Classifications

• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
  • G01B11/00—Measuring arrangements characterised by the use of optical techniques
  • G01B11/02—Measuring arrangements characterised by the use of optical techniques for measuring length, width or thickness
  • G01B11/06—Measuring arrangements characterised by the use of optical techniques for measuring length, width or thickness for measuring thickness ; e.g. of sheet material
  • G01B11/0616—Measuring arrangements characterised by the use of optical techniques for measuring length, width or thickness for measuring thickness ; e.g. of sheet material of coating
  • G01B11/0675—Measuring arrangements characterised by the use of optical techniques for measuring length, width or thickness for measuring thickness ; e.g. of sheet material of coating using interferometry
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
  • G01B9/00—Measuring instruments characterised by the use of optical techniques
  • G01B9/02—Interferometers
  • G01B9/02015—Interferometers characterised by the beam path configuration
  • G01B9/02017—Interferometers characterised by the beam path configuration with multiple interactions between the target object and light beams, e.g. beam reflections occurring from different locations
  • G01B9/02021—Interferometers characterised by the beam path configuration with multiple interactions between the target object and light beams, e.g. beam reflections occurring from different locations contacting different faces of object, e.g. opposite faces
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
  • G01B9/00—Measuring instruments characterised by the use of optical techniques
  • G01B9/02—Interferometers
  • G01B9/02015—Interferometers characterised by the beam path configuration
  • G01B9/02027—Two or more interferometric channels or interferometers
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
  • G01B9/00—Measuring instruments characterised by the use of optical techniques
  • G01B9/02—Interferometers
  • G01B9/02041—Interferometers characterised by particular imaging or detection techniques
  • G01B9/02044—Imaging in the frequency domain, e.g. by using a spectrometer
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
  • G01B9/00—Measuring instruments characterised by the use of optical techniques
  • G01B9/02—Interferometers
  • G01B9/02055—Reduction or prevention of errors; Testing; Calibration
  • G01B9/02056—Passive reduction of errors
  • G01B9/02057—Passive reduction of errors by using common path configuration, i.e. reference and object path almost entirely overlapping
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
  • G01B9/00—Measuring instruments characterised by the use of optical techniques
  • G01B9/02—Interferometers
  • G01B9/02055—Reduction or prevention of errors; Testing; Calibration
  • G01B9/02062—Active error reduction, i.e. varying with time
  • G01B9/02064—Active error reduction, i.e. varying with time by particular adjustment of coherence gate, i.e. adjusting position of zero path difference in low coherence interferometry
  • G01B9/02065—Active error reduction, i.e. varying with time by particular adjustment of coherence gate, i.e. adjusting position of zero path difference in low coherence interferometry using a second interferometer before or after measuring interferometer
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
  • G01B9/00—Measuring instruments characterised by the use of optical techniques
  • G01B9/02—Interferometers
  • G01B9/0209—Low-coherence interferometers
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
  • G01B2210/00—Aspects not specifically covered by any group under G01B, e.g. of wheel alignment, caliper-like sensors
  • G01B2210/40—Caliper-like sensors
  • G01B2210/44—Caliper-like sensors with detectors on both sides of the object to be measured
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
  • G01B2210/00—Aspects not specifically covered by any group under G01B, e.g. of wheel alignment, caliper-like sensors
  • G01B2210/40—Caliper-like sensors
  • G01B2210/48—Caliper-like sensors for measurement of a wafer
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
  • G01B2290/00—Aspects of interferometers not specifically covered by any group under G01B9/02
  • G01B2290/35—Mechanical variable delay line

Definitions

• the present invention relates to a device and a method for measuring heights or thicknesses of samples such as wafers in the presence of thin layers.
• the field of the invention is more particularly, but not exclusively, that of optical measurement systems for the semiconductor industry.
• optical techniques particularly low coherence interferometry techniques that implement broad-spectrum optical sources. These techniques are essentially of two kinds:
• Techniques with time domain detection use a time delay line that reproduces the propagation delays of the measurement waves reflected by the interfaces of the object to be measured and interferes with a reference wave. This results in a detector of peaks of interference representative of the position of the interfaces of the object.
• These temporal techniques make it possible to reach important measuring ranges limited only by the course of the delay line.
• a broad-spectrum source emitting in the infrared they make it possible to measure thicknesses of semiconductor materials such as silicon. The minimum measurable thicknesses are limited by the width of the interferogram envelope, which depends on the shape and width of the source spectrum.
