CA1258164A - Ellipsometric method and apparatus for studying physical properties of the surface of a testpiece - Google Patents
Ellipsometric method and apparatus for studying physical properties of the surface of a testpieceInfo
- Publication number
- CA1258164A CA1258164A CA000491057A CA491057A CA1258164A CA 1258164 A CA1258164 A CA 1258164A CA 000491057 A CA000491057 A CA 000491057A CA 491057 A CA491057 A CA 491057A CA 1258164 A CA1258164 A CA 1258164A
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- Canada
- Prior art keywords
- set forth
- testpiece
- portions
- surface portions
- radiation
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
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Classifications
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/21—Polarisation-affecting properties
- G01N21/211—Ellipsometry
Abstract
ABSTRACT OF THE INVENTION
In an ellipsometric method and apparatus which, in order to increase the degree of measuring accuracy, uses the principle of comparative ellipsometry in measuring a characteristic such as a layer thickness, a reference surface is divided into first and second equal surface portions with respectively different reflection characteristics which are in substantially symmetrical relationship to the reflection characteristics of the testpiece, the surface portions preferably comprising two different tapering surface layers extending in parallel relationship to each other.
In an ellipsometric method and apparatus which, in order to increase the degree of measuring accuracy, uses the principle of comparative ellipsometry in measuring a characteristic such as a layer thickness, a reference surface is divided into first and second equal surface portions with respectively different reflection characteristics which are in substantially symmetrical relationship to the reflection characteristics of the testpiece, the surface portions preferably comprising two different tapering surface layers extending in parallel relationship to each other.
Description
.
The invention relates to an ellipsometric apparatus.
An ellipsometric apparatus is disclosed in European patent speciflcation No 19088. That comparative ellipsometer makes it possible to investigate physical surface properties, for exanple the thiclcnesses of layers or films on the surfaces of testpieces or samples, in an evepiece, directly and wlthout the assistance of expensive electronic evaluation ec~uipment. For that purpose, light which is po]arisecl by a polariser is caused to be reflected at a reference surface with ]cnown reflection characteristics, and a surface of a testpiece which is to be investigated, with the angles of incidence at each surface being the same, the reference surface and the testpiece surface being perpendicular to each other with their angles of incidence or the direction of polarisation of the radiation being turned through 90 between the two surfaces in c~uestion.
If the reflection characteristics of the reference surface and the testpiece surface are the same, for example if a layer or film which is to be found on the surface of the testpiece is of the same thiclcness as a layer or film on the reference surface, the light is extinguished by an anlyser disposc~ downstrec~ of the testpiece.
When using a refererlce surface havillg a layer thereon which is of a wedge-lilce or tapered configuration, together with an associated suitable reading-off scale, the procedure is that, when the thiclcness of the layer or film on the surface of the testpiece is found to be the same as a given location on the tapered layer ~81~
on the reference surface, a dark measuring strip can be seen at a glven location on the scale, in the eyepiece which is disposed downstream of the anlyser. In that way it ls possible to measure layer thicknesses of from 2 nm up to 50 um, with a high degree of accuracy which in many cases may be better than + 2%.
In the apparatuses which have been disclosed hitherto in that respect, the degree of measuring accuracy is limited by virtue of the fact that the display of the measured thickness of the layer in question appears in the eyepiece in the form of a dark measuring strip which covers over a certain area on the scale.
According to the present invention there is provided an ellipsometric apparatus for investigating physical properties of a testpiece surface, comprising a polarising means for deflecting polarised radiation on to a reference surface with reflection characteristics varying in one direction and a said testpiece surface to be investigated, the reference surface comprising first and second surface portions with different reflection characteristics, at which the radiation is simultaneously reflected, said reflection characteristics thereof being in substantially symmetrical relation-ship with respect to those of the testpiece surface to beinvestigated, means for disposing saicl surfac~sin the apparatus such that said radiation is reflected with at least substantially the same angles of incidence and with a direction of polarisation rotated through 90, between said two surfaces, and analyser for extinguishing the radiation reflected by the testpiece surface, for the radiation component which has the same state of polarisation as prior to the first reflection.
~s will be seen by reference to a preferred embodiment of the apparatus of the invention, the apparatus permits physical surface properties to be ascertained readily but with an enhanced level of measuring accuracy.
In an advantageous embodiment of the apparatus, the reflection characteristics of the first and second surface portions of the reference surface are such that an analyser disposed downstream of the testpiece forms surface regions or grey zones with the same pattern of intensity, around the extinction strips. In another advantageous feature of the invention, the above-mentioned analyser forms two extinction strips whose mutually overlapping edge regions or grey zones, in their overlap region, forma measurement line in respect of the reflection characteristics of the testpiece. The reflection factor of the surface of the testpiece is between the two values of the two surface portions of the reference surface, while the reflection characteristics of the surface of the testpiece are approximately metln v~lues in resl~ct oE those o;E the two surface 6~
portlons of the reference surface. The difference between the reflection characteristics of the two surface portions of the reference surface advantageously remains the same in the direction of variation while the change in the reflection characteristics of the two surface portions is such as to be linear. The two surface portions of the reference surface may advantageously have surface layers which are of different thicknesses and which extend in mutually parallel relationship while in an advantageous feature the reflectlon charaeteristics, along the two surface portions in the same direction, have a ehange whieh is the same in percentage terms, for both surfaee portions. rrhe two surface portions of the reference surfaee may be formed by two halves of the reference surfaee, or they may be formed by a strip-like grid, with the respeetively adjoining strip portions of the grid pattern alternately having the different refleetion eharaeteristies referred to akove. rrhe surfaee portions of the referenee surfaee may also be formed by a grid eonfiguration made up of sc~uare or reetangular portions, or triangular portions.
