2237/3175Lithography

Definitions

  • the present invention relates to a method for determining astigmatic sensitivity in a charged particle beam exposure apparatus, and an exposure method using the same.
  • a charged particle emitted from a charged particle beam source is irradiated onto a reticle through an illumination optical system to illuminate the reticle, and a pattern formed on the reticle is projected through a projection optical system. Exposure transfer is performed by forming an image on a wafer.
  • FIG. 6 shows an example of a charged particle beam exposure apparatus.
  • the charged particle beam 2 emitted from the charged particle beam source 1 irradiates the shaped aperture 4 by the first irradiation lens 3.
  • the charged particle beam 2 having passed through the forming aperture 4 forms an image on the reticle 7 by the second irradiation lens 5 and the third irradiation lens 6.
  • a pattern to be transferred is formed on the reticle 7, and the charged particle beam 2 that has passed through the reticle 7 is exposed by the first projection lens 8 and the second projection lens 9 on an exposure target 10 such as a resist on a wafer.
  • An image of reticle 7 is formed.
  • the reticle is divided into about 1 mm squares, and the reticle is reduced to about 1/4 on the object to be exposed and transferred. Therefore, the size of the image is about 0.25 mm square.
  • Such an exposure area exposed at one time is called a subfield, and the subfields are connected to form an entire image, for example, a pattern of a semiconductor device.
  • the blur of the image projected on the object 10 is adjusted by adjusting the focal position by using the first projection lens 8, the second projection lens 9, or a dynamic focus corrector. This is done by adjusting the astigmatism blur and astigmatism using the astigmatism corrector SM.
  • the amount of adjustment of the astigmatism corrector that minimizes the amount of aberration according to the optical axis position or each deflection position has been determined by actual exposure or an aerial image sensor (AIS). .
  • the focus correction amount (the current flowing through the coil of the focus corrector or the voltage applied to the electrode of the focus corrector) is usually changed by changing the height of the object to be exposed in advance (ie, changing the focus position).
  • the amount of focus change per unit amount of bokeh (the focus correction sensitivity) is determined by measuring the amount of bokeh of the image at that time, and this amount of focus is determined by the amount of bokeh determined by simulation. It can be obtained by multiplying the correction sensitivity.
  • the astigmatism blur also changes due to the effect of the space charge effect. Therefore, in actual exposure, astigmatism Also need to be dynamically corrected.
  • the astigmatism has directionality, and the astigmatism corrector also consists of a combination of multiple coils. It has not been established how to adjust the current flowing through the coil of the astigmatism corrector or the voltage applied to the electrode of the astigmatism corrector with respect to the blur amount. Disclosure of the invention
  • the present invention has been made in view of such circumstances, and provides a method of correcting astigmatism in a charged particle beam optical system, a method of correcting astigmatism in a charged particle beam exposure apparatus, and a method of correcting astigmatism (astigmatism blur). It is an object of the present invention to provide a method of determining the correction sensitivity of the image and the sensitivity of occurrence of astigmatism blur), and an exposure method using the same.
  • the astigmatism blur correction sensitivity refers to a current flowing through an astigmatism corrector for correcting a unit amount of astigmatism blur converted to a focal position. Value means the amount of change in the value or applied voltage.
  • astigmatism blur occurrence sensitivity refers to a focus that occurs when a current value or a voltage value applied to an astigmatism corrector is changed by a unit amount.
  • a first invention for achieving the above object is a charged particle beam exposure apparatus having an astigmatism corrector, wherein a focus position is shifted by Ah to change a current value or a voltage value of the astigmatism corrector. Forming at least two different focal lines, obtaining a current value or a voltage value of the astigmatism corrector, shifting the focal position ⁇ h, and calculating the two different sets of focal lines.
  • the astigmatic sensitivity (correction sensitivity of astigmatism blur or astigmatism blur generation sensitivity) of the astigmatism corrector is obtained using a current value or a voltage value of the astigmatism corrector. This is a method for determining the point sensitivity.
  • the astigmatism sensitivity of the astigmatism corrector is obtained based on the current or voltage value of the astigmatism corrector when the focal line is formed, the astigmatism can be obtained by a simple method.
  • the astigmatic sensitivity of the corrector can be determined.
  • a second invention for achieving the above object is the first invention, wherein the astigmatism corrector has at least two coil groups or electrode groups.
  • a third invention for achieving the above object is the first invention, wherein, when the focal position is shifted by Ah, the focal position is shifted by ⁇ h from the normal focus position with respect to the normal focus position. It is characterized by the following.
  • the term “positive focus position” refers to the optical axis of the image plane on which a minimum circle of confusion centered on the optical axis is formed when the imaging state is changed by the projection lens.
  • Directional position that is, the position of the imaging plane in the optical axis direction where charged particles emitted from one point on the optical axis on the object plane are most narrowed isotropically.
  • the method of finding the positive focus position is to form a pinhole on the optical axis of the object surface and move the imaging plane in the optical axis direction. Is used to estimate the beam blur in that direction, find the image plane position that minimizes the blur in each direction, and use the midpoint as the focal point position.
  • the astigmatic sensitivity can be easily obtained as described later in the section of the embodiment.
  • a fourth invention for achieving the above object is the first invention, wherein the astigmatism is a correction sensitivity for astigmatism blur.
  • a fifth invention for achieving the above object is the first invention, wherein the astigmatism is an astigmatism blur occurrence sensitivity.
  • a sixth invention for achieving the above object is the fourth invention, wherein the focus position is shifted from the positive focus position by A h and then two sets of coils constituting an astigmatism corrector are provided.
  • the current value of the group (0 ° direction coil and 45 ° direction coil) or the voltage value of the two electrode groups (0 ° direction electrode and 45 ° direction electrode) was changed, and the measurement pattern was used as a reference.
  • 90 ° direction, 0 ° direction, 13.5 ° direction, and 45 ° direction minimize the blur in each of the two sets of current values or voltage values, and calculate the combination of these current values or voltage values. If it is (S 1 1, S 2 1), (S 1 2, S 2 2) (S 13, S 2 3), (S 14, S 24), at least one of the following expressions
  • the correction sensitivity of the astigmatism blur in at least one direction is determined.
  • Direction
  • the 0 ° direction with respect to the measurement pattern refers to the reference direction in which the measurement pattern is placed, and is often defined as the reference direction of the charged particle beam exposure system. Matches what was given.
  • a seventh invention for achieving the above object is the fourth invention, wherein a current value of two coil groups (0 ° direction coil and 45 ° direction coil) constituting an astigmatism corrector is provided. Or, change the voltage values of the two electrode groups (0 ° direction electrode and 45 ° direction electrode) to 90 ° direction, 0 ° direction, 135 ° direction, 45 ° direction based on the measurement pattern. 2) where the blur in the ° direction is minimized.
  • a current value or a voltage value of the set is determined respectively, and this is performed at arbitrary positions A and A in the optical axis direction at a position B which is separated by Ah in the optical axis direction from
  • the correction sensitivity for astigmatism blur in at least one direction is determined by at least one of the following expressions.
  • An eighth invention for achieving the object is the fifth invention, wherein the focus position is shifted from the right focus by Ah, and then two sets of coils forming an astigmatism corrector are provided. (0 ° direction coil and 45 ° direction coil) or the voltage value of two sets of electrodes ( ⁇ . Direction electrode and 45 ° direction electrode) were changed, and the measured pattern was used as a reference. 90 ° direction, 0 ° direction, 135 ° direction, and 45 ° direction, minimize the blur in each of the above two sets of current values or voltage values, and calculate the combination of these current values or voltage values. That it (S1
  • a ninth invention for achieving the above object is the fifth invention, wherein an astigmatism corrector is provided.
  • the two sets of current or voltage values that minimize the blur in the 90 ° direction, 0 ° direction, 135 ° direction, and 45 ° direction based on the measurement pattern are determined, and this is calculated as the optical axis.
  • the combination of these current values is (S11A, S21A), (S12A, S22A) ⁇ (S13A, S23A) ⁇ (S14A, (S24A) ⁇ (S11B, S21B), (S12B, S22B), (S13B, S23B), (S14B, S24
  • the sensitivity of occurrence of astigmatism blur in at least one direction is determined by at least one of the following expressions.
  • a tenth invention for achieving the above-mentioned object is the fifth invention, wherein the astigmatism corrector is configured such that the focus position is shifted from the right focus position by ⁇ h, and Current value of coil group (0 ° direction coil and 45 ° direction coil) or voltage value of two sets of electrodes (0 ° direction electrode and 45 ° direction electrode) (S1 and S2 respectively)
  • the current values of the two coil groups or the voltage values of the two electrode groups that minimize the blur in the two directions at which the angles differ by 0 are respectively obtained, and these current values or voltage values are obtained.
  • a circle passing through (S 15, S 25) and (S 16, S 26) is determined, and this circle is defined as the current or voltage value of the two sets of current values or voltage values forming a focal line.
  • a fifth invention in which, after shifting the focal position from the positive focal position by ⁇ h, two sets of coils (0 ° direction coil and 45 ° direction coil) constituting the astigmatism corrector Current value or voltage value of two electrode groups (0 ° direction electrode and 45 ° direction electrode)
  • a twelfth invention for achieving the above object is the fifth invention, wherein the astigmatism corrector is configured such that the focal position is shifted from the positive focal position by ⁇ h, and The current value of the coil group (0 ° direction coil and 45 ° direction coil) or the voltage value of two sets of electrodes (0 ° direction electrode and 45 ° direction electrode) are changed, and three or more with different angles.
  • the current value of the two sets of coils (0 ° direction coil and 45 ° direction coil) or the two sets of electrodes (0 ° direction electrode and 45 ° direction electrode) that minimize astigmatism blur in the direction ) Are calculated (S1 and S2), and the combination of these current or voltage values is calculated as (S11, S21), (S12, S2).
  • a thirteenth invention for achieving the above object is the fifth invention, wherein the focus position is shifted from the positive focus position by Ah, and the astigmatism corrector is constituted by two sets.
  • the current value of the coil group (0 ° direction coil and 45 ° direction coil) or the voltage value of two sets of electrodes (0 ° direction electrode and 45 ° direction electrode) is changed, and three or more angles are different.
  • the current value of the two sets of coils (0 ° direction coil and 45 ° direction coil) or the two sets of electrodes (0 ° direction electrode and 45 ° direction electrode) that minimize astigmatism blur in the direction ) (S1 and S2), and the combination of these current values or voltage values is (S11, S21), (S12, S12) 2 2), ..., (S in, S 2 n) (n is an integer of 3 or more), these points pass through in the SI-S 2 orthogonal coordinate system.
  • a circle is determined by solving an equation or by statistical fitting, and its center is set to (S1, S2,), and '90 ° and 135 ° directions on the circle with respect to the pattern reference direction.
  • the two sets of current values or voltage values that minimize the astigmatism blur of each of them are determined, and the combination of the two values is (Sll ,, S21 '), (S13, S23'). ), At least one of the following equations (19) to (22) is used to determine the sensitivity of occurrence of astigmatism blur in at least one direction. .
  • a fifteenth invention for achieving the above object is the fourteenth invention, wherein the statistical method uses a center point (S 1, S 2) of a circle formed by the focal point. ), Positive focus position h. , The proportionality constant r, and the angle 2t between the direction in which only the 0 ° direction blur changes with respect to the SI axis. Is a method of obtaining the above r and t D by obtaining these variables so that the following evaluation function minimizes P with the following as variables.
  • a sixteenth invention for achieving the above object is a charged particle beam exposure apparatus, comprising: a reticle; A method for exposing and transferring the image of the astigmatism onto a wafer, wherein the astigmatism blur determined by the method for determining astigmatism sensitivity in the charged particle beam exposure apparatus according to any one of the first to fifteenth inventions. Exposure transfer is performed while adjusting the astigmatism corrector so as to correct astigmatism blur for each subfield using the correction sensitivity or the sensitivity of occurrence of astigmatism blur. This is an exposure method in a charged particle beam exposure apparatus.
  • a seventeenth invention for solving the above-mentioned problems is the sixteenth means, wherein the astigmatism corrector includes two coil groups (a 0 ° direction coil and a 45 ° direction coil) or 2 A set of electrode groups (0 ° direction electrode and 45 ° direction electrode), and for the astigmatism blur amount ⁇ h 0 , A h 45 to be corrected, Voltage value ⁇ of two electrode groups. And it is characterized in that determined by the following equation ⁇ 45.
  • E is the astigmatism blur correction sensitivity when the 0-90 ° direction astigmatism blur is corrected by the 0 ° direction coil.
  • F is the sensitivity of astigmatism blur correction when the astigmatism blur in the 0-90 ° direction is corrected by the 45 ° direction coil.
  • G is the astigmatism blur correction sensitivity when astigmatism blur in the 45-135 ° direction is corrected by the 0 ° direction coil.
  • H is the astigmatism blur correction sensitivity when the 45-135 ° direction astigmatism blur is corrected by the 45 ° direction coil.
  • FIG. 1 is a diagram for explaining the principle of the first embodiment of the present invention.
  • FIG. 2 is a diagram for explaining the principle of the second embodiment of the present invention.
  • FIG. 3 is a diagram for explaining the principle of the fourth embodiment of the present invention.
  • FIG. 4 is a diagram for explaining the principle of the fifth embodiment of the present invention.
  • FIG. 5 is a diagram illustrating an example of a coil arrangement of the astigmatism corrector.
  • FIG. 6 is a diagram showing an outline of a charged particle beam exposure apparatus.
  • FIG. 7 is a diagram illustrating an example of a method for detecting blur.
  • a typical astigmatism corrector consists of four coils arranged at 90 ° intervals as shown in (a) as the first set of coils, and as shown in (b).
  • the four coil groups arranged at 90 ° intervals in a direction deviated by 45 ° from each other are used as a second set of coils, which are combined and arranged as shown in (c).
  • You. (D) is a sectional view taken along line AA in (c).
  • reference numerals 41 a to 41 d and 42 a to 42 d respectively show toroidal coils along the optical axis. Normally, 4 1 a to (!
  • the reference direction of the astigmatism corrector is set to 0 °.
  • the first set of coil groups will be referred to as 0 ° direction coils
  • the second set of coil groups will be referred to as 45 ° direction coils.
  • This reference direction Is conceptual to distinguish the two sets of coils. This direction does not always coincide with the 0 ° direction based on the measurement pattern.
  • the coil group may be a single set, but in this case, the description in this specification is made by ignoring either set of the coil groups (the current flowing through the coil group is 0). As).
  • the astigmatism corrector will be described as being constituted by such a coil group, but the astigmatism corrector uses a coil as described above, In addition to the method of correcting astigmatism by the Lorentz force, there is also a method of applying a voltage to the electrode and correcting the astigmatism by the electrostatic force.
  • the operation of such an astigmatism corrector using a coil and an astigmatism corrector using an electrode are basically the same. Therefore, those skilled in the art can easily read the embodiment of the present invention in an astigmatism corrector using an electrode by reading the coil in the following embodiment as an electrode and the current flowing through the coil as a voltage applied to the electrode. Can be inferred.
  • the astigmatism corrector described in the claims includes both a device using a coil and a device using an electrode.
  • FIG. Figure 1 shows that astigmatism blur changes the current flowing in the 0 ° direction coil (actually, the magnetic field is a problem, so the unit is AT.) S1, the current S2 flowing in the 45 ° direction coil is changed.
  • FIG. a is c Figure 1 showing how the changes by the horizontal axis the current S 1 flows to the first set of coil group, the current S 2 flowing through the second set of co-I le group vertical
  • An orthogonal coordinate system as an axis is shown. That is, it is a coordinate system for explaining the excitation of the astigmatism corrector.
  • the shape of the image shown is It is a shape (shape on the X-y plane) indicated by a rectangular coordinate system (X-y coordinate system) with the reference direction set to 0 °.
  • Fig. 1 the figure is drawn so that the S1 axis and the X axis coincide with each other, and the S2 axis and the y axis coincide with each other, but this is only displayed for convenience for easy understanding. It is. Since the X-y coordinate system and the S 1-S 2 coordinate system are completely different, there is no special meaning in giving them the same representation. Also, the origins of the S1-S2 coordinate system and the X-y coordinate system need not coincide.
  • the circle shown by the broken line in FIG. 1 is on the S1-S2 plane.
  • the focal position is shifted from the normal focal position by ⁇ h.
  • the focal position may be shifted by operating the charged particle beam optical system, but a simpler method can be realized by changing the height of the object to be exposed.
  • Reference numeral 15 indicates a beam shape in a state where astigmatism blur does not occur.
  • the beam shape changes as shown in the figure according to the respective values of S l and S 2.
  • a focal line is formed on a circle centered at 15.
  • 11 is at 0 ° to the axis
  • 12 is at 90 ° to the X-axis
  • 13 is 45 ° to the X-axis
  • 14 is at X-axis. It is tilted 135 ° to it.
  • a set of S 1 and S 2 giving these focal lines 11 to 14 is found, and the correction sensitivity of astigmatism blur is determined based on the set.
  • the coordinates of 11 are (S11, S21)
  • the coordinates of 12 are (S12, S22)
  • the coordinates of 13 are (S13, S23)
  • the coordinates of 14 Let (S14, S24) be the current flowing through the 0 ° directional coil from the state where there is no astigmatism blur at the same focal position as the measurement point and the 45 ° directional coil, as is clear from the figure.
  • Equation (1) and (2) the dimensions of equations (1) and (2) are expressed, for example, as [AT / mm] (voltage is expressed as [V / mm]). 511-512
  • the astigmatism blur in the 0-90 ° direction is not changed, and only the astigmatism blur in the 45 ° -135 ° direction is adjusted.
  • Astigmatism blur can be minimized (14 in Fig. 1). or, When the sign of the above equation is changed, the astigmatism blur in the 135 ° direction can be minimized (state 13 in Fig. 1).
  • equations (3) and (4) are expressed, for example, as [mm / AT] (for voltage, they are expressed as [V / mm]).
  • the magnitude of the astigmatism blur is represented by being converted into the magnitude of the focal position shift in the optical axis direction.
  • the absolute value of these two components of astigmatism blur is the absolute value of the amount of deviation of the imaging plane position, which becomes the focal line when there is astigmatism, from the positive focal point. It is expressed by the combination of the direction blur and the 45-degree direction blur.
  • the 0-degree direction component and the 45-degree direction component are the 0-degree direction blur for the astigmatism blur (9 if the 0-degree direction blur is negative). Contribution of 0 degree directional blur), 45 degree directional blur (If 45 degree directional blur is negative, it indicates that 135 degree directional blur is occurring) Is shown.
  • the current or voltage applied to the astigmatism corrector is calculated by applying the astigmatism bog to be corrected (inversion of the sign of the generated astigmatism blur) to the correction sensitivity matrix of the astigmatism blur.
  • the astigmatism blur is corrected by changing the current or voltage of the astigmatism corrector by that amount.
  • the current values S 1 and S 2 that give a focal line in each direction were found As described, it is not necessary to actually find the focal line. That is, for example, if a combination of the current values S 1 and S 2 that minimizes the blur in the X-axis direction is found, it corresponds to the focal line 12. If a combination of the current values S l and S 2 that minimizes the blur in the y-axis direction is found, it corresponds to the focal line 11. If a combination of the current values S 1 and S 2 that minimizes the blur in the 45 ° direction with respect to the X axis is found, it corresponds to the focal line 14. If a combination of the current values S 1 and S 2 that minimizes the blur in the 135 ° direction with respect to the X axis is found, it corresponds to the focal line 13.
  • FIG. 2 the concept of S1-S2 axis and X-y axis is the same as Fig.1.
  • the shape of the image is on the X-y plane, and the circle shown by the broken line is on the SI-S2 plane.
  • a focal line is detected at a certain focal position in the same manner as in the first method, and the focal line in the X-axis direction (0 ° direction) is inclined at 11 A and 90 ° with respect to the X-axis.
  • the focal line is 12 A
  • the focal line inclined at 45 ° to the X axis is 13 A
  • the focal line inclined at 135 ° to the x axis is 14 A.
  • the focal position is shifted Ah from this position, and the focal line is detected in the same manner.
  • the focal point may be shifted by operating the charged particle beam optical system, but a simpler method can be realized by changing the height of the object to be exposed.
  • the focal line in the X-axis direction is 1 1 B
  • the focal line inclined 90 ° to the X axis is 12 B
  • the focal line inclined 45 ° to the X axis is 13 B
  • the focal line inclined by 135 ° with respect to the x-axis is defined as 14B.
  • the coordinates of each point are 1 1 A (SI 1 A, S 2 1 A) s 1 2 A (S 12 A, S 22 A) 13 A (S 13 AS 23 A), 14 A (S 14 A, S 2 4 A), 1 1 B (S 1 1 B, S 2 1 B) 1 2 B (S 1 2 B, S 2 2 B), 1 3 B (S 1 3 B, S 2 3 B), 1 4 B (S14B, S24B).
  • the sensitivity of astigmatism blur which represents astigmatism blur (conversion in the optical axis direction) that occurs when the current flowing through the coil of the astigmatism corrector is changed by a unit amount, is For example, it is represented by a dimension such as [mm / AT].
  • the occurrence sensitivity of such astigmatism blur is as described in the above (1).
  • the amount of change in the current flowing through the 0 ° direction coil is ⁇ I. , 4 5 ° the amount of change current flowing in the direction coil and delta 1 4 5, the time of 0-9 0 those converted in the optical axis direction position astigmatism blur of ° direction A h. And those obtained by converting the astigmatism blur of 4 5-135 ° direction in the optical axis direction position and delta 1 4 5,
  • a ii represents the current flowing through the 0 ° Generating sensitivity astigmatism blur
  • a 2 i is 0 ° direction coil generating sensitivity astigmatism blur of 5-135 ° direction
  • a i have AA 2 have A 2 2 is determined easy by calculating the inverse matrix of (2 9). That is,
  • the current value of the two sets of coils or the voltage value of the two sets of electrodes constituting the astigmatism compensator are varied respectively, and the 0 ° direction, 90 ° direction, 45
  • the two sets of current values or voltage values that minimize the blur in the 135 ° direction and 135 ° direction are calculated accordingly, and these are determined as arbitrary positions A and A in the optical axis direction at positions ⁇ h away from the arbitrary optical axis directions in the optical axis direction.
  • [ ⁇ ( ⁇ 11, -S ⁇ 2 B )- ⁇ Sn A -S12 A ) ⁇ ⁇ (S23 B -S2 B )- ⁇ S23 A -S2 A ) ⁇ - ⁇ S13 B -514 ⁇ )- (513 ⁇ -S A ) ⁇ ⁇ ((S21 B -S22 B )- ⁇ S21 A -S22 A ) ⁇ ].
  • [ ⁇ (S11 B -512,)-(511, -S12 A ) ⁇ ⁇ S23 B -S24 B )-(S23 A -S24 A ) ⁇
  • FIG. 3 is a diagram for explaining a fourth embodiment of the present invention, and is similar to FIG. In this figure, it is assumed that the focal position is shifted from the normal focal position by ⁇ h. Note that 0 indicates the excitation condition in a state where astigmatism blur does not occur.
  • the combination of S 1 and S 2 which forms a long focal line in a direction shifted by 45 ° from the reference direction of the measurement pattern, is set to the position of point 22 (S 15, S 2 5),
  • these focal lines are indicated by lines. That is, points 22 and 23 respectively correspond to the reference direction of the measurement pattern. This is a point at which astigmatism blur in directions shifted by 135 ° and 0 ° is minimized. That is, at point 22 and point 23, the angle difference 0 in the direction that minimizes astigmatism blur is
  • the direction of the focal line at the point where the center angle of the circle where the combination of (S1, S2) forming the focal line exists changes by ⁇ changes by 0/2. It has been known. Conversely, since the direction of the focal line is shifted by 0 at points 2 2 and 2 3, the line connecting the center 0 of circle 2 1 and point 2 2 (or point 2 3) and this vertical 2 The angle formed by the bisectors 24 is 0.
  • the focal line in the 0 ° direction is symmetrical to point 23 with respect to zero. If it is 0 in Fig. 3, if S1 is excited positively, the blur in the 0 ° direction becomes stronger, but the other solution is reversed, so that it is easy to determine.
  • the circle connecting the points forming the focal line is determined as a circle centered on the point 0 and passing through the points 22 and 23.
  • the radius of the circle indicates the magnitude of astigmatism blur caused by the shift of the focal position by ⁇ h.
  • the sensitivity at the time of correction by the 45 ° directional coil (Sl) and the 45 ° directional coil (S2) can be obtained.
  • the point where the astigmatism blur in the 90 ° direction is minimized on this circle is determined, and the combination of the currents of the 0 ° direction coil and the 45 ° direction coil of the astigmatism corrector at that time is (S ll , S 2 1 '). Also, on this circle, 135 ° Find the point where the astigmatism blur in the azimuth is minimized. Then, the 0 ° direction coil of the astigmatism corrector, 45. The combination of the currents in the direction coils is (S13, S23 ').
  • the excitation current or voltage of the astigmatism corrector that minimizes the blur in the 0i direction is (S15S25), and the astigmatism that minimizes the blur in the 6> 2 direction.
  • the excitation current or voltage of the compensator is (S16 ', S26')
  • the point on the general focal line circle is the focal line radius S,
  • the point (S1, S2) on this focal line circle is a straight line parallel to the S1 axis, centered on the center of the circle (S1, S2) in (SI—S2) coordinates. If the angle formed is ⁇ ,
  • two points at which the astigmatism blur in the different directions is minimized are found on the S 1 —S 2 plane, and these are the focal lines on the S 1 —S 2 plane. If the center angle in the circle where the combination of (S1, S2) forms the focal line changes by ⁇ , the direction of the focal line will change by 0/2. Was used to find a circle forming a focal line. However, if three points at which the astigmatism blur in the different directions is minimized on the S 1 -S 2 plane are obtained, each of these points is on a circle forming a focal line on the S 1-S 2 plane. By taking advantage of this fact, a simultaneous equation can be solved to obtain a circle. After obtaining the circle, the same processing as described above is performed, and the generation sensitivity of the astigmatism corrector can be obtained.