• the techniques based on low coherence interferometry in the spectral domain are generally rather intended for measurements of thin layers, of the order of a few tens of nanometers to a few hundred microns.
• the light reflected by the interfaces of the object to be measured is analyzed in a spectrometer.
• the thicknesses or distances between the interfaces of the object at the origin of the reflections introduce modulations in the detected spectrum that make it possible to measure them.
• document EP 0 747 666 describes a system based on low coherence interferometry in the spectral domain making it possible to measure distances between interfaces in the presence of thin layers, from a mathematical modeling of the phase of the ripples of the measured spectrum.
• the wafers whose thickness is to be measured may be covered with a thin layer of transparent material.
• a thin layer of transparent material there are, for example, configurations in which it is desired to measure the thickness of 300 ⁇ m to 700 ⁇ m thick silicon wafers covered with a layer of polyimide of the order of 10 ⁇ m thick. This configuration is problematic because none of the techniques mentioned above makes it possible to measure the total thickness satisfactorily:
• the object of the present invention is to propose a device and a method which makes it possible to measure the heights of objects such as wafers in the presence of thin layers.
• the present invention also aims to provide a device and a method that allows to measure thicknesses of objects such as wafers in the presence of thin layers.
• the present invention also aims to provide a device and a method that allows to measure heights or thicknesses of objects such as wafers in the presence of thin layers without degradation of the measurement accuracy.
• Another object of the present invention is to provide a device and a method which makes it possible to measure heights or thicknesses of objects such as wafers, with both a large extent of measurement and a resolution making it possible to measure thin layers.
• This objective is achieved with a device for measuring heights and / or thicknesses on a measuring object such as a wafer,
• a first low-coherence interferometer illuminated by a polychromatic light and arranged to combine in a spectrometer a reference optical beam resulting from a reflection of said light on a reference surface and an optical measurement beam from reflections of said light on interfaces of the measurement object, so as to produce a fluted spectrum signal with spectral modulation frequencies, characterized in that it further comprises:
• displacement means for varying the relative optical length of the measurement and reference optical beams, and means for measuring a position information representative of said relative optical length
• electronic and computing means arranged to determine at least one spectral modulation frequency representative of a difference an optical path between the optical measuring beam and the reference optical beam, and for determining, by using said position information and said at least one spectral modulation frequency, at least one height and / or one thickness on said measurement object , and
• second optical means for measuring distance and / or thickness with a second measuring beam incident on the measuring object in a second face opposite to the measuring beam.
• the displacement means for varying the relative optical length of the measuring and reference optical beams may comprise, for example, a mechanical translation device enabling to move:
• the reference surface relative to a beam splitter element of the interferometer, so as to vary the length of the reference optical beam
• the means for measuring a position information may comprise any means, such as an optical ruler or a laser range finder, for measuring the position of the moving element.
• the polychromatic light may comprise a spectrum extending in visible wavelengths and / or infrared wavelengths.
• the spectrum signal is said to be "channeled spectrum” when the relative optical length difference of the measurement and reference optical beams is large enough to identify at least one spectral modulation period in the beam.
• spectrum signal (thus over the spectral width of the spectrum signal).
• the spectrum signal has oscillations as a function of wavelength or frequency, i.e. a periodically variable amplitude with wavelength or frequency.
• the spectrum signal may also comprise modulations with a period greater than the spectral width of the spectrum signal, corresponding to very thin layers.
• the device according to the invention may comprise a measurement head with the reference surface, and translational displacement means able to relatively move said measuring head and the measurement object in a substantially parallel direction. to an optical axis of the optical measuring beam.
• the displacement means make it possible to vary the optical length of the measuring beam relative to the reference beam.
• the device according to the invention may comprise a reference surface in the form of a semi-reflecting plate inserted in the path of the optical measuring beam.
• the device according to the invention may comprise a measuring head with a separating optical element capable of generating a measurement optical beam and a separate reference optical beam.
• the device according to the invention may in particular comprise a measurement head with a first interferometer of one of the following types: Mirau, Linnick, Michelson, to generate the measurement and reference optical beams.
• a Mirau interferometer comprises a separating optical element with a semi-reflecting plate perpendicular to the axis of the incident beam and a reference surface in the form of a mirror inserted in the center of the incident beam.