The two surface portions of the referenee surfaee are advantageously of substantially the same areas. The apparatus may also be sueh that the testpieee to be investigated and studied :i.s arrancJed to b~ movabl.e while, in order to canpensdl:e~ lor an asymllletry 1ll respect oE the intensity of distribution of radiation aroutld the radiation extinetion strips, the read-off scale may be suitably displaced by appropriate means.
In another advantageous feature, the spaeings of the scale portions from each other are of suitably dlfferent magnitudes in order to compensate for asymmetry of distrlbution of intensity of the radiation as referred to above.
Another advantageous feature provides that, where the surface portions of the reference surface have layers thereon of wedge-shaped or tapering cross-sectional configuration, of different thicknesses, the smallest thickness of the thicker of the layers on the one surface portic,n is at least substantially equal to the greatest thickness of the thinner layer on the other surface portion. The reference surface may ccmprise a plurality of sets of the first and second surface portions, each set being of different reflection characteristics from each other set, to permit the apparatus to be used for investigating a range of testpieces by using the appropriate set of surface portions on the reference surface in the apparatus. It would l-,kewise be possible for the reference surface to comprise first and second sets of the first and second reference surface portions, with the reflection characteristics of one set being different from those of the other set, to permit the apparatus to deal with two ma:in ranges of testpieces.
With a construction oi the apr~lratus in accordance with the invention, for example when measuring the thicknesses of layers or films on the surfaces of testpieces, it is possible to use a reference surface which has ]ayers thereon of shallow wedge-shaped or tapering cross--sectional configuration, for example in a range il ~ r~S ~
of from 5 ~lm to 500 nm. Such reference layer thicknesses, in conventionai manner, would form a relatively wide extinction or measuring strip in the eyepiece of the ellipsometer, so that the degree of measuring accuracy that can be attained cannot be increased.
In accordance with the apparatus of the present invention, that difficulty is avoided in that, by making use of the symmetry of distribution of intensity on both sides of the extinction strips, the reference surface is divided into two surface portions which have different reflection characteristics or properties, as indicated above, those characteristics varying in linear fashion in a given direction. As indicated, that variation is substantially the same in percentage terms for both surface portions of the reference surface, and is in the same direction. When the apparatus is to be used for measuring the thickness of a layer, it is possible for that purpose to employ wedge-shaped or tapered reference layers for the two surface port:ions of the reference surface, those layers or surface portions extending in parallel relationship with each other.
As will be more clearly apparent hereinafter, the reflection characteristics of the first and second surface portions are such that they are in substantially symmetrical relationship to the reflection characteristic of the testpiece. The tapering configuration of the layer thicknesses on the two surface portions of the reference surface makes it possible to cover a given range with which it is then possible to measure certain reflection characteristics, for example parameters which influence the reflection phenomenon at surfaces, such as the thickness of a layer on a surface of a testpiece.
Thus, the analyser which is disposed downstream of the testpiece to be studied, as will be described in greater detail hereinafter, produces two extinction strips whose mutually overlapping edge regions or grey zones, in their region of overlap, form a sharp measurin~ line which can be clearly perceived in the eyepiece, in respect of the reflection characteristic of the testpiece and more pa~ticularly for example the thickness of a layer on the surface thereof.
A method and appafatus according to the present.invention will now be described by way of example with reference to the accompanying drawings in which:
Figurel is a diagrammatic view of the variation in intensity of a measuring strip which appears in the eyepiece of a comparison ellipsometer, Figure 2 is a diagrammatic view in cross-section through an embodiment of a reference surface, Figure 3 shows a cross-sectional configuration of another embodi~ent of the reference surface, Figure 4 shows a plan view of the reference surface shown in Figure 2, Figure 5 shows a plan view of the reference surface shown in Figure 3, Figure 6 is a plan view of a further embodiment of the 1~5~
reference surface, Figure 7 is yet another embodiment of the reference surface, and Figure 8 is a diagrammatic view of an embodiment of the ellipsometer.
Reference will first be made to Figure 8 which in highly diagrammatic form shows an ellipsometer apparatus. In the arrangement shown in Figure 8, an incident parallel radiation is linearly polarised, at -45, by means of a polariser 5. The polarised radiation downstream of the polariser 5 impinges on a reference surface 2 by means of which it is reflected. The light reflected from the reference surface 2 is subjected to elliptical polarisation, depending on the nature of the reference surface. The reference surface has certain characteristics which affect the reflection phenomenon and may have the surface configurations shown in Figures
The invention relates to an ellipsometric apparatus.
An ellipsometric apparatus is disclosed in European patent speciflcation No 19088. That comparative ellipsometer makes it possible to investigate physical surface properties, for exanple the thiclcnesses of layers or films on the surfaces of testpieces or samples, in an evepiece, directly and wlthout the assistance of expensive electronic evaluation ec~uipment. For that purpose, light which is po]arisecl by a polariser is caused to be reflected at a reference surface with ]cnown reflection characteristics, and a surface of a testpiece which is to be investigated, with the angles of incidence at each surface being the same, the reference surface and the testpiece surface being perpendicular to each other with their angles of incidence or the direction of polarisation of the radiation being turned through 90 between the two surfaces in c~uestion.
If the reflection characteristics of the reference surface and the testpiece surface are the same, for example if a layer or film which is to be found on the surface of the testpiece is of the same thiclcness as a layer or film on the reference surface, the light is extinguished by an anlyser disposc~ downstrec~ of the testpiece.