  • FIG. 4 is a diagram for explaining a fifth embodiment of the present invention using a method for removing the influence of such an error as much as possible when there is such an error.
  • the points (combinations of the current values of the two coils) on the S1-S2 surface that minimize astigmatism in many directions (eight in the figure) are obtained.
  • the points are represented by 25-32.
  • the shape of the focal line at each point is indicated by a line.
  • the pattern direction is set to 0 ° in the S1 direction.
  • circle 21 is the circle connecting the points where the focal line is formed, and point 0 is the center.
  • points 25 to 32 are not on the circle 21. This is because there is an error in the determination of points 25-32.
  • the generation sensitivity of the astigmatism corrector can be obtained by the same method as the embodiment shown in FIG.
  • the blur detection charged particle beam image 51 is scanned by a scanning deflector, and passes over the charged particle beam blur detection mark 52. Then, a signal is obtained by a signal detector (not shown) (for example, a backscattered electron detector).
  • a signal detector for example, a backscattered electron detector.
  • This signal is proportional to the area of the overlapping portion of the charged particle beam blur detection mark 52 and the blur detection charged particle beam image 51, but the blurred charged particle beam image 51 If there is, it becomes a figure that is blurred by the amount of the blur. Therefore, this detection signal usually has a shape as shown in 53, and by differentiating it, a waveform like 54 is obtained.
  • the scanning distance of a portion from 12% to 88% of the rising portion in the differential signal is defined as a blur 55.
  • the Coulomb effect is corrected in consideration of the aperture ratio of the pattern for each subfield. This is performed for each subfield. That is, the focal position of the projection optical system is changed for each subfield so as to correct the Coulomb effect.
  • the astigmatism blur correction sensitivity is determined from the obtained astigmatism blur occurrence sensitivity. That is,
  • A is the sensitivity of astigmatism blur which causes astigmatism blur in the 0-90 ° direction by the 0 ° direction coil (that is, when the current flowing through the 0 ° direction coil is increased per unit, 0 ° directional blur increase)
  • C is the sensitivity of astigmatism blur which causes astigmatism blur in the 45 ° -135 ° direction by the 0 ° direction coil (that is, when the current flowing through the 0 ° direction coil is increased per unit, 90 ° increase in direction blur)
  • the astigmatism blur occurrence sensitivity matrix [X] is (AB ⁇
  • E is the astigmatism blur correction sensitivity when the 0 ° -90 ° direction astigmatism blur is corrected by the 0 ° direction coil.
  • F is the sensitivity of astigmatism blur correction when the astigmatism blur in the 0-90 ° direction is corrected by the 45 ° direction coil.
  • G is the astigmatism blur correction sensitivity when correcting the astigmatism blur in the 45-135 ° direction using the 0 ° direction coil.
  • H is the astigmatism blur correction sensitivity when the 45-135 ° direction astigmatism blur is corrected by the 45 ° coil.
  • astigmatism blur in the 0-90 ° direction is _ ⁇ h. Only occurs at 45 ° -135.
  • Square astigmatism blur countercurrent is - ⁇ If only occurs h 45, astigmatic blur quantity to be corrected ( ⁇ , ⁇ 1 ⁇ 45) becomes, the exciting current flowing in the 0 ° direction coils, a 45 ° direction co I le The exciting current that flows is
  • ⁇ I calculated by It may be changed by ⁇ I 4 5.
  • the sensitivity of occurrence of astigmatism blur was obtained with the focus position changed from the normal focus position by ⁇ h, but astigmatism correction in which focal lines are formed at a plurality of focus positions is performed.
  • the current values S 1 and S 2 of the detector may be obtained, and the occurrence sensitivity of astigmatism blur may be obtained by a statistical method. An example is shown below.
  • (S1, S2.) Is the center point of the circle created by the above-mentioned focal point, h. Is the focus position, and r is the proportional constant, which is the radius of the circle that changes when (h—]!) Changes by a unit amount, t. Is the half of the angle with respect to the S1 axis that only the 0 ° direction blur changes, and these are all unknowns. And these unknowns are A known statistical method may be selected and used as a method of obtaining an unknown that minimizes the evaluation function P by minimizing the evaluation function P expressed by:
  • the astigmatism blur in the 0 to 90 ° direction is ⁇ h due to changes in the influence of the Coulomb effect and changes in the deflection position. Only it occurs, 4 5 ° - 135 If the astigmatism blur of ° direction occurs only A h 4 5, the excitation current flowing in the direction of 0 ° to Koi Le, the exciting current applied to 4 5 ° direction coils, it it , ⁇ ⁇ calculated by equation (37). , ⁇ I 45 may be changed.
  • the excitation current flowing through the coil in the 0 ° direction and the excitation current flowing through the 45 ° direction coil are ⁇ ⁇ . , ⁇ I of 4 5 only when changing, 0 - 9 0 astigmatism blur of ° direction ⁇ , 4 5 ° - 135 astigmatism blur of ° direction ⁇ h 4
  • the charged particle beam exposure apparatus to which the embodiment of the present invention is applied is the same as that shown in FIG.
  • the correction sensitivity of astigmatism blur in each direction is obtained by the method described above, and the amount of change in astigmatism blur due to the space charge effect (positive focus) is determined by simulation.
  • the current value of each coil may be changed by the value obtained by multiplying the amount of change in astigmatism blur by the correction sensitivity of astigmatism blur in each direction.
  • an example of the charged particle beam exposure method using the correction sensitivity for astigmatism blur determined as described above will be described.
  • the Coulomb effect is corrected for each subfield in consideration of the aperture ratio of the pattern for each subfield.
  • the focal position of the projection optical system is changed for each subfield so as to correct the Coulomb effect.
  • the amount of astigmatism that occurs due to the change in the deflection position is converted into a change in the focal position, and the resulting value is multiplied by the correction sensitivity for astigmatism blur determined by the method described above, and the resulting value is calculated as the astigmatism.
  • the astigmatism associated with the deflection is also corrected by changing the current flowing through the 0 ° direction coil and the current flowing through the 45 ° direction coil of the astigmatism corrector. In this way, a good imaging pattern with small astigmatism can be obtained.

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Abstract

While shifting the focal point and varying the current values S1 and S2 of two sets of coil in an astigmatism correcting unit, a combination of current values where focal lines (11, 13, 12, 14) having inclinations of 0°, 45°, 90° and 135° with respect to the x axis is determined. A correction sensitivity of astigmatic blur is determined from the combination of current values according to a specified calculation expressions. The correction sensitivity of astigmatic blur can thereby be determined readily in a charged particle beam aligner.

Description

明 細 書 荷電粒子線露光装置における非点収差補正方法、 非点感度の決定方法、 及び露光方法 技術分野  Description Method for correcting astigmatism in charged particle beam exposure apparatus, method for determining astigmatism sensitivity, and exposure method
本発明は、 荷電粒子線露光装置における非点感度の決定方法、 及びそ れらを使用した露光方法に関するものである。 背景技術  The present invention relates to a method for determining astigmatic sensitivity in a charged particle beam exposure apparatus, and an exposure method using the same. Background art
半導体デバイスの高密度化に伴い、 その製造工程においてレチクルか らウェハに露光転写すべきパターンが微細化している。 このような微細 なパターンを露光転写するには、 光学式露光転写装置ではその解像度が 不足しており、 光学式露光転写装置に代わるものとして、 電子線等の荷 電粒子線を使用した露光転写装置の開発が進められている。  With the increase in the density of semiconductor devices, patterns to be exposed and transferred from a reticle to a wafer in the manufacturing process are becoming finer. In order to expose and transfer such fine patterns, the resolution is insufficient with an optical exposure / transfer device, and as an alternative to the optical exposure / transfer device, exposure transfer using a charged particle beam such as an electron beam is used. Equipment is being developed.
荷電粒子線露光装置においては、 荷電粒子線源から放出された荷電粒 子を、 照明光学系を介してレチクル上に照射して照明し、 レチクルに形 成されたパターンを、 投影光学系を介してウェハ上に結像させることに より、 露光転写を行っている。  In a charged particle beam exposure apparatus, a charged particle emitted from a charged particle beam source is irradiated onto a reticle through an illumination optical system to illuminate the reticle, and a pattern formed on the reticle is projected through a projection optical system. Exposure transfer is performed by forming an image on a wafer.
図 6に荷電粒子線露光装置の例を示す。 荷電粒子線源 1から放出され た荷電粒子線 2は第 1照射レンズ 3によって成形開口 4を照射する。 成 形開口 4を通過した荷電粒子線 2は第 2照射レンズ 5および第 3照射レ ンズ 6により成形開口をレチクル 7上に結像する。 レチクル 7上には転 写すべきパターンが形成されており、 レチクル 7を通過した荷電粒子線 2は第 1投影レンズ 8及び第 2投影レンズ 9によってウェハ上のレジス トなどの被露光物 1 0上にレチクル 7を結像する。 荷電粒子線露光装置 では通常、 レチクルを 1 mm角程度に分割し、 被露光物上には 1/4程度 に縮小して露光転写している。従って像の大きさは 0.25mm角程度にな つている。 このような 1度に露光される露光領域をサブフィ一ルドとい い、 サブフィール ドをつなぎあわせて全体の像、 例えば半導体デバイス のパターンを形成する。 FIG. 6 shows an example of a charged particle beam exposure apparatus. The charged particle beam 2 emitted from the charged particle beam source 1 irradiates the shaped aperture 4 by the first irradiation lens 3. The charged particle beam 2 having passed through the forming aperture 4 forms an image on the reticle 7 by the second irradiation lens 5 and the third irradiation lens 6. A pattern to be transferred is formed on the reticle 7, and the charged particle beam 2 that has passed through the reticle 7 is exposed by the first projection lens 8 and the second projection lens 9 on an exposure target 10 such as a resist on a wafer. An image of reticle 7 is formed. Charged particle beam exposure system Usually, the reticle is divided into about 1 mm squares, and the reticle is reduced to about 1/4 on the object to be exposed and transferred. Therefore, the size of the image is about 0.25 mm square. Such an exposure area exposed at one time is called a subfield, and the subfields are connected to form an entire image, for example, a pattern of a semiconductor device.
このような荷電粒子線露光装置では、 被露光物 1 0に投影される像の ボケの調整は、 第 1投影レンズ 8、 第 2投影レンズ 9又は動的な焦点補 正器により焦点位置を調整したり、 非点収差補正器 S Mにより非点収差 ボケや非点歪みを調整することにより行われている。 非点収差ボケや非 点歪みは光軸位置あるいは各偏向位置に応じて収差量が最小となるよう な非点収差補正器の調整量を実露光あるいは空間像センサー (A I S ) によって求められていた。  In such a charged particle beam exposure apparatus, the blur of the image projected on the object 10 is adjusted by adjusting the focal position by using the first projection lens 8, the second projection lens 9, or a dynamic focus corrector. This is done by adjusting the astigmatism blur and astigmatism using the astigmatism corrector SM. For astigmatism blur and astigmatism distortion, the amount of adjustment of the astigmatism corrector that minimizes the amount of aberration according to the optical axis position or each deflection position has been determined by actual exposure or an aerial image sensor (AIS). .
しかしながら、 要求される露光転写精度が高くなるに従い、 サブフィ —ルド内の開口率により露光電流が変化し、 そのために生じる空間電荷 効果によるボケ (空間電荷ボケ) が変化することが問題となってきた。 これに対処するために、 各サブフィ一ルド毎に空間電荷ボケの量をシミ ユレ一シヨンにより計算し、 それに対応するだけ、 焦点位置を変化させ る方法が採用されるようになつてきた。  However, as the required exposure transfer accuracy has increased, the exposure current has changed due to the aperture ratio in the subfield, and the blur caused by the space charge effect (space charge blur) has changed. . To cope with this, a method has been adopted in which the amount of space charge blur is calculated by simulation for each subfield, and the focus position is changed correspondingly.
このときの焦点補正量 (焦点補正器のコイルに流す電流、 又は焦点補 正器の電極に印加する電圧) は、 通常、 予め被露光物の高さを変化させ て (即ち焦点位置を変化させたと同じ状態を作り)、 そのときの像のボケ 量を測定することにより、 単位ボケ量あたりの焦点変化量 (焦点補正感 度) を決定しておき、 シミュレーションにより決定されたボケ量にこの 焦点補正感度をかけることにより求めることができる。  At this time, the focus correction amount (the current flowing through the coil of the focus corrector or the voltage applied to the electrode of the focus corrector) is usually changed by changing the height of the object to be exposed in advance (ie, changing the focus position). The amount of focus change per unit amount of bokeh (the focus correction sensitivity) is determined by measuring the amount of bokeh of the image at that time, and this amount of focus is determined by the amount of bokeh determined by simulation. It can be obtained by multiplying the correction sensitivity.
さらに、 露光電流が変化すると空間電荷効果の影響で非点収差ボケも 変化する。 よって、 実際の露光においては焦点補正と共に非点収差ボケ も動的に補正する必要がある。 しかしながら、 非点収差ボケの場合は非 点収差に方向性があり、 かつ非点収差補正器も複数コイルの組み合わせ から成り立っているので、 シミュレーションによって非点収差ボケ量を 求めてもこの非点収差ボケ量に対してどのように非点収差補正器のコィ ルに流す電流又は非点収差補正器の電極に印加する電圧を調整したらよ いのかが確立されていなかつた。 発明の開示 Furthermore, when the exposure current changes, the astigmatism blur also changes due to the effect of the space charge effect. Therefore, in actual exposure, astigmatism Also need to be dynamically corrected. However, in the case of astigmatism blur, the astigmatism has directionality, and the astigmatism corrector also consists of a combination of multiple coils. It has not been established how to adjust the current flowing through the coil of the astigmatism corrector or the voltage applied to the electrode of the astigmatism corrector with respect to the blur amount. Disclosure of the invention
本発明はこのような事情に鑑みてなされたものであり、 荷電粒子線光 学系の非点収差補正方法、 荷電粒子線露光装置における非点収差補正方 法、 非点感度 (非点収差ボケの補正感度、 非点収差ボケの発生感度) の 泱定方法、 及びそれを使用した露光方法を提供することを目的とする。 なお、 本明細書、 要約書及び請求の範囲において、 非点収差ボケの補 正感度とは、 焦点位置に換算した単位量の非点収差ボケを補正するため に非点収差補正器に流す電流値又は印加する電圧値の変化量を意味し、 0— 9 0 ° 方向の非点収差ボケを補正する場合には、 0 ° 方向に非点収 差ボケを発生する方向を正とし、 4 5 — 135 ° 方向の非点収差ボケを補 正する場合には、 4 5 ° 方向に非点収差ボケを発生する方向を正とする。 また、 本明細書、 及び請求の範囲において、 非点収差ボケの発生感度 とは、 非点収差補正器に流す電流値又は印加する電圧値を単位量だけ変 化させた場合に発生する、焦点位置に換算した非点収差ボケ量を意味し、 0— 9 0 ° 方向の非点収差ボケについては、 0 ° 方向の非点収差ボケが 増加する方向を正と し、 4 5— 135 ° 方向の非点収差ボケについては、 4 5 ° 方向の非点収差ボケが増加する方向を正とする。  The present invention has been made in view of such circumstances, and provides a method of correcting astigmatism in a charged particle beam optical system, a method of correcting astigmatism in a charged particle beam exposure apparatus, and a method of correcting astigmatism (astigmatism blur). It is an object of the present invention to provide a method of determining the correction sensitivity of the image and the sensitivity of occurrence of astigmatism blur), and an exposure method using the same. In this specification, the abstract and the claims, the astigmatism blur correction sensitivity refers to a current flowing through an astigmatism corrector for correcting a unit amount of astigmatism blur converted to a focal position. Value means the amount of change in the value or applied voltage. When correcting astigmatism blur in the 0-90 ° direction, the direction in which the astigmatism blur occurs in the 0 ° direction is defined as positive. — When correcting astigmatism blur in the 135 ° direction, the direction in which astigmatism blur occurs in the 45 ° direction shall be positive. In this specification and in the claims, astigmatism blur occurrence sensitivity refers to a focus that occurs when a current value or a voltage value applied to an astigmatism corrector is changed by a unit amount. This means the amount of astigmatism blur converted to the position.For astigmatism blur in the 0-90 ° direction, the direction in which astigmatism blur in the 0 ° direction increases is defined as positive, and in the direction of 45-135 ° Regarding the astigmatism blur, the direction in which the astigmatism blur in the 45 ° direction increases is defined as positive.
さらに、 本明細書、 及び請求の範囲において、 特に断らない限り、 「コ ィルにより」 とは、 コイル流す電流を調節することによることであり、 「電極により」 とは、 電極に印加する電圧を調整することによることは 言うまでもない。 前記目的を達成するための第 1の発明は、 非点収差補正器を有する荷 電粒子線露光装置において、 焦点位置を A hずらし、 前記非点収差補正 器の電流値又は電圧値を変化させることにより少なく とも異なる 2つの 焦線を形成する、 前記非点収差補正器の電流値又は電圧値を求め、 前記 焦点位置のずらし量 Δ h、 及び前記異なる 2組の焦線を形成する前記非 点収差補正器の電流値又は電圧値を用いて前記非点収差補正器の非点感 度 (非点収差ボケの補正感度、 又は非点収差ボケ発生感度) を求めるこ とを特徴とする非点感度の決定方法である。 Further, in this specification and the claims, unless otherwise specified, "by a coil" means that the current flowing through the coil is adjusted. It is needless to say that “by electrode” means that the voltage applied to the electrode is adjusted. A first invention for achieving the above object is a charged particle beam exposure apparatus having an astigmatism corrector, wherein a focus position is shifted by Ah to change a current value or a voltage value of the astigmatism corrector. Forming at least two different focal lines, obtaining a current value or a voltage value of the astigmatism corrector, shifting the focal position Δh, and calculating the two different sets of focal lines. The astigmatic sensitivity (correction sensitivity of astigmatism blur or astigmatism blur generation sensitivity) of the astigmatism corrector is obtained using a current value or a voltage value of the astigmatism corrector. This is a method for determining the point sensitivity.
本発明においては、 焦線が形成されるときの非点収差補正器の電流又 は電圧値に基づいて非点収差 正器の非点感度を求めているので、 簡単 な方法により、 非点収差補正器の非点感度を求めることができる。 前記目的を達成するための第 2の発明は、 前記第 1の発明であって、 前記非点収差補正器が少なく とも 2組のコイル群または電極群を有する ことを特徴とするものである。  In the present invention, since the astigmatism sensitivity of the astigmatism corrector is obtained based on the current or voltage value of the astigmatism corrector when the focal line is formed, the astigmatism can be obtained by a simple method. The astigmatic sensitivity of the corrector can be determined. A second invention for achieving the above object is the first invention, wherein the astigmatism corrector has at least two coil groups or electrode groups.
前記目的を達成するための第 3の発明は、 前記第 1の発明であって、 焦点位置を A hずらす際に、 正焦点位置を基準として、 焦点位置を正焦 点位置から△ hずらすことを特徴とするものである。  A third invention for achieving the above object is the first invention, wherein, when the focal position is shifted by Ah, the focal position is shifted by △ h from the normal focus position with respect to the normal focus position. It is characterized by the following.
本明細書、 及び請求の範囲で 「正焦点位置」 というのは、 投影レンズ で結像状態を変化させたときに、 光軸を中心とする最小錯乱円が形成さ れる結像面の光軸方向位置 (すなわち、 物面における光軸上の 1点から 出た荷電粒子が等方的に最も絞られる、結像面の光軸方向位置)をいう。 通常、 正焦点位置を求める方法としては、 物面の光軸上にピンホール を形成し、 結像面を光軸方向に移動させて、 たとえば、 X, Y方向走査 によってその方向のビームボケを見積も り、 それそれの方向でボケが最 小になる像面位置を見つけ、 その中点を正焦点位置とする方法が採用さ れている。 In this specification and claims, the term “positive focus position” refers to the optical axis of the image plane on which a minimum circle of confusion centered on the optical axis is formed when the imaging state is changed by the projection lens. Directional position (that is, the position of the imaging plane in the optical axis direction where charged particles emitted from one point on the optical axis on the object plane are most narrowed isotropically). Usually, the method of finding the positive focus position is to form a pinhole on the optical axis of the object surface and move the imaging plane in the optical axis direction. Is used to estimate the beam blur in that direction, find the image plane position that minimizes the blur in each direction, and use the midpoint as the focal point position.
本発明においては、 正焦点位置を基準にして焦点位置の移動量 Δ hを 定めているので、 後に実施の形態の欄で説明するように、 容易に非点感 度を求めることができる。  In the present invention, since the movement amount Δh of the focal position is determined based on the positive focal position, the astigmatic sensitivity can be easily obtained as described later in the section of the embodiment.
前記目的を達成するための第 4の発明は、 前記第 1の発明であって、 前記非点感度が、 非点収差ボケの補正感度であることを特徴とするもの である。  A fourth invention for achieving the above object is the first invention, wherein the astigmatism is a correction sensitivity for astigmatism blur.
前記目的を達成するための第 5の発明は、 前記第 1の発明であって、 前記非点感度が、 非点収差ボケ発生感度であることを特徴とするもので ある。  A fifth invention for achieving the above object is the first invention, wherein the astigmatism is an astigmatism blur occurrence sensitivity.
前記目的を達成するための第 6の発明は、 前記第 4の発明であって、 焦点位置を正焦点位置から A hだけずら した上で、 非点収差補正器を構 成する 2組のコイル群 ( 0 ° 方向コイル及び 4 5 ° 方向コイル) の電流 値又は 2組の電極群 ( 0 ° 方向電極及び 4 5 ° 方向電極) の電圧値をそ れそれ変化させ、 測定パターンを基準とした 9 0 ° 方向、 0 ° 方向、 1 3 5 ° 方向、 4 5 ° 方向のボケが最小となる前記 2組の電流値又は電圧 値をそれそれ求め、 これらの電流値又は電圧値の組み合わせをそれそれ ( S 1 1 , S 2 1 )、 ( S 1 2 , S 2 2 ) ( S 1 3 , S 2 3 )、 ( S 1 4 , S 2 4 ) とするとき、 次の少なく とも一つの式により、 少なく とも一つ の方向の非点収差ボケの補正感度を決定することを特徴とするものであ A sixth invention for achieving the above object is the fourth invention, wherein the focus position is shifted from the positive focus position by A h and then two sets of coils constituting an astigmatism corrector are provided. The current value of the group (0 ° direction coil and 45 ° direction coil) or the voltage value of the two electrode groups (0 ° direction electrode and 45 ° direction electrode) was changed, and the measurement pattern was used as a reference. 90 ° direction, 0 ° direction, 13.5 ° direction, and 45 ° direction, minimize the blur in each of the two sets of current values or voltage values, and calculate the combination of these current values or voltage values. If it is (S 1 1, S 2 1), (S 1 2, S 2 2) (S 13, S 2 3), (S 14, S 24), at least one of the following expressions Thus, the correction sensitivity of the astigmatism blur in at least one direction is determined.
0 ο 0 ο
(1)0 ° 方向コイル又は電極により、 0— 9 0 ° 方向の非点収差ボケを補 正する場合の非点収差ボケの補正感度 SI 1-512 (1) Sensitivity for correcting astigmatism blur when the 0 ° -90 ° direction astigmatism blur is corrected by a 0 ° direction coil or electrode SI 1-512
,·(1)  ,
2Ah  2Ah
(2)4 5 ° 方向コイル又は電極によ り、 0— 9 0 ° 方向の非点収差ボケ を補正する場合の非点収差ボケの補正感度  (2) Sensitivity for correcting astigmatism blur when correcting astigmatism blur in the 0-90 ° direction using a 45 ° direction coil or electrode
521-522 ^  521-522 ^
."(2)  . "(2)
2Ah )  2Ah)
(3)0 ° 方向コイル又は電極により、 4 5— 135° 方向の非点収差ボケを 補正する場合の非点収差ボケの補正感度 13- 14 .-.(3) The (3) 0 ° direction coils or electrodes, the correction sensitivity of astigmatism blur when correcting astigmatism blur of 4 5-135 ° direction 1 3 -. 14 .- (3)
2Δ/ι } 2Δ / ι }
(4)4 5 ° 方向コイル又は電極により、 4 5 — 135° 方向の非点収差ボケ を補正する場合の非点収差ボケの補正感度  (4) Sensitivity of astigmatism blur correction when astigmatism blur in the direction of 45-135 ° is corrected by a 45 ° direction coil or electrode
523-524  523-524
-^r -(4) -^ r- (4)
ただし、 S i j ( i = l , 2 j = l 4 ) の iは、 それそれ 0 ° 方 向コイル又は電極 ( i = 1 )、 4 5 ° 方向コイル又は電極 ( i = 2 ) を示 し、 jは、 それそれ非点収差ボケが最小となる方向 ( j = 1は 9 0 ° 方 向、 《]' = 2は 0 ° 方向、 j = 3は 1 3 5 ° 方向、 j = 4は 4 5。 方向) を示す。  Where i in S ij (i = l, 2 j = l 4) indicates a 0 ° direction coil or electrode (i = 1) and a 45 ° direction coil or electrode (i = 2), respectively. j is the direction that minimizes astigmatism blur (j = 1 is 90 ° direction, «] '= 2 is 0 ° direction, j = 3 is 1 35 ° direction, j = 4 is 4 5. Direction)
本明細書及び請求の範囲において、 測定パターンを基準とした 0 ° 方 向とは、 測定パターンが置かれる基準方向のことであり、 多くの場合荷 電粒子線露光装置のシステムの基準方向として定められたものと一致す る。  In this specification and the appended claims, the 0 ° direction with respect to the measurement pattern refers to the reference direction in which the measurement pattern is placed, and is often defined as the reference direction of the charged particle beam exposure system. Matches what was given.
