Source: https://patents.google.com/patent/JP5890531B2/en
Timestamp: 2019-10-22 04:07:51
Document Index: 219167942

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JP5890531B2 - Small encoder head for interferometric encoder systems - Google Patents
Small encoder head for interferometric encoder systems Download PDF
JP5890531B2
JP5890531B2 JP2014541271A JP2014541271A JP5890531B2 JP 5890531 B2 JP5890531 B2 JP 5890531B2 JP 2014541271 A JP2014541271 A JP 2014541271A JP 2014541271 A JP2014541271 A JP 2014541271A JP 5890531 B2 JP5890531 B2 JP 5890531B2
JP2014541271A
JP2014535061A (en
リーゼナー、ヤン
2011-11-09 Priority to US201161557776P priority Critical
2011-11-09 Priority to US201161557755P priority
2011-11-09 Priority to US61/557,776 priority
2011-11-09 Priority to US61/557,755 priority
2012-11-08 Application filed by ザイゴ コーポレーションＺｙｇｏ Ｃｏｒｐｏｒａｔｉｏｎ, ザイゴ コーポレーションＺｙｇｏ Ｃｏｒｐｏｒａｔｉｏｎ filed Critical ザイゴ コーポレーションＺｙｇｏ Ｃｏｒｐｏｒａｔｉｏｎ
2012-11-08 Priority to PCT/US2012/064211 priority patent/WO2013070957A1/en
2014-12-25 Publication of JP2014535061A publication Critical patent/JP2014535061A/en
2016-03-22 Publication of JP5890531B2 publication Critical patent/JP5890531B2/en
In some cases, the interferometric measurement system monitors changes in the relative position of the object to be measured based on the optical interference signal. For example, the interferometer generates an optical interference signal by superimposing a measurement beam reflected from the object to be measured with a second beam, sometimes referred to as a “reference beam”, to generate an optical interference signal. The reference beam is obtained from a common light source. The change in the relative position of the object to be measured corresponds to the change in the phase of the measured optical interference signal.
An example of such an interferometric measurement system is an interferometric encoder system, which evaluates the movement of an object by tracking a measurement scale called an encoder scale. In general, an interferometric encoder system includes an encoder scale and an encoder head. The encoder head is an assembly that includes an interferometer. The interferometer directs the measurement beam to the encoder scale, and the light is diffracted by the encoder scale. The interferometer combines the diffracted measurement beam with a reference beam to form an output beam that includes a phase that is related to the position of the object. Encoder systems are widely used in lithography applications to monitor the movement of a movable stage within a lithography tool. The encoder system can be beneficial in such applications because it is relatively insensitive to atmospheric fluctuations.
The present application relates to a small encoder head. Various aspects of the invention are summarized as follows.
In general, in a first aspect, the subject matter of the present application can be embodied in an encoder head for use with an encoder scale, the encoder head combining each of a plurality of twice diffracted measurement beams with a corresponding reference beam. The encoder head includes a monolithic optical component having a plurality of facets, the plurality of facets i) receiving a plurality of one-time diffraction measurement beams from the surface of the encoder scale. Ii) configured to redirect a plurality of one-time diffractive measurement beams back to the surface of the encoder scale, the encoder scale being positioned in the path of the one-time diffractive measurement beam to generate a two-time diffractive measurement beam To do.
In another aspect, the subject matter of the present application can be embodied in an encoder system, the encoder system including an encoder scale and an encoder head, the encoder head corresponding to each of a plurality of twice diffracted measurement beams. And the encoder head includes a monolithic optic having a plurality of facets, the plurality of facets receiving a plurality of one-time diffraction measurement beams from the surface of the encoder scale. A plurality of one-time diffractive measurement beams are arranged to be redirected back to the surface of the encoder scale, the encoder scale being positioned in the path of the one-time diffractive measurement beam to produce a two-time diffractive measurement beam. The encoder system can further include a plurality of detector elements positioned to detect the output beam and an electronic processor, the electronic processor being an interference signal from each of the detector elements, wherein the diffraction measurement is performed twice. Configured to receive an interference signal that includes a phase related to an optical path difference between one of the beams and a corresponding reference beam, and to determine information about encoder scale freedom based on the phase related to each interference signal. The
System implementations can include one or more of the following features and / or features of other aspects. For example, the monolithic optical component can take the shape of a cube. In some implementations, the monolithic optical component takes the shape of a rectangular parallelepiped.