When using a refererlce surface havillg a layer thereon which is of a wedge-lilce or tapered configuration, together with an associated suitable reading-off scale, the procedure is that, when the thiclcness of the layer or film on the surface of the testpiece is found to be the same as a given location on the tapered layer ~81~
on the reference surface, a dark measuring strip can be seen at a glven location on the scale, in the eyepiece which is disposed downstream of the anlyser. In that way it ls possible to measure layer thicknesses of from 2 nm up to 50 um, with a high degree of accuracy which in many cases may be better than + 2%.
In the apparatuses which have been disclosed hitherto in that respect, the degree of measuring accuracy is limited by virtue of the fact that the display of the measured thickness of the layer in question appears in the eyepiece in the form of a dark measuring strip which covers over a certain area on the scale.
According to the present invention there is provided an ellipsometric apparatus for investigating physical properties of a testpiece surface, comprising a polarising means for deflecting polarised radiation on to a reference surface with reflection characteristics varying in one direction and a said testpiece surface to be investigated, the reference surface comprising first and second surface portions with different reflection characteristics, at which the radiation is simultaneously reflected, said reflection characteristics thereof being in substantially symmetrical relation-ship with respect to those of the testpiece surface to beinvestigated, means for disposing saicl surfac~sin the apparatus such that said radiation is reflected with at least substantially the same angles of incidence and with a direction of polarisation rotated through 90, between said two surfaces, and analyser for extinguishing the radiation reflected by the testpiece surface, for the radiation component which has the same state of polarisation as prior to the first reflection.
~s will be seen by reference to a preferred embodiment of the apparatus of the invention, the apparatus permits physical surface properties to be ascertained readily but with an enhanced level of measuring accuracy.
In an advantageous embodiment of the apparatus, the reflection characteristics of the first and second surface portions of the reference surface are such that an analyser disposed downstream of the testpiece forms surface regions or grey zones with the same pattern of intensity, around the extinction strips. In another advantageous feature of the invention, the above-mentioned analyser forms two extinction strips whose mutually overlapping edge regions or grey zones, in their overlap region, forma measurement line in respect of the reflection characteristics of the testpiece. The reflection factor of the surface of the testpiece is between the two values of the two surface portions of the reference surface, while the reflection characteristics of the surface of the testpiece are approximately metln v~lues in resl~ct oE those o;E the two surface 6~
portlons of the reference surface. The difference between the reflection characteristics of the two surface portions of the reference surface advantageously remains the same in the direction of variation while the change in the reflection characteristics of the two surface portions is such as to be linear. The two surface portions of the reference surface may advantageously have surface layers which are of different thicknesses and which extend in mutually parallel relationship while in an advantageous feature the reflectlon charaeteristics, along the two surface portions in the same direction, have a ehange whieh is the same in percentage terms, for both surfaee portions. rrhe two surface portions of the reference surfaee may be formed by two halves of the reference surfaee, or they may be formed by a strip-like grid, with the respeetively adjoining strip portions of the grid pattern alternately having the different refleetion eharaeteristies referred to akove. rrhe surfaee portions of the referenee surfaee may also be formed by a grid eonfiguration made up of sc~uare or reetangular portions, or triangular portions.
The two surface portions of the referenee surfaee are advantageously of substantially the same areas. The apparatus may also be sueh that the testpieee to be investigated and studied :i.s arrancJed to b~ movabl.e while, in order to canpensdl:e~ lor an asymllletry 1ll respect oE the intensity of distribution of radiation aroutld the radiation extinetion strips, the read-off scale may be suitably displaced by appropriate means.
In another advantageous feature, the spaeings of the scale portions from each other are of suitably dlfferent magnitudes in order to compensate for asymmetry of distrlbution of intensity of the radiation as referred to above.
Another advantageous feature provides that, where the surface portions of the reference surface have layers thereon of wedge-shaped or tapering cross-sectional configuration, of different thicknesses, the smallest thickness of the thicker of the layers on the one surface portic,n is at least substantially equal to the greatest thickness of the thinner layer on the other surface portion. The reference surface may ccmprise a plurality of sets of the first and second surface portions, each set being of different reflection characteristics from each other set, to permit the apparatus to be used for investigating a range of testpieces by using the appropriate set of surface portions on the reference surface in the apparatus. It would l-,kewise be possible for the reference surface to comprise first and second sets of the first and second reference surface portions, with the reflection characteristics of one set being different from those of the other set, to permit the apparatus to deal with two ma:in ranges of testpieces.
With a construction oi the apr~lratus in accordance with the invention, for example when measuring the thicknesses of layers or films on the surfaces of testpieces, it is possible to use a reference surface which has ]ayers thereon of shallow wedge-shaped or tapering cross--sectional configuration, for example in a range il ~ r~S ~
of from 5 ~lm to 500 nm. Such reference layer thicknesses, in conventionai manner, would form a relatively wide extinction or measuring strip in the eyepiece of the ellipsometer, so that the degree of measuring accuracy that can be attained cannot be increased.
In accordance with the apparatus of the present invention, that difficulty is avoided in that, by making use of the symmetry of distribution of intensity on both sides of the extinction strips, the reference surface is divided into two surface portions which have different reflection characteristics or properties, as indicated above, those characteristics varying in linear fashion in a given direction. As indicated, that variation is substantially the same in percentage terms for both surface portions of the reference surface, and is in the same direction. When the apparatus is to be used for measuring the thickness of a layer, it is possible for that purpose to employ wedge-shaped or tapered reference layers for the two surface port:ions of the reference surface, those layers or surface portions extending in parallel relationship with each other.