前記目的を達成するための第 7の発明は、 前記第 4の発明であって、 非点収差補正器を構成する 2組のコイル群 ( 0 ° 方向コイル及び 4 5 ° 方向コィル) の電流値又は 2組の電極群 ( 0 ° 方向電極及び 4 5 ° 方向 電極) の電圧値をそれそれ変化させ、 測定パターンを基準とした 9 0 ° 方向、 0 ° 方向、 1 3 5 ° 方向、 4 5 ° 方向のボケが最小となる前記 2 組の電流値又は電圧値をそれそれ求め、 これを、 光軸方向の任意の位置 Aと Aから光軸方向に△ hだけ離れた位置 Bにおいて行い、 A seventh invention for achieving the above object is the fourth invention, wherein a current value of two coil groups (0 ° direction coil and 45 ° direction coil) constituting an astigmatism corrector is provided. Or, change the voltage values of the two electrode groups (0 ° direction electrode and 45 ° direction electrode) to 90 ° direction, 0 ° direction, 135 ° direction, 45 ° direction based on the measurement pattern. 2) where the blur in the ° direction is minimized. A current value or a voltage value of the set is determined respectively, and this is performed at arbitrary positions A and A in the optical axis direction at a position B which is separated by Ah in the optical axis direction from
これらの電流値の組み合わせをそれそれ ( S 1 1 A, S 2 1 A;)、 ( S 1 2 A, S 2 2 A) ( S 1 3 A, S 2 3 A) ( S 1 4 A, S 2 4 A)、 ( S 1 1 B, S 2 1 B)、 ( S 1 2 B, S 2 2 B)S ( S 1 3 B, S 2 3 B) ( S 1 4 B , S 2 4 B ) とするとき、 次の少なく とも一つの式により、 少な く とも一つの方向の非点収差ボケの補正感度を決定することを特徴とす るものである。 The combination of these current values is (S11A, S21A;), (S12A, S22A) (S13A, S23A) (S14A, (S24A), (S11B, S21B), (S12B, S22B) S (S13B, S23B) (S14B, S24) In the case of B), the correction sensitivity for astigmatism blur in at least one direction is determined by at least one of the following expressions.
(1)0 ° 方向コイル又は電極により、 0— 9 0 ° 方向の非点収差ボケを補 正する場合の非点収差ボケの補正感度  (1) Sensitivity for correcting astigmatism blur when the 0 ° -90 ° direction astigmatism blur is corrected by a 0 ° direction coil or electrode
511,- 12, 11^- 12^ )  511,-12, 11 ^-12 ^)
、 2Δ/ι 2Δ/ι 、 ) , 2Δ / ι 2Δ / ι,)
(2) 4 5。 方向コイル又は電極により、 0— 9 0 ° 方向の非点収差ボケを 補正する場合の非点収差ボケの補正感度  (2) 4 5. Correction sensitivity of astigmatism blur when correcting astigmatism blur in the 0 to 90 ° direction using a directional coil or electrode
S21B-S22B _S21A-S22A ) (S21 B -S22 B _S21 A -S22 A )
V 2Ah 2Ah 、 ) V 2Ah 2Ah,)
(3) 0 ° 方向コィル又は電極により、 4 5— 135° 方向の非点収差ボケを 補正する場合の非点収差ボケの補正感度  (3) Sensitivity of astigmatism blur when correcting astigmatism blur in the 45-135 ° direction using a 0 ° direction coil or electrode
S13,-S14. _513,-S14, ) S13, -S14._513, -S14, )
K 2Ah 2Ah ) K 2Ah 2Ah)
(4) 4 5 ° 方向コイル又は電極により、 4 5— 135° 方向の非点収差ボケ を補正する場合の非点収差ボケの補正感度  (4) Sensitivity of astigmatism blur when 45-135 ° direction astigmatism blur is corrected by 45 ° direction coil or electrode
S23c-S24 ΤΒ„ _ S23„ -S24, S23 c -S24 Τ Β „_ S23„ -S24,
) -(8)  )-(8)
\ 2Ah 2Ah  \ 2Ah 2Ah
ただし、 S i j A、 S i j B ( i = l, 2、 j = l〜4) の iは、 そ れそれ 0 ° 方向コィル又は電極( i = l )、 4 5 ° 方向コィル又は電極( i Here, i of SijA and SijB (i = l, 2, j = l to 4) are 0 ° direction coil or electrode (i = l), 45 ° direction coil or electrode (i
= 2 ) を示し、 jは、 それそれ非点収差ボケが最小となる方向 ( j = l は 9 0 ° 方向、 | = 2は 0 ° 方向、 j = 3は 1 3 5 ° 方向、 j = 4は 4 5 ° 方向) を示す。 = 2), where j is the direction in which astigmatism blur is minimized (j = l is the 90 ° direction, | = 2 is the 0 ° direction, j = 3 is the 1 35 ° direction, j = 4 is 4 5 ° direction).
前記目的を達成するための第 8の発明は、 前記第 5の発明であって、 焦点位置を正焦点から A hだけずらした上で、 非点収差補正器を構成す る 2組のコィル群 ( 0 ° 方向コィル及び 4 5 ° 方向コイル) の電流値又 は 2組の電極群 (◦。 方向電極及び 4 5 ° 方向電極) の電圧値をそれそ れ変化させ、測定パターンを基準とした 9 0 ° 方向、 0 ° 方向、 1 3 5 ° 方向、 4 5 ° 方向のボケが最小となる前記 2組の電流値又は電圧値をそ れそれ求め、 これらの電流値又は電圧値の組み合わせをそれそれ ( S 1 An eighth invention for achieving the object is the fifth invention, wherein the focus position is shifted from the right focus by Ah, and then two sets of coils forming an astigmatism corrector are provided. (0 ° direction coil and 45 ° direction coil) or the voltage value of two sets of electrodes (◦. Direction electrode and 45 ° direction electrode) were changed, and the measured pattern was used as a reference. 90 ° direction, 0 ° direction, 135 ° direction, and 45 ° direction, minimize the blur in each of the above two sets of current values or voltage values, and calculate the combination of these current values or voltage values. That it (S1
1 , S 2 1 )、 ( S 1 2 , S 2 2 )、 ( S 1 3 , S 2 3 )、 ( S 1 4 , S 2 4 ) とするとき、 次の少なく とも一つの式により、 少なく とも一つの方向の 非点収差ボケの発生感度を決定することを特徴とするものである。 1, S 2 1), (S 12, S 2 2), (S 13, S 23), (S 14, S 24) Both are characterized in that the sensitivity of occurrence of astigmatism blur in one direction is determined.
(1) 0 ° 方向コイル又は電極により、 0— 9 0 ° 方向の非点収差ボケを発 生させる非点収差ボケの発生感度
Figure imgf000010_0001
(1) Sensitivity of astigmatism blur that causes astigmatism blur in the 0-90 ° direction by the 0 ° direction coil or electrode
Figure imgf000010_0001
- S12)(S23 - 24) - (S13 - S14XS21 - S22)} 、)  -S12) (S23-24)-(S13-S14XS21-S22)},)
(2) 4 5 ° 方向コイル又は電極により、 0 ° — 9 0 ° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度 -2Ah(S13-SU) … (2) Sensitivity of astigmatism blur that generates astigmatism blur in the 0 ° to 90 ° direction by using a 45 ° direction coil or electrode -2Ah (S13-SU)…
{(511-512XS23 - 24) -(513 -514)(521 -522)} 1 , {(511-512XS23-24)-(513 -514) (521 -522)} 1 ,
(3) 0 ° 方向コイル又は電極により、 4 5 ° — 135° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度 -2Ah(S21-S22) (3) Sensitivity of astigmatism blur which generates astigmatism blur in 45 ° -135 ° direction by 0 ° direction coil or electrode -2Ah (S21-S22)
{(S11- S12)(S23 - 24) - (S13 - S14)(S21 - S22)}  {(S11- S12) (S23-24)-(S13-S14) (S21-S22)}
(4)4 5 ° 方向コィル又は電極により、 4 5 ° ― 135° 方向の非点収差ボ ケを発生させる非点収差ボケの発生感度 2Δ/ι(511-512) ...(12) (4) Sensitivity of occurrence of astigmatism blur that causes astigmatism blur in the direction of 45 ° to 135 ° using a 45 ° direction coil or electrode 2Δ / ι (511-512) ... (12)
{(511- 512)(S23一 24)一 (513 - 514)(521 - 522)} 前記目的を達成するための第 9の発明は、 前記第 5の発明であって、 非点収差補正器を構成する 2組のコイル群 ( 0 ° 方向コイル及び 4 5 ° 方向コィル) の電流値又は 2組の電極群 ( 0。 方向電極及び 4 5 ° 方向 電極) の電圧値をそれそれ変化させ、 測定パターンを基準とした 9 0 ° 方向、 0 ° 方向、 1 3 5 ° 方向、 4 5 ° 方向のボケが最小となる前記 2 組の電流値又は電圧値をそれそれ求め、 これを、 光軸方向の任意の位置 Aと Aから光軸方向に△ hだけ離れた位置 Bにおいて行い、 {(511-512) (S23-24) 1-1 (513-514) (521-522)} A ninth invention for achieving the above object is the fifth invention, wherein an astigmatism corrector is provided. The current value of the two coil groups (0 ° direction coil and 45 ° direction coil) or the voltage value of the two electrode groups (0. direction electrode and 45 ° direction electrode), The two sets of current or voltage values that minimize the blur in the 90 ° direction, 0 ° direction, 135 ° direction, and 45 ° direction based on the measurement pattern are determined, and this is calculated as the optical axis. At any position A in the direction and at position B that is △ h away from the
これらの電流値の組み合わせをそれぞれ ( S 1 1 A, S 2 1 A)、 ( S 1 2 A, S 2 2 A)ヽ ( S 1 3 A , S 2 3 A)ヽ ( S 1 4 A, S 2 4 A)ヽ ( S 1 1 B , S 2 1 B)、 ( S 1 2 B, S 2 2 B)、 ( S 1 3 B , S 2 3 B)、 ( S 1 4 B, S 24 B ) とするとき、 次の少なく とも一つの式により、 少な く とも一つの方向の非点収差ボケの発生感度を決定することを特徴とす るものである。 The combination of these current values is (S11A, S21A), (S12A, S22A) ヽ (S13A, S23A) ヽ (S14A, (S24A) ヽ (S11B, S21B), (S12B, S22B), (S13B, S23B), (S14B, S24 In the case of B), the sensitivity of occurrence of astigmatism blur in at least one direction is determined by at least one of the following expressions.
(1)0 ° 方向コイル又は電極により、 0— 9 0 ° 方向の非点収差ボケを発 生させる非点収差ボケの発生感度 (1) Sensitivity of astigmatism blur that causes 0-90 ° direction astigmatism blur by a 0 ° direction coil or electrode
2AA{(S23,-S24j?)-(S23/t-S24J} …( 2AA {(S23, -S24 j? )-(S23 / t -S24J}… (
Δ  Δ
(2) 4 5 ° 方向コイル又は電極により、 0。 — 9 0 ° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度  (2) 0 by the 45 ° direction coil or electrode. — Sensitivity of astigmatism blur which causes astigmatism blur in 90 ° direction
-2AA{(S13g-S14B)-(S13,-S14 } -2AA {(S13 g -S14 B )-(S13, -S14}
Δ 、 )  Δ,)
(3) 0 ° 方向コィル又は電極により、 4 5 ° _ 135° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度  (3) Sensitivity of astigmatism blur that causes astigmatism blur in the 45 ° -135 ° direction by the 0 ° direction coil or electrode
-2^hj(S21B-S22B)-{S21A-S22A)} … ) -2 ^ hj (S21 B -S22 B )-{S21 A -S22 A )}…)
Δ  Δ
(4) 4 5 ° 方向コィル又は電極により、 4 5 ° — 135° 方向の非点収差ボ ケを発生させる非点収差ボケの発生感度 (4) 45 ° -135 ° astigmatism by 45 ° direction coil or electrode. Sensitivity of astigmatism blur causing blur
2A (^llg-^12g)-(Sll/4 -S12,)} … 2A (^ ll g- ^ 12 g )-(Sll / 4 -S12,)}…
Δ ^  Δ ^
ただし、 S i j A、 S i j B ( i = 1 , 2、 j = 1 ~ 4 ) の iは、 そ れそれ 0 ° 方向コイル又は電極( i = 1 )、 4 5 ° 方向コイル又は電極( i = 2 ) を示し、 jは、 それそれ非点収差ボケが最小になる方向 ( j = l は 9 0。 方向、 <]' = 2は 0 ° 方向、 j = 3は 1 3 5 ° 方向、 j = 4は 4Where i of S ij A and S ij B (i = 1, 2, j = 1 to 4) are 0 ° direction coil or electrode (i = 1) and 45 ° direction coil or electrode (i = 2), where j is the direction in which astigmatism blur is minimized (j = l is 90. direction, < ] '= 2 is 0 ° direction, j = 3 is 135 ° direction, j = 4 is 4
5 ° 方向) を示し、 △は、 5 ° direction), and △ indicates
A = [{(S11B -S12B)-(S11A -S12A)}{(S23B-S24B)-(S23A-S24A)} ~{(S13B -SUB)-(S13A -SUA)}{(S21B -S22B)-(S21A -522,)}]で 示される値である。 A = [{(S11 B -S12 B )-(S11 A -S12 A )} {(S23 B -S24 B )-(S23 A -S24 A )} ~ {(S13 B -SU B )-(S13 A -SU A )} {((S21 B -S22 B )-(S21 A -522,)}].
前記目的を達成するための第 1 0の発明は、前記第 5の発明であって、 焦点位置を正焦点位置から△ hだけずら した上で、 前記非点収差補正器 を構成する 2組のコイル群 ( 0 ° 方向コイル及び 4 5 ° 方向コイル) の 電流値又は 2組の電極群 ( 0 ° 方向電極及び 4 5 ° 方向電極) の電圧値 (それそれを S l, S 2 とする) をそれぞれ変化させ、 角度が 0だけ異 なる 2つの方向のボケが最小となる前記 2組のコイル群の電流値又は 2 組の電極群の電圧値をそれそれ求め、 これらの電流値又は電圧値の組み 合わせをそれそれ ( S 1 5 , S 2 5 )、 ( S 1 6, S 2 6 ) とし、 S 1 — S 2'直交座標系において、 下に示す ( S 1。 , S 2。 ) を中心とし、 ( S 1 5 , S 2 5 )、 ( S 1 6, S 2 6 ) を通る円を求め、 この円を、 焦線を 形成する前記 2組の電流値又は電圧値の組み合わせを表す円とし、 この 円の所定の点における、 非点収差ボケが最小となる方向に基づいて、 少 なく とも一つの方向の非点収差ボケの発生感度を決定することを特徴と するものである。 51 {(515 + S16) ± (525 -526) cot Θ} … S2 {(S25 + S26) + (515 - S16) cot Θ} … 前記目的を達成するための第 1 1の発明は、前記第 5の発明であって、 焦点位置を正焦点位置から Δ hだけずら した上で、 前記非点収差補正器 を構成する 2組のコィル群 ( 0 ° 方向コイル及び 4 5 ° 方向コイル) の 電流値又は 2組の電極群 ( 0 ° 方向電極及び 4 5 ° 方向電極) の電圧値A tenth invention for achieving the above-mentioned object is the fifth invention, wherein the astigmatism corrector is configured such that the focus position is shifted from the right focus position by △ h, and Current value of coil group (0 ° direction coil and 45 ° direction coil) or voltage value of two sets of electrodes (0 ° direction electrode and 45 ° direction electrode) (S1 and S2 respectively) The current values of the two coil groups or the voltage values of the two electrode groups that minimize the blur in the two directions at which the angles differ by 0 are respectively obtained, and these current values or voltage values are obtained. Are defined as (S 15, S 25) and (S 16, S 26), respectively, and are shown below in the S 1 — S 2 ′ rectangular coordinate system (S 1, S 2.) , A circle passing through (S 15, S 25) and (S 16, S 26) is determined, and this circle is defined as the current or voltage value of the two sets of current values or voltage values forming a focal line. A circle representing astigmatism, wherein the sensitivity of occurrence of astigmatism blur in at least one direction is determined based on a direction in which the astigmatism blur is minimized at a predetermined point on the circle. Things. 51 {(515 + S16) ± (525-526) cot Θ}… S 2 {(S25 + S26) + (515-S16) cot Θ}… The first invention for achieving the above object is the above-mentioned invention. A fifth invention, in which, after shifting the focal position from the positive focal position by Δh, two sets of coils (0 ° direction coil and 45 ° direction coil) constituting the astigmatism corrector Current value or voltage value of two electrode groups (0 ° direction electrode and 45 ° direction electrode)
(それそれを S l, S 2とする) をそれぞれ変化させ、 角度が 6>だけ異 なる 2つの方向のボケが最小となる前記 2組のコイル群の電流値又は 2 組の電極群の電圧値をそれそれ求め、 これらの電流値又は電圧値の組み 合わせをそれぞれ ( S 1 5, S 2 5 )、 ( S 1 6 , S 2 6 ) とし、 S I— S 2直交座標系において、 下に示す ( S l。 , S 2。 ) を中心とし、 ( S(They are S 1 and S 2), respectively, and the angles differ by 6> The current value of the two sets of coils or the voltage of the two sets of electrodes that minimize the blur in the two directions The values of the current and voltage values are defined as (S15, S25) and (S16, S26), respectively. (Sl., S2.)
1 5 , S 2 5 )、 ( S 1 6 , S 2 6 ) を通る円上において、 パターン基準 方向に対して 9 0 ° 方向、 135° 方向の非点収差ボケが最小となる前記15, S 25), and (S 16, S 26) on a circle passing through, the astigmatism blur in the 90 ° direction and 135 ° direction with respect to the pattern reference direction is minimized.
2組の電流値又は電圧値をそれそれ求め、 それそれの組み合わせを ( SObtain two sets of current or voltage values, and determine the combination of each (S
1 1,, S 2 1,)、 ( S 1 3,, S 2 3,) とするとき、 次の ( 1 9 ) ~ ( 2 2 ) 式の少なく とも一つにより、 少なく とも一つの方向の非点収差ボケ の発生感度を決定することを特徴とするものである。 1 1, S 2 1) and (S 1 3, S 2 3), at least one of the following equations (1 9) to (2 2) It is characterized by determining the sensitivity of occurrence of astigmatism blur.
{(515 + 516) ± (525 - 26)cot Θ} …  {(515 + 516) ± (525-26) cot Θ}…
S2 {(^25 + 526) + (515 -516) cot 6>} …( ) S2 {(^ 25 + 526) + (515 -516) cot 6>}… ()
(1) )0 ° 方向コイル又は電極により、◦一 9 0 ° 方向の非点収差ボケを発 生させる非点収差ボケの発生感度 (1)) Sensitivity of astigmatism blur which generates astigmatism blur in 90 ° direction by 0 ° direction coil or electrode
AA(S23*-S20) AA (S23 * -S2 0 )
—(19)  — (19)
{ (SI 1 '- Sl0 )(S 23 '- S 2n ) - (S13 '- S 10 )(S 2Γ- S 20 )} ' {(SI 1 '- Sl 0 ) (S 23' - S 2 n) - (S13 '- S 1 0) (S 2Γ- S 2 0)}'
(2) 4 5 ° 方向コイル又は電極により、 ◦ ° — 9 0 ° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度 (2) Astigmatism blur in the ◦ ° — 90 ° direction due to the 45 ° direction coil or electrode Sensitivity of Astigmatism Blurring that Generates
-ΔΛ(513'-510) -ΔΛ (513'-51 0 )
{(Sir-S10)(S23,-S20)-(S13'-S10)(S21,-S20)} 、 ) {(Sir-S1 0 ) (S23 , -S2 0 )-(S13'-S1 0 ) (S21 , -S2 0 )},)
(3) 0 ° 方向コイル又は電極により、 4 5 ° — 135° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度  (3) Sensitivity of astigmatism blur that generates astigmatism blur in 45 ° -135 ° direction by 0 ° direction coil or electrode
- (S21'-S20) -(S21'-S2 0 )
{{S1Y- 510)(S 23 '- S 20) - (S13 S10)(S 21 '- S 20)} ) {{S1Y- 51 0) (S 23 '- S 2 0) - (S13 S1 0) (S 21' - S 2 0)})
(4) 4 5 ° 方向コィル又は電極により、 4 5 ° — 135° 方向の非点収差ボ ケを発生させる非点収差ボケの発生感度  (4) Sensitivity of astigmatism blur that generates astigmatism blur in the direction of 45 ° -135 ° using a 45 ° direction coil or electrode
{(S11,-S10XS23,-S20)-(S13'-S10)(S21,-S20)} ) {(S11 , -S1 0 XS23 , -S2 0 )-(S13'-S1 0 ) (S21 , -S2 0 )})
前記目的を達成するための第 1 2の発明は、前記第 5の発明であって、 焦点位置を正焦点位置から△ hだけずらした上で、 前記非点収差補正器 を構成する 2組のコィル群 ( 0 ° 方向コイル及び 4 5 ° 方向コイル) の 電流値又は 2組の電極群 ( 0 ° 方向電極及び 4 5 ° 方向電極) の電圧値 をそれそれ変化させ、 角度が異なる 3つ以上の方向の非点収差ボケが最 小となる前記 2組のコイル群 ( 0 ° 方向コイル及び 4 5 ° 方向コイル) の電流値又は 2組の電極群 ( 0 ° 方向電極及び 4 5 ° 方向電極) の電圧 値 (それそれを S l, S 2 とする) をそれぞれ求め、 これらの電流値又 は電圧値の組み合わせをそれそれ( S 1 1,S 2 1 )、 ( S 1 2,S 2 2 )、 ···、 ( S i n, S 2 n) とするとき (nは 3以上の整数)、 S 1— S 2直 交座標系において、 これらの点を通る円を、 方程式を解くか又は統計的 な当てはめ法により求め、 この円の所定の点における、 非点収差ボケが 最小となる方向に基づいて、 少なく とも一つの方向の非点収差ボケの発 生感度を決定することを特徴とするものである。 なお、 本発明において 使用する ( S i n, S 2 n) の符号は、 他の発明における符号と重複す るものがあるが、 両者の間には関係のないことは言うまでもない。 これ は、 本発明に対応する請求項についても同じである。 A twelfth invention for achieving the above object is the fifth invention, wherein the astigmatism corrector is configured such that the focal position is shifted from the positive focal position by △ h, and The current value of the coil group (0 ° direction coil and 45 ° direction coil) or the voltage value of two sets of electrodes (0 ° direction electrode and 45 ° direction electrode) are changed, and three or more with different angles The current value of the two sets of coils (0 ° direction coil and 45 ° direction coil) or the two sets of electrodes (0 ° direction electrode and 45 ° direction electrode) that minimize astigmatism blur in the direction ) Are calculated (S1 and S2), and the combination of these current or voltage values is calculated as (S11, S21), (S12, S2). 2), ..., (S in, S 2 n) (n is an integer of 3 or more), these points pass through in the S1-S2 Cartesian coordinate system. Is determined by solving an equation or by a statistical fitting method. Based on the direction in which the astigmatism blur is minimized at a given point on the circle, the generation of the astigmatism blur in at least one direction is determined. It is characterized by determining the raw sensitivity. The sign of (S in, S 2 n) used in the present invention may overlap with the sign of other inventions, but it goes without saying that there is no relation between the two. this The same applies to the claims corresponding to the present invention.
前記目的を達成するための第 1 3の発明は、前記第 5の発明であって、 焦点位置を正焦点位置から A hだけずらした上で、 前記非点収差補正器 を構成する 2組のコイル群 ( 0 ° 方向コイル及び 4 5 ° 方向コイル) の 電流値又は 2組の電極群 ( 0 ° 方向電極及び 4 5 ° 方向電極) の電圧値 をそれそれ変化させ、 角度が異なる 3つ以上の方向の非点収差ボケが最 小となる前記 2組のコイル群 ( 0 ° 方向コイル及び 4 5 ° 方向コイル) の電流値又は 2組の電極群 ( 0 ° 方向電極及び 4 5 ° 方向電極) の電圧 値を (それそれを S l, S 2とする) それそれ求め、 これらの電流値又 は電圧値の組み合わせをそれそれ( S 1 1, S 2 1 )、 (S 1 2, S 2 2 )、 ···、 ( S i n, S 2 n) とするとき (nは 3以上の整数)、 S I— S 2直 交座標系において、 これらの点を通る円を、 方程式を解くか又は統計的 な当てはめ法により求め、 その中心を ( S 1。 , S 2。 ) とし、' その円 上において、 パターン基準方向に対して 9 0 ° 方向、 135° 方向の非点 収差ボケが最小となる前記 2組の電流値又は電圧値をそれそれ求め、 そ れそれの組み合わせを ( S l l,, S 2 1 ')、 ( S 1 3,, S 2 3 ') とす るとき、 次の ( 1 9 ) 〜 ( 2 2 ) 式の少なく とも一つにより、 少なく と も一つの方向の非点収差ボケの発生感度を決定することを特徴とするも のである。  A thirteenth invention for achieving the above object is the fifth invention, wherein the focus position is shifted from the positive focus position by Ah, and the astigmatism corrector is constituted by two sets. The current value of the coil group (0 ° direction coil and 45 ° direction coil) or the voltage value of two sets of electrodes (0 ° direction electrode and 45 ° direction electrode) is changed, and three or more angles are different. The current value of the two sets of coils (0 ° direction coil and 45 ° direction coil) or the two sets of electrodes (0 ° direction electrode and 45 ° direction electrode) that minimize astigmatism blur in the direction ) (S1 and S2), and the combination of these current values or voltage values is (S11, S21), (S12, S12) 2 2), ..., (S in, S 2 n) (n is an integer of 3 or more), these points pass through in the SI-S 2 orthogonal coordinate system. A circle is determined by solving an equation or by statistical fitting, and its center is set to (S1, S2,), and '90 ° and 135 ° directions on the circle with respect to the pattern reference direction. The two sets of current values or voltage values that minimize the astigmatism blur of each of them are determined, and the combination of the two values is (Sll ,, S21 '), (S13, S23'). ), At least one of the following equations (19) to (22) is used to determine the sensitivity of occurrence of astigmatism blur in at least one direction. .