In some implementations, the monolithic optical component includes a first facet configured to receive a non-diffracting measurement beam and emit a two-time diffracting measurement beam. The first facet can substantially transmit radiation propagating in a direction perpendicular to the first facet, and radiation incident at an angle of inclination with respect to the first facet can be substantially reflected. The monolithic optic can include a second facet configured to receive a one-time diffracted or two-time diffracted measurement beam from an encoder scale. The second facet can substantially transmit radiation propagating in a direction perpendicular to the second facet. The second facet can be positioned opposite the first facet and opposite the first facet.
Alternatively, the second facet can be arranged perpendicular to the first facet. The second facet reflects radiation incident on the second facet at a first tilt angle range relative to the second facet, and the second facet at a second different tilt angle range relative to the second facet. It can be configured to transmit radiation incident on the facets.
In some implementations, the side facets of the monolithic optic substantially reflect radiation incident at an angle of inclination with respect to the side facets.
In some implementations, the encoder scale includes a 1D or 2D grid. The grating can be configured with grooves extending along the first direction. In some cases, the plane that includes the side facets of the monolithic optic can be oriented at an angle of inclination with respect to the first direction.
In some implementations, the monolithic optic can include a regular hexagonal prism or a regular pentagonal prism.
In certain implementations, the encoder head can be configured to direct a non-diffracting measurement beam along a first beam path to an encoder scale, where the first beam path of the non-diffracting measurement beam is monolithic optical On the outside of the part. The encoder scale can be positioned relative to the monolithic optic to diffract the incident beam along a second beam path, the second beam path of the diffracted incident beam being outside the monolithic optic.
In some implementations, the one-time diffraction measurement beam is a first one-diffractive measurement beam obtained from the positive diffraction order from the encoder scale and a second one obtained from the negative diffraction order from the encoder scale. Includes a diffraction diffraction measurement beam. The first and second one-time diffractometer beams can include positive and negative diffraction orders in the first plane. The one-time diffractive measurement beam comprises third and fourth one-time diffractive measurement beams, each including a positive diffraction order and a negative diffraction order from the encoder scale in a second plane perpendicular to the first plane. Further can be included.
In some implementations, the system receives an input beam from which (1) a corresponding reference beam for each two diffracted measurement beam and (2) an incident measurement beam are obtained. It further includes a plurality of configured optical elements. The plurality of optical elements can include a plurality of beam splitters and retroreflectors.
In some implementations, the monolithic optic receives an input beam and derives from this input beam (1) a corresponding reference beam for each two diffracted measurement beam and (2) an incident measurement beam. Configured as follows. Monolithic optics can include beam separation facets, which separate the input beam based on the polarization of the input beam and a specified angle of incidence with respect to the beam separation facet and at an incident angle other than the specified angle of incidence. It is configured to reflect light incident on the beam separation facet. The system can further include a reference grating positioned to receive the reference beam from the monolithic optic and redirect the diffracted reference beam into the monolithic optic.
In other aspects, the subject matter of the present application can be embodied in a system, the system including a movable stage and an encoder system, wherein either the encoder system or the device under test is attached to the movable stage. The encoder system can include an encoder scale and an encoder head, wherein the encoder head combines each twice diffracted measurement beam of the plurality of twice diffracted measurement beams with a corresponding reference beam to form a plurality of output beams. Configured as follows. In some implementations, the encoder head includes a monolithic optic having a plurality of facets, the plurality of facets receiving a plurality of one-time diffracted measurement beams from a surface of the encoder scale, and a plurality of one-time diffracted measurement beams. It is arranged to turn to return to the surface of the encoder scale. In some implementations, the encoder scale is positioned in the path of the one-time diffractive measurement beam to produce a two-time diffractive measurement beam. The encoder system may further include a plurality of detector elements positioned to detect the output beam and an electronic processor configured to receive an interference signal from each of the detector elements, each interference signal being 2 It includes a phase related to the optical path difference between one of the diffraction diffraction measurement beams and the corresponding reference beam. The electronic processor can be further configured to determine information regarding degrees of freedom of the encoder scale based on the phase for each interference signal.