As will be more clearly apparent hereinafter, the reflection characteristics of the first and second surface portions are such that they are in substantially symmetrical relationship to the reflection characteristic of the testpiece. The tapering configuration of the layer thicknesses on the two surface portions of the reference surface makes it possible to cover a given range with which it is then possible to measure certain reflection characteristics, for example parameters which influence the reflection phenomenon at surfaces, such as the thickness of a layer on a surface of a testpiece.
Thus, the analyser which is disposed downstream of the testpiece to be studied, as will be described in greater detail hereinafter, produces two extinction strips whose mutually overlapping edge regions or grey zones, in their region of overlap, form a sharp measurin~ line which can be clearly perceived in the eyepiece, in respect of the reflection characteristic of the testpiece and more pa~ticularly for example the thickness of a layer on the surface thereof.
A method and appafatus according to the present.invention will now be described by way of example with reference to the accompanying drawings in which:
Figurel is a diagrammatic view of the variation in intensity of a measuring strip which appears in the eyepiece of a comparison ellipsometer, Figure 2 is a diagrammatic view in cross-section through an embodiment of a reference surface, Figure 3 shows a cross-sectional configuration of another embodi~ent of the reference surface, Figure 4 shows a plan view of the reference surface shown in Figure 2, Figure 5 shows a plan view of the reference surface shown in Figure 3, Figure 6 is a plan view of a further embodiment of the 1~5~
reference surface, Figure 7 is yet another embodiment of the reference surface, and Figure 8 is a diagrammatic view of an embodiment of the ellipsometer.
Reference will first be made to Figure 8 which in highly diagrammatic form shows an ellipsometer apparatus. In the arrangement shown in Figure 8, an incident parallel radiation is linearly polarised, at -45, by means of a polariser 5. The polarised radiation downstream of the polariser 5 impinges on a reference surface 2 by means of which it is reflected. The light reflected from the reference surface 2 is subjected to elliptical polarisation, depending on the nature of the reference surface. The reference surface has certain characteristics which affect the reflection phenomenon and may have the surface configurations shown in Figures
2 to 6, as will be described in greater detail hereinafter.
Downstream of the reference surface 2 is a testpiece surface as indicated at 7 which is so arranged that the light impinges on the testpiece surface 7 with the same angle of incidence, as indicated by i, as the angle of incidence on the reference surface 2. In the embodiment illustrated herein, the reference surface 2 and the testpiece surface 7 are so arranged that their planes of incidence are normal to each other, thereby ensuring that the direction of polarisation of the radiation or light is turned through 90, that is to say, the light leaving the testpiece surface 7 is ~ r} ~ L~
linearly polarised at +45.
It will be appreciated that, instead of the arrangement of the reference surface 2 and the testplece surface 7 as illustrated in Figure 8, it is also possible to use for example an optical component such as a prism which turns the direction of polarisation of the light through 90 between the surfaces 2 and 7.
Finally, disposed downstream of the testpiece surface 7 is an analyser as indicated at 6 in Figure 8. The polariser 5 and the analyser 6 remain fixed in their set positions and their directions of polarisation are at a right angle to each other.
When the ellipsometric apparatus illustrated is used for measuring the thickness of a layer at the testpiece surface as indicated at 7, the reference surface 2 has first and second substantially identical surface portions 3 and 4, as shown in greater detail in Figures 2 to 7. The surface portions 3 and 4 have different reflection properties or characteristics by virtue of the fact that films or layers which are of a wedge-like or tapering configuration are provided on a base body l, as can be clearly seen for example from Figures 2 and 4~ As can be seen more particularly frcm the embodiment shown in Figures 2 and 4, the surface (not referenced) of the body l is covered over one hal:E oE l~ e ~urEace (surEace portion 4) by a layer or :Eilm which is of a shallow wedge-like or tapering configuration in regard to its thickness, as can be seen most clearly from Figure 2. Likewise, the other half of the surface of the body 1., constituting the surface portion 3, is covered ,4 by a film or layer which is also of a wedge-like or tapering configuration. The configurations of the two layers are in parallel relationship to each other, although it will be appreciated by looking at Figure 2 that the layer on the surface portion 3 is thicker than that on the surface portion 4. In the illustrated embodiment, the difference in thickness between the layers on the surface portions 3 and 4 is 5 nm along the entire layer configuration. In the case of the surface portion 4 shown in Figure 2, the thickness of the layer in the illustrated embodiment begins at 15 nm and finishes at 20 nm.
On the other hand, in respect of the surface portion 3, the thickness of the layer begins at 20 nm and finishes at 25 nm.
The two layers on the surface portions 3 and 4 shown in Figures 2 and 4 comprise a material having the same refractive index, for example SiO2. When a reference surface 2 which is of the above-defined nature and configuration is introduced into the ellipsometricapparatus, together with a testpiece surface to be investigated or studied, it is possible precisely to ascertain the thicknesses of layers on the testpiece surface if such thicknesses lie within a range of from 17.5 nm to 22.5 nm. For that range of thicknesses of layers on the testpiece surface, the apparatus ensures that, by virtue of the two surface portions 3 and 4 constituting the reference surface 2, two extinction strips are formed by th~ analyser 6, the edge portions or grey zones of which overlap each other and, in the region of overlap, form a relatively sharp measuring line which on the display scale shows the precise thickness of the layer or film 6~
on the testpiece surface 7.
