JP2015153630A - Charged particle beam irradiation device and charged particle beam axis adjustment method - Google Patents

Abstract

PROBLEM TO BE SOLVED: To enhance the axis adjustment operability of a charged particle beam in a charged particle beam irradiation device, and to enhance the accuracy thereof.SOLUTION: A charged particle beam irradiation device 100 includes a beam source 101 for emitting a charged particle beam, an aperture plate 103a having an aperture 130, a deflection unit 102 for deflecting the charged particle beam, a control unit 110 for scanning the deflection unit 102 with the charged particle beam, in a scanning range wider than the aperture 130 above the aperture plate 103a, a detector 140 provided insertably on an axis passing through the beam source 101 and the center of the aperture 130, and detecting passage of the deflected charged particle beam through the aperture 130, a beam position extraction unit 141 for determining the centroid position of a region of the charged particle beam passed through the aperture 130 in the scanning range, and a correction unit 142 for determining the current amount supplied to the deflection unit 102, the centroid position of which becomes the center of the scanning range.

Description

  The present invention includes an electron beam, an ion beam, etc., such as a scanning electron microscope, an analysis device / observation device such as an electron beam microanalyzer, an electron beam drawing device, an electron beam processing machine, an ion beam micromachining device, etc. The present invention relates to a charged particle beam irradiation apparatus for irradiating an object such as a sample with a charged particle beam in various apparatuses using charged particles, and an axis adjustment method for adjusting the optical axis of the charged particle beam in such a charged particle beam irradiation apparatus.

  Patent Document 1 discloses such a charged particle beam irradiation apparatus and its axis adjustment method. FIG. 4 shows a schematic configuration diagram of a conventional charged particle beam irradiation apparatus. A charged particle beam irradiation apparatus 400 shown in FIG. 4 is an apparatus that irradiates a sample with an electron beam as a charged particle beam. A beam source 401 including an electron gun that emits an electron beam E and a sample stage 409 on which the electron beam is irradiated. A first aperture plate 414, first focusing lens 419, X direction and Y direction deflectors 421, 422 are arranged along the axis C connecting the beam source 401 and the sample 408 between the sample 408 and the sample 408 installed on the top. , A second focusing lens 403, a second aperture plate 405, a scanning coil 406, and an objective lens 407. Further, a control unit 410, a lens power supply unit 411, a deflection power supply unit 412, a beam scanning power supply unit 413, a secondary electron measurement unit 415, an image processing unit 416, an operation unit 417, and a display unit 418 for controlling these units. It has. The electron beam emitted from the beam source 401 and passed through the first aperture plate 414 is focused by the first focusing lens 419, and the beam deflecting unit 402 causes the second aperture lens (capacitor aperture plate) 403a of the second focusing lens 403 to be focused. Adjustment is made to pass through one opening 430. The focused electron beam that has passed through the second focusing lens 403 passes through the second aperture plate 405 and is then deflected by the scanning coil 406 so as to scan the sample 408. Thereafter, the light is focused on the surface of the sample 408 by the objective lens 407.

JP 2011-054426

  In such a charged particle beam irradiation apparatus, the center position of the first opening 430 of the aperture plate 403a for the capacitor that restricts the electron beam emission position of the beam source 401 and the electron beam passage area of the second focusing lens 403. It is ideal if the center position of the second opening 450 of the second aperture plate 405 and the center position of the objective lens 407 are both in a straight line and these positions do not move. However, in reality, it is difficult to arrange each component so that there is no displacement of each position, and even if it is ideally arranged, the displacement of each position is caused by impact or vibration applied to the device. Will occur. In such a charged particle beam irradiation apparatus, in order to accurately irradiate a predetermined position on a sample or workpiece with a charged particle beam having a small diameter, the charged particle beam passes as it travels from the beam source 401 to the sample 408. It is necessary to perform adjustment with which the trajectory is aligned with the axis C (hereinafter referred to as axis adjustment) with high accuracy.

  The axis adjustment of the charged particle beam in the conventional charged particle beam irradiation apparatus 400 has been performed as follows. First, the axis adjustment sample 408 a is placed on the sample stage 409. The axis adjusting sample 408a is a sample that emits secondary electrons when irradiated with a charged particle beam. For example, zirconium oxide is used.