なお、 本発明において使用する ( S 1 n, S 2 n) の符号は、 他の発 明における符号と重複するものがあるが、 両者の間には関係のないこと は言うまでもない。 これは、 本発明に対応する請求項についても同じで のる。  The sign of (S 1 n, S 2 n) used in the present invention may overlap with the sign of other inventions, but it goes without saying that there is no relationship between the two. This applies to the claims corresponding to the present invention.
(1)0 ° 方向コイル又は電極により、 0 _ 9 0 ° 方向の非点収差ボケを発 生させる非点収差ボケの発生感度 A (S23'-S20) … (1) Sensitivity of astigmatic blur that causes astigmatic blur in the 0 to 90 ° direction by a 0 ° direction coil or electrode A (S23'-S2 0 )…
{(5ir-Sl0)(523'-S20) - (S13'-S10)(S 2Γ-520)} {(5ir-Sl 0 ) (523'-S2 0 )-(S13'-S1 0 ) (S 2Γ-52 0 )}
(2)4 5 ° 方向コイル又は電極により、 0 ° — 9 0 ° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度  (2) Sensitivity of astigmatism blur that causes astigmatism blur in the 0 ° to 90 ° direction by using a 45 ° direction coil or electrode
- (513·-510) -(513-51 0 )
{(S1V- S1Q)(S 23 '- S 20) - (513 '- Slo)(S 21'-S 20)} ) {(S1V- S1 Q) (S 23 '- S 2 0) - (513' - Slo) (S 21'-S 2 0)})
(3)0 ° 方向コイル又は電極により、 4 5 ° — 135° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度 (3) Sensitivity of astigmatism blur that generates astigmatism blur in 45 ° -135 ° direction by 0 ° direction coil or electrode
- (S21'-520) … -(S21'-52 0 )…
{ (SI 1 '- Sl0 )(S 23 '- S 20 ) - (S 13 '- S 10 )(521 '- S 20 )} ) {(SI 1 '-Sl 0 ) (S 23'-S 2 0 )-(S 13 '-S 1 0 ) (521'-S 2 0 )})
(4)4 5 ° 方向コィル又は電極により、 4 5 ° — 135° 方向の非点収差ボ ケを発生させる非点収差ボケの発生感度 (S11'-S10) (4) 4 5 ° direction Koiru or electrode, 4 5 ° - 135 ° direction generation sensitivity astigmatism blur to generate astigmatism Bo Ke (S11 '-S1 0)
-(22)  -(twenty two)
{ (511 '- Sl0 )(S 23 S 20 ) - (SI 3 '- S 10 )(S 21 '- S 20 )} 、 ) 前記目的を達成するための第 1 4の発明は、前記第 5の発明であって、 焦点位置 hを複数変化させ (各光軸方向位置を h i ( i = l〜n ) とす る)、 かつ、 前記非点収差補正器を構成する 2組のコイル群 ( 0 °方向コ ィル及び 4 5 °方向コイル) の電流値又は 2組の電極群 ( 0 °方向電極及 び 4 5。方向電極) の電圧値、 (それそれを S I , S 2 とする)、 をそれそ れ変化させ、 そのときの非点収差ボケパターンの角度を t iとし、 これ らのデ一夕から、 統計的手法により、 ( h— h。) が単位量変化するとき ( h。は正焦点が形成される焦点位置) の、 焦線を形成する点 ( S 1 , S 2 ) の組が S 1 - S 2直交座標平面で形成する円の半径の変化量を示 す比例定数 rと、 S 1軸に対する、 0°方向ボケだけが変化する方向のな す角 2 t。を決定し、 これらのデ一夕から、 次の ( 2 3 ) 〜 ( 2 6 ) 式 により、 少なく とも一つの方向の非点収差ボケの発生感度を決定するこ とを特徴七するものである。 (1) 0 ° 方向コイル又は電極により、 0 — 9 0 ° 方向の非点収差ボケを発 生させる非点収差ボケの発生感度 {(511 '- Sl 0) (S 23 S 2 0) - (SI 3' - S 1 0) (S 21 '- S 2 0)},) the invention of the first 4 to achieve the above object In the fifth aspect, two sets of changing the focal position h (where each optical axis direction position is hi (i = l to n)), and configuring the astigmatism corrector Current value of coil group (0 ° direction coil and 45 ° direction coil) or voltage value of two sets of electrode group (0 ° direction electrode and 45. direction electrode) (SI, S 2), and are respectively changed. The angle of the astigmatism blur pattern at that time is denoted by ti. From these data, (h−h.) Changes by a unit amount by a statistical method. When (h. Is the focal position where the positive focus is formed), the set of points (S 1, S 2) forming the focal line indicates the amount of change in the radius of the circle formed by the S 1-S 2 rectangular coordinate plane. The proportional constant r shown and only the 0 ° direction blur with respect to the S1 axis Change direction of such to the corner 2 t. And determining the sensitivity of occurrence of astigmatism blur in at least one direction according to the following equations (23) to (26). . (1) Sensitivity of astigmatism blur that causes astigmatism blur in the direction of 0 to 90 ° by a 0 ° direction coil or electrode
cos(2t0)/r -(23) cos (2t 0 ) / r-(23)
(2) 4 5 ° 方向コイル又は電極により、 0 ° — 9 0 ° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度  (2) Sensitivity of astigmatism blur that generates astigmatism blur in the 0 ° to 90 ° direction by a 45 ° direction coil or electrode
sin(2t0)/r -(24) sin (2t 0 ) / r-(24)
(3) 0 ° 方向コィル又は電極により、 4 5 ° — 135° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度  (3) Sensitivity of astigmatism blur that causes astigmatism blur in 45 ° -135 ° direction by 0 ° direction coil or electrode
-sin(2t0)/r -(25) -sin (2t 0 ) / r-(25)
(4) 4 5 ° 方向コイル又は電極により、 4 5 ° — 135° 方向の非点収差ボ ケを発生させる非点収差ボケの発生感度  (4) Sensitivity of astigmatism blur that generates astigmatism blur in the direction of 45 ° to 135 ° using a coil or electrode in the direction of 45 °
cos(2t0)/r —(26) cos (2t 0 ) / r — (26)
前記目的を達成するための第 1 5の発明は、前記第 1 4の発明であって、 前記統計的手法が、前記焦線となる点が作る円の中心点( S 1 。, S 2。)、 正焦点位置 h。、 比例定数 r、 S I軸に対する、 0 ° 方向ボケだけが変 化する方向のなす角 2 t 。を変数として、 以下の評価関数が Pが最小と なるように、 これらの変数を求めることにより、 前記 r と t Dを求める 手法であることを特徴とするものである。 A fifteenth invention for achieving the above object is the fourteenth invention, wherein the statistical method uses a center point (S 1, S 2) of a circle formed by the focal point. ), Positive focus position h. , The proportionality constant r, and the angle 2t between the direction in which only the 0 ° direction blur changes with respect to the SI axis. Is a method of obtaining the above r and t D by obtaining these variables so that the following evaluation function minimizes P with the following as variables.
([ -SI。- r( - /¾)C0S{2ft+i。)} ([-SI.-R (-/ ¾) C0S { 2 ft + i.)}
-[52,-520-^ -/i0)sin{2ft "。)}] -(27) 前記目的を達成するための第 1 6の発明は、 荷電粒子線露光装置にお いて、 レチクルの像をウェハ上に露光転写する方法であって、 前記第 1 の発明から第 1 5の発明のうちいずれかの荷電粒子線露光装置における 非点感度の決定方法により決定した非点収差ボケの補正感度又は非点収 差ボケの発生感度を使用して、 サブフィールド毎に非点収差ボケを修正 するように非点収差補正器を調整しながら露光転写を行うことを特徴と する荷電粒子線露光装置における露光方法である。 -[52, -52 0 -^-/ i 0 ) sin {2ft ".)}]-(27) A sixteenth invention for achieving the above object is a charged particle beam exposure apparatus, comprising: a reticle; A method for exposing and transferring the image of the astigmatism onto a wafer, wherein the astigmatism blur determined by the method for determining astigmatism sensitivity in the charged particle beam exposure apparatus according to any one of the first to fifteenth inventions. Exposure transfer is performed while adjusting the astigmatism corrector so as to correct astigmatism blur for each subfield using the correction sensitivity or the sensitivity of occurrence of astigmatism blur. This is an exposure method in a charged particle beam exposure apparatus.
前記課題を解決するための第 1 7の発明は、 前記第 1 6の手段であつ て、 前記非点収差補正器が 2組のコイル群 ( 0 ° 方向コイル及び 4 5 ° 方向コイル) または 2組の電極群 ( 0 ° 方向電極及び 4 5 ° 方向電極) を有し、 補正すべき非点収差ボケ量△ h0, A h45に対して、 前記 2組 のコイル群の電流値又は前記 2組の電極群の電圧値 ΔΙ。、 ΔΙ45を以下 の式により求めることを特徴とするものである。
Figure imgf000018_0001
A seventeenth invention for solving the above-mentioned problems is the sixteenth means, wherein the astigmatism corrector includes two coil groups (a 0 ° direction coil and a 45 ° direction coil) or 2 A set of electrode groups (0 ° direction electrode and 45 ° direction electrode), and for the astigmatism blur amount △ h 0 , A h 45 to be corrected, Voltage value ΔΙ of two electrode groups. And it is characterized in that determined by the following equation ΔΙ 45.
Figure imgf000018_0001
但し、 E、 F、 G、 Hは各々、 Where E, F, G and H are
Eは、 0 ° 方向コイルにより、 0— 9 0 ° 方向の非点収差ボケを補正す る場合の非点収差ボケの補正感度  E is the astigmatism blur correction sensitivity when the 0-90 ° direction astigmatism blur is corrected by the 0 ° direction coil.
Fは、 4 5 ° 方向コイルにより、 0— 9 0 ° 方向の非点収差ボケを補正 する場合の非点収差ボケの補正感度  F is the sensitivity of astigmatism blur correction when the astigmatism blur in the 0-90 ° direction is corrected by the 45 ° direction coil.
Gは、 0 ° 方向コイルにより、 4 5— 135° 方向の非点収差ボケを補正 する場合の非点収差ボケの補正感度  G is the astigmatism blur correction sensitivity when astigmatism blur in the 45-135 ° direction is corrected by the 0 ° direction coil.
Hは、 4 5 ° 方向コイルによ り、 4 5— 135° 方向の非点収差ボケを補 正する場合の非点収差ボケの補正感度  H is the astigmatism blur correction sensitivity when the 45-135 ° direction astigmatism blur is corrected by the 45 ° direction coil.
である。 図面の簡単な説明 It is. BRIEF DESCRIPTION OF THE FIGURES
図 1は、本発明の第 1の実施の形態の原理を説明するための図である。 図 2は、本発明の第 2の実施の形態の原理を説明するための図である。 図 3は、本発明の第 4の実施の形態の原理を説明するための図である。 図 4は、本発明の第 5の実施の形態の原理を説明するための図である。 図 5は、 非点収差補正器のコイル配置の例を示す図である。 図 6は、 荷電粒子線露光装置の概要を示す図である。 FIG. 1 is a diagram for explaining the principle of the first embodiment of the present invention. FIG. 2 is a diagram for explaining the principle of the second embodiment of the present invention. FIG. 3 is a diagram for explaining the principle of the fourth embodiment of the present invention. FIG. 4 is a diagram for explaining the principle of the fifth embodiment of the present invention. FIG. 5 is a diagram illustrating an example of a coil arrangement of the astigmatism corrector. FIG. 6 is a diagram showing an outline of a charged particle beam exposure apparatus.
図 7は、 ボケを検出する方法の例を示す図である。 発明を実施するための最良の形態  FIG. 7 is a diagram illustrating an example of a method for detecting blur. BEST MODE FOR CARRYING OUT THE INVENTION
以下、 本発明の実施の形態の例を、 図を用いて説明する。 代表的な非 点収差補正器は、 図 5に示すように、 ( a ) に示すように 9 0 ° おきに配 置された 4個のコイル群を第 1組のコイルとし、 ( b )に示すように、 こ れと 4 5 ° ずれた方向に 9 0 ° おきに配置された 4個のコイル群を第 2 組のコイルとし、 これを組み合わせて ( c ) のように配置したものであ る。 ( d ) は ( c ) における A— A断面図を示す。 図において、 4 1 a〜 4 1 d、 4 2 a〜4 2 dは、 それぞれトロイダル型のコィルを光軸に沿 つて見たものである。通常 4 1 a〜(!は直列に接続され同じ電流で励磁さ れるが、 たとえばある電流を流すと 4 1 aと 4 1 c とは時計回りに磁場 を発生し、 4 1 bと 4 1 dとは反時計回りに磁場を発生するように巻か れており、 光軸上で 4極子場を発生する。 4 2 a〜 4 2 dについても同 様に設定される。 本発明でコイルに流す電流は、 これら直列に繋がった コイルに流す電流を示している。 実際に使用されるコイルがトロイダル 型に限定されないことは言うまでもない。 また、 図には示さないが静電 型非点収差補正器においては、 0 ° 電極、 1 8 0 ° 電極は同電位を与え、 9 0 ° 電極、 2 7 0度電極にはこれらと逆の電位を与える。 4 5 ° 方向 の非点収差補正器についても同様な設定になっている。 本発明で非点収 差補正器に与える電圧と記載した場合、 0 ° 方向電極、 4 5 ° 方向電極 に与える電圧を代表値としている。  Hereinafter, embodiments of the present invention will be described with reference to the drawings. As shown in Fig. 5, a typical astigmatism corrector consists of four coils arranged at 90 ° intervals as shown in (a) as the first set of coils, and as shown in (b). As shown in the figure, the four coil groups arranged at 90 ° intervals in a direction deviated by 45 ° from each other are used as a second set of coils, which are combined and arranged as shown in (c). You. (D) is a sectional view taken along line AA in (c). In the figure, reference numerals 41 a to 41 d and 42 a to 42 d respectively show toroidal coils along the optical axis. Normally, 4 1 a to (! Are connected in series and are excited by the same current. For example, when a certain current flows, 41 1 a and 41 c generate a magnetic field clockwise, and 41 b and 41 d It is wound so as to generate a magnetic field in a counterclockwise direction, and generates a quadrupole field on the optical axis.The same applies to 42 a to 42 d. The flowing current indicates the current flowing through these serially connected coils.Of course, the coils actually used are not limited to the toroidal type.Although not shown in the figure, the electrostatic astigmatism correction is performed. The 0 ° and 180 ° electrodes have the same potential, and the 90 ° and 270 ° electrodes have the opposite potentials. In the present invention, when the voltage applied to the astigmatism compensator is described, the 0 ° direction electrode The voltage applied to the 4 5 °-direction electrodes have a representative value.
非点収差補正器の基準方向を 0 ° とする。 本明細書及び請求の範囲に おいては、 この方向に従い、 前記第 1組のコイル群を 0 ° 方向コイル、 第 2組のコイル群を 4 5 ° 方向コイルと呼ぶことにする。 この基準方向 は 2組のコイルを区別するための概念的なものである。 この方向は、 前 記測定パターンを基準とした 0 ° 方向とは必ずしも一致しない。 もちろ ん、 補正すべき非点収差ボケの方向が第 1組のコイル群で補正可能な非 点収差ボケの方向と一致するような場合は、 第 1組のコイル群のみで非 点収差補正を行うことができるので、 コイル群は一組でよいが、 その場 合、 本明細書における記述を、 どちらかの組のコイル群を無視して (コ ィル群に流す電流が 0であるとして) 読めばよい。 The reference direction of the astigmatism corrector is set to 0 °. In this specification and in the claims, according to this direction, the first set of coil groups will be referred to as 0 ° direction coils, and the second set of coil groups will be referred to as 45 ° direction coils. This reference direction Is conceptual to distinguish the two sets of coils. This direction does not always coincide with the 0 ° direction based on the measurement pattern. Of course, if the direction of the astigmatism blur to be corrected matches the direction of the astigmatism blur that can be corrected by the first set of coil groups, the astigmatism correction is performed only by the first set of coil groups. Therefore, the coil group may be a single set, but in this case, the description in this specification is made by ignoring either set of the coil groups (the current flowing through the coil group is 0). As).
以下に示す発明の実施の形態においては、 非点収差補正器は、 このよ うなコイル群により構成されたものとして説明するが、 非点収差補正器 には、 上述のようにコイルを利用し、 そのローレンツ力により非点収差 補正を行うものの他に、 電極に電圧を印加し、 その静電力により非点収 差補正を行うものもある。 このような、 コイルを使用した非点収差補正 器と電極を使用した非点収差補正器は、その働きは基本的に同じである。 よって、 当業者は、 以下の実施の形態におけるコイルを電極と、 コイル に流す電流を電極に印加する電圧と読み替える等により、 容易に電極を 使用した非点収差補正器における本発明の実施の形態を推考することが できるであろう。 請求の範囲に記載される非点収差補正器が、 コイルを 使用したもの、電極を使用したものの両方を含むことは言うまでもない。 まず、 本発明の第 1の実施の形態の原理を、 図 1を用いて説明する。 図 1は、 非点収差ボケが、 0 ° 方向コイルに流す電流 (実際には磁界が 問題となるので単位は A Tで考える) S l、 4 5 ° 方向コイルに流す電 流 S 2を変化させることによりどのように変化するかを示した図である c 図 1においては、 第 1組のコイル群に流す電流 S 1 を横軸、 第 2組のコ ィル群に流す電流 S 2を縦軸とする直交座標系が示されている。 すなわ ち、 非点収差補正器の励磁を説明するための座標系である。 In the embodiments of the invention described below, the astigmatism corrector will be described as being constituted by such a coil group, but the astigmatism corrector uses a coil as described above, In addition to the method of correcting astigmatism by the Lorentz force, there is also a method of applying a voltage to the electrode and correcting the astigmatism by the electrostatic force. The operation of such an astigmatism corrector using a coil and an astigmatism corrector using an electrode are basically the same. Therefore, those skilled in the art can easily read the embodiment of the present invention in an astigmatism corrector using an electrode by reading the coil in the following embodiment as an electrode and the current flowing through the coil as a voltage applied to the electrode. Can be inferred. It goes without saying that the astigmatism corrector described in the claims includes both a device using a coil and a device using an electrode. First, the principle of the first embodiment of the present invention will be described with reference to FIG. Figure 1 shows that astigmatism blur changes the current flowing in the 0 ° direction coil (actually, the magnetic field is a problem, so the unit is AT.) S1, the current S2 flowing in the 45 ° direction coil is changed. in FIG. a is c Figure 1 showing how the changes by the horizontal axis the current S 1 flows to the first set of coil group, the current S 2 flowing through the second set of co-I le group vertical An orthogonal coordinate system as an axis is shown. That is, it is a coordinate system for explaining the excitation of the astigmatism corrector.
しかし、 図 1 において、 図示されている像の形状は、 測定パターンの 基準方向を 0 ° とする直交座標系 (X— y座標系) で示される形状 (X — y平面上の形状) である。 図 1においては、 たまたま S 1軸と X軸、 S 2軸と y軸が一致したように図が描かれているが、 これは理解し易く するために便宜上このような表示をしているだけである。 X— y座標系 と S 1— S 2座標系は全く別のものであるので、 実質的に同じ表示をす ることには格別の意味はない。 また、 S 1— S 2座標系と X— y座標系 の原点も一致する必要はない。 また、 図 1において破線で図示されてい る円は、 S 1— S 2平面上のものである。 However, in FIG. 1, the shape of the image shown is It is a shape (shape on the X-y plane) indicated by a rectangular coordinate system (X-y coordinate system) with the reference direction set to 0 °. In Fig. 1, the figure is drawn so that the S1 axis and the X axis coincide with each other, and the S2 axis and the y axis coincide with each other, but this is only displayed for convenience for easy understanding. It is. Since the X-y coordinate system and the S 1-S 2 coordinate system are completely different, there is no special meaning in giving them the same representation. Also, the origins of the S1-S2 coordinate system and the X-y coordinate system need not coincide. The circle shown by the broken line in FIG. 1 is on the S1-S2 plane.
この図において、 焦点位置が△ hだけ正焦点位置からずれているもの とする。 焦点位置をずらすには、 荷電粒子線光学系を操作して焦点位置 をずらせてもよいが、 もっと簡単な方法は、 被露光物の高さを変えるこ とにより実現できる。  In this figure, it is assumed that the focal position is shifted from the normal focal position by Δh. The focal position may be shifted by operating the charged particle beam optical system, but a simpler method can be realized by changing the height of the object to be exposed.
なお、 1 5は非点収差ボケが発生しない状態におけるビーム形状を示 すものである。  Reference numeral 15 indicates a beam shape in a state where astigmatism blur does not occur.
S l、 S 2を変化させることにより、 各々の S l、 S 2の値に対応し て、 ビーム形状は図に示すように変化する。 そして、 1 5を中心とする 円上で焦線が形成される。 これらの焦線のうち、 1 1は 軸に 0 ° 傾ぃ ており、 1 2は X軸に 9 0 ° 傾いており、 1 3は X軸に対して 4 5 ° 、 1 4は X軸に対して 135° 傾いている。 本実施の形態は、 これらの焦線 1 1〜 1 4を与える S 1 と S 2の組を見いだし、 それを基に非点収差ボ ケの補正感度を決定しょうとするものである。すなわち 1 1の座標を( S 1 1 , S 2 1 )、 1 2の座標を ( S 1 2, S 2 2 )、 1 3の座標を ( S 1 3, S 2 3 )、 1 4の座標を ( S 1 4, S 24 ) とすれば、 図から明らか なように、 測定点と同じ焦点位置で非点収差ボケがない状態から 0 ° 方 向コイルに流す電流、 及び 4 5 ° 方向コイルに流す電流をそれそれ、 512-511 By changing S l and S 2, the beam shape changes as shown in the figure according to the respective values of S l and S 2. Then, a focal line is formed on a circle centered at 15. Of these focal lines, 11 is at 0 ° to the axis, 12 is at 90 ° to the X-axis, 13 is 45 ° to the X-axis, and 14 is at X-axis. It is tilted 135 ° to it. In the present embodiment, a set of S 1 and S 2 giving these focal lines 11 to 14 is found, and the correction sensitivity of astigmatism blur is determined based on the set. In other words, the coordinates of 11 are (S11, S21), the coordinates of 12 are (S12, S22), the coordinates of 13 are (S13, S23), and the coordinates of 14 Let (S14, S24) be the current flowing through the 0 ° directional coil from the state where there is no astigmatism blur at the same focal position as the measurement point and the 45 ° directional coil, as is clear from the figure. The current flowing through 512-511
2  Two
522-521  522-521
2  Two
だけ変化させれば、 4 5— 135° 方向の非点収差ボケは変化させずに、 0 ° — 9 0 ° 方向の非点収差ボケだけを調整して、 0 ° 方向の非点収差 ボケを最小にすることができる (図 1の 1 2の状態)。 逆に、 これらの式 の符号を変えた分だけ変化させると、 9 0 ° 方向の非点収差ボケを最小 にすることができる (図 1の 1 1の状態)。 By changing only the astigmatism blur in the 45 ° -135 ° direction, only the astigmatism blur in the 0 ° -90 ° direction is adjusted, and the astigmatism blur in the 0 ° direction is adjusted. It can be minimized (state 1 and 2 in Figure 1). Conversely, when the sign of these equations is changed by as much as the sign is changed, the astigmatism blur in the 90 ° direction can be minimized (state 11 in FIG. 1).
これが、 焦点位置が光軸方向に△ hだけ変化したときの値であるので、 非点収差ボケを光軸方向の焦点位置ずれに換算したとき、 単位長さあた りの焦点ずれに対する非点収差ボケの補正感度は、 それそれ ( 1 ) 式、 ( 2 ) 式のようになる。 ここで ( 1 ) 式、 ( 2 ) 式のディメンジョンは例 えば [A T/mm]のように表される (電圧の場合は [V/mm]のように表 される)。 511-512 Since this is the value when the focal position changes by △ h in the optical axis direction, when astigmatism blur is converted into a focal position deviation in the optical axis direction, astigmatism with respect to defocus per unit length is obtained. The blur correction sensitivity is as shown in Equations (1) and (2). Here, the dimensions of equations (1) and (2) are expressed, for example, as [AT / mm] (voltage is expressed as [V / mm]). 511-512
-(1)  -(1)
2Δ/ι  2Δ / ι
521-522 521-522
〜(2)  ~ (2)
2Ah 同様、 測定点と同じ焦点位置で非点収差ボケの無い状態から、 0 ° 方 向コイルに流す電流、 及び 4 5 ° 方向コイルに流す電流をそれそれ、 Similarly to 2Ah, the current flowing through the 0 ° directional coil and the current flowing through the 45 ° directional coil from the same focal position as the measurement point and no astigmatism blur,
S14-S13 S14-S13
2  Two
524-S23  524-S23
2  Two
だけ変化させれば、 非点収差ボケ 0— 9 0 ° 方向の非点収差ボケは変化 させずに、 4 5 ° —135° 方向の非点収差ボケだけを調整して、 4 5 ° 方向の非点収差ボケを最小にすることができる(図 1の 1 4の状態)。又、 上記の式の符号を変えた分だけ変化させると、 135° 方向の非点収差ボ ケを最小にすることができる (図 1の 1 3の状態)。 If only the astigmatism blur is changed, the astigmatism blur in the 0-90 ° direction is not changed, and only the astigmatism blur in the 45 ° -135 ° direction is adjusted. Astigmatism blur can be minimized (14 in Fig. 1). or, When the sign of the above equation is changed, the astigmatism blur in the 135 ° direction can be minimized (state 13 in Fig. 1).