In the above-described embodiment of Figures 2 and 4, and likewise in regard to the other embodiments illustrated by way of example in Figures 3 and 5 to 7, the layers on the surface portions
Downstream of the reference surface 2 is a testpiece surface as indicated at 7 which is so arranged that the light impinges on the testpiece surface 7 with the same angle of incidence, as indicated by i, as the angle of incidence on the reference surface 2. In the embodiment illustrated herein, the reference surface 2 and the testpiece surface 7 are so arranged that their planes of incidence are normal to each other, thereby ensuring that the direction of polarisation of the radiation or light is turned through 90, that is to say, the light leaving the testpiece surface 7 is ~ r} ~ L~
linearly polarised at +45.
It will be appreciated that, instead of the arrangement of the reference surface 2 and the testplece surface 7 as illustrated in Figure 8, it is also possible to use for example an optical component such as a prism which turns the direction of polarisation of the light through 90 between the surfaces 2 and 7.
Finally, disposed downstream of the testpiece surface 7 is an analyser as indicated at 6 in Figure 8. The polariser 5 and the analyser 6 remain fixed in their set positions and their directions of polarisation are at a right angle to each other.
When the ellipsometric apparatus illustrated is used for measuring the thickness of a layer at the testpiece surface as indicated at 7, the reference surface 2 has first and second substantially identical surface portions 3 and 4, as shown in greater detail in Figures 2 to 7. The surface portions 3 and 4 have different reflection properties or characteristics by virtue of the fact that films or layers which are of a wedge-like or tapering configuration are provided on a base body l, as can be clearly seen for example from Figures 2 and 4~ As can be seen more particularly frcm the embodiment shown in Figures 2 and 4, the surface (not referenced) of the body l is covered over one hal:E oE l~ e ~urEace (surEace portion 4) by a layer or :Eilm which is of a shallow wedge-like or tapering configuration in regard to its thickness, as can be seen most clearly from Figure 2. Likewise, the other half of the surface of the body 1., constituting the surface portion 3, is covered ,4 by a film or layer which is also of a wedge-like or tapering configuration. The configurations of the two layers are in parallel relationship to each other, although it will be appreciated by looking at Figure 2 that the layer on the surface portion 3 is thicker than that on the surface portion 4. In the illustrated embodiment, the difference in thickness between the layers on the surface portions 3 and 4 is 5 nm along the entire layer configuration. In the case of the surface portion 4 shown in Figure 2, the thickness of the layer in the illustrated embodiment begins at 15 nm and finishes at 20 nm.
On the other hand, in respect of the surface portion 3, the thickness of the layer begins at 20 nm and finishes at 25 nm.
The two layers on the surface portions 3 and 4 shown in Figures 2 and 4 comprise a material having the same refractive index, for example SiO2. When a reference surface 2 which is of the above-defined nature and configuration is introduced into the ellipsometricapparatus, together with a testpiece surface to be investigated or studied, it is possible precisely to ascertain the thicknesses of layers on the testpiece surface if such thicknesses lie within a range of from 17.5 nm to 22.5 nm. For that range of thicknesses of layers on the testpiece surface, the apparatus ensures that, by virtue of the two surface portions 3 and 4 constituting the reference surface 2, two extinction strips are formed by th~ analyser 6, the edge portions or grey zones of which overlap each other and, in the region of overlap, form a relatively sharp measuring line which on the display scale shows the precise thickness of the layer or film 6~
on the testpiece surface 7.
In the above-described embodiment of Figures 2 and 4, and likewise in regard to the other embodiments illustrated by way of example in Figures 3 and 5 to 7, the layers on the surface portions
3 and 4 of the reference surface are of such a dimension that the smallest thickness of the thicker layer, on the surface portion 3 in the case of the embodiment shown in Figures 2 and 4, is equal to the greatest thickness of the thinner layer which is on the surface portion 4. It will be seen with reference to Figure 2 that for example the smallest thickness of the layer ont~e surface portion 3, which is 20 nm, is equal to the greatest thickness of the thinner layer on the surface portion 4, being also therefore 20 nm. In the embodiment illustrated in Figures 2 and 4, the difference between 'he two layer configurations which extend in mutually parallel relationship on the respective surface portions 3 and 4 is 5 nm.
That means that, with the illustrated em~odiment, it is possible precisely to measure the thicknesses of layers on the testpiece surface, which are in a range of from 17.5 nm to 22.5 nm, as indicated acove.
At this point reference will be made to Figure 1 which shows that the extinction line has a distribution in respect of intensity which is in the form of a parabola and which is of substantially symmetrical configuration at both sides of the blackening maximum as indicated at dM which represents the ideal measurement value in respect of the layer thickness to be measured. When using the ~t~
above-described apparatus, use is made of the effect which occurs when measuring thin layers or films, that the reference layer thicknesses on the reference surface 2 are on the two sides of the above-indicated maximum dM, and have a constant spacing of ~ d over their entire range. In the illustrated embodiment a d is 5 nm, as indicated above.
As has already been mentioned hereinbefore, in the embodiment shown in Figures 2 and 4 the reference surface 2 is formed by two halves 3 and 4, with layers of a generally shallow tapering configuration which are disposed in mutually parallel relationship, with a difference of 5 nm between the thicknesses of the two layers.
Reference will now be made to Figures 3 and 5 showing a reference surface having surface portions thereon formed by a strip grid, as can be clearly seen frGm Figure 5. It will be seen therefore that the surfaces on the tops of the raised portions of the grid configuration, that can be clearly seen in cross-section from Figure 3, constitute one surface portion while the floors of the depressions between the raised portions constitute the other surface portion 4.
In the case of the cons-truction shown in Figure 6, the surface portions of the reference surface are defined by a grid configuration made up of square or rectangular portions while in the construction shown in Figure 7 the grid configuration is made up of triangular portions. It will be appreciated that it is also possible to use other grid forms and configurations for the two surface portions 3 i4 and 4, on which the various tapering layer thicknesses of the reference surface are disposed.
