Systems for and methods of measuring photomask flatness with reduced gravity-induced error
10871369 ยท 2020-12-22
Assignee
Inventors
- THOMAS JAMES DUNN (Penfield, NY, US)
- John Weston Frankovich (Fairport, NY, US)
- Robert Dennis Grejda (Fairport, NY, US)
- Christopher Alan Lee (Pittsford, NY, US)
- Matthew Ronald Millecchia (Fairport, NY, US)
- Yoshihiro Nakamura (Saitama, JP)
Cpc classification
G03F7/70783
PHYSICS
G03F7/707
PHYSICS
International classification
G03F1/22
PHYSICS
Abstract
The methods disclosed herein include recording at near-vertical first and second measurement positions respective first and second interferograms of the photomask surface and defining a difference map as the difference between the first and second interferograms. Respective first and second normal forces on the photomask are also measured at the first and second measurement positions. The change in the normal force is used define a scaling factor, which is applied to the difference map to define a scaled difference map. A compensated flatness measurement with a reduced shape contribution due to gravity is obtained by subtracting the scaled difference map from the first interferogram. An interferometer-based flatness measurement system is also disclosed.
Claims
1. A method of interferometrically measuring flatness of a photomask supported at a support location, comprising: recording at first and second measurement positions respective first and second interferograms of a surface of the photomask, and measuring respective first and second normal forces F.sub.1 and F.sub.2 at the support location, wherein the first and second measurement positions define a difference F=F.sub.2F.sub.1 in the normal force; defining a difference map as a difference between the first and second interferograms; and using the difference in normal force F and the normal force F.sub.1 at the first measurement position to define a scaling factor S and applying the scaling factor S to the difference map to define a scaled difference map.
2. The method according to claim 1, further comprising: defining a compensated flatness by subtracting the scaled difference map from the first interferogram.
3. The method according to claim 1, wherein the photomask comprises an extreme ultraviolet (EUV) photomask.
4. The method according to claim 1, wherein the photomask is a patterned photomask.
5. The method according to claim 1, wherein the recording of the first and second interferograms is performed using a Fizeau interferometer.
6. The method according to claim 5, further comprising adjusting the Fizeau interferometer between first and second measurement angles .sub.1 and .sub.2 that define the first and second measurement positions.
7. The method according to claim 6, wherein the first and second measurement angles .sub.1 and .sub.2 are between 1 and 5.
8. The method according to claim 1, wherein the photomask is supported by an adjustable support apparatus that comprises three support members configured to provide three support locations for the photomask, the adjustable support apparatus configured to place the photomask in a stand-off configuration, the recording of the first and second interferograms performed in the stand-off configuration.
9. The method according to claim 1, further comprising: recording a first plurality of interferograms at the first measurement position and combining the first plurality of interferograms to form the first interferogram; and recording a second plurality of interferograms at the second measurement position and combining the second plurality of interferograms to form the second interferogram.
10. The method of claim 1, further comprising classifying the photomask based on the scaled difference map.
11. A method of interferometrically measuring flatness of a photomask, comprising: recording at first and second measurement angles .sub.1 and .sub.2 respective first and second interferograms IF.sub.1 and IF.sub.2 of a surface of the photomask supported by an adjustable support apparatus, wherein .sub.2>.sub.1 and wherein .sub.1 and .sub.2 are each within 11.46 of vertical; measuring at the first and second measurement angle .sub.1 and .sub.2 respective first and second normal forces F.sub.1 and F.sub.2 of the photomask on the adjustable support apparatus, wherein a force difference is defined as F=F.sub.2F.sub.1; defining a difference map DM=IF.sub.2IF.sub.1 as a difference between the second and first interferograms IF.sub.2 and IF.sub.1; defining either a first scaled difference map DM.sub.1=(F.sub.1/F).Math.DM or a second scaled difference map DM.sub.2=(F.sub.2/F).Math.DM; and defining a compensated flatness measurement CFM by either: i) subtracting the first difference map from the first interferogram (CFM=IF.sub.1DM.sub.1); or ii) subtracting the second difference map from the second interferogram (CFM=IF.sub.2DM.sub.2).
12. The method according to claim 11, further comprising supporting the photomask on a support apparatus comprising two base support members and a top support member, wherein the top support member is operably connected to a force sensor, and determining the first and second normal forces F.sub.1 and F.sub.2 using the force sensor.