これが、 焦点位置が光軸方向に△ hだけ変化したときの値であるので、 単位長さあたりの焦点ずれに対する非点収差ボケの補正感度は、 それそ れ ( 3 ) 式、 ( 4 ) 式のようになる。 ここで ( 3 ) 式、 ( 4) 式のディメ ンジョンは例えば [mm/ A T]のように表される (電圧の場合は [V/ mm]のように表される)。 Since this is the value when the focal position changes by △ h in the optical axis direction, the correction sensitivity of the astigmatism blur for the defocus per unit length is expressed by the equations (3) and (4), respectively. become that way. Here, the dimensions of equations (3) and (4) are expressed, for example, as [mm / AT] (for voltage, they are expressed as [V / mm]).
S13-SU S13-SU
-(3)  -(3)
2Ah  2Ah
523-524 523-524
•••(4)  •••(Four)
2Δ/ι 又、 本明細書においては、 非点収差ボケの大きさを光軸方向の焦点位 置ずれの大きさに換算して表している。 この 2成分ある非点収差ボケの 絶対値は、 非点収差がある場合に焦線となる結像面位置の正焦点からの ずれ量の絶対値になり、 任意の非点収差ボケは 0度方向ボケと、 4 5度 方向ボケとの合成で表され、 0度方向成分、 4 5度方向成分は、 その非 点収差ボケに対する 0度方向ボケ ( 0度方向ボケが負になる場合は 9 0 度方向ボケが発生していることを示す)、 4 5度方向ボケ (4 5度方向ボ ケが負になる場合は 1 3 5度方向ボケが発生していることを示す) の寄 与を示している。 当然非点収差ボケが無いときには 0度方向成分、 4 5 度方向成分共に 0となる。 そして、 補正すべき非点収差ボグ(発生してい る非点ボケの符号を反転したもの)を非点収差ボケの補正感度行列にか けることによって非点補正器に与える電流又は電圧を計算し、 その量だ け非点補正器の電流又は電圧を変化させることで非点収差ボケを補正す る。  2Δ / ι Further, in the present specification, the magnitude of the astigmatism blur is represented by being converted into the magnitude of the focal position shift in the optical axis direction. The absolute value of these two components of astigmatism blur is the absolute value of the amount of deviation of the imaging plane position, which becomes the focal line when there is astigmatism, from the positive focal point. It is expressed by the combination of the direction blur and the 45-degree direction blur. The 0-degree direction component and the 45-degree direction component are the 0-degree direction blur for the astigmatism blur (9 if the 0-degree direction blur is negative). Contribution of 0 degree directional blur), 45 degree directional blur (If 45 degree directional blur is negative, it indicates that 135 degree directional blur is occurring) Is shown. Of course, when there is no astigmatism blur, both the 0-degree component and the 45-degree direction component become 0. Then, the current or voltage applied to the astigmatism corrector is calculated by applying the astigmatism bog to be corrected (inversion of the sign of the generated astigmatism blur) to the correction sensitivity matrix of the astigmatism blur. The astigmatism blur is corrected by changing the current or voltage of the astigmatism corrector by that amount.
以上の説明は各方向での焦線を与える電流値 S 1、 S 2が見つかった ものとして説明したが、 実際には焦線を見つける必要はない。 即ち、 例 えば X軸方向のボケが最小となる電流値 S 1、 S 2の組み合わせを見つ ければ、 それが焦線 1 2に対応する。 y軸方向のボケが最小となる電流 値 S l、 S 2の組み合わせを見つければ、 それが焦線 1 1に対応する。 X軸に対して 4 5 ° 方向のボケが最小となる電流値 S 1、 S 2の組み合 わせを見つければ、 それが焦線 1 4に対応する。 X軸に対して 135° 方 向のボケが最小となる電流値 S 1、 S 2の組み合わせを見つければ、 そ れが焦線 1 3に対応する。 In the above explanation, the current values S 1 and S 2 that give a focal line in each direction were found As described, it is not necessary to actually find the focal line. That is, for example, if a combination of the current values S 1 and S 2 that minimizes the blur in the X-axis direction is found, it corresponds to the focal line 12. If a combination of the current values S l and S 2 that minimizes the blur in the y-axis direction is found, it corresponds to the focal line 11. If a combination of the current values S 1 and S 2 that minimizes the blur in the 45 ° direction with respect to the X axis is found, it corresponds to the focal line 14. If a combination of the current values S 1 and S 2 that minimizes the blur in the 135 ° direction with respect to the X axis is found, it corresponds to the focal line 13.
各方向のボケが最小となる S 1、 S 2の組み合わせを見つける方法の 例については、 後に説明する。  An example of a method for finding the combination of S1 and S2 that minimizes the blur in each direction will be described later.
以下、 本発明の第 2の実施の形態について説明する。 この実施の形態 は第 1の実施の形態とは異なり、 焦点位置を変化させることにより、 非 点収差ボケの補正感度を決定する方法である。 この方法の原理を、 図 2 を用いて説明する。 図 2においても S 1— S 2軸、 X — y軸の考え方は 図 1 と同じである。 また、 像の形状は X — y平面上の形状であり、 破線 で示される円は S I— S 2平面上のものである。  Hereinafter, a second embodiment of the present invention will be described. This embodiment is different from the first embodiment in that the focus position is changed to determine the correction sensitivity for astigmatism blur. The principle of this method will be described with reference to FIG. In Fig. 2, the concept of S1-S2 axis and X-y axis is the same as Fig.1. The shape of the image is on the X-y plane, and the circle shown by the broken line is on the SI-S2 plane.
図 2において、 ある焦点位置で前記第 1の方法と同じようにして焦線 を検出し、 X軸方向 ( 0 ° 方向) の焦線を 1 1 A、 X軸に対して 9 0 ° 傾いた焦線を 1 2 A、 X軸に対して 4 5 ° 傾いた焦線を 1 3 A、 x軸に 対して 1 3 5 ° 傾いた焦線を 1 4 Aとする。 次に、 この位置から焦点位 置を A hずらせて、 同じように焦線の検出を行う。 焦点位置をずらすに は、 荷電粒子線光学系を操作して焦点位置をずらせてもよいが、 もっと 簡単な方法は、 被露光物の高さを変えることにより実現できる。  In FIG. 2, a focal line is detected at a certain focal position in the same manner as in the first method, and the focal line in the X-axis direction (0 ° direction) is inclined at 11 A and 90 ° with respect to the X-axis. The focal line is 12 A, the focal line inclined at 45 ° to the X axis is 13 A, and the focal line inclined at 135 ° to the x axis is 14 A. Next, the focal position is shifted Ah from this position, and the focal line is detected in the same manner. To shift the focal point, the focal point may be shifted by operating the charged particle beam optical system, but a simpler method can be realized by changing the height of the object to be exposed.
焦点をずら した後の、 X軸方向の焦線を 1 1 B、 X軸に対して 9 0 ° 傾いた焦線を 1 2 B、 X軸に対して 4 5 ° 傾いた焦線を 1 3 B、 x軸に 対して 1 3 5 ° 傾いた焦線を 1 4 Bとする。 そして、 各点の座標を 1 1 A ( S I 1 A, S 2 1 A)s 1 2 A ( S 1 2 A, S 2 2 A) 1 3 A ( S 1 3 A S 2 3 A)、 1 4 A ( S 1 4 A, S 2 4 A)、 1 1 B ( S 1 1 B , S 2 1 B) 1 2 B ( S 1 2 B , S 2 2 B)、 1 3 B ( S 1 3 B , S 2 3 B)、 1 4 B ( S 1 4 B , S 2 4 B ) とする。 After defocusing, the focal line in the X-axis direction is 1 1 B, the focal line inclined 90 ° to the X axis is 12 B, and the focal line inclined 45 ° to the X axis is 13 B, the focal line inclined by 135 ° with respect to the x-axis is defined as 14B. And the coordinates of each point are 1 1 A (SI 1 A, S 2 1 A) s 1 2 A (S 12 A, S 22 A) 13 A (S 13 AS 23 A), 14 A (S 14 A, S 2 4 A), 1 1 B (S 1 1 B, S 2 1 B) 1 2 B (S 1 2 B, S 2 2 B), 1 3 B (S 1 3 B, S 2 3 B), 1 4 B (S14B, S24B).
すると、 図 1を用いて説明した原理を差分的に使用することにより、 以下のように、 0 ° — 9 0 ° 方向、 及び 4 5 ° —135° 方向の非点収差ボ ケの補正感度を決定することができる。  Then, by differentially using the principle described with reference to FIG. 1, the correction sensitivity of astigmatism blur in the 0 ° -90 ° direction and the 45 ° -135 ° direction can be obtained as follows. Can be determined.
(1) 0 ° 方向コイル又は電極により、 0— 9 0 ° 方向の非点収差ボケを補 正する場合の非点収差ボケの補正感度 (1) Sensitivity for correcting astigmatism blur when correcting astigmatism blur in the 0 to 90 ° direction using a 0 ° direction coil or electrode
11B -S12B Sll. -S12A 11 B -S12 B Sll.-S12 A
( ^ 一 ~~ ά ·'·(5) (^ 1 ~~ ά
2Ah 2Ah ,  2Ah 2Ah,
(2) 4 5 ° 方向コィル又は電極により、 0— 9 0 ° 方向の非点収差ボケを 補正する場合の非点収差ボケの補正感度  (2) Sensitivity for correcting astigmatism blur when correcting astigmatism blur in the 0-90 ° direction using a 45 ° direction coil or electrode
S2\B-S12B _S2\A-S12A ) S2 \ B -S12 B _S2 \ A -S12 A )
、 2Ah 2Ah ) , 2Ah 2Ah)
(3) 0 ° 方向コィル又は電極により、 4 5— 135° 方向の非点収差ボケを 補正する場合の非点収差ボケの補正感度  (3) Sensitivity of astigmatism blur when correcting astigmatism blur in the 45-135 ° direction using a 0 ° direction coil or electrode
S13B-S14, _S13,-S14, ) S13 B -S14, _S13, -S14, )
、 2Ah 2Ah ) , 2Ah 2Ah)
(4) 4 5 ° 方向コイル又は電極により、 4 5— 135° 方向の非点収差ボケ を補正する場合の非点収差ボケの補正感度  (4) Sensitivity of astigmatism blur when 45-135 ° direction astigmatism blur is corrected by 45 ° direction coil or electrode
S23B-S2AB _S23A-S24A ) (S23 B -S2A B _S23 A -S24 A)
2Ah 2Ah )  2Ah 2Ah)
ただし、 S i j A S i j B ( i = 1 , 2 j = 1 4 ) の iは、 そ れぞれ 0 ° 方向コイル ( i = l )、 4 5 ° 方向コイル ( i = 2 ) を示し、 jは、 それそれ非点収差ボケが最小となる方向 ( j = 1は 9 0 ° 方向、 j = 2は 0 ° 方向、 j = 3は 1 3 5 ° 方向、 j = 4は 4 5 ° 方向) を示 す。 以下、本発明の第 3の実施の形態を説明する。非点収差補正器の感度(非 点収差ボケの補正感度) としては前述のものとは別に、 ある非点収差補正 器のコィルに流す電流を変化させた場合に、 どの程度 0— 9 0 ° 方向の非 点収差ボケ、 4 5— 135° 方向の非点収差ボケが変わるかを知りたい場合Where i in S ij AS ij B (i = 1, 2j = 14) indicates a 0 ° directional coil (i = l) and a 45 ° directional coil (i = 2), respectively, and j Is the direction in which astigmatism blur is minimized (j = 1 is 90 ° direction, j = 2 is 0 ° direction, j = 3 is 13.5 ° direction, j = 4 is 45 ° direction) Is shown. Hereinafter, a third embodiment of the present invention will be described. The sensitivity of the astigmatism corrector (correction sensitivity for astigmatism blur) is different from the one described above. When the current flowing through the coil of a certain astigmatism corrector is changed, how much is 0 to 90 ° If you want to know if the astigmatism blur in the direction changes, as well
5 Five
がある。 このような意味で、 単位量だけ非点収差補正器のコイルに流す電 流を変化させた場合に発生する非点収差ボケ (光軸方向位置換算) を表す 非点収差ボケの発生感度は、 例えば [mm/A T]のようなディメンジョン で表されるものである。このような非点収差ボケの発生感度は、前記( 1 ) There is. In this sense, the sensitivity of astigmatism blur, which represents astigmatism blur (conversion in the optical axis direction) that occurs when the current flowing through the coil of the astigmatism corrector is changed by a unit amount, is For example, it is represented by a dimension such as [mm / AT]. The occurrence sensitivity of such astigmatism blur is as described in the above (1).
〜 ( 4 ) 式から簡単に求めることができる。 It can be easily obtained from Eq. (4).
10  Ten
すなわち、 0 ° 方向コイルに流す電流の変化量を△ I 。、 4 5 ° 方向 コイルに流す電流の変化量を Δ 14 5とし、 そのときの 0— 9 0 ° 方向の 非点収差ボケを光軸方向位置に換算したものを A h。、 4 5— 135° 方向 の非点収差ボケを光軸方向位置に換算したものを Δ 1 4 5 とする と、That is, the amount of change in the current flowing through the 0 ° direction coil is △ I. , 4 5 ° the amount of change current flowing in the direction coil and delta 1 4 5, the time of 0-9 0 those converted in the optical axis direction position astigmatism blur of ° direction A h. And those obtained by converting the astigmatism blur of 4 5-135 ° direction in the optical axis direction position and delta 1 4 5,
( 1 ) 〜 ( 4 ) より、 From (1) to (4),
Figure imgf000026_0001
Figure imgf000026_0001
であるから、  Because
Δん Δn
Ah ■45 Ah ■ 45
Figure imgf000026_0002
となる 二れを、
Figure imgf000026_0002
The two
2 / 、Δ 452 /, Δ 45 no
Figure imgf000026_0003
Figure imgf000026_0003
と表すと、 A i iが 0 ° 方向コイルに流す電流に対する 0— 9 0 ° 方向の 非点収差ボケの発生感度、 A 1 2が 4 5 ° 方向コイルに流す電流に対する 0— 9 0 ° 方向の非点収差ボケの発生感度、 A2 iが 0 ° 方向コイルに流 す電流に対する 4 5— 135° 方向の非点収差ボケの発生感度、 A2 2が 4 5 ° 方向コイルに流す電流に対する 4 5— 135° 方向の非点収差ボケの 発生感度となる。 A i い A A 2い A2 2は、 ( 2 9 ) 式における逆 行列を計算することにより簡単に求まる。 すなわち、 Where A ii represents the current flowing through the 0 ° Generating sensitivity astigmatism blur, A 1 2 4 against to current flow in 4 5 generation sensitivity astigmatism blur of ° 0- 9 0 ° direction with respect to the current flowing in the direction coil, A 2 i is 0 ° direction coil generating sensitivity astigmatism blur of 5-135 ° direction, the occurrence sensitivity astigmatism blur of 4 5-135 ° direction with respect to the current a 2 2 shed to 4 5 °-direction coil. A i have AA 2 have A 2 2 is determined easy by calculating the inverse matrix of (2 9). That is,
2ΔΑ(523-524) 2ΔΑ (523-524)
^11 =  ^ 11 =
{( - - 512)(523 - 24)一 ( 513一 4)( 521 -522)}  {(--512) (523-24) one (513-four) (521 -522)}
-2Ah(S13 - S14)  -2Ah (S13-S14)
A {^11- -S12)(S23 -24) -(SL3 -SL4)( S21 -S22)}  A {^ 11- -S12) (S23 -24)-(SL3 -SL4) (S21 -S22)}
-2Δ/ι(521-522)  -2Δ / ι (521-522)
{(Sll- -512)(523 -24) -(513 -514)( Sll -《22)}
Figure imgf000027_0001
となる。
{(Sll- -512) (523 -24)-(513 -514) (Sll-《22)}
Figure imgf000027_0001
It becomes.
同様にして、 非点収差補正器を構成する 2組のコイルの電流値又は 2 組の電極の電圧値をそれそれ変化させ、 測定パターンを基準とした 0 ° 方向、 9 0 ° 方向、 4 5 ° 方向、 135° 方向のボケが最小となる前記 2組 の電流値又は電圧値をそれそれ求め、 これを、 光軸方向の任意の位置 A と Aから光軸方向に△ hだけ離れた位置 Bにおいて行い、  Similarly, the current value of the two sets of coils or the voltage value of the two sets of electrodes constituting the astigmatism compensator are varied respectively, and the 0 ° direction, 90 ° direction, 45 The two sets of current values or voltage values that minimize the blur in the 135 ° direction and 135 ° direction are calculated accordingly, and these are determined as arbitrary positions A and A in the optical axis direction at positions △ h away from the arbitrary optical axis directions in the optical axis direction. Done in B,
これらの電流値の組み合わせをそれそれ ( S 1 1 A, S 2 1 A)、 ( S I 2 A, S 2 2 A)、 ( S 1 3 A , S 2 3 A)ヽ ( S 1 4 A, S 2 4 A)s ( S 1 1 B , S 2 1 B)、 ( S 1 2 B, S 2 2 B)、 ( S 1 3 B , S 2 3 B)S ( S 1 4 B , S 2 4 B ) とするとき、 次の少なく とも一つの式により、 少な く とも一つの方向の非点収差ボケの発生感度を決定する場合には、 差分 を取ることにより、 The combination of these current values is (S11A, S21A), (SI2A, S22A), (S13A, S23A) ヽ (S14A, S 2 4 A) s (S 11 B, S 21 B), (S 12 B, S 22 B), (S 13 B, S 23 B) S (S 14 B, S 2 4B), when determining the sensitivity of occurrence of astigmatism blur in at least one direction by at least one of the following equations, by taking the difference,
(1)0 ° 方向コイルにより、 0— 9 0 ° 方向の非点収差ボケを発生させる 非点収差ボケの発生感度 (1) 0-90 ° direction astigmatism blur is generated by the 0 ° direction coil Sensitivity of astigmatism blur
2^{{S23B-S2^B)-(S2 A-S2AA)} …( 2 ^ {{S23 B -S2 ^ B )-(S2 A -S2A A )}… (
Δ  Δ
(2) 4 5 ° 方向コイルにより、 0 ° — 9 0 ° 方向の非点収差ボケを発生さ せる非点収差ボケの発生感度  (2) Sensitivity of astigmatism blur which generates astigmatism blur in the 0 ° to 90 ° direction by the 45 ° direction coil
-2AA{(S13g-S14,)-(S13,-S14J} -2AA {(S13 g -S14,)-(S13, -S14J}
Δ 、 )  Δ,)
(3) 0 ° 方向コイルにより、 4 5 ° _ 135° 方向の非点収差ボケを発生さ せる非点収差ボケの発生感度 (3) Sensitivity of astigmatism blur that generates astigmatism blur in the 45 ° -135 ° direction by the 0 ° direction coil
(15)式の最初にマイナス &最後に力ッコ閉じ } が入る  (15) Minus at the beginning & Close at the end}
-2Ah{(S21B -S22B)-(S2\A -S22J} -2Ah {(S21 B -S22 B )-(S2 \ A -S22J}
ー(15)  ー (15)
Δ  Δ
(4) 4 5 ° 方向コイルにより、 4 5 ° - 135° 方向の非点収差ボケを発生 させる非点収差ボケの発生感度 (4) Sensitivity of astigmatism blur which generates astigmatism blur in the direction of 45 °-135 ° by the 45 ° direction coil
(16)式の最初のマイナスは削除  Remove the minus sign at the beginning of equation (16)
2^{{S1\B -S12B)-{SY1A-S12A)} 2 ^ {{S1 \ B -S12 B )-{SY1 A -S12 A )}
•(16)  • (16)
Δ  Δ
を得ることができる。 Can be obtained.
ただし、 S i j A、 S i j B ( i 2、 j = 1〜 4 ) の iは、 そ れそれ 0 ° 方向コイル ( i = l )、 4 5。 方向コイル ( i = 2 ) を示し、 jは、 それそれ非点収差ボケが最小になる方向 ( j = 1は 9 0 ° 方向、 j = 2は 0 ° 方向、 j = 3は 1 3 5 ° 方向、 j = 4は 4 5 ° 方向) を示 し、 △は、  However, i of SijA and SijB (i2, j = 1 to 4) are 0 ° direction coils (i = l) and 45, respectively. Indicates the direction coil (i = 2), j is the direction in which astigmatism blur is minimized (j = 1 is 90 ° direction, j = 2 is 0 ° direction, j = 3 is 1 35 ° Direction, j = 4 indicates 45 ° direction), and △ indicates
Δ = [{(^11, -S\2B)-{SnA -S12A)}{(S23B -S2 B)-{S23A-S2 A)} -{{S13B -514β)-(513Λ -S A)}{(S21B-S22B)-{S21A-S22A)}]で 示される値である。 Δ = [{(^ 11, -S \ 2 B )-{Sn A -S12 A )} {(S23 B -S2 B )-{S23 A -S2 A )}-{{S13 B -514 β )- (513 Λ -S A )} {((S21 B -S22 B )-{S21 A -S22 A )}].
又、 第 2の実施の形態で示した ( 5 ) 式〜 ( 8 ) 式より、 上述の ( 2 8 ) 式に対応する式は、 Also, from the equations (5) to (8) shown in the second embodiment, the above-mentioned (2) 8) The expression corresponding to the expression is
511. -512, _ SHA-S12A ) ,513Β- 14 S13, -S t 511.-512, _ SH A -S12 A ), 513 Β -14 S13, -S t
2ΔΛ 2ΔΛ 2ΔΛ 2ΔΛ  2ΔΛ 2ΔΛ 2ΔΛ 2ΔΛ
■(31) ■ (31)
ΑΙ ' 45 521„_-522β一 S21A -522, S23B -S24B 523. -Ξ24Λ 45 , ΑΙ '45 521 „_- 522 β- one S21 A -522, S23 B -S24 B 523.-Ξ24 Λ 45,
2Δ/ι 2ΔΛ 2ΔΛ 2ΔΛ  2Δ / ι 2ΔΛ 2ΔΛ 2ΔΛ
であるから、 ( 3 0 ) 式に対応する A 、 A 12、 A2い A22を求める と、 Therefore, if A, A 12 , A 2 and A 22 corresponding to the equation (30) are obtained,
2ΔΑ{(523β - S24B)- (S23A- -•524,)} 2ΔΑ {(523 β - S24 B ) - (S23 A - - • 524,)}
Δ  Δ
-2Ah{(S13B -suB) -(^13, -514,)} -2Ah {(S13 B -su B )-(^ 13, -514,)}
Δ  Δ
-2Ah{(S21B -522 -(^21, -2Ah {(S21 B -522-(^ 21,
1 =  1 =
Δ  Δ
A 一 2Ah{(SllB - 512β) - (^ιι.一 S12A) A i 2Ah {(Sll B -512 β )-(^ ιι.i S12 A )
Λ22 ― Λ 22 ―
Δ  Δ
となる。 ただし It becomes. However
Δ = [{(S11B -512,) -(511, -S12A)}{{S23B -S24B)-(S23A- S24A)} Δ = [{(S11 B -512,)-(511, -S12 A )} {{S23 B -S24 B )-(S23 A -S24 A )}
-{(^13, -S B)-(S13A -S A)}{(S21B -S22B)-(S21A-S22A)}] である。 -{(^ 13, -S B )-(S13 A -S A )} {((S21 B -S22 B )-(S21 A -S22 A )}].
図 3は、 本発明の第 4の実施の形態を説明するための図であり、 図 1 と同様の図である。 この図において、 焦点位置が△ hだけ正焦点位置か らずれているものとする。 なお、 0は非点収差ボケが発生しない状態に おける励磁条件を示すものである。  FIG. 3 is a diagram for explaining a fourth embodiment of the present invention, and is similar to FIG. In this figure, it is assumed that the focal position is shifted from the normal focal position by Δh. Note that 0 indicates the excitation condition in a state where astigmatism blur does not occur.
図 3に示す例では、 測定パターンの基準方向に対して 4 5 ° ずれた方 向に長い焦線が形成される S 1 と S 2の組み合わせを点 2 2の位置 ( S 1 5 , S 2 5 )、 測定パターンの基準方向に対して 9 0 ° ずれた方向に長 い焦線が形成される S 1 と S 2の組み合わせを点 2 3の位置 ( S 1 6, S 2 6 ) としている。 図では、 これらの焦線を線で示している。 すなわ ち、 点 2 2 と点 2 3は、 測定パターンの基準方向に対して、 それぞれ 135° 、 0 ° ずれた方向での非点収差ボケが最小となる点である。 つま り、 点 2 2と点 2 3では、 非点収差ボケが最小となる方向の角度差 0がIn the example shown in FIG. 3, the combination of S 1 and S 2, which forms a long focal line in a direction shifted by 45 ° from the reference direction of the measurement pattern, is set to the position of point 22 (S 15, S 2 5), The combination of S1 and S2, which forms a long focal line in a direction shifted 90 ° from the reference direction of the measurement pattern, is defined as the position of point 23 (S16, S26) . In the figure, these focal lines are indicated by lines. That is, points 22 and 23 respectively correspond to the reference direction of the measurement pattern. This is a point at which astigmatism blur in directions shifted by 135 ° and 0 ° is minimized. That is, at point 22 and point 23, the angle difference 0 in the direction that minimizes astigmatism blur is
4 5度である。 4 5 degrees.
ところで、 一般的に、 焦点が正焦点位置からずれた場合、 結像面に焦 線を形成するような S 1 と S 2の組み合わせは、 S 1— S 2平面で円の 軌跡を描く ことが知られている。 そして、 この円での中心角度が øだけ 変わった点における焦線の方向は、 + 2または一 ノ2だけ変化す ることが知られている。 このことを利用して、 円 2 1の中心点 0、 すな わち非点収差ボケが発生しない位置を求める。 点 0の位置を ( S 1。 , By the way, in general, when the focal point deviates from the right focal point position, the combination of S 1 and S 2 that forms a focal line on the image forming plane can draw a circular locus on the S 1—S 2 plane. Are known. It is known that the direction of the focal line at the point at which the center angle of the circle changes by ø changes by +2 or one-two. Using this, the center point 0 of the circle 21, that is, the position where astigmatism blur does not occur is obtained. The position of point 0 is defined as (S1,
52。) とする。 52. ).