In other aspects, the subject matter of the present application can be embodied in a lithography system, which includes an encoder system and a movable stage, to which either the encoder system or the device under test is attached; An illumination system coupled to the encoder system, a detector that detects the output beam from the encoder system during operation of the lithography system, and an electronic processor coupled to adjust the position of the stage based on information about the displacement of the encoder scale A positioning system configured to: The illumination system can include a radiation source that directs the radiation to the encoder system during operation of the lithography system. The encoder system can include an encoder scale and an encoder head configured to combine each of the plurality of twice diffracted measurement beams with a corresponding reference beam to generate a plurality of output beams. The encoder head may include a monolithic optical component having a plurality of facets, the plurality of facets receiving a plurality of one-time diffracted measurement beams from the surface of the encoder scale, and the plurality of one-time diffracted measurement beams on the surface of the encoder scale. It is arranged to change direction to return to The encoder scale can be positioned in the path of the one-time diffractive measurement beam to produce a two-time diffractive measurement beam. The encoder system can further include a plurality of detector elements positioned to detect the output beam and an electronic processor, the electronic processor being an interference signal from each of the detector elements, wherein the diffraction measurement is performed twice. An interference signal is received that includes a phase related to the optical path difference between one of the beams and a corresponding reference beam, and is configured to determine information related to encoder scale freedom based on the phase of each interference signal.
Advantages of various aspects of the presently disclosed subject matter include, for example, that an interferometric encoder system requires fewer optical elements and / or separate encoder heads for position measurement. Can do. Other advantages include, for example, a low cost and / or simple design for the interferometric encoder system and / or encoder head.
It is the schematic of the interference system encoder system as an example. It is the schematic of the cross section of the optical component as an example. 2B is a three-dimensional (3D) schematic diagram of the optical component shown in FIG. 2A. FIG. It is 3D schematic of the optical component as an example. FIG. 2 is a 3D schematic diagram of an exemplary monolithic optical component. FIG. 2 is a 3D schematic diagram of an exemplary monolithic optical component. It is the schematic of the cross section of the optical component as an example. 4B is a 3D schematic diagram of the optical component shown in FIG. 4A. FIG. FIG. 2 is a 3D schematic diagram of an example optical component. FIG. 2 is a 3D schematic diagram of an example optical component. FIG. 2 is a 3D schematic diagram of an example optical component. It is the schematic of the interference system encoder head as an example. It is the schematic of the interference system encoder head as an example. It is 3D schematic of the interference system encoder head as an example. It is the schematic of the interference system encoder head as an example. It is the schematic of the interference system encoder head as an example. FIG. 6 is a schematic diagram illustrating an example of the use of an optical element to separate a desired output beam from an undesirable output beam of an interferometric encoder head. 1 is a schematic diagram of an example lithography tool. FIG. It is a flowchart of the manufacturing sequence of a semiconductor device. It is a flowchart which shows the detail of a wafer process. FIG. 2 is a schematic diagram illustrating an example of an encoder head that uses transmissive and reflective grating patches. FIG. 2 is a schematic diagram illustrating an example of an encoder head that uses transmissive and reflective grating patches. FIG. 16D is a 3D schematic diagram of the encoder head shown in FIG. 16B.
Referring to FIG. 1, an interferometric encoder system 100 includes a light source module 120 (eg, including a laser), an optical assembly 110, a device under test 101, and a detector module 130 (eg, a polarizer and a photodetector). And an electronic processor 150. In general, the light source module 120 includes a light source and also includes beam shaping optics (eg, light collimating optics), light guiding components (eg, fiber optic waveguides), and / or polarization control optics (eg, polarizers and Other components such as (or wave plates) can also be included. Various embodiments of the optical assembly 110 are described below. In some implementations, the optical assembly may also be referred to as an “encoder head”. A Cartesian coordinate system is shown for reference, and the Y direction (not shown) extends into the page.
The device under test 101 is positioned at a nominal distance from the optical assembly 110 along the Z axis. In many applications, for example, when an encoder system is used to monitor the position of a wafer stage or reticle stage within a lithography tool, the device under test 101 moves in the x and / or y direction relative to the optical assembly 110. While the z-axis is nominally maintained at a constant distance from the optical assembly. This constant distance can be relatively small (eg, a few centimeters or less). However, in such applications, the position of the object to be measured generally changes by a small amount from a nominally constant distance, and the relative orientation of the object to be measured in the Cartesian coordinate system may change by a small amount. In operation, the encoder system 100 includes one or more of these degrees of freedom of the device under test 101 with respect to the optical assembly 110, including the position of the device under test 101 with respect to the x axis, and even the y axis and / or z. Monitor the position of the device under test 101 with respect to the axis and / or with respect to the pitch and yaw angular orientation.
In order to monitor the position of the device under test 101, the light source module 120 directs the input beam 122 to the optical assembly 110. The optical assembly 110 obtains a measurement beam 112 from the input beam 122 and directs the measurement beam 112 toward the device under test 101. The optical assembly 110 also obtains a reference beam (not shown) from the input beam 122 and directs the reference beam along a different path than the measurement beam. For example, the optical assembly 110 can include a beam splitter that separates the input beam 122 into a measurement beam 112 and a reference beam. The measurement and reference beams can have orthogonal polarization (eg, orthogonal linear polarization).