13. The method according to claim 11, wherein the measurement angles .sub.1 and .sub.2 are between 1 and 5.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
(1) The accompanying drawings are included to provide a further understanding, and are incorporated in and constitute a part of this specification. The drawings illustrate one or more embodiment(s), and together with the Detailed Description explain the principles and operation of the various embodiments. As such, the disclosure will become more fully understood from the following Detailed Description, taken in conjunction with the accompanying Figures, in which:
(2)
(3)
(4)
(5)
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(7)
DETAILED DESCRIPTION
(8) Reference is now made in detail to various embodiments of the disclosure, examples of which are illustrated in the accompanying drawings. Whenever possible, the same or like reference numbers and symbols are used throughout the drawings to refer to the same or like parts. The drawings are not necessarily to scale, and one skilled in the art will recognize where the drawings have been simplified to illustrate the key aspects of the disclosure.
(9) The claims as set forth below are incorporated into and constitute part of this Detailed Description.
(10) Relative terms like top, bottom, side, horizontal, vertical, etc. are used for convenience and ease of explanation and are not intended to be limiting as to direction or orientation, unless otherwise specified.
(11) Cartesian coordinates are shown in some of the Figures for the sake of reference and are not intended to be limiting as to direction or orientation. The direction of gravity is taken to be in the vertical direction V, which corresponds to the y direction, and wherein the horizontal plane is the x-z plane.
(12) The term near vertical with reference to a measurement angle as introduced below means within 11.46 (0.2 radians) of vertical.
(13) The terms first measurement position and second measurement position or first measurement angle and second measurement angle as used herein are not intended to imply a specific temporal or spatial order to the measurement position or the measurement angle when carrying out the methods disclosed herein or adjusting the systems disclosed herein, so that for example setting the photomask to the first measurement angle (position) can be performed after having set the photomask to the second measurement angle (position). The terms first and second are used in this context to indicate that the measurement angles (positions) being considered are different, and is equivalent to saying one measurement angle (position) and another measurement angle (position).
(14) The Photomask
(15)
(16) The top surface 12 can be patterned with features 25, as shown in the close-up inset. In an example of an EUV photomask, the features 25 are absorbing at the EUV wavelength (e.g., 13.5 nm) while the top surface 12 of the photomask is reflective. In an example, an EUV photomask is made reflective by forming a multilayer reflective thin-film stack (not shown) on top surface 12, such as by forming forty to fifty alternating layers of molybdenum (Mo) and silicon (Si), atop a photomask substrate. Low thermal expansion materials (e.g. TiO.sub.2SiO.sub.2 glass) are preferred photomask substrate materials. In the description below, the photomask 10 is treated as a single substrate for ease of illustration and discussion. It is also noted that a photomask 10 that does have a reflective layer on top surface 12, but does not yet have features 25 on the reflective thin-film stack is referred to as a blank photomask, while a photomask having features 25 on a reflective thin-film stack is referred to as a patterned photomask. A photomask 10 which does not have a reflective layer and consists only of a substrate is referred to as a photomask substrate. The systems and methods disclosed herein can be used on a blank photomask or a photomask substrate, as well as a patterned photomask, as well as at any of the photomask-forming steps between a photomask substrate and a patterned photomask. Unless otherwise specified, the term photomask without further qualification refers to any of a photomask substrate, a blank photomask, or a patterned photomask.
(17) Flatness Measurement System
(18)
(19) The system 40 includes an interferometer 50, which in example is a Fizeau interferometer. An example mask flatness measurement system that employs a Fizeau interferometer is the UltraFlat 200 Mask System from Corning Tropel Corporation, Fairport, N.Y.
(20) The example interferometer 50 has a central axis (interferometer axis) A1 and a front end 52 with an aperture 54. The interferometer 50 is tiltable, as explained below. The example interferometer 50 also includes, in order along the interferometer axis A1, a laser light source 60 (e.g., a laser diode), a focusing lens assembly 64, a beam splitter 68 that forms a second axis A2, a collimating lens 70, and a reference element 72 having a reference surface 74. The interferometer 50 also includes along the second axis A2 a photodetector 80, such as CCD image sensor. An exemplary photodetector is a CCD camera having 4 Megapixels (MP). Not shown along the second axis A2 is an imaging lens disposed between the beam splitter 68 and the photodetector 80. Other configurations for the interferometer 50 can be effectively employed and the Fizeau configuration shown is by way of non-limiting example and for ease of illustration and discussion.