The apparatus as described hereinbefore preferably employs monochromatic light because that then gives a monochrome distribution of intensity of the two measuring strips produced, which in their overlap region form a measuring line with sharp contours, as indicated above.
By virtue of the fact that the testpiece 7 is so disposed in the apparatus that it can be moved, it is possible to detect local raised portions on the testpiece surface~ Such raised portions may be formed for example in biomolecular reactions, for example in antigen-antibody reactions.
Minor asymmetry of the distribution of intensity at the extinction strips can be compensated for by suitable displacement of the scale, which is related to the tapering layer thickness configurations in the surface portions 3 and 4 of the reference surface 2.
The degree of measuring accuracy that the invention can be found to achieve is of the order of magnitude of 0.1 nm.
In the illustrated embodiments, as can be seen for example from Figures 2 and 3, the layer configurations at the surface portions 3 and 4 of the reference surface 2 are of a shallow wedge-like or tapered configuration. It should be observed however that it is also possible for the layer configuration in each surface portion 3 and 4 not to be of a straight-line nature but to be of a curved form, although in that case the two curved configurations on the surface portions 3 and 4 are to be in parallel relationship -to e~ch other, that is to say, ~le difference in thickness between the two layers in the two surface portions 3 and 4 always remains constant over the entire reference surface 2.
It is also possible for the reference surface 2 to comprise a multiple arrangement of the two surface portions 3 and 4, that is to say, the surface 2 may comprise two or more sets or pairs of surface portions 3 and 4 which are of the above-indicated nature. It is then possible to measure or detect, on the testpiece, a correspondingly large number of surface layers with respectively different reflection characteristics, such as and more particularly different layer thicknesses thereon.
It will be appreciated that the foregoing description is given solely by way of example of the apparatus according to the invention and that various modifications and alterations may be made in the described apparatus and structures without thereby departing from the scope of the invention as defined by the appended claims.
That means that, with the illustrated em~odiment, it is possible precisely to measure the thicknesses of layers on the testpiece surface, which are in a range of from 17.5 nm to 22.5 nm, as indicated acove.
At this point reference will be made to Figure 1 which shows that the extinction line has a distribution in respect of intensity which is in the form of a parabola and which is of substantially symmetrical configuration at both sides of the blackening maximum as indicated at dM which represents the ideal measurement value in respect of the layer thickness to be measured. When using the ~t~
above-described apparatus, use is made of the effect which occurs when measuring thin layers or films, that the reference layer thicknesses on the reference surface 2 are on the two sides of the above-indicated maximum dM, and have a constant spacing of ~ d over their entire range. In the illustrated embodiment a d is 5 nm, as indicated above.
As has already been mentioned hereinbefore, in the embodiment shown in Figures 2 and 4 the reference surface 2 is formed by two halves 3 and 4, with layers of a generally shallow tapering configuration which are disposed in mutually parallel relationship, with a difference of 5 nm between the thicknesses of the two layers.
Reference will now be made to Figures 3 and 5 showing a reference surface having surface portions thereon formed by a strip grid, as can be clearly seen frGm Figure 5. It will be seen therefore that the surfaces on the tops of the raised portions of the grid configuration, that can be clearly seen in cross-section from Figure 3, constitute one surface portion while the floors of the depressions between the raised portions constitute the other surface portion 4.
In the case of the cons-truction shown in Figure 6, the surface portions of the reference surface are defined by a grid configuration made up of square or rectangular portions while in the construction shown in Figure 7 the grid configuration is made up of triangular portions. It will be appreciated that it is also possible to use other grid forms and configurations for the two surface portions 3 i4 and 4, on which the various tapering layer thicknesses of the reference surface are disposed.
The apparatus as described hereinbefore preferably employs monochromatic light because that then gives a monochrome distribution of intensity of the two measuring strips produced, which in their overlap region form a measuring line with sharp contours, as indicated above.
By virtue of the fact that the testpiece 7 is so disposed in the apparatus that it can be moved, it is possible to detect local raised portions on the testpiece surface~ Such raised portions may be formed for example in biomolecular reactions, for example in antigen-antibody reactions.
Minor asymmetry of the distribution of intensity at the extinction strips can be compensated for by suitable displacement of the scale, which is related to the tapering layer thickness configurations in the surface portions 3 and 4 of the reference surface 2.
The degree of measuring accuracy that the invention can be found to achieve is of the order of magnitude of 0.1 nm.
In the illustrated embodiments, as can be seen for example from Figures 2 and 3, the layer configurations at the surface portions 3 and 4 of the reference surface 2 are of a shallow wedge-like or tapered configuration. It should be observed however that it is also possible for the layer configuration in each surface portion 3 and 4 not to be of a straight-line nature but to be of a curved form, although in that case the two curved configurations on the surface portions 3 and 4 are to be in parallel relationship -to e~ch other, that is to say, ~le difference in thickness between the two layers in the two surface portions 3 and 4 always remains constant over the entire reference surface 2.
It is also possible for the reference surface 2 to comprise a multiple arrangement of the two surface portions 3 and 4, that is to say, the surface 2 may comprise two or more sets or pairs of surface portions 3 and 4 which are of the above-indicated nature. It is then possible to measure or detect, on the testpiece, a correspondingly large number of surface layers with respectively different reflection characteristics, such as and more particularly different layer thicknesses thereon.
It will be appreciated that the foregoing description is given solely by way of example of the apparatus according to the invention and that various modifications and alterations may be made in the described apparatus and structures without thereby departing from the scope of the invention as defined by the appended claims.