まず、 点 0は、 点 2 2と点 2 3の垂直 2等分線 2 4上にあることは、 点 2 2、 点 2 3が円 2 1上の点であることから明らかである。 この垂直 2等分線の方程式は、  First, it is clear that point 0 is on the perpendicular bisector 24 of points 22 and 23 because points 22 and 23 are points on the circle 21. The equation of this vertical bisector is
(S1 - S15 + S16 (S15 -S16) + (S2- S2:> + S2 (S25 -S26) = 0 … ( 32 ) (S1- S15 + S16 (S15 -S16) + (S2- S2:> + S2 (S25 -S26) = 0… (32)
 M
を満足する。 又、 前述のように、 焦線を形成する ( S 1、 S 2 ) の組み 合わせが存在する円での中心角度が øだけ変わった点における焦線の方 向は 0/2だけ変化することが知られている。 逆に言えば、 点 2 2と点 2 3では焦線の方向が 0だけずれているので、 円 2 1の中心 0と点 2 2 (又は点 2 3 ) を結んだ線と、 この垂直 2等分線 2 4がなす角度は 0で め 。 To be satisfied. Also, as described above, the direction of the focal line at the point where the center angle of the circle where the combination of (S1, S2) forming the focal line exists changes by ø changes by 0/2. It has been known. Conversely, since the direction of the focal line is shifted by 0 at points 2 2 and 2 3, the line connecting the center 0 of circle 2 1 and point 2 2 (or point 2 3) and this vertical 2 The angle formed by the bisectors 24 is 0.
このことから、 ベク トルの内積を用いて  From this, using the inner product of the vector
(51 - S15XS1 - S16) + (52 - S25)(S2 - S26) (51-S15XS1-S16) + (52-S25) (S2-S26)
= (51 - S15)2 + (S2一 S25)2 - S16)2 + (S2 - S26)2 cos 2Θ -<33) の関係が成り立つ。 = (51-S15) 2 + (S2-S25) 2 -S16) 2 + (S2-S26) 2 cos 2Θ-<33)
よって、 点 0の位置は ( 3 2 ) 式と ( 3 3 ) 式を S l、 S 2について 連立させて解いた解 ( S 1。、 S 2。) として求まる。 すなわち、 Therefore, the position of point 0 is obtained as a solution (S1, S2) obtained by simultaneously solving equations (32) and (33) for S1 and S2. That is,
_{(S15 + S16)±(S25-S26)cote} … _ {(S15 + S16) ± (S25-S26) cote}…
 M
S2 {(525 + 526) + (515 - 516) cot Θ} …ひ 8) なお、 解 ( S 1。、 S 2。) は 2組求まるので、 このうちのどちらを使 用するかが問題となる。 しかし、 これは容易に決定することができる。 一番簡単な方法は求まったそれそれの ( S 1 D、 S 2。) の条件で非点収 差補正器を励磁し、 非点収差ボケがゼロに近くなるものを採用する方法 である。 又、 一般的には、 設計上、 各非点収差補正器の各電流で発生す る非点収差ボケの傾向は分かっているので、 それに合った方を採用する ようにすればよい。 例えば、 S 1を正側に励磁すると非点収差ボケの 0 — 9 0 ° 方向は 0 ° 方向の方が強くなるように設計されているとする。 0 ° 方向の焦線は 0に対して点 2 3 と対称な位置にある。 図 3の 0であ れば S 1 を正に励磁すると 0 ° 方向のボケは強くなるが、 もう一つの解 では逆になるので、 容易に判別が可能である。 S2 {(525 + 526) + (515-516) cot Θ}… hi 8) Since two sets of solutions (S1, S2.) Are obtained, it is important to decide which one to use. Become. However, this can be easily determined. The simplest method is to excite the astigmatism compensator under the conditions (S 1 D, S 2) that were found, and to adopt the one that has astigmatism blur close to zero. In general, the tendency of astigmatism blur generated by each current of each astigmatism corrector is known from the design, so that the one that matches the tendency may be adopted. For example, it is assumed that when S1 is excited to the positive side, the astigmatism blur is designed so that the 0-90 ° direction becomes stronger in the 0 ° direction. The focal line in the 0 ° direction is symmetrical to point 23 with respect to zero. If it is 0 in Fig. 3, if S1 is excited positively, the blur in the 0 ° direction becomes stronger, but the other solution is reversed, so that it is easy to determine.
このようにして、 円 2 1の中心 0が求まると、 焦線を形成する点を結 んだ円は、 点 0を中心とし、 点 2 2、 2 3を通る円として決定される。 そして、 この円の半径が、 焦点位置が△ hだけずれたことによって発生 した非点収差ボケの大きさを示している。  In this way, when the center 0 of the circle 21 is determined, the circle connecting the points forming the focal line is determined as a circle centered on the point 0 and passing through the points 22 and 23. The radius of the circle indicates the magnitude of astigmatism blur caused by the shift of the focal position by Δh.
この円が求まると、 パターンの基準方向に対して 0 ° — 9 0 ° 方向の 非点収差ボケ、 4 5 ° — 135° 方向の非点収差ボケを、 それそれ非点収 差補正器の 0 ° 方向コイル ( S l )、 4 5 ° 方向コイル ( S 2 ) によって 補正するときの発生感度を求めることができる。  When this circle is obtained, the astigmatism blur in the direction of 0 ° to 90 ° and the astigmatism blur in the direction of 45 ° to 135 ° with respect to the reference direction of the pattern, and the astigmatic blur in the direction of The sensitivity at the time of correction by the 45 ° directional coil (Sl) and the 45 ° directional coil (S2) can be obtained.
まず、 この円上で、 90°方向の非点収差ボケが最小となる点を求め、 そのときの非点収差補正器の 0 °方向コイル、 4 5 °方向コイルの電流の 組み合わせを ( S l l ,、 S 2 1 ') とする。 又、 この円上で、 135° 方 向の非点収差ボケが最小となる点を求め、 そのときの非点収差補正器の 0 °方向コイル、 4 5。方向コィルの電流の組み合わせを ( S 1 3,、 S 2 3 ') とする。 First, the point where the astigmatism blur in the 90 ° direction is minimized on this circle is determined, and the combination of the currents of the 0 ° direction coil and the 45 ° direction coil of the astigmatism corrector at that time is (S ll , S 2 1 '). Also, on this circle, 135 ° Find the point where the astigmatism blur in the azimuth is minimized. Then, the 0 ° direction coil of the astigmatism corrector, 45. The combination of the currents in the direction coils is (S13, S23 ').
一般的には、 例えば、 0 i方向のボケが最小になる非点収差補正器の 励磁電流または電圧を ( S 1 5 S 2 5,)、 6> 2方向のボケが最小に なる非点収差補正器の励磁電流または電圧を ( S 1 6 ', S 2 6 ') とし て In general, for example, the excitation current or voltage of the astigmatism corrector that minimizes the blur in the 0i direction is (S15S25), and the astigmatism that minimizes the blur in the 6> 2 direction. The excitation current or voltage of the compensator is (S16 ', S26')
一般的な焦線円上の点は、 焦線半径 Sを、 The point on the general focal line circle is the focal line radius S,
_ v (S15 '一 S16J + (S 25 '― S 26 J cos ec^ _ v (S15 'One S16J + (S 25' ― S 26 J cos ec ^
2  Two
として、 ( S I— S 2 ) 座標で、 この焦線円上の点 ( S 1 , S 2 ) が、 円 の中心 ( S 1。、 S 2。) を中心とし、 S 1軸と平行な直線となす角を ø とすると、 The point (S1, S2) on this focal line circle is a straight line parallel to the S1 axis, centered on the center of the circle (S1, S2) in (SI—S2) coordinates. If the angle formed is ø,
51- S1。 = S cos0  51- S1. = S cos0
52- S2。 = S sin^  52- S2. = S sin ^
と表され、 よって And thus
tan =(S2-S20)バ S1-S10) tan = (S2-S2 0 ) bar S1-S1 0 )
となる。 It becomes.
0 i方向のボケが最小になる S 1— S 2座標系での回転角 ø iは、 φ J = tan" 1((S25* - S20)/(S15* - Sl0)) 0 Rotation angle in the S 1—S 2 coordinate system that minimizes blur in the i direction ø i is φ J = tan " 1 ((S25 *-S2 0 ) / (S15 *-Sl 0 ))
したがって、 Therefore,
φ: ± 2 (0-6>】) + φ! φ: ± 2 (0-6>)) + φ!
となる—。 -
0度方向焦線になると思われるのは 6> = 0のときで、 ^iBJ) S13' 二 S cos0 o + Sl0 It is considered that the focal line becomes 0 degree direction when 6> = 0, ^ iBJ) S13 'Two S cos0 o + Sl 0
S23* = S sin ø o + S20 S23 * = S sin ø o + S2 0
同様に 4 5度方向焦線になると思われるのは 0 = ττ/4のときで φ5 = +2Θ,土 一 + tan 1 ¾ Similarly, the 45 ° directional focal line is considered to be 0 = ττ / 4 when φ 5 = + 2Θ, Satichi + tan 1 ¾
5 1 2 15' - Sl0
Figure imgf000033_0001
5 1 2 15 '-Sl 0 no
Figure imgf000033_0001
S23' 二 S sin ø 4 ε + S2。 S23 'two S sin ø 4 ε + S2.
と表すことができる。 It can be expressed as.
このようにすると、 図 3に示した幾何学的な関係より、  In this way, from the geometric relationship shown in Figure 3,
(1) )0 ° 方向コイルにより、 0 — 9 0 ° 方向の非点収差ボケを発生させる 非点収差ボケの発生感度  (1)) 0 ° -90 ° direction astigmatism blur caused by 0 ° direction coil
AA(S23'-S20) AA (S23'-S2 0 )
{ (SI 1 '- S10)(S 23 '- S 20 ) - (513 '- 510 )(S 21 '- S 20 )} ) {(SI 1 '-S1 0 ) (S 23'-S 2 0 )-(513 '-51 0 ) (S 21'-S 2 0 )})
(2) 4 5 ° 方向コイルにより、 0 ° — 9 0 ° 方向の非点収差ボケを発生さ せる非点収差ボケの発生感度  (2) Sensitivity of astigmatism blur which generates astigmatism blur in the 0 ° to 90 ° direction by the 45 ° direction coil
- (S13'-S10) … - (S13'-S1 0) ...
{ (511 Sl0 )(S 23 S 20) - (SI 3 '- S 10 )(S 21 '- S 20)} 、 ) {(511 Sl 0 ) (S 23 S 2 0 )-(SI 3 '-S 1 0 ) (S 21' -S 2 0 )},)
(3) 0 ° 方向コイルにより、 4 5 ° — 135° 方向の非点収差ボケを発生さ せる非点収差ボケの発生感度 (3) Sensitivity of astigmatism blur that causes astigmatism blur in the 45 ° -135 ° direction by the 0 ° direction coil
- (S21'-S20) -(S21'-S2 0 )
{ (SI 1 Sl0 )(S 23 S 20 ) - (S 13 '- S 10 )(S 21 520 )} 、 ) {(SI 1 Sl 0 ) (S 23 S 2 0 )-(S 13 '-S 1 0 ) (S 21 52 0 )},)
(4)4 5 ° 方向コイルにより、 4 5 ° — 135° 方向の非点収差ボケを発生 させる非点収差ボケの発生感度  (4) Sensitivity of astigmatism blur which generates astigmatism blur in the direction of 45 ° to 135 ° by the 45 ° direction coil
Ah(SlV-Sl0) Ah (SlV-Sl 0 )
{(S1V- S1Q)(S 23 '- S 20) - (S13 '- Sl0)(521 '-S 20)} ' {(S1V- S1 Q ) (S 23 '-S 2 0 )-(S13'-Sl 0 ) (521 '-S 2 0 )}'
となる。 It becomes.
以上の実施の形態においては、 異なる方向の非点収差ボケが最小とな る点を S 1 — S 2平面上で 2点求め、 これらが S 1 — S 2平面上で焦線 を形成する円上にあること、 焦線を形成する ( S 1、 S 2 ) の組み合わ せが存在する円での中心角度が øだけ変化すると、 焦線の方向は 0 / 2 だけ変化することを利用して、焦線を形成する円を求めていた。しかし、 異なる方向の非点収差ボケが最小となる点を S 1 - S 2平面上で 3点求 めれば、 これらがいずれも S 1— S 2平面上で焦線を形成する円上にあ ることを利用して、 連立方程式を解くことにより、 円を求めることがで きる。 円を求めた後は、 前述の処理と同じ処理を行い、 非点収差補正器 の発生感度を求めることができる。 In the above embodiment, two points at which the astigmatism blur in the different directions is minimized are found on the S 1 —S 2 plane, and these are the focal lines on the S 1 —S 2 plane. If the center angle in the circle where the combination of (S1, S2) forms the focal line changes by ø, the direction of the focal line will change by 0/2. Was used to find a circle forming a focal line. However, if three points at which the astigmatism blur in the different directions is minimized on the S 1 -S 2 plane are obtained, each of these points is on a circle forming a focal line on the S 1-S 2 plane. By taking advantage of this fact, a simultaneous equation can be solved to obtain a circle. After obtaining the circle, the same processing as described above is performed, and the generation sensitivity of the astigmatism corrector can be obtained.
以上の議論は、 所定の方向の非点収差ボケを最小とする S 1— S 2平 面上の点に決定誤差がないことを前提としていた。 しかし、 これらの点 を決定するときに誤差があるとそれが、 非点収差補正器の発生感度の誤 差となって現れる。  The above discussion has been based on the assumption that there is no determination error at a point on the S 1—S 2 plane that minimizes astigmatism blur in a predetermined direction. However, if there are errors in determining these points, they will appear as errors in the sensitivity of the astigmatism corrector.
図 4は、 このような誤差がある場合に、 この誤差の影響をできるだけ 取り除く方法を使用した、 本発明の第 5の実施の形態を説明するための 図である。 この実施の形態においては、 多数 (図においては 8つ) の方 向の非点収差を最小とするような S 1— S 2面上の点 ( 2組のコイルの 電流値の組み合わせ) を求め、 それらの点を 2 5〜 3 2で表している。 そして、 それそれの点における焦線の形状を線で示している。 この例に おいても、 説明の都合上、 パターンの方向の 0 ° を S 1方向にとってい る o  FIG. 4 is a diagram for explaining a fifth embodiment of the present invention using a method for removing the influence of such an error as much as possible when there is such an error. In this embodiment, the points (combinations of the current values of the two coils) on the S1-S2 surface that minimize astigmatism in many directions (eight in the figure) are obtained. The points are represented by 25-32. The shape of the focal line at each point is indicated by a line. In this example as well, for the sake of explanation, the pattern direction is set to 0 ° in the S1 direction.
図 3 と同じように、 円 2 1は、 焦線が形成される点を結んだ円、 点 0 はその中心を示している。 図から明らかなように、 点 2 5〜 3 2は、 円 2 1の上に載っていない。 これは、 点 2 5〜 3 2の決定に誤差があるか らである。 この実施の形態においては、 これら 8つの点を用いて、 最小 二乗法によ り、 円 2 1を推定している。 すなわち点 2 5〜 3 2の座標を それそれ ( S l i, S 2 とすると ( i = 2 5〜 3 2 )、
Figure imgf000035_0001
As in FIG. 3, circle 21 is the circle connecting the points where the focal line is formed, and point 0 is the center. As is clear from the figure, points 25 to 32 are not on the circle 21. This is because there is an error in the determination of points 25-32. In this embodiment, the circle 21 is estimated by the least squares method using these eight points. In other words, if the coordinates of points 25-32 are different (Sli, S2) (i = 25-32),
Figure imgf000035_0001
を最小にするような、 S l 。、 S 2。、 rを求めてやればよい。 S l such that is minimized. , S2. , R can be obtained.
このようにして円 2 1が求まれば、 図 3に示した実施の形態と同じ方 法により、 非点収差補正器の発生感度を求めることができる。  When the circle 21 is obtained in this manner, the generation sensitivity of the astigmatism corrector can be obtained by the same method as the embodiment shown in FIG.
以上の実施の形態を実施するためには、 所定方向のボケが最小となる 非点収差補正器の電流の組み合わせを見つけなければならない。これは、 図 7に示すような方法により行う。  In order to implement the above-described embodiment, it is necessary to find a combination of currents of the astigmatism corrector that minimizes blur in a predetermined direction. This is performed by the method shown in FIG.
図においてボケ検出用荷電粒子線像 5 1を走査偏向器で走査し、 荷電 粒子線ボケ検出用マーク 5 2上を通過させる。 そして、 不図示の信号検 出器(たとえば反射電子検出器)により信号を得る。 この信号は、 荷電粒 子線ボケ検出用マーク 5 2 とボケ検出用荷電粒子線像 5 1の重なった部 分の面積に比例したものとなるが、 ボケ検出用荷電粒子線像 5 1にボケ があると、 そのボケの分だけなまった図形となる。 よって、 この検出信 号は通常 5 3に示すような形状となり、 それを微分すると 5 4のような 波形が得られる。 通常、 この微分信号における立ち上がり部分の 1 2 % から 8 8 %の部分の走査距離をボケ 5 5 と定義する。  In the figure, the blur detection charged particle beam image 51 is scanned by a scanning deflector, and passes over the charged particle beam blur detection mark 52. Then, a signal is obtained by a signal detector (not shown) (for example, a backscattered electron detector). This signal is proportional to the area of the overlapping portion of the charged particle beam blur detection mark 52 and the blur detection charged particle beam image 51, but the blurred charged particle beam image 51 If there is, it becomes a figure that is blurred by the amount of the blur. Therefore, this detection signal usually has a shape as shown in 53, and by differentiating it, a waveform like 54 is obtained. Usually, the scanning distance of a portion from 12% to 88% of the rising portion in the differential signal is defined as a blur 55.
非点収差補正器の電流値 S 1、 S 2の組み合わせを変えながら、 以上 のようにして X軸方向への走査を行ってそのボケを測定し、 ボケが最小 となる組み合わせを見つければ、 それが y軸に平行な焦線に対応するも のとなる。 以上のようにして、 荷電流粒子線の走査方向を変化させなが らボケを測定することにより、 所定方向のボケが最小となる非点収差補 正器の電流値の組み合わせを見つけることができる。  While changing the combination of the current values S 1 and S 2 of the astigmatism corrector, scan in the X-axis direction and measure the blur as described above, and find the combination that minimizes the blur. Corresponds to a focal line parallel to the y-axis. As described above, by measuring the blur while changing the scanning direction of the charged current particle beam, it is possible to find the combination of the current values of the astigmatism corrector that minimizes the blur in the predetermined direction. .
以下、 このようにして求まつた非点収差ボケの発生感度を使用した荷 電粒子線露光方法の例について説明する。 この露光方法においては、 サ ブフィールド毎のパターンの開口率を考慮して、 クーロン効果の補正を サブフィールド毎に行う。 すなわち、 クーロン効果を補正するように、 投影光学系の焦点位置をサブフィールド毎に変える。 Hereinafter, an example of the charged particle beam exposure method using the sensitivity of occurrence of astigmatism blur determined in this way will be described. In this exposure method, the Coulomb effect is corrected in consideration of the aperture ratio of the pattern for each subfield. This is performed for each subfield. That is, the focal position of the projection optical system is changed for each subfield so as to correct the Coulomb effect.
まず、 求められた非点収差ボケの発生感度より、 非点収差ボケの補正 感度を求める。 すなわち、  First, the astigmatism blur correction sensitivity is determined from the obtained astigmatism blur occurrence sensitivity. That is,
Aを、 0 ° 方向コイルによる、 0— 9 0 ° 方向の非点収差ボケを発生さ せる非点収差ボケの発生感度 (すなわち、 0 ° 方向コイルに流す電流を 単位当たり増加させた場合の、 0 ° 方向ボケの増加量) A is the sensitivity of astigmatism blur which causes astigmatism blur in the 0-90 ° direction by the 0 ° direction coil (that is, when the current flowing through the 0 ° direction coil is increased per unit, 0 ° directional blur increase)
Bを、 4 5 ° 方向コイルによる、 0 ° — 9 0 ° 方向の非点収差ボケを発 生させる非点収差ボケの発生感度 (すなわち、 4 5 ° 方向コイルに流す 電流を単位当たり増加させた場合の、 0 ° 方向ボケの増加量) B, the sensitivity of astigmatism blur which causes astigmatism blur in the 0 ° -90 ° direction by the 45 ° direction coil (that is, the current flowing through the 45 ° direction coil was increased per unit) 0 ° direction bokeh increase in case)
Cを、 0 ° 方向コイルによる、 4 5 ° —135° 方向の非点収差ボケを発生 させる非点収差ボケの発生感度 (すなわち、 0 ° 方向コイルに流す電流 を単位当たり増加させた場合の、 9 0 ° 方向ボケの増加量)  C is the sensitivity of astigmatism blur which causes astigmatism blur in the 45 ° -135 ° direction by the 0 ° direction coil (that is, when the current flowing through the 0 ° direction coil is increased per unit, 90 ° increase in direction blur)
Dを、 4 5 ° 方向コイルにより、 4 5 ° —135° 方向の非点収差ボケを発 生させる非点収差ボケの発生感度 (すなわち、 4 5 ° 方向コイルに流す 電流を単位当たり増加させた場合の、 4 5 ° 方向ボケの増加量) とするとき、 非点収差ボケの発生感度行列 [X]を (A B\ D, the sensitivity of the astigmatism blur which causes 45 ° -135 ° direction astigmatism blur by the 45 ° direction coil (that is, the current flowing through the 45 ° direction coil was increased per unit) In the case, the amount of increase in the 45 ° direction blur), the astigmatism blur occurrence sensitivity matrix [X] is (AB \
[X} =  [X} =
1 1 、 Cし D u ) で定義し、 その逆行列である非点収差ボケの補正感度行列 [Y]を求める。 即ち
Figure imgf000036_0001
11 1 , C and Du), and find the inverse sensitivity matrix of the correction sensitivity matrix [Y] for astigmatism blur. That is
Figure imgf000036_0001
となる。 ここで、 It becomes. here,
Eは、 0 ° 方向コイルにより、 0— 9 0 ° 方向の非点収差ボケを補正す る場合の非点収差ボケの補正感度 Fは、 45 ° 方向コイルにより、 0— 90 ° 方向の非点収差ボケを補正 する場合の非点収差ボケの補正感度 E is the astigmatism blur correction sensitivity when the 0 ° -90 ° direction astigmatism blur is corrected by the 0 ° direction coil. F is the sensitivity of astigmatism blur correction when the astigmatism blur in the 0-90 ° direction is corrected by the 45 ° direction coil.
Gは、 0 ° 方向コイルにより、 45— 135° 方向の非点収差ボケを補正 する場合の非点収差ボケの補正感度  G is the astigmatism blur correction sensitivity when correcting the astigmatism blur in the 45-135 ° direction using the 0 ° direction coil.
Hは、 4 5° 方向コイルによ り、 4 5— 135° 方向の非点収差ボケを補 正する場合の非点収差ボケの補正感度  H is the astigmatism blur correction sensitivity when the 45-135 ° direction astigmatism blur is corrected by the 45 ° coil.
である。 It is.
クーロン効果による影響の変化や偏向位置が変わった等の理由により、 0— 90° 方向の非点収差ボケが _△ h。だけ発生し、 45 ° ― 135。 方 向の非点収差ボケが—△ h45だけ発生した場合、補正すべき非点ボケ量 は(Δΐΐο, Δ1ι45)になり、 0 ° 方向コイルに流す励磁電流、 45° 方向コ ィルに流す励磁電流を、 それそれ、
Figure imgf000037_0001
Due to changes in the influence of the Coulomb effect and changes in the deflection position, astigmatism blur in the 0-90 ° direction is _ △ h. Only occurs at 45 ° -135. Square astigmatism blur countercurrent is - △ If only occurs h 45, astigmatic blur quantity to be corrected (Δΐΐο, Δ1ι 45) becomes, the exciting current flowing in the 0 ° direction coils, a 45 ° direction co I le The exciting current that flows is
Figure imgf000037_0001
で計算される Δ I。、 △ I 4 5だけ変化させればよい。 ΔI calculated by It may be changed by △ I 4 5.
このようにして、 非点収差の小さい良好な結像パターンを得ることがで きる。 In this way, a good imaging pattern with small astigmatism can be obtained.
以上の説明においては、 焦点位置を正焦点位置から△ hだけ変化させ た状態で、 非点収差ボケの発生感度を求めたが、 複数の焦点位置におい て焦線が形成される非点収差補正器の電流値 S 1、 S 2を求め、 統計的 手法により非点収差ボケの発生感度を求めるようにしてもよい。 その一 例を、 以下に示す。  In the above description, the sensitivity of occurrence of astigmatism blur was obtained with the focus position changed from the normal focus position by △ h, but astigmatism correction in which focal lines are formed at a plurality of focus positions is performed. The current values S 1 and S 2 of the detector may be obtained, and the occurrence sensitivity of astigmatism blur may be obtained by a statistical method. An example is shown below.
焦点位置 hを h i ( i = l〜n ) と して、 n段階変化させ、 各焦点位 置において焦線が形成される場合の非点収差補正器の電流値の組み合わ せを前述のように表して (S 1い S 2 とし、 そのときの非点収差ボ ケパターンの角度を t iとする。 なお、 t iは通常は設計値を用いるが、 測定値を用いてもよい。 Assuming that the focal position h is hi (i = l to n) and is changed by n steps, the combination of the current values of the astigmatism corrector when a focal line is formed at each focal position is described above. Expressed as (S 1 or S 2, the angle of the astigmatism blur pattern at that time is ti. Note that ti is usually a design value, The measured value may be used.