(21) The photodetector 80 of the interferometer 50 is operably connected to a controller 90. In an example, the controller 90 comprises a programmable computer configured with a non-transitory computer readable medium for storing instructions for causing the controller to carry out the flatness measurement methods disclosed herein.
(22) The system 40 also includes an adjustable support apparatus 100 configured to operably support the photomask 10. The support apparatus 100 includes a support base 110 having a top surface 112, a top end 116 and a bottom end 118. The surface 112 of the support apparatus 100 includes mask support members 126 and in a particular example includes two spaced apart bottom mask support members 126B and a top mask support member 126T (see
(23) The support apparatus 100 also includes a rotation device 150 operably attached at the bottom end 118 of the support base 110 and configured to rotate the base (and the photomask operably supported thereon) between a horizontal (loading) position (x-z plane) as shown in
(24) In an example, the system 40 includes an interferometer support structure 56 that includes an anti-vibration device 58 to reduce or eliminate the adverse effects of vibration on the flatness measurement.
(25) As shown in
(26)
(27) With reference to
(28) In some cases, it is advantageous to set the photomask 10 in a measurement position without engaging the force sensors 128. For example, force measurements need not be made at the same time flatness measurements are being made with the interferometer 50. Also, it may be convenient to calibrate the force sensors 128 when the support apparatus 100 is moved into the measurement position. Thus, in an embodiment shown in
(29)
(30) Flatness Measurement Method
(31) Both modeling and experimental data have confirmed that the gravity component of the photomask shape error is a linear function of the measurement angle over the range of measurement angles typically used when making flatness measurements (e.g., 0<10, and further in an example, between 1 and 5). Thus, the flatness measurement method disclosed herein generally includes making flatness measurements and force measurements at two different measurement positions as defined by two different measurement angles and then using the two flatness measurements and two force measurements to reduce if not eliminate the gravitational component of the flatness measurement, as well as flatness measurement errors due to the particular mounting configuration defined by the support members 126.
(32) The method of measuring the flatness of the photomask 10 includes loading the photomask 10 onto the support members 126 of the support apparatus 100, as shown in
(33) An interferometric measurement of the flatness of the front surface 12 of the photomask 10 is then made using the system 40 and the interferometer 50 therein. This includes activating the light source 60 to emit the light 62. The light 62 is expanded by the focusing lens assembly 64 and propagates to the collimating lens 70, which collimates the light. The collimated light 62 is then transmitted through the reference member 72 (including the reference surface 74) and through the aperture 54 to the front surface 12 of the photomask 10. The front surface 12 of the photomask 10 reflects the collimated light 62 back through the aperture 54 as reflected light 62R. The reflected light 62R passes through the reference member 72 (including the reference surface 74) and is redirected by the beam splitter 68 to be imaged onto the photodetector 80, which generates an electrical photodetector signal SPD representative of the detected light as a first digital image or first interferogram IF.sub.1. The electrical photodetector signal SPD is then sent to the controller 90, which can perform signal processing (e.g., filtering) and then stores the captured first interferogram IF.sub.1 associated with the first measurement angle .sub.1. In an example, the first interferogram IF.sub.1 can be formed by combining multiple interferometric measurements (e.g., more than 2, and more preferably between 12 and 60) made at different nominal phase offsets.
(34) When the photomask 10 is at the first measurement angle .sub.1, the top and bottom force sensors 128T and 128B measure respective first amounts of top and bottom force FT.sub.1 and FB.sub.1 of the photomask 10 pressing against the top and bottom mask support members 126T and 126B. For a photomask 10 that weighs about 300 grams, the top and bottom forces FT1 and FB1 can be about 6 grams and about 2 grams respectively for a measurement angle .sub.1=2.
(35) The detected first top and bottom forces FT.sub.1 and FB.sub.1 are respectively detected by the top and bottom force sensors 128T and 128B which in response generate respective first top and bottom force signals SFT.sub.1 and SFB.sub.1, which are sent to the controller 90 and are associated with the first measurement of the photomask 10 that generates the first interferogram IF.sub.1.
(36) Thus, a first measurement data set DS1 at the first measurement angle .sub.1 includes the first interferogram IF.sub.1, and the first amounts of force FT.sub.1 and FB.sub.1. This data set DS1 can be represented in shorthand notation as DS1={IF.sub.1, FT.sub.1, FB.sub.1} and is stored in the controller 90. Note that in our example support apparatus configuration that employs one top support member 126T and two bottom support members 126B, there will be one first top force signal SFT and two first bottom force signals SFB for each measurement angle .