• a Michelson interferometer or a Linnick interferometer comprises a splitting optical element with a semi-reflective plate or a splitter cube arranged to generate a substantially perpendicular measuring beam and reference beam, and a reference surface in the form of a mirror inserted into the reference beam.
• a Linnick interferometer further includes lenses or lenses inserted into the arms of the interferometer corresponding to the reference beam and the measurement beam.
• the device according to the invention may further comprise second translation means able to relatively move the optical beam of measurement and the measuring object in a plane substantially perpendicular to an optical axis of the measuring beam.
• These second translation means make it possible to move the optical measuring beam on the surface of the object (or vice versa) so as to be able to measure heights and / or thicknesses at different points of this object.
• the device according to the invention may further comprise a support adapted to receive the measurement object, and a reference object with known height and / or thicknesses arranged on or forming part of said support.
• the support may be for example a wafer chuck, to receive a measuring object in the form of a wafer.
• the reference object may be for example a wafer portion of known characteristics placed on or secured to the support. It may also consist of a portion of the support or chuck height calibrated.
• the reference object may also be constituted by a bearing surface of the support intended to receive the object to be measured, or a coplanar surface of this bearing face.
• the reference object makes it possible to calibrate the measurement system, by taking measurements of known heights and / or thicknesses on its surface.
• the device according to the invention may comprise a first low-coherence interferometer illuminated by a polychromatic light which emits light in the visible spectrum.
• Such a broad-spectrum source with relatively short wavelengths makes it possible to measure thin films, for example dielectric materials that are transparent from a few tens of nanometers to a few microns.
• the device according to the invention may further comprise second optical distance measuring means and / or thickness with a second measurement beam incident on the object to be measured in a second face opposite the measuring beam.
• This configuration makes it possible to make caliper measurements, for example to carry out measurements of total thickness on the measurement object. These measurements of total thickness can in particular be deduced from distance measurements made on either side of the measuring object.
• the second optical means for measuring distance and / or thickness can also be calibrated by taking measurements on the reference object.
• the device according to the invention may further comprise second mechanical distance measuring means with a mechanical probe in contact with a second face of the object to be measured opposite the measurement beam.
• the device according to the invention may comprise second optical distance measuring means and / or thickness of one of the following types:
• a low coherence interferometer in the spectral domain, it may be identical or different from the first interferometer. It can also implement a light with visible wavelengths and / or infrared.
• a chromatic confocal system is a measurement system that uses a dispersive optical element to focus different wavelengths at different distances, and a spectral detection to identify the reflected wavelengths and thus the position of the interfaces at the origin of these reflections.
• the device according to the invention may comprise second optical distance measurement and / or thickness means with a interferometer with low coherence in the time domain.
• This low coherence interferometer in the time domain may comprise a delay line which makes it possible to vary a delay (time) between optical beams.
• the low coherence interferometer in the time domain may include a light source emitting in the infrared.
• the low coherence interferometer in the time domain may comprise a Michelson double interferometer with a coding interferometer and a decoding interferometer, and an optical measuring fiber with a collimator for generating the second optical beam. measured.
• the decoding interferometer may include a delay line arranged to reproduce an optical delay between a measurement beam from reflections on interfaces of the measurement object and a reference beam.
• This delay line may comprise for example a mirror movable in translation in the axis of the optical beam, or any other means known to those skilled in the art to vary an optical path (optical fibers subjected to stretching, parallel-sided blade in rotation, ).
• the reference beam may be generated in the collimator, for example by the Fresnel reflection at the interface between the end of the optical fiber measurement and the air.
• Such an interferometer has the advantage of being easily integrable because the heart of the interferometer can be remote from the measuring object and only the collimator must be placed near this object.
• a method for measuring heights and / or thicknesses on a measurement object such as a wafer, implementing a first low coherence interferometer illuminated by a polychromatic light and arranged to combine in a spectrometer a reference optical beam resulting from a reflection of said light on a reference surface and a measurement optical beam originating from reflections of said light on the interfaces of the measurement object, so as to produce a grooved spectrum signal with spectral modulation frequencies, which method comprises steps:
• the method according to the invention may further comprise a step of identifying the spectral modulation frequencies, the value of which varies with a variation of the relative optical length of the measurement and reference optical beams.
• the method according to the invention may further comprise a step of varying the relative optical length of the measurement and reference optical beams so as to obtain at least one spectral modulation frequency in a predetermined range of values.