Claims (22)
1. An ellipsometric apparatus for investigating physical properties of a testpiece surface, comprising a polarising means for deflecting polarised radiation on to a reference surface with reflection characteristics varying in one direction and a said testpiece surface to be investigated, the reference surface comprising first and second surface portions with different reflection characteristics, at which the radiation is simultaneously reflected, said reflection characteristics thereof being in substantially symmetrical relationship with respect to those of the testpiece surface to be investigated, means for disposing said surfaces in the apparatus such that said radiation is reflected with at least substantially the same angles of incid-ence and a direction of polarisation which is rotated through 90°, between said two surfaces, and an analyser for extinguishing the radiation reflected by the downstream surface, for the radiation component which has the same state of polarisation as prior to the first reflection.
2. Apparatus as set forth in claim 1 wherein the reflection characteristics of said surface portions are such that the analyser forms surface regions (grey zones) with the same pattern of intensity around the extinction strips.
3. Apparatus as set forth in claim 1 wherein said analyser forms two extinction strips having mutually overlapping edge regions (grey zones) which in their overlap region form a measurement line in respect of the reflection characteristics of the testpiece.
4. Apparatus as set forth in claim 1 wherein the reflection characteristic value of said testpiece surface is between the reflection characteristic values of said surface portions of said reference surface.
5. Apparatus as set forth in claim 1 wherein the reflection characteristics of said testpiece are approximately mean values of the reflection characterises of said surface portions of said reference surface.
6. Apparatus as set forth in claim 1 wherein the difference between the reflection characteristics of said surface portions remains the same in the direction of variation thereof.
7. Apparatus as set forth in claim 1 wherein the change in the reflection characteristics of said surface portions is linear.
8. Apparatus as set forth in claim 1 wherein said surface portions have surface layers of different thicknesses extending in mutually parallel relationship.
9. Apparatus as set forth in claim 1 wherein said reflection characteristics of said surface portions vary therealong in the same direction by the same amount in percentage terms.
10. Apparatus as set forth in claim 1 wherein said surface portions are formed by first and second halves of said reference surface.
11. Apparatus as set forth in claim 1 wherein said surface portions are formed by a strip-like grid configuration, with the alternate strip portions thereof having the respectively different reflection characteristics.
12. Apparatus as set forth in claim 1 wherein said surface portions are formed by a grid of rectangular portions.
13. Apparatus as set forth in claim 1 wherein said surface portions are formed by a grid of square portions.
14. Apparatus as set forth in claim 1 wherein said surface portions are formed by a grid of triangular portions.
15. Apparatus as set forth in claim 1 wherein said surface portions of said reference surface are of at least substantially equal areas.
16. Apparatus as set forth in claim 1 including means for moving same testpiece.
17. Apparatus as set forth in claim 1 and further including means for displacing the read-off scale for compensation for asymmetry in respect of the distribution of intensity of radiation around the radiation extinction strips.
18. Apparatus as set forth in claim 1 wherein the spacings of the scale portions from each other are of different magnitudes to compensate for asymmetry of distribution of intensity of the radiation around the radiation extinction strips.
19. Apparatus as set forth in claim 1 wherein each said surface portion comprises a layer of tapering configuration, the thickness of the layers forming the respective surface portions being different from each other and the smallest thickness of the thicker said layer being at least substantially equal to the greatest thickness of the thinner said layer.
20. Apparatus as set forth in claim 1 wherein said reference surfaces comprise a plurality of sets of said first and second surface portions.
21. Apparatus as set forth in claim 20 including a double set of said first and second surface portions.
22. An ellipsometric method of investigating physical properties of a testpiece surface comprising: subjecting a radiation to polarisation; directing said polarised radiation on to a reference surface comprising first and second surface portions with different reflection characteristics, said radiation being simultaneously reflected at said first and second surface portions, and on to a said testpiece surface, the reflection characteristics of said first and second surface portions of said reference surface being in substantially symmetrical relationship with respect to those of the testpiece surface to be investigated, said radiation being reflected with at least substantially the same angles of incidence and with polarisation which is rotated through 90° between said reference and testpiece surfaces; and extinguishing the radiation reflected by the downstream surface, in respect of the component having the same state of polarisation as prior to reflection at the upstream surface.