そして、 以下の ( 3 5 ) 式、 ( 3 6 ) 式のような推定方程式を考える。 51-510 =r(/i-/i0)cos{2(i+i0)} ·'·(35) Then, an estimation equation such as the following equations (35) and (36) is considered. 51-51 0 = r (/ i- / i 0 ) cos {2 (i + i 0 )} '' (35)
<S2 - 52。 = — /¾)sin{2(i + i0)} '··(36) <S2-52. = — / ¾) sin {2 (i + i 0 )} '· (36)
ここで、 ( S I , S 2 ) は前述のような励磁電流の組み合わせ、 tは、 非点収差ボケパターンの角度(焦線が X軸になす角度と直角方向の角度) であり、 hと共に変数である。  Where (SI, S 2) is the combination of the exciting current as described above, t is the angle of the astigmatic blur pattern (the angle between the focal line and the X axis and the angle in the direction perpendicular to the X axis), and the variable together with h It is.
これに対し、 ( S 1。, S 2。) は、 前述のような焦線となる点が作る 円の中心点、 h。は正焦点位置、 rは (h— ]!。) が単位量変化するとき 変化する上記円の半径で比例定数、 t。は、 S 1軸に対する、 0 ° 方向 ボケだけが変化する方向のなす角の半分であって、 これらは、 いずれも 未知数である。 そして、 これらの未知数を、
Figure imgf000038_0001
であらわされる評価関数 Pが最小となるようにすることによって求める, 評価関数 Pを最小とする未知数を求める手法は、 周知の統計的手法を選 択して使用すればよい。
On the other hand, (S1, S2.) Is the center point of the circle created by the above-mentioned focal point, h. Is the focus position, and r is the proportional constant, which is the radius of the circle that changes when (h—]!) Changes by a unit amount, t. Is the half of the angle with respect to the S1 axis that only the 0 ° direction blur changes, and these are all unknowns. And these unknowns are
Figure imgf000038_0001
A known statistical method may be selected and used as a method of obtaining an unknown that minimizes the evaluation function P by minimizing the evaluation function P expressed by:
このようにして、 ( S l 。, S 2。)、 h。、 t 。、 rが求まると、 非点 収差ボケの補正感度行列は、  Thus, (S l., S 2.), h. , T. , R, the astigmatism blur correction sensitivity matrix is
frcos[itQ) 一 rsin(20)、 frcos [it Q ) rsin (2 0 ),
rsiru iQ) rcos(2t0) rsiru i Q ) rcos (2t 0 )
として求ま り、 その逆数である非点収差ボケの発生感度行列は、
Figure imgf000038_0002
The reciprocal of the astigmatism blur occurrence sensitivity matrix is
Figure imgf000038_0002
となる。 よって'、 ( 3 4 ) 式に対応する式は、
Figure imgf000039_0001
It becomes. Therefore, ', the equation corresponding to equation (34) is
Figure imgf000039_0001
となり、 クーロン効果による影響の変化や偏向位置が変わった等の理由 により、 0 — 9 0 ° 方向の非点収差ボケが Δ h。だけ発生し、 4 5 ° — 135° 方向の非点収差ボケが A h4 5だけ発生した場合、 0 ° 方向にコィ ルに流す励磁電流、 4 5 ° 方向コイルに流す励磁電流を、 それそれ、 ( 3 7 ) 式で計算される Δ Ι 。、 △ I 45だけ変化させればよい。 The astigmatism blur in the 0 to 90 ° direction is Δh due to changes in the influence of the Coulomb effect and changes in the deflection position. Only it occurs, 4 5 ° - 135 If the astigmatism blur of ° direction occurs only A h 4 5, the excitation current flowing in the direction of 0 ° to Koi Le, the exciting current applied to 4 5 ° direction coils, it it , Δ 計算 calculated by equation (37). , ΔI 45 may be changed.
逆に、 0 ° 方向にコイルに流す励磁電流、 4 5 ° 方向コイルに流す励 磁電流を、 それそれ Δ Ι 。、 △ I 4 5だけ変化させたときの、 0 — 9 0 ° 方向の非点収差ボケ△ と、 4 5 ° — 135° 方向の非点収差ボケ△ h 4 Conversely, the excitation current flowing through the coil in the 0 ° direction and the excitation current flowing through the 45 ° direction coil are Δ Δ. , △ I of 4 5 only when changing, 0 - 9 0 astigmatism blur of ° direction △, 4 5 ° - 135 astigmatism blur of ° direction △ h 4
5は、 5 is
Ah0 \ ( cos( 2t0)/r sin(2/0) / ( Δ/。、 Ah 0 \ (cos (2t 0 ) / r sin (2/0) / (Δ /.,
•(38)  • (38)
Ah45 J I - sin(2i0) I r cos(2i0)/ rj Δ 45Ah 45 JI-sin (2i 0 ) I r cos (2i 0 ) / rj Δ 45 no
で与えられることになる。 Will be given by
本発明の実施の形態を適用する荷電粒子線露光装置は、 図 6に示すも のと同じである。 本実施の形態においては、 前述のような方法により、 各方向の非点収差ボケの補正感度を求めておき、 シミュレーショ ンによ り、 空間電荷効果による非点収差ボケの変化量 (正焦点位置の変化に換 算したもの) を求め、 この非点収差ボケの変化量に各方向の非点収差ボ ケの補正感度をかけた値だけ各コィルの電流値を変化させればよい。 以下、 このようにして求まった非点収差ボケの補正感度を使用した荷 電粒子線露光方法の例について説明する。 この露光方法においては、 サ ブフィール ド毎のパターンの開口率を考慮して、 クーロン効果の補正を サブフィール ド毎に行う。 すなわち、 クーロン効果を補正するように、 投影光学系の焦点位置をサブフィールド毎に変える。 また、 同時に偏向位置の変化に伴って発生する非点収差の量を、 焦点 位置の変化に換算し、 それに前述のような方法で求めた非点収差ボケの 補正感度をかけた値だけ、非点収差補正器の 0 ° 方向コイルに流す電流、 及び 4 5 ° 方向コイルに流す電流を、 合わせて変化させることにより、 偏向に伴う非点収差その物も補正する。 このようにして、 非点収差の小 さい良好な結像パターンを得ることができる。 The charged particle beam exposure apparatus to which the embodiment of the present invention is applied is the same as that shown in FIG. In the present embodiment, the correction sensitivity of astigmatism blur in each direction is obtained by the method described above, and the amount of change in astigmatism blur due to the space charge effect (positive focus) is determined by simulation. The current value of each coil may be changed by the value obtained by multiplying the amount of change in astigmatism blur by the correction sensitivity of astigmatism blur in each direction. Hereinafter, an example of the charged particle beam exposure method using the correction sensitivity for astigmatism blur determined as described above will be described. In this exposure method, the Coulomb effect is corrected for each subfield in consideration of the aperture ratio of the pattern for each subfield. That is, the focal position of the projection optical system is changed for each subfield so as to correct the Coulomb effect. At the same time, the amount of astigmatism that occurs due to the change in the deflection position is converted into a change in the focal position, and the resulting value is multiplied by the correction sensitivity for astigmatism blur determined by the method described above, and the resulting value is calculated as the astigmatism. The astigmatism associated with the deflection is also corrected by changing the current flowing through the 0 ° direction coil and the current flowing through the 45 ° direction coil of the astigmatism corrector. In this way, a good imaging pattern with small astigmatism can be obtained.

Claims

請 求 の 範 囲 The scope of the claims
1. 非点収差補正器を有する荷電粒子線露光装置において、 焦点位置 を厶 hずらし、 前記非点収差補正器の電流値又は電圧値を変化させるこ とにより少なく とも異なる 2つの焦線を形成する、 前記非点収差補正器 の電流値又は電圧値を求め、 前記焦点位置のずらし量 Δ h、 及び前記異 なる 2組の焦線を形成する前記非点収差補正器の電流値又は電圧値を用 いて前記非点収差補正器の非点感度 (非点収差ボケの補正感度、 又は非 点収差ボケ発生感度) を求めることを特徴とする非点感度の決定方法。 1. In a charged particle beam exposure apparatus having an astigmatism corrector, at least two different focal lines are formed by shifting a focal position by h and changing a current value or a voltage value of the astigmatism corrector. A current value or a voltage value of the astigmatism corrector, the shift amount Δh of the focal position, and a current value or a voltage value of the astigmatism corrector forming the two different sets of focal lines. A method for determining astigmatic sensitivity, wherein the astigmatic sensitivity of the astigmatism corrector (the astigmatic blur correction sensitivity or the astigmatic blur occurrence sensitivity) is obtained using the following formula.
2. 前記非点収差補正器が少なく とも 2組のコイル群または電極群を 有することを特徴とする請求の範囲第 1項に記載の非点感度の決定方法, 2. The method for determining astigmatism according to claim 1, wherein the astigmatism corrector has at least two coil groups or electrode groups.
3. 焦点位置を Δ hずらす際に、 正焦点位置を基準として、 焦点位置 を正焦点位置から△ hずらすことを特徴とする請求の範囲第 1項に記載 の非点感度の決定方法。 3. The method for determining astigmatism sensitivity according to claim 1, wherein, when the focal position is shifted by Δh, the focal position is shifted by △ h from the positive focal position with reference to the positive focal position.
4. 前記非点感度が、 非点収差ボケの補正感度であることを特徴とす る請求の範囲第 1項に記載の非点感度の決定方法。 4. The method for determining astigmatism according to claim 1, wherein the astigmatism is a correction sensitivity for astigmatism blur.
5. 前記非点感度が、 非点収差ボケ発生感度であることを特徴とする 請求の判に第 1項に記載の非点感度の決定方法。  5. The method for determining astigmatism according to claim 1, wherein the astigmatism is an astigmatism blur occurrence sensitivity.
6. 請求の範囲第 4項に記載の非点感度の決定方法であって、 焦点位 置を正焦点位置から△ hだけずらした上で、 非点収差補正器を構成する 6. The method for determining astigmatism according to claim 4, wherein the astigmatism corrector is configured after shifting the focal position from the positive focal position by 正 h.
2組のコィル群 ( 0 ° 方向コィル及び 4 5 ° 方向コィル) の電流値又は 2組の電極群 ( 0 ° 方向電極及び 4 5 ° 方向電極) の電圧値をそれそれ 変化させ、 測定パターンを基準とした 9 0 ° 方向、 0 ° 方向、 1 3 5 ° 方向、 4 5 ° 方向のボケが最小となる前記 2組の電流値又は電圧値をそ れそれ求め、 これらの電流値又は電圧値の組み合わせをそれそれ ( S 1 1, S 2 1 )、 ( S 1 2 , S 2 2 )、 ( S 1 3 , S 2 3 )、 ( S 1 , S 2 4 ) とするとき、 次の少なく とも一つの式により、 少なく とも一つの方向の 非点収差ボケの補正感度を決定することを特徴とする荷電粒子線露光装 置における非点感度の決定方法。 The current value of the two coil groups (0 ° direction coil and 45 ° direction coil) or the voltage value of the two electrode groups (0 ° direction electrode and 45 ° direction electrode) is varied, and the measurement pattern is changed. The two sets of current values or voltage values that minimize the blur in the 90 ° direction, 0 ° direction, 135 ° direction, and 45 ° direction as the reference are obtained, and these current values or voltage values are obtained. (S11, S21), (S12, S22), (S13, S23), (S1, S24) A method for determining astigmatism in a charged particle beam exposure apparatus, wherein the sensitivity for correcting astigmatism blur in at least one direction is determined by at least one of the following expressions.
(1)0 ° 方向コイル又は電極により、 0— 90° 方向の非点収差ボケを補 正する場合の非点収差ボケの補正感度  (1) Sensitivity for correcting astigmatism blur when correcting 0-90 ° direction astigmatism blur using a 0 ° direction coil or electrode
511-512  511-512
2Δ/ι  2Δ / ι
(2)45 ° 方向コイル又は電極によ り、 0— 90° 方向の非点収差ボケ を補正する場合の非点収差ボケの補正感度  (2) Sensitivity for correcting astigmatism blur when correcting astigmatism blur in the 0-90 ° direction using a 45 ° direction coil or electrode
521-522 ^  521-522 ^
·'·(2)  · '· (2)
2Ah ,  2Ah,
(3) 0 ° 方向コィル又は電極により、 45— 135° 方向の非点収差ボケを 補正する場合の非点収差ボケの補正感度 13- 14 ...(3) (3) by 0 ° direction Koiru or electrodes, correction sensitivity 1 3 astigmatism blur when correcting astigmatism blur of 45- 135 ° direction - 14 ... (3)
(4) 45 ° 方向コイル又は電極により、 45— 135° 方向の非点収差ボケ を補正する場合の非点収差ボケの補正感度 (4) Sensitivity of astigmatic blur correction when 45-135 ° astigmatic blur is corrected by a 45 ° coil or electrode
523-524 523-524
•(4)  •(Four)
2Δ/ι  2Δ / ι
ただし、 S i j ( i = 1 , 2、 j = 1〜 4 ) の iは、 それそれ 0。 方 向コイル又は電極 ( i二 1 )、 45° 方向コイル又は電極 ( i = 2 ) を示 し、 jは、 それそれ非点収差ボケが最小となる方向 ( j = 1は 9 0 ° 方 向、 = 2は0 ° 方向、 j = 3は 1 35。 方向、 j = 4は 45。 方向) を示す。  However, i of S i j (i = 1, 2, j = 1 to 4) is 0 for each. A directional coil or electrode (i2 1) indicates a 45 ° directional coil or electrode (i = 2), and j indicates the direction in which astigmatism blur is minimized (j = 1 is 90 ° direction). , = 2 is 0 ° direction, j = 3 is 135. direction, j = 4 is 45. direction).
7. 請求の範囲第 4項に記載の非点感度の決定方法であって、 非点収 差補正器を構成する 2組のコイル群 (0° 方向コイル及び 45 ° 方向コ ィル) の電流値又は 2組の電極群 ( 0 ° 方向電極及び 45 ° 方向電極) の電圧値をそれそれ変化させ、 測定パターンを基準とした 9 0 ° 方向、 0 ° 方向、 1 3 5 ° 方向、 4 5 ° 方向のボケが最小となる前記 2組の電 流値又は電圧値をそれそれ求め、 これを、 光軸方向の任意の位置 Aと A か.ら光軸方向に△ hだけ離れた位置 Bにおいて行い、 7. The method for determining astigmatism according to claim 4, wherein the currents of two sets of coils (0 ° direction coil and 45 ° direction coil) constituting the astigmatic error compensator are set. Value or the voltage value of the two sets of electrodes (0 ° direction electrode and 45 ° direction electrode), respectively, to change the 90 ° direction with respect to the measurement pattern. Determine the two sets of current values or voltage values that minimize the blur in the 0 ° direction, the 135 ° direction, and the 45 ° direction, and determine whether these are arbitrary positions A and A in the optical axis direction. At the position B, which is △ h away from the optical axis direction,
これらの電流値の組み合わせをそれそれ ( S 1 1 A S 2 1 A)、 ( S 1Each combination of these current values (S1 1A S2 1A), (S1
2 A S 2 2 A) ( S 1 3 A, S 2 3 A) ( S 1 4 A, S 2 4 A)s ( S2 AS 2 2 A) (S 13 A, S 23 A) (S 14 A, S 24 A) s (S
1 1 B , S 2 1 B)、 ( S 1 2 B S 2 2 B)、 ( S 1 3 B , S 2 3 B) ( S1 1 B, S 2 1 B), (S 1 2 B S 2 2 B), (S 13 B, S 23 B) (S
1 4 B , S 2 4 B ) とするとき、 次の少なく とも一つの式により、 少な く とも一つの方向の非点収差ボケの補正感度を決定することを特徴とす る荷電粒子線露光装置における非点感度の決定方法。 14B, S24B), the charged particle beam exposure apparatus characterized in that the correction sensitivity of at least one direction of astigmatism blur is determined by at least one of the following equations: Method for determining astigmatism sensitivity in
(1)0 ° 方向コィル又は電極により、 0— 9 0 ° 方向の非点収差ボケを補 正する場合の非点収差ボケの補正感度  (1) Sensitivity of astigmatism blur correction when astigmatism blur in the 0-90 ° direction is corrected by a 0 ° direction coil or electrode
snB-si2B _snA-si2A ) sn B -si2 B _sn A -si2 A )
、 2Ah 2Ah )  , 2Ah 2Ah)
(2) 4 5 ° 方向コイル又は電極により、 0— 9 0 ° 方向の非点収差ボケを 補正する場合の非点収差ボケの補正感度  (2) Sensitivity for correcting astigmatism blur when correcting astigmatism blur in the 0 to 90 ° direction using a 45 ° direction coil or electrode
/S2L-S22„ S21.-S22. / S2L-S22 „S21.-S22.
( ^ ^ ^ ,··(6) (^ ^ ^, (6)
2ΔΛ 2Ah  2ΔΛ 2Ah
(3) 0 ° 方向コィル又は電極により、 4 5 — 135° 方向の非点収差ボケを 補正する場合の非点収差ボケの補正感度  (3) Sensitivity for correcting astigmatism blur when correcting astigmatism blur in the direction of 45-135 ° using a 0 ° direction coil or electrode
,S13。 — S14„ S13. -S14, , S13. — S14 „S13. -S14,
-) …(フ)  -)… (F)
、 2Ah 2Ah  , 2Ah 2Ah
(4)4 5 ° 方向コィル又は電極により、 4 5 — 135° 方向の非点収差ボケ を補正する場合の非点収差ボケの補正感度(4) Sensitivity of astigmatic blur correction when astigmatic blur in the direction of 45-135 ° is corrected with a 45 ° directional coil or electrode
523。ー 24。一 S23 S24  523.ー 24. One S23 S24
■ ) .-.(8)  ■) .-. (8)
2Ah 2Ah  2Ah 2Ah
ただし、 S i j A、 S i j B ( i 二 1 , 2、 j 二 1〜 4 ) の iは、 そ れそれ 0。 方向コィル又は電極( i = 1 )、 4 5 ° 方向コィル又は電極( i = 2 ) を示し、 jは、 それそれ非点収差ボケが最小となる方向 ( j = l は 9 0。 方向、 (]' = 2は 0 ° 方向、 j = 3は 1 3 5 ° 方向、 j = 4は 4 50 方向) を示す。 However, i of S ij A and S ij B (i 2 1,2, j 2 1 to 4) is 0 for each. Indicates the direction coil or electrode (i = 1), 45 ° direction coil or electrode (i = 2), and j is the direction in which astigmatism blur is minimized (j = l). Is 90. Direction, ( ] '= 2 indicates 0 ° direction, j = 3 indicates 135 ° direction, j = 4 indicates 450 direction).
8. 請求の範囲第 5項に記載の非点感度の決定方法であって、 焦点位 置を正焦点から A hだけずらした上で、 非点収差補正器を構成する 2組 のコイル群 ( 0 ° 方向コイル及び 4 5。 方向コイル) の電流値又は 2組 の電極群 ( 0。 方向電極及び 4 5 ° 方向電極) の電圧値をそれそれ変化 させ、測定パターンを基準とした 9 0 ° 方向、 0 ° 方向、 1 3 5 ° 方向、 4 50 方向のボケが最小となる前記 2組の電流値又は電圧値をそれそれ 求め、 これらの電流値又は電圧値の組み合わせをそれぞれ ( S 1 1 , S 2 1 )、 ( S 1 2 , S 2 2 )、 ( S 1 3 , S 2 3 )、 ( S 1 4 , S 2 4 ) とす るとき、 次の少なく とも一つの式により、 少なく とも一つの方向の非点 収差ボケの発生感度を決定することを特徴とする荷電粒子線露光装置に おける非点感度の決定方法。 8. The method for determining astigmatism according to claim 5, wherein the focus position is shifted from the positive focus by Ah, and then two sets of coils forming the astigmatism corrector ( The current value of the 0 ° directional coil and 45. directional coil) or the voltage value of two sets of electrodes (0. directional electrode and 45 ° directional electrode) are varied, and 90 ° based on the measurement pattern. direction, 0 ° direction, 1 3 5 ° directions, the 4 5 0 the direction of the blur is minimum two pairs of current value or voltage value which it asked, each a combination of these current values or voltage values (S 1 1, S 21), (S 12, S 22), (S 13, S 23), (S 14, S 24), by at least one of the following equations: A method for determining astigmatism in a charged particle beam exposure apparatus, wherein the method determines the sensitivity of occurrence of astigmatism blur in at least one direction.
(1) 0 ° 方向コイル又は電極により、 0— 9 0 ° 方向の非点収差ボケを発 生させる非点収差ボケの発生感度 一 2AA(S23-S24)  (1) Sensitivity of astigmatism blur that causes astigmatism blur in the 0-90 ° direction by a 0 ° direction coil or electrode-1AA (S23-S24)
{(Sll - SI 2)(S23 - 24) - (S13 - S14)(S21 - 522)} ( )  {(Sll-SI 2) (S23-24)-(S13-S14) (S21-522)} ()
(2) 4 5 ° 方向コイル又は電極により、 0 ° — 9 0 ° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度 -2 (S13-^14) (2) Sensitivity of astigmatism blur that generates astigmatism blur in the 0 ° to 90 ° direction using a 45 ° direction coil or electrode -2 (S13- ^ 14)
{(511-S12)(523 - 24)-(513-S14XS21-S22)} 、 ) (3)0 ° 方向コイル又は電極により、 4 5 ° — 135° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度
Figure imgf000044_0001
{(511-S12) (523-24)-(513-S14XS21-S22)},) (3) Astigmatism that causes astigmatism blur in the 45 ° -135 ° direction by the 0 ° direction coil or electrode Occurrence sensitivity of aberration blur
Figure imgf000044_0001
{(SI 1 - S12)(S23 - 24) - (S13 - S14)(S21 - S22)} (4)4 5 ° 方向コィル又は電極により、 4 5。 一 135° 方向の非点収差ボ ケを発生させる非点収差ボケの発生感度 {(SI1-S12) (S23-24)-(S13-S14) (S21-S22)} (4) 45 ° with a directional coil or electrode. 135 ° astigmatism Sensitivity of astigmatism blur causing blur
2 (511-512)  2 (511-512)
•(12)  • (12)
{(511- 512)(523 - 24、 - (513 - 514)(S21 -522)}  {(511-512) (523-24,-(513-514) (S21 -522)}
9. 請求の範囲第 5項に記載の非点感度の決定方法であって、 非点収 差補正器を構成する 2組のコイル群 ( 0 ° 方向コイル及び 4 5 ° 方向コ ィル) の電流値又は 2組の電極群 ( 0 ° 方向電極及び 4 5 ° 方向電極) の電圧値をそれそれ変化させ、 測定パターンを基準とした 9 0 ° 方向、 0 ° 方向、 1 3 5 ° 方向、 4 5 ° 方向のボケが最小となる前記 2組の電 流値又は電圧値をそれそれ求め、 これを、 光軸方向の任意の位置 Aと A から光軸方向に△ hだけ離れた位置 Bにおいて行い、 9. The method for determining astigmatism sensitivity according to claim 5, wherein the two groups of coils (0 ° direction coil and 45 ° direction coil) constituting the astigmatic error compensator are provided. The current value or the voltage value of the two sets of electrodes (0 ° direction electrode and 45 ° direction electrode) is changed, and the 90 ° direction, 0 ° direction, 135 ° direction, 45 The two sets of current values or voltage values at which the blur in the 5 ° direction is minimized are determined, and these are determined as arbitrary positions A and A in the optical axis direction at a position B that is △ h away from the arbitrary optical axis direction in the optical axis direction. Done in
これらの電流値の組み合わせをそれそれ ( S 1 1 A, S 2 1 A)、 ( S 1 2 A, S 2 2 A)S ( S 1 3 A, S 2 3 A)ヽ ( S 1 4 A, S 2 4 A)ヽ ( S 1 1 B, S 2 1 B)ヽ ( S 1 2 B , S 2 2 B)s ( S 1 3 B, S 2 3 B)、 ( S 1 4 B , S 2 4 B) とするとき、 次の少なく とも一つの式により、 少な く とも一つの方向の非点収差ボケの発生感度を決定することを特徴とす る荷電粒子線露光装置における非点感度の決定方法。 The combination of these current values is (S11A, S21A), (S12A, S22A) S (S13A, S23A) ヽ (S14A , S 24 A) ヽ (S 11 B, S 21 B) ヽ (S 12 B, S 22 B) s (S 13 B, S 23 B), (S 14 B, S 24 B), the sensitivity of occurrence of astigmatism blur in at least one direction is determined by at least one of the following expressions. Decision method.
(1) 0 ° 方向コイル又は電極により、 0— 9 0 ° 方向の非点収差ボケを発 生させる非点収差ボケの発生感度  (1) Sensitivity of astigmatism blur that causes astigmatism blur in the 0-90 ° direction by the 0 ° direction coil or electrode
2Ah{(S23B-S24B)-(S23A-S24A)} … ) 2Ah {(S23 B -S24 B )-(S23 A -S24 A )}…)
Δ  Δ
(2) 4 5 ° 方向コイル又は電極により、 0 ° — 9 0 ° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度  (2) Sensitivity of astigmatism blur that generates astigmatism blur in the 0 ° to 90 ° direction by a 45 ° direction coil or electrode
-2 h{(S13B-SUB)-(S13A-SUA)} -2 h {(S13 B -SU B )-(S13 A -SU A )}
Δ 、 )  Δ,)
(3) 0 ° 方向コイル又は電極により、 4 5 ° — 135° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度  (3) Sensitivity of astigmatism blur that generates astigmatism blur in 45 ° -135 ° direction by 0 ° direction coil or electrode
-2Ahj(S21B-S22B)-(S21A-S22A)} … ) -2Ahj (S21 B -S22 B )-(S21 A -S22 A )}…)
Δ (4)45 ° 方向コィル又は電極により、 45 ° — 135° 方向の非点収差ボ ケを発生させる非点収差ボケの発生感度 Δ (4) Sensitivity of astigmatic blur that causes 45 ° to 135 ° astigmatic blur by 45 ° directional coil or electrode
2 h{(SllB-S12B)-(SllA-S12A)} 2 h {(Sll B -S12 B )-(Sll A -S12 A )}
Δ  Δ
ただし、 S i j A、 S i j B ( i = 1 , 2、 j = 1〜 4 ) の iは、 そ れそれ 0° 方向コィル又は電極( i = 1 )、 45 ° 方向コイル又は電極( i Here, i of SijA and SijB (i = 1, 2, j = 1 to 4) are 0 ° direction coil or electrode (i = 1), 45 ° direction coil or electrode (i
= 2) を示し、 jは、 それそれ非点収差ボケが最小になる方向 (j = l は 90° 方向、 ' = 2は0。 方向、 j = 3は 1 35° 方向、 j =4は 4= 2) where j is the direction in which the astigmatism blur is minimized (j = l is the 90 ° direction, '= 2 is the 0. direction, j = 3 is the 135 ° direction, and j = 4 is the Four
5 ° 方向) を示し、 厶は、 5 ° direction).