• the method according to the invention may further comprise steps:
• spectral modulation signal for calculating a spectral modulation signal representative of the amplitude of the Fourier transform of the fluted spectrum signal, identifying amplitude peaks representative of spectral modulation frequencies in said spectral modulation signal.
• the method according to the invention may further comprise a calibration step comprising a measurement of height and / or thickness on a reference object of known height and / or thickness, so that establishing a relationship between at least one position information of the reference surface, at least one spectral modulation frequency, and at least one height and / or one thickness.
• the measurement of a second information of height and / or thicknesses can comprise steps:
• the measurement method according to the invention implements a low coherence interferometer with detection in spectral mode in a configuration that makes it possible to perform absolute distance measurements over relatively large measuring ranges. It is thus possible to exploit an advantage of this type of spectral detection which is to make it possible to distinguish very close interfaces, and to obtain a device and a method for measuring distances and / or thicknesses which combines a large extent of measurement and a resolution. (or an ability to distinguish nearby interfaces) equally important.
• the relative optical length difference of the measurement and reference optical beams is adjusted by moving in a known manner an element of the interferometer (or the measurement object) so that the corresponding spectral modulation frequency of the fluted spectrum signal either in a range of values where it can be measured under good conditions;
• This displacement information of an element of the interferometer is used as well as the frequency or frequencies of spectral modulations measured to calculate an absolute height of the measurement object.
• the measurement is calibrated on a reference object of known height to establish a relationship between the displacement information of an element of the interferometer and the absolute height;
• FIG. 1 illustrates an embodiment of the device according to the invention
• FIG. 2 illustrates an embodiment of the interferometer in the form of a Michelson interferometer
• FIG. 3 illustrates an embodiment of the interferometer in the form of a Mirau interferometer
• FIG. 4 illustrates, (a) a fluted spectrum signal, and (b) a Fourier transform of the fluted spectrum
• FIG. 5 illustrates the steps of the method according to the invention
• FIG. 6 illustrates an embodiment of second optical measuring means.
• a first device embodiment according to the invention for measuring heights or thicknesses of measurement objects 24 will be described with reference to FIG.
• the device according to the invention is more particularly intended to measure measuring objects 24 in the form of wafers 24 during the process.
• these wafers 24 may comprise one or more thin layers deposited on their surface.
• These wafers 24 may for example comprise a thickness of silicon of 450 .mu.m to 700 .mu.m and a layer of polyimide, silicon oxide, silicon nitride or other dielectrics transparent from a few tens of nanometers to a few microns.
• these thin layers are at least partially transparent at visible wavelengths.
• Silicon is transparent to infrared wavelengths.
• the silicon layer may comprise opaque layers (component, transistors, layers or metal tracks, etc.).
• the known methods for measuring the total thickness of the wafer are generally not able to separate or solve the interfaces of the thin layers, especially when they are transparent in the measurement wavelengths. same if one does not try to measure the thickness of these layers but only the total thickness of the wafer 24, the accuracy of the measurement is limited by the indeterminacy on the detection of thin-film interfaces 25.
• these thin layers can be measured or their interfaces distinguished with low coherence interferometry techniques operating in the spectral domain, using a light source with a spectrum sufficiently extended in frequencies.
• these techniques do not make it possible to measure significant optical thicknesses (such as 700 ⁇ m of silicon, which correspond to an optical thickness greater than 2 mm, taking into account the refractive index of silicon, which is of the order of 3.5). In this case the oscillations of the fluted spectrum become too close together to be sampled by the detector.
• the wafers 24 to be measured can be highly deformed, which requires a measurement system with a large extent of measurement.
• the heart of the measuring device according to the invention consists of a low coherence interferometer integrated in a measuring head 10.
• the measuring head 10 is fixed to displacement means 21 with a motorized translation stage which makes it possible to move it along an axis Z relative to the frame of the apparatus on which this translation stage is fixed.
• the translation stage is equipped with means for measuring a position information in the form of an optical ruler, which makes it possible to measure precisely its displacement and its position.
• the interferometer is illuminated by a broad-spectrum optical source 11 which emits a polychromatic light 12 in the visible spectrum.
• this source comprises a halogen source, or deuterium halogen with a spectrum extending up to 300 nm in the ultraviolet.
• the interferometer comprises a separating plate 13 which directs the light from the source 11 towards the object to be measured 24.
• Part of the light is reflected on a reference surface 14 constituted by a semi-reflecting plate 14, to form a reference optical beam 17.