(37) The force sensors 128 are designed to measure only that component of the gravitational force which is normal to the photomask surface, i.e., normal forces. If the mask support apparatus 100 is positioned to be at =0 with respect to the X-Y plane, the gravitational component that is normal to the photomask surface will reduce to a force which is nominally zero. For measurement angles that are small but not zero, the measured force will be linear with measurement angle. Since both the measured force, and the expected gravity-induced shape on the photomask surface are both linear with angle, it is not necessary to measure the measurement angle of the photomask support apparatus 100. However, at least an approximate measurement angle can be known by operation of the tiltable interferometer support structure 56 and/or by adjusting the anti-vibration device 58 and the different measurement angles referred to herein are a convenient way to distinguish between different flatness measurement conditions.
(38) Once the first flatness measurement is completed and the first data set DS1 established and stored in the controller 90, the anti-vibration device 58 or support structure 56 can be adjusted to set the photomask 10 at a second measurement position as defined by a second measurement angle =.sub.2 different from the first measurement angle .sub.1. In an example, the second measurement angle .sub.2=3.
(39) A second interferometric measurement of the flatness of the front surface 12 of the photomask 10 is then made using the system 40 as described above at the second measurement angle .sub.2 to obtain a second data set DS2={IF.sub.2, FT.sub.2, FB.sub.2}, where IF.sub.2 is a second interferogram and FT.sub.2 and FB.sub.2 are the second amounts of top and bottom force measured by the top and bottom force sensors 128T and 128B of the top and bottom support members 126T and 126B, respectively. If only one top force sensor (e.g. 128T) is used to measure the force, then the first and second data sets become DS1={IF.sub.1, F.sub.1} and DS2={IF.sub.2, F.sub.2}, where the T or the B has been dropped from the force symbol since there is only a single force sensor. As with the first interferogram IF.sub.1, in an example, the second interferogram IF.sub.2 can be formed by combining multiple interferometric measurements (e.g., more than 2, and more preferably between 12 and 60) made at different nominal phase offsets.
(40) Next, a difference map DM between the two interferograms is calculated, e.g., DM=IF.sub.2IF.sub.1. The difference map DM is an image that represents the gravitational sag, i.e., a measurement of the change in shape induced on the photomask 10 from the change in the amount of gravitational force on the mask due to the change =.sub.2.sub.1 in the measurement angle . The difference map will also include any shape-induced errors from the configuration of the support apparatus 100.
(41) Since the effect on the flatness measurement (i.e., photomask shape) due to gravity is linear with the measurement position (measurement angle ), the difference map DM can be scaled by a scaling factor S so that the scaled difference map (S.Math.DM) corresponds to (i.e., is matched to) the contribution of gravity to one of the first or second interferograms IF.sub.1 or IF.sub.2 taken at the first or second measurement angle .sub.1 or .sub.2, respectively. The scaled difference map S.Math.DM is denoted DM.sub. to indicate that is it scaled to a select measurement angle . The scaling factor S.sub.i=FT.sub.i/F for the i.sup.th measurement angle .sub.i, where F is the change in the measured force between the two measurement angles .sub.2 and .sub.1. The scaled difference map DM.sub. is said to have a matched measurement angle with the given interferogram to which the difference map has been scaled. For the single force sensor embodiment, F=F2F1. When using multiple force sensors 128, the force measurements from the sensors can be averaged to determine the forces F1 and F2.
(42) For example, when the difference map DM is for a measurement (incremental) angle change =1, then using a scaling factor S=FT.sub.1/F=2 provides a scaled difference map DM.sub.=S.Math.DM=2.Math.DM, which corresponds to the first measurement angle .sub.1=2 and the first interferogram IF.sub.1. Likewise, using a scaling factor S=FT.sub.2/F=3 provides a scaled difference map DM.sub.=S.Math.DM=3.Math.DM, which corresponds to the second measurement .sub.2=3 and the second interferogram IF.sub.2. The two different scaling factors S can also respectively be referred to as first and second scaling factors and respectively denoted S.sub.1 and S.sub.2, respectively for convenience.