  Next, an electron beam is emitted from the beam source 401 and the first focusing lens 419 is adjusted to focus the electron beam on the first opening 430 of the condenser aperture plate 403a. The control unit 410 gives a scanning signal to the deflection power source unit 412 and scans the electron beam on the condenser aperture plate 403 a using the X-direction and Y-direction deflectors 421 and 422 of the beam deflection unit 402. When the electron beam passes through the first opening 430, the electron beam is incident on the axis adjustment sample 408a, and secondary electrons are emitted therefrom, but the electron beam is shielded by the capacitor aperture plate 403a. In this case, secondary electrons are not emitted from the axis adjustment sample 408a.

  The secondary electron measurement unit 415 detects secondary electrons emitted from the axis adjustment sample 408a at each scanning position of the electron beam. The image processing unit 416 creates an aperture image from the information on the scanning position of the electron beam held by the control unit 410 and the information on the secondary electrons detected by the secondary electron measurement unit 415, and displays the aperture image on the display unit 418. .

  An example of the aperture image is shown in FIG. In FIG. 5, a frame line 57 indicates a range in which the electron beam is scanned on the capacitor aperture plate 403a. The scanning center position 56 indicated by a cross corresponds to the center of the range in which the beam deflecting unit 402 scanned the electron beam on the condenser aperture plate 403a, and the circular pattern 55 of the aperture image indicates that the electron beam is an axis adjustment sample. This corresponds to a range incident on 408 a, that is, a region that has passed through the first opening 430. The deviation between the scanning center position 56 and the center position of the circular pattern 55 reflects the deviation of the electron beam from the axis C.

  While viewing the aperture image displayed on the screen of the display unit 418, the user moves the operation unit 417 so that the center of the circular pattern 55 of the aperture image comes to the scanning center position 56 displayed as a cross as shown in FIG. Use to move the aperture image. The control unit 410 determines the deflection direction of the electron beam corresponding to the scanning center position 56 from the data of the movement amount by such an operation on the image, and the X direction so that the deflection direction corresponds to the center of the scanning range. , Control parameters such as a supply current to the Y-direction deflectors 421 and 422 are adjusted.

  The charged particle beam axis adjustment in the conventional charged particle beam irradiation apparatus performed in such a procedure is performed by the user in order to place the axis adjustment sample 408a on the sample stage 409 or to adjust the control parameter. The operability is poor, for example, it is necessary to manually manipulate the image while viewing the screen 418. In addition, since the adjustment is based on the axis adjustment sample 408a and the user, the accuracy of the axis adjustment of the charged particle beam varies for each adjustment.

  The present invention has been made in view of the above points, and an object of the present invention is to improve the operability of the axis adjustment of the charged particle beam in the charged particle beam irradiation apparatus and to improve the accuracy thereof. It is in.

The charged particle beam irradiation apparatus according to the present invention, which has been made to solve the above problems,
a) a beam source for emitting a charged particle beam;
b) an aperture plate having an opening;
c) a deflection unit for deflecting the charged particle beam;
d) a control unit that causes the deflection unit to scan the charged particle beam in a scanning range that is wider than the opening on the aperture plate;
e) a detection unit provided so as to be insertable on an axis passing through the center of the beam source and the opening, and detecting the passing of the deflected charged particle beam through the opening;
f) a beam position extraction unit that obtains the position of the center of gravity of the charged particle region that has passed through the opening in the scanning range;
g) a correction unit that determines an amount of current to be supplied to the deflecting unit, wherein the position of the center of gravity is the center of the scanning range;
Is provided.

Further, the charged particle beam axis adjusting method according to the present invention, which has been made to solve the above problems,
a) an injection step of emitting a charged particle beam from a beam source;
b) a deflection step for deflecting the charged particle beam on the aperture plate so that the charged particle beam is scanned in a scanning range that is wider than the aperture of the aperture plate;
c) a detection step of inserting a detector on an axis passing through the center of the beam source and the opening, and detecting the passing of the deflected charged particle beam through the opening;
d) a beam position extraction step for obtaining a gravity center position of a charged particle region that has passed through the opening in the scanning range;
e) a determination step of determining an amount of current to be supplied to the deflection unit, wherein the position of the center of gravity is the center of the scanning range;
Is provided.