• This optical measuring beam 16 is focused on the object to be measured 24 (the wafer 24) by an objective lens or a lens 15.
• the optical measuring beam 16 is positioned relative to the measuring object 24 so that its optical axis 19 is substantially perpendicular to the interfaces of this object 24. In the embodiment shown, this optical axis 19 is substantially parallel to the displacement axis Z of the displacement means 21.
• the light of the measuring beam 16 is reflected on the interfaces of the object to be measured 24, and in particular in the example illustrated by the interfaces of the thin layer 25.
• the reflected measurement 16 and reference 17 beams are directed through the separator plate 13 to a detection spectrometer 18.
• This spectrometer 18 comprises a diffractive grating which disperses spatially as a function of optical frequencies the combined light of the measurement beams 16 and reference 17, and a linear sensor (CCD or CMOS) from which each pixel receives light from the diffractive grating corresponding to a particular range of optical frequencies.
• a diffractive grating which disperses spatially as a function of optical frequencies the combined light of the measurement beams 16 and reference 17, and a linear sensor (CCD or CMOS) from which each pixel receives light from the diffractive grating corresponding to a particular range of optical frequencies.
• the spectrometer is connected to electronic and computing means 20 in the form of a computer 20.
• the object to be measured 24, which is in the illustrated embodiment a wafer 24, is positioned on a support 23, which has the form of a wafer support 23 ("chuck" in English).
• the device further comprises a reference object 26 in the form of a wafer portion 26 of known thickness.
• This reference object 26 is positioned on a wafer support 23.
• the wafer support 23 is fixed on second translation means 22 in the form of a translation plate 22 which ensures its displacement (relative to the frame of the apparatus for example) in an XY plane substantially perpendicular to the optical axis 19 of the measuring beam 16.
• These second translation means 22 make it possible to position the measuring beam 16 at any point on the surface of the wafer 24, and on the reference object 26.
• the device according to the invention further comprises second optical distance measuring means and / or thickness 27 with a second beam measurement 28 incident on the object to be measured 24 in a second face opposite the measuring beam 16.
• these second optical measuring means 27 comprise a low coherence interferometer 27 operating in the time domain, with a time delay line which makes it possible to introduce a variable optical path delay or variation.
• Light from a broad-spectrum source is separated between an internal reference beam and a measurement beam 28 incident on the object to be measured.
• the measuring beam 28 is reflected on the interfaces of the object.
• Each reflection is delayed proportionally to the optical path to the interface considered. This delay is reproduced in the delay line so as to re-phase the measurement and reference beams and thus generate interference peaks during the displacement of the delay line.
• the knowledge of the displacement of this delay line makes it possible to determine the position of the interfaces at the origin of the interference peaks.
• an infrared light source (around 1310 nm for example), which makes it possible to penetrate the silicon and thus also to measure on wafer internal layers where appropriate.
• FIG. 6 illustrates a schematic representation of such a low coherence interferometer 27 operating in the time domain.
• the heart of the interferometer 27 is a double Michelson interferometer based on monomode optical fibers, with a coding interferometer 60 and a decoding interferometer 61. It is illuminated by a fiber light source 62 which is a superluminescent diode (SLD). ) whose central wavelength is of the order of 1300 nm to 1350 nm and the spectral width of the order of 60 nm. The choice of this wavelength corresponds in particular to criteria of availability of the components.
• SLD superluminescent diode
• the light from the source 62 is directed through a coupler 60 which constitutes the coding interferometer 60 and a measurement optical fiber 67 to a collimator 66, to constitute the second measurement beam 28.
• Part of the beam from the source 62 is reflected in the fiber of measuring 67 at the collimator 66, to constitute the internal reference beam.
• the reference beam is generated by the Fresnel reflection at the interface between the end of the measurement optical fiber 67 and the air in the collimator. This reflection is usually of the order of 4%.
• the retro-reflections from the interfaces of the wafer 24 are coupled in the fiber 67 and directed with the reference wave to the decoding interferometer 61 built around the fiber coupler 61.
• This decoding interferometer has an optical correlator function which the two arms are, respectively, a fixed reference 64 and a time delay line 65.
• the signals reflected at the reference 64 and the delay line 65 are combined, through the coupler 61, on a detector 63 which is a photodiode.