(43) It is noted that the scaling factor S is inversely proportional to a difference .sub.2.sub.1 between the second measurement angle .sub.2 and the first measurement angle .sub.1. Thus, in an example, the scaling factor S can be defined in terms of the measurement angles, i.e., S=.sub.2/(.sub.2.sub.1) or S=.sub.1/(.sub.2.sub.1).
(44) Once the scaled difference map DM.sub. is established, it is subtracted from the corresponding interferogram IF.sub. (i.e., the interferogram having the measurement angle to which the difference map was scaled) to provide a compensated flatness measurement CFM, i.e.,
CFM=IF.sub.DM.sub.
wherein the compensated flatness measurement comprises a flatness map of the photomask 10 having minimal contributions due to gravity effects and the support apparatus 100. In one example CFM=IF.sub.12.Math.DM (measurement angle =.sub.1=2) while in another example CFM=IF.sub.23.Math.DM (measurement angle =.sub.2=3). In an example, two compensated flatness measurements CFM can be calculated, one for each measurement angle , and the results averaged. In another example, measurements at more than two measurement angles can be made and more than two compensated flatness measurements CFM can be calculated and two or more of the results averaged. The compensated flatness measurement CFM can be used to classify the photomask on the basis of the flatness of its surface. For example, an application may require a photomask that meets a certain surface flatness specification and the compensated flatness measurement CFM of the photomask can be used to determine whether the photomask meets the specification. Photomasks that meet the specification can be selected for the application and photomasks that fail to meet the specification can be rejected for the application. The compensated flatness measurement CFM includes use of the scaled difference map DM to classify the photomask.
(45) Advantages
(46) The flatness measurement systems and methods for photomasks 10 as described herein have at least the following advantages over conventional flatness measurement methods for photomask.
(47) A first advantage is increased measurement throughput since rotation of the photomask about its central axis AM to different rotation angles is not required. In an example, the measurement throughput is increased by a factor of between 2 and 3.
(48) A second advantage is that multiple photomask handling steps that put the photomask at risk of contamination and/or damage are eliminated. The movement of the photomask to different measurement angles does not require removing the photomask from the support apparatus.
(49) A third advantage is that the symmetric component of gravitational sag that results in residual measurement error can be reduced or eliminated.
(50) A fourth advantage is that the measurement methods account for variations between different photomasks, such as geometrical variations and different flatness shapes which may have an impact on the resulting error shape induced by gravity.
(51) Aspect 1 of the description is:
(52) A method of interferometrically measuring flatness of a photomask supported at a support location, comprising:
(53) recording at first and second measurement positions respective first and second interferograms of a surface of the photomask, and measuring respective first and second normal forces F.sub.1 and F.sub.2 at the support location, wherein the first and second measurement positions define a difference F=F.sub.2F.sub.1 in the normal force;
(54) defining a difference map as a difference between the first and second interferograms; and
(55) using the difference in normal force F and the normal force F.sub.1 at the first measurement position to define a scaling factor S and applying the scaling factor S to the difference map to define a scaled difference map.
(56) Aspect 2 of the description is:
(57) The method according to aspect 1, further comprising:
(58) defining a compensated flatness by subtracting the scaled difference map from the first interferogram.
(59) Aspect 3 of the description is:
(60) The method according to aspect 1 or 2, wherein the photomask comprises an extreme ultraviolet (EUV) photomask.
(61) Aspect 4 of the description is:
(62) The method according to any of aspects 1-3, wherein the photomask is a patterned photomask.
(63) Aspect 5 of the description is:
(64) The method according to any of aspects 1-4, wherein the recording of the first and second interferograms is performed using a Fizeau interferometer.
(65) Aspect 6 of the description is:
(66) The method according to aspect 5, further comprising adjusting the Fizeau interferometer between first and second measurement angles .sub.1 and .sub.2 that define the first and second measurement positions.
(67) Aspect 7 of the description is:
(68) The method according to aspect 6, wherein the first and second measurement angles .sub.1 and .sub.2 are between 1 and 5.
(69) Aspect 8 of the description is:
(70) The method according to any of aspects 1-7, wherein the photomask is supported by an adjustable support apparatus that comprises three support members configured to provide three support locations for the photomask.
(71) Aspect 9 of the description is:
(72) The method according to aspect 8, wherein the adjustable support apparatus is configured to place the photomask in a stand-off configuration.
(73) Aspect 10 of the description is:
(74) The method according to aspect 9, wherein the recording of the first and second interferograms is performed in the stand-off configuration.