The device under test 101 includes an encoder scale 105. The encoder scale 105 is, for example, a measurement scale that diffracts a measurement beam from an encoder head to one or more diffraction orders. In general, the encoder scale can include a wide variety of diffractive structures, such as gratings or holographic diffractive structures. Examples of grids include sine grids, rectangular grids, or sawtooth grids. Gratings can be characterized not only by periodic structures with a constant pitch, but also by more complex periodic structures (eg, chirped gratings). In general, the encoder scale can diffract the measurement beam into a plurality of planes. For example, the encoder scale can be a two-dimensional grating that diffracts the measurement beam into diffraction orders in the xz and yz planes. The encoder scale extends over a distance corresponding to the moving range of the DUT 101 in the xy plane.
In this embodiment, the encoder scale 105 is a grid whose grid lines extend perpendicular to the plane of the page and extend parallel to the y-axis of the Cartesian coordinate system as shown in FIG. The grid lines are periodic along the x axis. The grating plane of the encoder scale 105 corresponds to the xy plane, and the encoder scale diffracts the measurement beam 112 to one or more diffraction orders in the yz plane.
At least one of these diffraction orders (eg, +1 or −1st order diffraction) of the measurement beam (shown as beam 114) is returned to optical assembly 110, where the diffractive measurement beam is used as a reference beam using the optical element. And an output beam 132 is formed. Alternatively, using the optical elements in assembly 110, the diffracted measurement beam is redirected back to the encoder scale and a second diffraction is performed before being combined with the reference beam.
The output beam 132 includes phase information regarding the optical path length difference between the measurement beam and the reference beam. Optical assembly 110 directs output beam 132 to detector module 130, which detects the output beam and transmits a signal to electronic processor 150 in response to the detected output beam. The electronic processor 150 receives and analyzes the signal to determine information regarding one or more degrees of freedom of the device under test 101 with respect to the optical assembly 110. An example of an exemplary technique for determining information about one or more degrees of freedom based on a detected output beam can be found in US Pat. No. 8,300,233, which is incorporated by reference in its entirety. This is incorporated into the present application.
In certain embodiments, there is a small frequency difference (eg, a difference in the kHz to MHz range) in the measurement and reference beams, and an interference signal of interest of a frequency that generally corresponds to this frequency difference is generated. . This frequency is hereinafter referred to interchangeably with the “heterodyne” frequency. Information regarding changes in the relative position of the device under test generally corresponds to the phase of the interference signal at this heterodyne frequency. This phase can be extracted using signal processing techniques. In general, the phase term changes with time depending on the movable object to be measured. In this respect, the frequency of the interference signal is shifted from the heterodyne frequency by a certain amount due to the first time derivative of the motion of the device under test, which is referred to herein as a “Doppler shift”.
Different frequencies of the measurement and reference beam are generated, for example, by Zeeman separation of the laser, by acousto-optic modulation, using two different laser modes, using a birefringent element, inside the laser and by other techniques it can. With orthogonal polarization, the polarizing beam splitter can direct the measurement and reference beams along different paths and combine them to form the output beam, which then passes through the polarizer and mixes with the orthogonal polarization component , These can interfere. Without target movement, the interference signal oscillates at the heterodyne frequency, which is exactly the difference between the optical frequencies of the two components. If there is target movement, this heterodyne frequency will cause a change in target velocity through the well-known Doppler relationship. Thus, by monitoring the change in heterodyne frequency, the movement of the target relative to the optical assembly can be monitored.
In the embodiments described below, an “input beam” generally refers to a beam emitted from a light source module. In the case of heterodyne detection, the input beam includes components having slightly different frequencies as described above.
In certain embodiments, the interferometer system is designed not to operate with Littrow. For example, in general, the measurement beam is incident on the device under test 101 at an incident angle, and the once-diffracted measurement beam does not satisfy the Littrow condition. The Littrow condition refers to the orientation of an incident beam of a diffractive structure such as a grating such that the diffractive structure returns the diffracted beam back to the light source. In other words, in the encoder system 100, the one-time diffracted measurement beam does not satisfy the Littrow condition because the one-time diffracted measurement beam is not collinear with the measurement beam before it is diffracted on the encoder scale.