• the function of the delay line 65 is to introduce an optical delay between the incident and reflected waves, variable over time in a known manner. This delay is obtained for example by the displacement of a mirror 68 in translation in the axis of the optical beam.
• the length of the arms 64 and 65 of the decoding interferometer 61 is adjusted so as to reproduce with the delay line 65 the differences in optical paths between the reference wave reflected at the collimator 66 and the retroreflections from of the object to be measured 24.
• an interference peak is obtained on the detector 43 whose shape and width depend on the spectral characteristics of the source 62 (FIG. the wider the spectrum of the source 62, the smaller the interference peak).
• the measurement range is determined by the difference in optical length between the arms 64 and 65 of the decoder interferometer 61, and by the maximum stroke of the delay line 65.
• This type of interferometer thus presents the advantage of allowing large measurement ranges.
• the successive interfaces of the object to be measured 24 appear as successions of interference peaks separated by the optical distances separating these interfaces (as reproduced for example by the path of the mirror 68), it is possible to measure without ambiguity Stacks of many layers.
• the implementation of a double interferometer system, with a coding interferometer 60 and a decoding interferometer 61, and the generation of the reference at the end of the measurement fiber 67 makes it possible to make the system insensitive to disturbances in the field. Measurement fiber 67.
• the true optical distances between the collimator and the interfaces of the object to be measured can be measured with great accuracy.
• this configuration with a measurement optical fiber 67 makes it possible to deport the interferometer 27.
• the collimator 66 is in the vicinity of the object to be measured. This advantage is important when the object to be measured 24 is a wafer 24 on a wafer support 23, for which the access along its face on the wafer support 23 is more difficult.
• the second translation means 22 also make it possible to position the second measurement beam 28 at any point on the second surface of the wafer 24, and on a second face of the reference object 26 opposite the first beam of measure 16.
• FIG. 2 and FIG. 3 illustrate alternative embodiments of the interferometer which have the advantage of spatially separating the measuring beams 16 and reference 17. These configurations allow in particular to increase the working distance between the interferometer and the object to be measured 24 without increasing the optical path difference between the measuring beam 16 and the reference beam 17.
• Fig. Figure 2 illustrates a Michelson interferometer configuration.
• the light of the source is divided by a splitter cube 31 to form a measuring beam 16 directed towards the object 24 and a reference beam 17 directed towards a reference surface in the form of a mirror 14.
• the measuring beams and reference are substantially perpendicular.
• Fig. Figure 3 illustrates a Mirau interferometer configuration.
• the light of the source is divided by a semi-reflecting plate 32 substantially perpendicular to the optical axis 19 of the incident beam to form a measurement beam 16 directed towards the object 24 and a reference beam 17 directed towards a reference surface under
• the reference mirror 14 is on the optical axis 19 of the incident beam, of which it forms a central obscuration.
• Fig. 4 (a) illustrates a splined spectrum signal 41 as obtained at the output of the spectrometer 18.
• This signal represents a spectral intensity I (v) expressed as a function of the optical frequency v.
• This intensity I (v) can be represented as a sum of i harmonic functions each corresponding to an interference signal between two incident waves on the spectrometer 18:
• a 0 and Ai are intensity coefficients, ⁇ , a phase coefficient, c the speed of light, and 2 Lj the difference in optical paths between the two interfering waves.
• This "frequency” of spectral modulation is therefore representative of the difference in optical paths 2L, between the two waves that interfere.
• this spectral modulation signal 42 is representative of an envelope of the time autocorrelation function of measurement beams 16 and reference 17. It comprises an amplitude peak 43, 44, 45 for each delay Tj corresponding to a difference in paths. 2L optics, between two waves that interfere.
• the spectral modulation signal 42 illustrated in FIG. 4 (b) qualitatively corresponds to the situation illustrated in FIG. 1 in which there is a measuring object 24 with a thin layer 25.
• FIGS. 4 (a) and FIG. 4 (b) are purely illustrative.
• the spectral modulation signal 42 comprises a first peak 43 centered on a delay ⁇ corresponding to the optical path difference 2E, where E is the optical thickness of the thin layer 25.
• This first peak 43 therefore corresponds to an interference between two components of the measuring beam 16 reflected on the two interfaces of the object 24 located on either side of the thin layer 25.
• It also comprises a second peak 44 and a third peak 45 respectively corresponding to interference between the reference beam 17 and the components of the measuring beam 16 reflected on the one and the other interfaces of the object 24 located on either side. else of the thin layer 25.