  The center-of-gravity position is a weighted average (weighted average) of the scanning positions of the scanning range with the center of the scanning range as the origin, with the measurement value by the detection unit in the charged particle region that has passed through the opening as a weight. You may make it the structure which calculates | requires and calculates | requires. Here, the detection unit may include a Faraday cup, and a beam current amount (absolute intensity of the charged particle beam) detected by the Faraday cup may be used as a measurement value, or a beam current amount detected by the Faraday cup. The difference from the predetermined current (relative intensity of the charged particle beam) may be used as a measured value.

  According to the charged particle beam irradiation apparatus and the charged particle beam axis adjusting method according to the present invention, the charged particle beam axis can be adjusted regardless of the sample or the user, so that the operability of the charged particle beam axis adjustment is improved. In addition, the accuracy can be improved.

The schematic block diagram of the charged particle beam irradiation apparatus which concerns on an Example. The flowchart which shows the procedure of the axis adjustment of the charged particle beam in the charged particle beam irradiation apparatus which concerns on an Example. The figure explaining the axis adjustment in the case of (a) fine adjustment in the charged particle beam irradiation apparatus which concerns on an Example, and (b) rough adjustment. The schematic block diagram of the conventional charged particle beam irradiation apparatus. The figure explaining the axis adjustment of the charged particle beam in the conventional charged particle beam irradiation apparatus. The figure explaining the axis adjustment of the charged particle beam in the conventional charged particle beam irradiation apparatus.

  Hereinafter, the form for implementing this invention is demonstrated using an Example, referring FIGS. 1-3.

  A schematic configuration diagram of the charged particle beam irradiation apparatus 100 of the present embodiment is shown in FIG. A charged particle beam irradiation apparatus 100 shown in FIG. 1 is an apparatus that irradiates a sample with an electron beam as a charged particle beam. A beam source 101 including an electron gun that emits an electron beam E and a sample stage 109 that is irradiated with the electron beam. The first aperture plate 114, the first focusing lens 119, the X direction, and the Y direction deflectors 121 and 122 are arranged along the axis C connecting the beam source 101 and the sample 108 between the sample 108 and the sample 108 installed on the upper side. A beam deflection unit 102, a second focusing lens 103, a detection unit 140, a second aperture plate 105, a scanning coil 106, and an objective lens 107. Further, a control unit 110, a lens power supply unit 111, a deflection power supply unit 112, a beam scanning power supply unit 113, an operation unit 117, a beam position extraction unit 141, and a correction unit 142 are provided for controlling these units.

  The charged particle beam irradiation apparatus 100 according to the present embodiment is characterized in that a charged particle beam axis is adjusted using a detection unit 140, a beam position extraction unit 141, and a correction unit 142. The detection unit 140 includes a Faraday cup, and this Faraday cup is deviated from the axis C connecting the beam source 101 and the sample 108 between the second focusing lens 103 having the condenser aperture plate 103a and the second aperture plate 105. The case where it can be inserted on the axis C from the position 140a will be described.

  Here, “axis C” is a position at which the electron beam is emitted from the beam source 101, and a position immediately below the beam source 101 that reaches the sample 108 when the electron beam is not subjected to any disturbance. Tie. Further, the “Faraday cup” is a metal cup, and when a charged particle beam hits the metal portion, electric charges are accumulated in the metal. When an ammeter is connected to the Faraday cup, a current corresponding to the number of charged particles that hit the metal portion flows. Therefore, the detection unit 140 including the Faraday cup can detect the intensity of the charged particle beam as a current value. .

  The axis adjustment of the charged particle beam is performed in advance before the measurement of the sample, and the procedure of this axis adjustment will be described below with reference to FIG.

  First, the user operates the mouse, keyboard, or the like constituting the operation unit 117 to instruct the charged particle beam irradiation apparatus 100 to perform axis adjustment. When the control unit 110 of the charged particle beam irradiation apparatus 100 receives this instruction, the control unit 110 controls a power source such as a motor (not shown) so that the detection unit 140 formed of a Faraday cup is placed under the aperture plate 103a for the capacitor. Then, it is moved on an axis (axis C) passing through the center of the beam source 101 and the first opening 130 of the condenser aperture plate 103a. The beam source 101 emits an electron beam E (step S21).