A = [{(S11B -S12B)-(S11A -S12A)}{(S23B-S24B)-(S23A-S24A)} ~{(S13B -S14B)-(S13A - S14A)}{(S21B -S22B) - {S2\A -S22A)}}で 示される値である。 A = [{(S11 B -S12 B )-(S11 A -S12 A )} {(S23 B -S24 B )-(S23 A -S24 A )} ~ {(S13 B -S14 B )-(S13 A - S14 a)} - is the value represented by {(S21 B -S22 B) { S2 \ a -S22 a)}}.
10. 請求の範囲第 5項に記載の非点感度の決定方法であって、 焦点 位置を正焦点位置から Δ hだけずらした上で、 前記非点収差補正器を構 成する 2組のコィル群 ( 0 ° 方向コィル及び 45 ° 方向コイル) の電流 値又は 2組の電極群 ( 0 ° 方向電極及び 45 ° 方向電極) の電圧値 (そ れそれを S I , S 2とする) をそれそれ変化させ、 角度が 0だけ異なる 2つの方向のボケが最小となる前記 2組のコイル群の電流値又は 2組の 電極群の電圧値をそれそれ求め、 これらの電流値又は電圧値の組み合わ せをそれそれ (S 1 5 , S 25)、 (S 1 6, S 26) とし、 S I— S 2 直交座標系において、下に示す( S 1。 , S 2。 )を中心とし、 ( S 1 5 , S 25)、 (S 1 6 , S 2 6 ) を通る円を求め、 この円を、 焦線を形成す る前記 2組の電流値又は電圧値の組み合わせを表す円とし、 この円の所 定の点における、 非点収差ボケが最小となる方向に基づいて、 少なく と も一つの方向の非点収差ボケの発生感度を決定することを特徴とする荷 電粒子線露光装置における非点感度の決定方法。 {(515 + 516) ±(525- S26) cot Θ} … ?) 10. The method for determining astigmatism according to claim 5, wherein a focus position is shifted from a positive focus position by Δh, and then two coils constituting the astigmatism corrector are provided. The current value of the group (0 ° directional coil and 45 ° directional coil) or the voltage value of the two electrode groups (0 ° directional electrode and 45 ° directional electrode) (these shall be SI and S2), respectively. The current value of the two sets of coils or the voltage value of the two sets of electrodes, which minimize the blur in the two directions where the angles differ by 0, are determined, and a combination of these current values or voltage values is obtained. Are defined as (S 15, S 25) and (S 16, S 26), respectively, and in the SI—S 2 rectangular coordinate system, centered on (S 1, S 2.) 5, S25) and a circle passing through (S16, S26) are obtained, and this circle is defined as a circle representing the combination of the two sets of current values or voltage values forming the focal line. A charged particle beam exposure method for determining the sensitivity of occurrence of astigmatism blur in at least one direction based on a direction in which astigmatism blur is minimized at a predetermined point of the circle. A method for determining astigmatism in an apparatus. {(515 + 516) ± (525- S26) cot Θ}…? )
S2 {(525 + 526) + (515 - 516) cot Θ} … ) S2 {(525 + 526) + (515-516) cot Θ}…)
0一 2 0-1 2
1 1. 請求の範囲第 5項に記載の非点感度の決定方法であって、 焦点 位置を正焦点位置から Δ hだけずら した上で、 前記非点収差補正器を構 成する 2組のコイル群 ( 0 ° 方向コイル及び 4 5 ° 方向コイル) の電流 値又は 2組の電極群 ( 0 ° 方向電極及び 4 5 ° 方向電極) の電圧値 (そ れそれを S l, S 2とする) をそれそれ変化させ、 角度が Θだけ異なる 1 1. The method for determining astigmatism according to claim 5, wherein the astigmatism corrector is configured such that a focus position is shifted from a positive focus position by Δh, and Current value of coil group (0 ° direction coil and 45 ° direction coil) or voltage value of two sets of electrodes (0 ° direction electrode and 45 ° direction electrode) (S1 and S2 respectively) ), And the angle differs by Θ
2つの方向のボケが最小となる前記 2組のコイル群の電流値又は 2組の 電極群の電圧値をそれそれ求め、 これらの電流値又は電圧値の組み合わ せをそれそれ ( S 1 5, S 2 5 )、 ( S 1 6 , S 2 6 ) とし、 S I— S 2 直交座標系において、下に示す( 3 1。 , 32。 )を中心とし、 ( 3 1 5 , S 2 5 )、 ( S 1 6, S 2 6 ) を通る円上において、 パターン基準方向に 対して 9 0 ° 方向、 135° 方向の非点収差ボケが最小となる前記 2組の 電流値又は電圧値をそれそれ求め、 それそれの組み合わせを ( S 1 1 ', S 2 1,)、 ( S 1 3 S 2 3 ' ) とするとき、 次の ( 1 9 ) 〜 ( 2 2 ) 式 の少なく とも一つにより、 少なく とも一つの方向の非点収差ボケの発生 感度を決定することを特徴とする荷電粒子線露光装置における非点感度 の決定方法。 The current value of the two sets of coils or the voltage value of the two sets of electrodes that minimizes the blur in the two directions is determined, and the combination of these current values or voltage values is determined as (S15, S 2 5), (S 16, S 26), and in the SI-S 2 rectangular coordinate system, centered on (31., 32.) shown below, (3 15, S 25), On a circle passing through (S16, S26), the two sets of current or voltage values that minimize astigmatism blur in the 90 ° direction and 135 ° direction with respect to the pattern reference direction are deviated. When (S 1 1 ', S 21) and (S 13 S 2 3') are combined, at least one of the following equations (1 9) to (2 2) A method for determining astigmatic sensitivity in a charged particle beam exposure apparatus, comprising determining sensitivity to occurrence of astigmatism blur in at least one direction.
S1 ― {(515 + ± (525 -526) cot Θ} …" S1 ― {(515 + ± (525 -526) cot Θ}… "
 M
S2 _ {(525 + 526) + (515 -516) cot 6>} …"^ S2 _ {(525 + 526) + (515 -516) cot 6>}… "^
(1))0 ° 方向コイル又は電極により、 0— 9 0 ° 方向の非点収差ボケを発 生させる非点収差ボケの発生感度
Figure imgf000047_0001
(2) 4 5 ° 方向コイル又は電極により、 0 ° — 9 0 ° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度
(1) Sensitivity of astigmatism blur which causes astigmatism blur in 0-90 ° direction by 0 ° direction coil or electrode
Figure imgf000047_0001
(2) Sensitivity of astigmatism blur that generates astigmatism blur in the 0 ° to 90 ° direction by a 45 ° direction coil or electrode
- (S13'-S10) … - (S13'-S1 0) ...
{rSll,-Sl0)(S23'-S20)-(S13,-Sl0XS21,-S20)} ) (rSll , -Sl 0 ) (S23'-S2 0 )-(S13 , -Sl 0 XS21 , -S2 0 )})
(3) 0 ° 方向コイル又は電極により、 4 5 ° — 135° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度  (3) Sensitivity of astigmatism blur that generates astigmatism blur in 45 ° -135 ° direction by 0 ° direction coil or electrode
- (S21'-S20) -(S21'-S2 0 )
{(S11'-S10)(S23,-S20)-(S13,-S10)(S21,-S20)} {(S11'-S1 0) ( S23, -S2 0) - (S13, -S1 0) (S21, -S2 0)}
(4) 4 5 ° 方向コイル又は電極により、 4 5 ° —135° 方向の非点収差ボ ケを発生させる非点収差ボケの発生感度 ^IV-S^) ...(22) (4) Sensitivity of astigmatism blur that generates astigmatism blur in the direction of 45 ° -135 ° using a 45 ° direction coil or electrode ^ IV-S ^) ... (22)
{ (511 '- Sl0 )(523 '- S 20 ) - (S 13 '- 510 )(521 '- 520 )} 1 2. 請求の範囲第 5項に記載の非点感度の決定方法であって、 焦点 位置を正焦点位置から Δ hだけずらした上で、 前記非点収差補正器を構 成する 2組のコィル群 ( 0 ° 方向コィル及び 4 5。 方向コイル) の電流 値又は 2組の電極群 (.0 ° 方向電極及び 4 50 方向電極) の電圧値をそ れそれ変化させ、 角度が異なる 3つ以上の方向の非点収差ボケが最小と なる前記 2組のコイル群 ( 0 ° 方向コイル及び 4 5 ° 方向コイル) の電 流値又は 2組の電極群( 0 ° 方向電極及び 4 5 ° 方向電極)の電圧値(そ れそれを S l, S 2 とする) をそれそれ求め、 これらの電流値又は電圧 値の組み合わせをそれそれ ( S l l, S 2 1 )、 ( S 1 2 , S 2 2 )、 ···、 ( S l n, S 2 n) とするとき (ηは 3以上の整数)、 S 1 — S 2直交座 標系において、 これらの点を通る円を、 方程式を解くか又は統計的な当 てはめ法により求め、 この円の所定の点における、 非点収差ボケが最小 となる方向に基づいて、 少なく とも一つの方向の非点収差ボケの発生感 度を決定することを特徴とする荷電粒子線露光装置における非点感度の 決定方法。 {(511 '- Sl 0) (523' - S 2 0) - (S 13 '- 51 0) (521' - 52 0)} 1 2. Determination of astigmatism sensitivity according to claim 5 After shifting the focus position from the positive focus position by Δh, the current values of the two coil groups (0 ° direction coil and 45. direction coil) constituting the astigmatism corrector are obtained. Alternatively, the voltage values of the two electrode groups ( 0.0 ° direction electrode and 450 direction electrode) are varied, and the astigmatism blur in three or more directions at different angles is minimized. The current value of the coil group (0 ° direction coil and 45 ° direction coil) or the voltage value of two sets of electrodes (0 ° direction electrode and 45 ° direction electrode) (S1 and S2, respectively) (S ll, S 21), (S 12, S 22), ..., (S ln, S 2 n) (Η is an integer of 3 or more), S 1 — S 2 In a co-ordinated coordinate system, a circle passing through these points is determined by solving an equation or by a statistical fitting method, and based on the direction at which the astigmatism blur at a given point on this circle is minimized. A method for determining astigmatism in a charged particle beam exposure apparatus, comprising determining a sensitivity of occurrence of astigmatism blur in at least one direction.
1 3. 請求の範囲第 5項に記載の非点感度の決定方法であって、 焦点 位置を正焦点位置から A hだけずらした上で、 前記非点収差補正器を構 成する 2組のコイル群 ( 0。 方向コイル及び 4 5 ° 方向コイル) の電流 値又は 2組の電極群 ( 0 ° 方向電極及び 4 5 ° 方向電極) の電圧値をそ れそれ変化させ、 角度が異なる 3つ以上の方向の非点収差ボケが最小と なる前記 2組のコイル群 ( 0。 方向コイル及び 4 5 ° 方向コイル) の電 流値又は 2組の電極群 ( 0 ° 方向電極及び 4 5 ° 方向電極) の電圧値を (それそれを S I , S 2 とする) それそれ求め、 これらの電流値又は電 圧値の組み合わせをそれそれ( S 1 1 , S 2 1 )、 ( S 1 2 , S 2 2 )、 ···、 ( S l n, S 2 n) とするとき (nは 3以上の整数)、 S 1— S 2直交座 標系において、 これらの点を通る円を、 方程式を解くか又は統計的な当 てはめ法により求め、 その中心を ( S 1 。 , S 2。 ) とし、 その円上に おいて、 パターン基準方向に対して 9 0 ° 方向、 135° 方向の非点収差 ボケが最小となる前記 2組の電流値又は電圧値をそれそれ求め、 それそ れの組み合わせを ( S l l,, S 2 1,)、 ( S 1 3,, S 2 3 ') とすると き、 次の ( 1 9 ) 〜 ( 2 2 ) 式の少なく とも一つにより、 少なく とも一 つの方向の非点収差ボケの発生感度を決定することを特徴とする荷電粒 子線露光装置における非点感度の決定方法。 1 3. The method for determining astigmatism according to claim 5, wherein the focus position is shifted from the positive focus position by Ah, and then the astigmatism corrector is configured. The current value of the coil group (0. directional coil and 45 ° directional coil) or the voltage value of two sets of electrode groups (0 ° directional electrode and 45 ° directional electrode) are changed, and three angles are different. The current values of the two sets of coils (0. direction coil and 45 ° direction coil) or the two sets of electrode groups (0 ° direction electrode and 45 ° direction) that minimize astigmatism blur in the above directions The voltage value of the electrode is determined as SI, S2, and the combination of these current values or voltage values is determined as (S11, S21), (S12, S12). 2 2),..., (S ln, S 2 n) (n is an integer of 3 or more), the circle passing through these points in the S 1—S 2 orthogonal coordinate system is Solve the equations or find them by statistical fitting, center them at (S 1, S 2), and on the circle, 90 ° and 135 ° directions with respect to the pattern reference direction The two sets of current values or voltage values that minimize the astigmatism blur of each of them are determined, and the combinations thereof are defined as (Sll ,, S21,), (S13, S23 '). ), The charged particle beam exposure characterized in that the sensitivity of occurrence of astigmatism blur in at least one direction is determined by at least one of the following equations (19) to (22). A method for determining astigmatism in an apparatus.
(1) 0 ° 方向コイル又は電極により、 0— 9 0 ° 方向の非点収差ボケを発 生させる非点収差ボケの発生感度 (1) Sensitivity of astigmatism blur that causes astigmatism blur in the 0-90 ° direction by the 0 ° direction coil or electrode
h(S23'-S20) h (S23'-S2 0 )
{(Sir-S10)(S23'-S20)-(S13,-S10)(S21,-S20)} ^ ' {(Sir-S1 0) ( S23'-S2 0) - (S13, -S1 0) (S21, -S2 0)} ^ '
(2) 4 5 ° 方向コイル又は電極により、 0 ° — 9 0 ° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度  (2) Sensitivity of astigmatism blur that generates astigmatism blur in the 0 ° to 90 ° direction by a 45 ° direction coil or electrode
- (513'-S10) … -(513'-S1 0 )…
{(Sir-Sl0)(S23,-S20)-(S13,-510)(S2r-S20)} 、 ) {(Sir-Sl 0 ) (S23 , -S2 0 )-(S13 , -51 0 ) (S2r-S2 0 )},)
(3) 0 ° 方向コイル又は電極によ り、 4 5 ° — 135° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度 (3) 45 ° -135 ° astigmatism blur due to 0 ° coil or electrode Sensitivity of Astigmatism Blurring that Generates
-Ah(S2V-S20) … -Ah (S2V-S2 0 )…
{(S11' - S1。)(S23' - S2。)-(S13' - S10)(S21, - S20)} {(S11 '-S1.) (S23'-S2.)-(S13 '-S1 0 ) (S21, -S2 0 )}
(4)4 5 ° 方向コィル又は電極により、 4 5 ° — 135° 方向の非点収差ボ ケを発生させる非点収差ボケの発生感度  (4) Sensitivity of astigmatism blur which causes astigmatism blur in the direction of 45 ° -135 ° by 45 ° direction coil or electrode
, A^Sll'-Slo) , A ^ Sll'-Slo)
{(S11'-S10)(S23'-S20)-(513'_S10)(S21,-S20)} {(S11'-S1 0 ) (S23'-S2 0 )-(513'_S1 0 ) (S21 , -S2 0 )}
1 4. 請求の範囲第 5項に記載の非点感度の決定方法であって、 焦点位 置 hを複数変化させ (各光軸方向位置を h i ( i = l〜! 1 ) とする)、 か つ、 前記非点収差補正器を構成する 2組のコイル群( 0 °方向コイル及び 4 5 °方向コイル) の電流値又は 2組の電極群 ( 0 °方向電極及び 4 5。0 方向電極) の電圧値、 (それそれを S I , S 2 とする)、 をそれそれ変化 させ、 そのときの非点収差ボケ評価パターンの角度を t iとし、 これら のデ一夕から、統計的手法により、(h— h。)が単位量変化するとき (h 。は正焦点が形成される焦点位置) の、 焦線を形成する点 ( S 1 , S 2 ) の組が S 1 — S 2直交座標平面で形成する円の半径の変化量を示す比例 定数 rと、 S 1軸に対する、 0 °方向ボケだけが変化する方向のなす角 2 t。を決定し、 これらのデ一夕から、 次の ( 2 3 )〜 ( 2 6 ) 式により、 少なく とも一つの方向の非点収差ボケの発生感度を泱定することを特徴 とする荷電粒子線露光装置における非点感度の決定方法。 1 4. The method for determining astigmatism according to claim 5, wherein a plurality of focal positions h are changed (each optical axis direction position is hi (i = l ~! 1)). In addition, the current values of two sets of coils (0 ° direction coil and 45 ° direction coil) constituting the astigmatism corrector or two sets of electrode groups (0 ° direction electrode and 45. 0 direction electrode) ), Which are assumed to be SI and S 2, respectively, and the angle of the astigmatism-blur evaluation pattern at that time is assumed to be ti. When (h-h.) Changes by a unit amount (h is the focus position where a positive focus is formed), the set of points (S1, S2) forming the focal line is the S1-S2 rectangular coordinates. The proportional constant r indicating the amount of change in the radius of the circle formed by the plane, and the angle 2t between the S1 axis and the direction in which only the 0 ° direction blur changes. The charged particle beam is characterized by determining the sensitivity of occurrence of astigmatism blur in at least one direction by the following equations (23) to (26). A method for determining astigmatic sensitivity in an exposure apparatus.
(1) 0 ° 方向コイル又は電極により、 0 — 9 0 ° 方向の非点収差ボケを発 生させる非点収差ボケの発生感度  (1) Sensitivity of astigmatism blur that causes astigmatism blur in the direction of 0 to 90 ° by a 0 ° direction coil or electrode
cos(2t0)/r —(23) cos (2t 0 ) / r — (23)
(2) 4 5 ° 方向コイル又は電極により、 0 ° — 9 0 ° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度 (2) Sensitivity of astigmatism blur that generates astigmatism blur in the 0 ° to 90 ° direction by a 45 ° direction coil or electrode
sin(2t0)/r -(24) (3) 0 ° 方向コィル又は電極により、 4 5 ° — 135° 方向の非点収差ボケ を発生させる非点収差ボケの発生感度 sin (2t 0 ) / r-(24) (3) Sensitivity of astigmatism blur that causes astigmatism blur in 45 ° -135 ° direction by 0 ° direction coil or electrode
-sin(2t0)/r 〜(25) -sin (2t 0 ) / r 〜 (25)
(4) 4 5 。 方向コイル又は電極により、 4 5 ° — 135° 方向の非点収差ボ ケを発生させる非点収差ボケの発生感度  (4) 4 5. Sensitivity of astigmatism blur which causes astigmatism blur in 45 ° -135 ° direction by directional coil or electrode
cos(2t0)/r -"(26) cos (2t 0 ) / r-"(26)
1 5 . 前記統計的手法が、 前記焦線となる点が作る円の中心点 ( S 1 。, S 2。)、 正焦点位置 h0、 比例定数 r、 S 1軸に対する、 0 ° 方向ボ ケだけが変化する方向のなす角 2 t 。を変数として、 以下の評価関数 P が最小となるように、 これらの変数を求めることにより、 前記 rと t 。 を求める手法であることを特徴とする請求の範囲第 1 4項に記載の非点 感度の決定方法。
Figure imgf000051_0001
15 5. The statistical method calculates the center point (S 1, S 2) of the circle formed by the point serving as the focal line, the positive focus position h 0 , the proportionality constant r, and the 0 ° direction axis with respect to the S 1 axis. The angle 2t between the directions in which only ケ changes. The variables r and t are determined by determining these variables so that the following evaluation function P is minimized. 15. The method for determining astigmatism according to claim 14, wherein the method is a method for determining the astigmatism.
Figure imgf000051_0001
1 6 . 荷電粒子線露光装置において、 レチクルの像をウェハ上に露光 転写する方法であって、 請求の範囲第 1項に記載の荷電粒子線露光装置 における非点収差補正器の非点感度の決定方法により決定した非点収差 ボケの補正感度又は非点収差ボケの発生感度を使用して、 サブフィール ド毎に非点収差ボケを修正するように非点収差補正器を調整しながら露 光転写を行うことを特徴とする荷電粒子線露光装置における露光方法。  16. A method for exposing and transferring an image of a reticle onto a wafer in a charged particle beam exposure apparatus, wherein the astigmatism correction of the astigmatism corrector in the charged particle beam exposure apparatus according to claim 1 is performed. Using the astigmatism blur correction sensitivity or astigmatism blur generation sensitivity determined by the determination method, the exposure is adjusted while adjusting the astigmatism corrector to correct the astigmatism blur for each subfield. An exposure method in a charged particle beam exposure apparatus, wherein transfer is performed.
1 7 . 前記非点収差補正器は 2組のコイル群 ( 0 ° 方向コイル及び 4 5 ° 方向コイル) または 2組の電極群 ( 0。 方向電極及び 4 5 ° 方向電 極) を有し、 補正すべき非点収差ボケ量 Δ 1ι 0, A h 4 5に対して、 前記 2組のコイル群の電流値又は前記 2組の電極群の電圧値 ΔΙ。、 ΔΙ4 5を 以下の式により求めることを特徴とする請求の範囲第 1 6項に記載の荷 鼋粒子線露光装置における露光方法。
Figure imgf000052_0001
17. The astigmatism corrector has two sets of coils (0 ° direction coil and 45 ° direction coil) or two sets of electrodes (0. direction electrode and 45 ° direction electrode), astigmatism blur delta 1Iota to be corrected 0 for a h 4 5, the two pairs of voltage values ΔΙ the current value or the two sets of electrode groups of the coil group. The exposure method in luggage鼋粒Ko beam exposure apparatus according to the first item 6 claims, characterized in that determined by the following equation ΔΙ 4 5.
Figure imgf000052_0001
但し、 E、 F、 G、 Hは各々、 Where E, F, G and H are
Eは、 0 ° 方向コイルにより、 0— 9 0 ° 方向の非点収差ボケを補正す る場合の非点収差ボケの補正感度  E is the astigmatism blur correction sensitivity when the 0-90 ° direction astigmatism blur is corrected by the 0 ° direction coil.
Fは、 4 5 ° 方向コイルにより、 0— 9 0 ° 方向の非点収差ボケを補正 する場合の非点収差ボケの補正感度  F is the sensitivity of astigmatism blur correction when the astigmatism blur in the 0-90 ° direction is corrected by the 45 ° direction coil.
Gは、 0 ° 方向コイルにより、 4 5 — 135° 方向の非点収差ボケを補正 する場合の非点収差ボケの補正感度  G is the sensitivity of astigmatism blur correction when astigmatism blur in the direction of 4 5-135 ° is corrected by a 0 ° direction coil.
Hは、 4 5 ° 方向コイルによ り、 4 5 — 135° 方向の非点収差ボケを補 正する場合の非点収差ボケの補正感度  H is the sensitivity of astigmatism blur correction when correcting astigmatism blur in the direction of 45-135 ° using a 45 ° direction coil.
である。 It is.
PCT/JP2003/011879 2002-09-24 2003-09-18 Method for correcting astigmatism, method for determining astigmatic sensitivity and method for exposure in charged particle beam aligner WO2004030056A1 (en)

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JP2007188950A (en) * 2006-01-11 2007-07-26 Nuflare Technology Inc Method for computing deflected aberration-compensating voltage, and method for drawing charged particle beam

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JPS5946745A (en) * 1982-09-09 1984-03-16 Nichidenshi Tekunikusu:Kk Automatic focal point aligning unit for charged particle beam device
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JPH07307136A (en) * 1994-05-12 1995-11-21 Nikon Corp Irradiator for charged particle beam
JPH07335531A (en) * 1994-06-10 1995-12-22 Hitachi Ltd Adjusting method of electron beam lithography system
JPH08306331A (en) * 1995-04-28 1996-11-22 Nikon Corp Charged particle beam irradiation device
JP2000077291A (en) * 1998-09-02 2000-03-14 Toshiba Corp Charged beam writing apparatus and method of correcting astigmatism of charged beam

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JPS5946745A (en) * 1982-09-09 1984-03-16 Nichidenshi Tekunikusu:Kk Automatic focal point aligning unit for charged particle beam device
JPS612251A (en) * 1984-06-15 1986-01-08 Hitachi Ltd Charged particle beam device
JPH07307136A (en) * 1994-05-12 1995-11-21 Nikon Corp Irradiator for charged particle beam
JPH07335531A (en) * 1994-06-10 1995-12-22 Hitachi Ltd Adjusting method of electron beam lithography system
JPH08306331A (en) * 1995-04-28 1996-11-22 Nikon Corp Charged particle beam irradiation device
JP2000077291A (en) * 1998-09-02 2000-03-14 Toshiba Corp Charged beam writing apparatus and method of correcting astigmatism of charged beam

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007188950A (en) * 2006-01-11 2007-07-26 Nuflare Technology Inc Method for computing deflected aberration-compensating voltage, and method for drawing charged particle beam

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