• the measuring head 10 is moved relative to the object to be measured 24 with the displacement means 21, which makes the optical path difference between the measuring and reference beams 16 vary. 17.
• they can be positioned in a preferred area of the measuring range where they can be distinguished and measured under good conditions. For this, we set the peaks of interest 44, 45:
• This measurement range extends from zero (zero delay) to delays for which the spectral modulation frequencies can no longer be sampled due to the spectral resolution of the spectrometer.
• the measuring head 10 positions the measuring head 10 relative to the object 24 so that the optical path length of the reference optical beam 17 is intermediate between the lengths of the optical paths of the measuring beam 16 as reflected by the respective interfaces of the thin layer 25.
• the reference surface 14 appears optically as being between the interfaces of the thin layer 25, and the peaks of the interest 44, 45 are at times ⁇ (or differences in optical paths 2L) less than that corresponding to the thickness of the thin layer 25 of the object 24.
• the total measurement range is thus essentially determined by the travel of the displacement means 21, and
• the resolution that is to say the ability to discriminate near interfaces is determined by the resolution of the spectral detection.
• the interferometer makes it possible to determine differences in optical paths 2L between the reference beam and the measuring beam reflected by the interfaces of the object 24. It thus makes it possible to determine the optical heights of these interfaces by relation to an origin defined by an optical path equality in the interferometer.
• the optical distances or height correspond to the distances or geometric heights multiplied by the refractive index of the mediums traversed.
• these heights l_i correspond to the optical distance between the reference surface 14 and the interfaces of the object 24 along the Z axis.
• optical height measurements Hl j of the measurement object interfaces 24 in its opposite side in a similar manner with the second optical measuring means 27.
• these optical HLJ height measurements are measured by relation to the same origin of the coordinate system (X, Y, Z).
• Optical thicknesses T of the object can then be determined by adding (or subtracting according to the sign conventions) the optical heights Hu and Hl obtained along the two faces of the object 24.
• the measuring beam is positioned on the surface of the object to be measured 24 by means of the second translation means 22 (step 50);
• the measurement head Z is moved relative to the object to be measured with the displacement means 21 to vary the optical path difference between the measurement and reference beams 17 (step 51);
• the peak or points of interest 44, 45 are identified as explained above and or positioned in a preferential zone of the measurement range (step 52); the difference (s) of the optical paths l_i corresponding to these peaks of interest 44, 45 are measured in the measurement range of the interferometer (with respect to the zero delay corresponding to an equality of optical paths of the measurement beams 16 and reference 17 (step 53);
• the optical height is calculated HU ⁇ interfaces of the object 24 by taking into account the position P H of the interferometer as described above (step 54);
• an optical height measurement Hlj of the interfaces of the measurement object 24 is also performed along its opposite face with the second optical measurement means 27, and a combination of optical heights Hu and Hl is combined. to determine the (optical) thickness T (step 55).
• the measurement beams can then be moved to another point on the surface of the object 24 to make another measurement and thus to map or topology the object 24.
• the step 51 of displacement of the measuring head 10 can be omitted between the measurement points on the surface of the object if the identification of the peaks of interest is retained.
• the method according to the invention also comprises a calibration step 56 which makes it possible to determine the value of the position P H of the interferometer or of the measurement head 10 along the Z axis. For this, one or more measurements on the reference object 26 whose height Hu is known, and the value of the position P H is deduced therefrom. It is also possible to calibrate in a similar way the second optical measuring means 27.
• This calibration procedure can be performed once before performing a set of measurements on the surface of an object 24.

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• Physics & Mathematics (AREA)
• General Physics & Mathematics (AREA)
• Length Measuring Devices By Optical Means (AREA)

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• 2015
  • 2015-12-22 FR FR1563128A patent/FR3045813B1/fr active Active
• 2016
  • 2016-12-07 CN CN201680074722.9A patent/CN108431545A/zh active Pending
  • 2016-12-07 US US16/061,268 patent/US20180364028A1/en not_active Abandoned
  • 2016-12-07 WO PCT/EP2016/080005 patent/WO2017108400A1/fr active Application Filing
  • 2016-12-07 KR KR1020187017326A patent/KR20180098255A/ko unknown
  • 2016-12-07 EP EP16816597.5A patent/EP3394560A1/de not_active Withdrawn
  • 2016-12-14 TW TW105141398A patent/TW201728869A/zh unknown

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