  Next, the control unit 110 sends a signal for adjusting the first focusing lens 119 to the lens power supply unit 111, and the lens power supply unit 111 supplies a control current to the first focusing lens 119. The first focusing lens 119 focuses the electron beam E near the first opening 130 according to the control current.

  The control unit 110 gives a scanning signal for changing the deflection direction of the electron beam E by the X-direction and Y-direction deflectors 121 and 122 to the deflection power supply unit 112. The deflection power supply unit 112 supplies a predetermined current to the X-direction and Y-direction deflectors 121 and 122 according to the scanning signal. In accordance with the amount of supplied control current, the deflector 121 deflects the electron beam E in the X direction, and the deflector 122 deflects the electron beam E in the Y direction (step S22). Here, the X direction and the Y direction are directions in a plane (XY plane) orthogonal to the axis C. Thus, the scanning signal deflects the electron beam E in the X direction and the Y direction, and scans the electron beam E over a scanning range wider than the first opening 130 in the XY plane. As an example, when the first opening 130 is a circle having a diameter of 25 μm, a square range of 80 μm in the X direction and 80 μm in the Y direction can be set as the scanning range.

  3A and 3B are enlarged views of the vicinity of the first opening 130 when the electron beam E is focused near the first opening 130. FIG. When the electron beam E is focused in the XY plane where the first opening 130 is formed as shown in FIG. 3A, the range R of the XY plane irradiated with the electron beam E is the electron beam. Since E is in the same range as the range S scanned on the condenser aperture plate 103a, fine adjustment of the axis adjustment can be performed. On the other hand, if the position for focusing the electron beam E is shifted by several μm from the XY plane to the + Z direction, which is the traveling direction of the electron beam along the axis C, as shown in FIG. Since the range R ′ of the XY plane irradiated with the beam E is wider than the range S in which the electron beam E is scanned on the condenser aperture plate 103a, rough adjustment of the axis adjustment can be performed.

  If the above-mentioned scanning range is expressed by coordinates with the center of the above-mentioned scanning range as the origin, the scanning range is a square range of ± 40 μm in the X direction and ± 40 μm in the Y direction. In this range, when there is no region where the electron beam E passes through the first opening 130 or only a part of the region, the axial deviation is large. In this case, for example, the scanning range is expanded to a square range of ± 120 μm in the X direction and ± 120 μm in the Y direction, and coarse adjustment is performed, so that the entire region of the first opening 130 is within the scanning range. Know the direction of deflection. After the deflection direction is made to correspond to the center of the next scanning range, fine adjustment for adjusting control parameters such as supply current to the X-direction and Y-direction deflectors 121 and 122 is performed. Hereinafter, a case where fine adjustment is performed will be described.

  The detection unit 140 including the Faraday cup moved below the condenser aperture plate 103a and on the axis C has a current value corresponding to the intensity of the electron beam E deflected by the X-direction and Y-direction deflectors 121 and 122. Is output. Thereby, the passage of the electron beam E through the first opening 130 is detected for each deflection direction within the scanning range (step S23). When the electron beam E is shielded by the capacitor aperture plate 103a, the current value decreases. However, when the electron beam E passes through the first opening 130, the current value increases.

  Next, the beam position extraction unit 141 acquires information on the measurement value obtained by the detection unit 140 and information on the scanning position grasped by the control unit 110, and sets the center of the scanning range using the measurement value obtained by the detection unit 140 as a weight. A weighted average (weighted average) of the scanning positions as the origin is calculated, and the barycentric position of the charged particle region that has passed through the first opening 130 is obtained (step S24). That is, i is a variable assigned to all scanning positions from which measured values are obtained, the center of the scanning range is the origin, and the scanning position from which measured values are obtained is expressed as Txi [μm] for the x coordinate and Tyi [ μm] and the measured value is Ii, the x-coordinate position Tcx and the y-coordinate position Tcy of the centroid position are Tcx = Σ (Ii × Txi) / ΣIi and Tcy = Σ (Ii × Tyi) / ΣIi, respectively. Calculate to find. Here, the beam current amount (absolute intensity of the charged particle beam) detected by the Faraday cup may be used as a measurement value, or the difference between the beam current amount detected by the Faraday cup and a predetermined current (charged particle beam). Relative intensity) may be used as a measured value.