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| DEP3434575.2 | 1984-09-20 | ||
| DE3434575A DE3434575C1 (en) | 1984-09-20 | 1984-09-20 | Ellipsometric device for examining the physical properties of the surface of a sample |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CA1258164A true CA1258164A (en) | 1989-08-08 |
Family
ID=6245910
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA000491057A Expired CA1258164A (en) | 1984-09-20 | 1985-09-18 | Ellipsometric method and apparatus for studying physical properties of the surface of a testpiece |
Country Status (7)
| Country | Link |
|---|---|
| US (1) | US4655595A (en) |
| EP (1) | EP0175142A3 (en) |
| JP (1) | JPS61258104A (en) |
| CA (1) | CA1258164A (en) |
| DE (1) | DE3434575C1 (en) |
| DK (1) | DK424985A (en) |
| FI (1) | FI853170L (en) |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6060237A (en) * | 1985-02-26 | 2000-05-09 | Biostar, Inc. | Devices and methods for optical detection of nucleic acid hybridization |
| US5482830A (en) * | 1986-02-25 | 1996-01-09 | Biostar, Inc. | Devices and methods for detection of an analyte based upon light interference |
| US5468606A (en) * | 1989-09-18 | 1995-11-21 | Biostar, Inc. | Devices for detection of an analyte based upon light interference |
| AU609573B2 (en) * | 1988-01-11 | 1991-05-02 | Commonwealth Of Australia, The | Differential ellipsometer |
| US5042951A (en) * | 1989-09-19 | 1991-08-27 | Therma-Wave, Inc. | High resolution ellipsometric apparatus |
| US5639671A (en) * | 1989-09-18 | 1997-06-17 | Biostar, Inc. | Methods for optimizing of an optical assay device |
| US5541057A (en) * | 1989-09-18 | 1996-07-30 | Biostar, Inc. | Methods for detection of an analyte |
| US5166752A (en) * | 1990-01-11 | 1992-11-24 | Rudolph Research Corporation | Simultaneous multiple angle/multiple wavelength ellipsometer and method |
| US5955377A (en) * | 1991-02-11 | 1999-09-21 | Biostar, Inc. | Methods and kits for the amplification of thin film based assays |
| US5550063A (en) * | 1991-02-11 | 1996-08-27 | Biostar, Inc. | Methods for production of an optical assay device |
| US5418136A (en) * | 1991-10-01 | 1995-05-23 | Biostar, Inc. | Devices for detection of an analyte based upon light interference |
| US5494829A (en) * | 1992-07-31 | 1996-02-27 | Biostar, Inc. | Devices and methods for detection of an analyte based upon light interference |
| US5552272A (en) * | 1993-06-10 | 1996-09-03 | Biostar, Inc. | Detection of an analyte by fluorescence using a thin film optical device |
| US6734967B1 (en) * | 1995-01-19 | 2004-05-11 | Kla-Tencor Technologies Corporation | Focused beam spectroscopic ellipsometry method and system |
| US5608526A (en) * | 1995-01-19 | 1997-03-04 | Tencor Instruments | Focused beam spectroscopic ellipsometry method and system |
| US5835220A (en) * | 1995-10-27 | 1998-11-10 | Nkk Corporation | Method and apparatus for detecting surface flaws |
| US5958704A (en) * | 1997-03-12 | 1999-09-28 | Ddx, Inc. | Sensing system for specific substance and molecule detection |
| US6483580B1 (en) | 1998-03-06 | 2002-11-19 | Kla-Tencor Technologies Corporation | Spectroscopic scatterometer system |
| US20120077206A1 (en) | 2003-07-12 | 2012-03-29 | Accelr8 Technology Corporation | Rapid Microbial Detection and Antimicrobial Susceptibility Testing |
| US7687239B2 (en) | 2003-07-12 | 2010-03-30 | Accelrs Technology Corporation | Sensitive and rapid determination of antimicrobial susceptibility |
| US7336359B1 (en) | 2004-05-03 | 2008-02-26 | Purdue Research Foundation | System and method for nonlinear optical null ellipsometry |
| US7515253B2 (en) * | 2005-01-12 | 2009-04-07 | Kla-Tencor Technologies Corporation | System for measuring a sample with a layer containing a periodic diffracting structure |
| US7551294B2 (en) * | 2005-09-16 | 2009-06-23 | University Of Rochester | System and method for brewster angle straddle interferometry |
| CA2634066A1 (en) * | 2005-12-13 | 2007-06-21 | Great Basin Scientific | Improved thin film biosensor and method and device for detection of analytes |
| ES2551922T3 (en) | 2011-03-07 | 2015-11-24 | Accelerate Diagnostics, Inc. | Rapid cell purification systems |
| US10254204B2 (en) | 2011-03-07 | 2019-04-09 | Accelerate Diagnostics, Inc. | Membrane-assisted purification |
| US9677109B2 (en) | 2013-03-15 | 2017-06-13 | Accelerate Diagnostics, Inc. | Rapid determination of microbial growth and antimicrobial susceptibility |
| US10023895B2 (en) | 2015-03-30 | 2018-07-17 | Accelerate Diagnostics, Inc. | Instrument and system for rapid microogranism identification and antimicrobial agent susceptibility testing |
| US10253355B2 (en) | 2015-03-30 | 2019-04-09 | Accelerate Diagnostics, Inc. | Instrument and system for rapid microorganism identification and antimicrobial agent susceptibility testing |
| CN109827850A (en) * | 2019-01-15 | 2019-05-31 | 广东工业大学 | A kind of fexible film stretch bending device |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| SE416681B (en) * | 1979-04-17 | 1981-01-26 | Johan Emanuel Stenberg | SET YEMFORA TWO SURFACE REFLECTION FEATURES |
-
1984
- 1984-09-20 DE DE3434575A patent/DE3434575C1/en not_active Expired
-
1985
- 1985-08-13 EP EP85110146A patent/EP0175142A3/en not_active Withdrawn
- 1985-08-19 FI FI853170A patent/FI853170L/en not_active Application Discontinuation
- 1985-09-18 CA CA000491057A patent/CA1258164A/en not_active Expired
- 1985-09-19 DK DK424985A patent/DK424985A/en not_active Application Discontinuation
- 1985-09-19 US US06/777,646 patent/US4655595A/en not_active Expired - Lifetime
- 1985-09-20 JP JP60208544A patent/JPS61258104A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| EP0175142A3 (en) | 1987-08-26 |
| FI853170L (en) | 1986-03-21 |
| US4655595A (en) | 1987-04-07 |
| JPS61258104A (en) | 1986-11-15 |
| DE3434575C1 (en) | 1986-03-13 |
| EP0175142A2 (en) | 1986-03-26 |
| DK424985A (en) | 1986-03-21 |
| JPH0478122B2 (en) | 1992-12-10 |
| DK424985D0 (en) | 1985-09-19 |
| FI853170A0 (en) | 1985-08-19 |
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