(75) Aspect 11 of the description is:
(76) The method according to any of aspects 1-10, further comprising:
(77) recording a first plurality of interferograms at the first measurement position and combining the first plurality of interferograms to form the first interferogram; and
(78) recording a second plurality of interferograms at the second measurement position and combining the second plurality of interferograms to form the second interferogram.
(79) Aspect 12 of the description is:
(80) The method according to aspect 11, wherein the first plurality of interferograms comprises between 12 and 60 interferograms and the second plurality of interferograms comprises between 12 and 60 interferograms.
(81) Aspect 13 of the description is:
(82) The method of any of aspects 1-12, further comprising classifying the photomask based on the scaled difference map.
(83) Aspect 14 of the description is:
(84) A method of interferometrically measuring flatness of a photomask, comprising:
(85) recording at first and second measurement angles .sub.1 and .sub.2 respective first and second interferograms IF.sub.1 and IF.sub.2 of a surface of the photomask supported by an adjustable support apparatus, wherein .sub.2>.sub.1 and wherein .sub.1 and .sub.2 are each within 11.46 of vertical;
(86) measuring at the first and second measurement angle .sub.1 and .sub.2 respective first and second normal forces F.sub.1 and F.sub.2 of the photomask on the adjustable support apparatus, wherein a force difference F=F.sub.2F.sub.1;
(87) defining a difference map DM=IF.sub.2IF.sub.1 as a difference between the second and first interferograms IF.sub.2 and IF.sub.1;
(88) defining either a first scaled difference map DM.sub.1=(F.sub.1/F).Math.DM or a second scaled difference map DM.sub.Z=(F.sub.2/F).Math.DM; and
(89) defining a compensated flatness measurement CFM by either:
(90) subtracting the first difference map from the first interferogram (CFM=IF.sub.1DM.sub.1); or
(91) subtracting the second difference map from the second interferogram (CFM=IF.sub.2DM.sub.2).
(92) Aspect 15 of the description is:
(93) The method according to aspect 14, wherein the photomask comprises an extreme ultraviolet (EUV) photomask.
(94) Aspect 16 of the description is:
(95) The method according to aspect 14 or 15, wherein the photomask is a patterned photomask.
(96) Aspect 17 of the description is:
(97) The method according to any of aspects 14-16, wherein the recording of the first and second interferograms is performed using a Fizeau interferometer.
(98) Aspect 18 of the description is:
(99) The method according to aspect 17, wherein the Fizeau interferometer is adjustable to define the first and second measurement angles .sub.1 and .sub.2.
(100) Aspect 19 of the description is:
(101) The method according to any of aspects 14-18, further comprising supporting the photomask on a support apparatus comprising two base support members and a top support member, wherein the top support member is operably connected to a force sensor, and determining the first and second normal forces F.sub.1 and F.sub.2 using the force sensor.
(102) Aspect 20 of the description is:
(103) The method according to aspect 19, wherein the photomask has a back surface and wherein the adjustable support apparatus comprises three support members configured to provide three support locations for the photomask.
(104) Aspect 21 of the description is:
(105) The method according to any of aspects 14-20, wherein the adjustable support apparatus is configured to place the photomask in a stand-off configuration.
(106) Aspect 22 of the description is:
(107) The method according to aspect 21, wherein the recording of the first and second interferograms is performed is in the stand-off configuration.
(108) Aspect 23 of the description is:
(109) The method according to any of aspects 14-22, wherein the measurement angles .sub.1 and .sub.2 are between 1 and 5.
(110) Aspect 24 of the description is:
(111) The method according to any of aspects 14-23, wherein:
(112) the first interferogram IF.sub.1 is formed by combining multiple recorded first interferograms; and
(113) the second interferogram IF.sub.2 is formed by combining multiple recorded second interferograms.
(114) Aspect 25 of the description is:
(115) The method according to aspect 24, wherein the multiple recorded first interferograms comprise between 12 and 60 first interferograms and the multiple recorded second interferograms comprise between 12 and 60 second interferograms.
(116) Aspect 26 of the description is:
(117) The method of any of aspects 1-25, further comprising classifying the photomask based on the scaled difference map.