  The correction unit 142 determines the amount of current supplied to the X-direction and Y-direction deflectors 121 and 122 included in the deflection unit 102 in which the barycentric position obtained in step S24 is the center of the scanning range (step S25). As a result, the center of gravity of the charged particle region that has passed through the first opening 130 becomes the center (origin) of the scanning range, and the axis adjustment of the charged particle beam ends.

  As described above, according to the charged particle beam irradiation apparatus and the charged particle beam axis adjusting method of the present embodiment, the charged particle beam axis adjustment can be performed without variation for each adjustment regardless of the sample and the user. The accuracy of the axis adjustment can be improved. Further, since the beam position extraction unit quantitatively obtains the position of the center of gravity of the intensity two-dimensional spatial distribution, quantitative adjustment is also possible. Furthermore, since the charged particle beam irradiation apparatus according to the present embodiment performs an operation that is conventionally performed manually by a user, the operability is improved.

  In this embodiment, the case where an electron beam is used as the charged particle beam has been described. However, the present invention is not limited to this, and any ion beam or the like that has a charge and whose deflection direction can be changed by a deflector. Any charged particle beam may be used.

55 ... Circular pattern 56 ... Scanning center position 57 ... Frame line 100, 400 ... Charged particle beam irradiation apparatus 101, 401 ... Beam source 102, 402 ... Beam deflection section 103, 403 ... Condensing lens 103a, 403a ... Aperture plate 105 for condenser 405 ... second aperture plate 106,406 ... scanning coil 107,407 ... objective lens 108,408 ... sample 109,409 ... sample stage 110,410 ... control unit 111,411 ... lens power supply unit 112,412 ... deflection power supply unit 113, 413 ... beam scanning power supply units 114, 414 ... first aperture plates 117, 417 ... operation units 119, 419 ... focusing lenses 121, 122, 421, 422 ... deflectors 130, 430 ... first opening 140 ... detection unit 141: Beam position extraction unit 142: Correction unit 150, 450: Second opening 415 ... secondary electron measurement unit 416 ... image processing unit 418 ... display unit

Claims (6)

a) a beam source for emitting a charged particle beam;
b) an aperture plate having an opening;
c) a deflection unit for deflecting the charged particle beam;
d) a control unit that causes the deflection unit to scan the charged particle beam in a scanning range that is wider than the opening on the aperture plate;
e) a detection unit provided so as to be insertable on an axis passing through the center of the beam source and the opening, and detecting the passing of the deflected charged particle beam through the opening;
f) a beam position extraction unit that obtains the position of the center of gravity of the charged particle region that has passed through the opening in the scanning range;
g) a correction unit that determines an amount of current to be supplied to the deflecting unit, wherein the position of the center of gravity is the center of the scanning range;
A charged particle beam irradiation apparatus comprising:   The center-of-gravity position is obtained by calculating a weighted average of the scanning positions of the scanning range with the center of the scanning range as the origin, with the measurement value by the detection unit in the charged particle region that has passed through the opening as a weight. The charged particle beam irradiation apparatus according to claim 1.   The charged particle beam irradiation apparatus according to claim 2, wherein the detection unit includes a Faraday cup, and a beam current amount detected by the Faraday cup is used as the measurement value. a) an injection step of emitting a charged particle beam from a beam source;
b) a deflection step for deflecting the charged particle beam on the aperture plate so that the charged particle beam is scanned in a scanning range that is wider than the aperture of the aperture plate;
c) a detection step of inserting a detector on an axis passing through the center of the beam source and the opening, and detecting the passing of the deflected charged particle beam through the opening;
d) a beam position extraction step for obtaining a gravity center position of a charged particle region that has passed through the opening in the scanning range;
e) a determination step of determining an amount of current to be supplied to the deflection unit, wherein the position of the center of gravity is the center of the scanning range;
A charged particle beam axis adjusting method comprising:   The center-of-gravity position is obtained by calculating a weighted average of the scanning positions of the scanning range with the center of the scanning range as the origin, with the measurement value by the detection unit in the charged particle region that has passed through the opening as a weight. The charged particle beam axis adjusting method according to claim 4.   6. The charged particle beam axis adjusting method according to claim 5, wherein the beam current amount detected by a Faraday cup is used as the measurement value.

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