(118) Aspect 27 of the description is:
(119) A support apparatus for an interferometric measurement system for measuring flatness of a photomask having a back surface, a bottom end and a top end, comprising:
(120) a support base comprising at least three support members, the at least three support members comprising two bottom support members that support the bottom end of the photomask and a top support member that supports the photomask at or adjacent the top end of the photomask;
(121) a rotation device mechanically attached to the support base and configured to rotate the support base to a measurement position relative to the interferometric measurement system;
(122) a top force sensor in mechanical communication with the top support member; and
(123) wherein the at least three support members are arranged to mechanically support the photomask by contacting the photomask so that the top force sensor measures an amount of force on the top support member from the photomask due to gravity.
(124) Aspect 28 of the description is:
(125) The support apparatus according to aspect 27, wherein the top force sensor comprises either a flexural-based force sensor or a strain-based force sensor.
(126) Aspect 29 of the description is:
(127) The support apparatus according to aspect 27 or 28, further comprising two bottom force sensors respectively in mechanical communication the two base support members.
(128) Aspect 30 of the description is:
(129) The support apparatus according to any of aspects 27-29, wherein the support base has an end and wherein the rotation device resides at or near the end of the support base.
(130) Aspect 31 of the description is:
(131) An interferometric flatness measurement system for measuring flatness of a photomask, comprising:
(132) the support apparatus according to aspect 27; and
(133) an interferometer operably arranged adjacent the support apparatus and that is tiltable relative to the support apparatus.
(134) Aspect 32 of the description is:
(135) The interferometric measurement system according to aspect 31, wherein the interferometer comprises a Fizeau interferometer.
(136) Aspect 33 of the description is:
(137) The interferometric measurement system according to aspect 31 or 32, wherein the support apparatus is configured to move the photomask between a stand-off configuration and a force-measurement configuration.
(138) Aspect 34 of the description is:
(139) A method of measuring flatness of a photomask, comprising:
(140) positioning a photomask at a first measurement position, the first measurement position having a first measurement angle .sub.1 relative to a vertical direction;
(141) recording a first interferogram IF.sub.1 of a surface of the photomask at the first measurement position;
(142) repositioning the photomask to a second measurement position, the second measurement position having a second measurement angle .sub.2 relative to the vertical direction;
(143) recording a second interferogram IF.sub.2 of the surface of the photomask at the second measurement position;
(144) computing a difference map DM by subtracting the first interferogram IF.sub.1 from the second interferogram IF.sub.2; and
(145) computing a scaled difference map DM.sub. by multiplying the difference map DM by a scaling factor S, the scaling factor S being computed from a first measurement of the photomask made at the first measurement position and a second measurement of the photomask made at the second measurement position.
(146) Aspect 35 of the description is:
(147) The method of aspect 34, wherein the first measurement is a measurement of the first measurement angle .sub.1 and the second measurement is a measurement of the second measurement angle .sub.2.
(148) Aspect 36 of the description is:
(149) The method of aspect 34 or 35, wherein the scaling factor S is inversely proportional to a difference .sub.2.sub.1 between the second measurement angle .sub.2 and the first measurement angle .sub.1.
(150) Aspect 37 of the description is:
(151) The method of aspect 36, wherein the scaling factor S=.sub.1/(.sub.2.sub.1).
(152) Aspect 38 of the description is:
(153) The method of aspect 34, wherein the first measurement is a measurement of a normal force F.sub.1 at a first location of the photomask positioned at the first measurement position and the second measurement is a measurement of a normal force F.sub.2 at a second location of the photomask positioned at the second measurement position.
(154) Aspect 39 of the description is:
(155) The method of aspect 38, wherein the scaling factor S is inversely proportional to a difference F.sub.2F.sub.1 between the normal force F.sub.2 at the second measurement position and the normal force F.sub.1 at the first measurement position.
(156) Aspect 40 of the description is:
(157) The method of aspect 39, wherein the scaling factor S=F.sub.1/(F.sub.2F.sub.1).
(158) Aspect 41 of the description is:
(159) The method of any of aspects 38-40, wherein the first location is the same as the second location.
(160) Aspect 42 of the description is:
(161) The method of any of aspects 34-41, further comprising subtracting the scaled difference map DM.sub. from the first interferogram IF.sub.1.
(162) It will be apparent to those skilled in the art that various modifications to the preferred embodiments of the disclosure as described herein can be made without departing from the spirit or scope of the disclosure as defined in the appended claims. Thus, the disclosure covers the modifications and variations provided they come within the scope of the appended claims and the equivalents thereto.