Although the encoder scale 105 is depicted as a periodic structure in one direction in FIG. 1, more generally the device under test can include a variety of different diffractive structures that suitably diffract the measurement beam. In some embodiments, the device under test can include a diffractive structure (e.g., an encoder scale) that is periodic in two directions (e.g., along the x and y axes) and directs the measurement beam into two orthogonal planes. Diffraction into the inner beam. In general, an encoder scale diffractive structure and a light source module produce one or more detectable interference signals when the encoder system is combined with the corresponding reference beam within the geometrical constraints of the system. Selected to provide one or more diffractive measurement beams of sufficient intensity to establish. In some embodiments, the light source module provides an input beam having a wavelength in the range of 400 nm to 1,600 nm. For example, the input beam can have a wavelength of about 633 nm or about 980 nm. It should be noted that in general, the frequency division of the heterodyne light source results in only a very small difference between the wavelengths of the two components of the input beam, so that even if the input beam is not strictly monochromatic, it still remains the input beam. Is realistic with one wavelength. In some embodiments, the light source module includes a heat source such as a gas laser (eg, HeNe laser), a laser diode or other solid state laser source, a light emitting diode, or a halogen lamp with or without a spectral bandwidth modulation filter. be able to.
In general, the diffractive structure (eg, grating pitch) can vary depending on the wavelength of the input beam and the diffraction order used for placement and measurement of the optical assembly. In some embodiments, the diffractive structure is a grating having a pitch in the range of about 1λ to about 20λ, where λ is the wavelength of the light source. The pitch of the grating can be about 0.5 μm to about 10 μm. Another embodiment of an interferometric optical encoder system and operation is described in US Pat. No. 8,300,233, which is hereby incorporated by reference in its entirety.
As described above, the device under test diffracts the incident measurement beam into a beam in one or more planes (eg, two orthogonal planes). These diffracted beams can include, for example, a beam from a positive diffraction order and a beam from a negative diffraction order. In some implementations, a diffracted beam is combined with a corresponding reference beam to generate a plurality of output beams, feed the beam to an encoder scale, receive an once-diffracted beam from the encoder scale, A plurality of components are used to redirect the one-time diffracted beam toward the encoder scale so that a second diffraction is performed and to receive a twice-diffracted beam. Such a system can be complex to place and expensive to construct and manufacture, depending on the number of parts required to receive and redirect each of the diffracted beams.
To substantially retroreflect multiple components used to receive and redirect the diffracted measurement beam in order to reduce the cost of the system, simplify system design, and streamline the use of light energy. A monolithic optical component having a combination of two or more optical surfaces can be substituted. In some implementations, a one-time diffracted beam enters the monolithic optic and is redirected back to the diffraction grating by the surface and / or facet of the monolithic optic, where two or more two-time diffracted beams are Generated. In some implementations, the surface and / or facet of the monolithic optic acquires a measurement beam from the input beam and redirects the measurement beam toward the encoder scale to produce a one-time diffracted measurement beam. Configured to get. The two diffracted beams can be interfered with each other or by a corresponding reference beam to produce an output beam, which is recorded by the detector. Thereafter, using the interference signal obtained from the detector, the position information regarding the grating position can be determined based on the phase information from the interference signal. In order to measure the change in position of the encoder scale in N dimensions, at least N measurement beams are required. Compared to configurations where multiple separate input beams are required and one diffraction order for each input beam is detected from multiple separate input beams, the system disclosed herein has one input The beam can be used to obtain different diffraction orders and therefore the light source can be used efficiently. Thus, in some implementations, the power required to perform the measurement can be saved. Alternatively, in some implementations, position measurements can be made with lower noise.
Similarly, in some implementations, the surface and / or facet of the monolithic optic is configured to receive and redirect the one-time and / or two-time diffracted reference beams from the reference grating. In some cases, the surface and / or facet of the monolithic optic is configured to acquire a reference beam prior to diffraction from the input beam.
For the purposes of this disclosure, monolithic optical component is understood to mean an optical device that includes one or more optical elements that constitute a single continuous component. In some implementations, a single part can be formed without joints or seams. In some implementations, a single component can include a facet that extends through at least a portion of the component, the facet being a single continuous component that fuses or bonds two separate optical elements together. (For example, using an optical adhesive). For example, a single component can include a polarizing beam splitter, with facets extending from the beam splitter body into two separate beams that propagate an incident beam of orthogonal polarization in different directions based on different polarizations of the input beam. And separate.
A single monolithic optic can be used to receive and redirect diffractometry and / or reference beams, but the monolithic optic can be combined with one or more beam steering, beam separation and / or beam synthesis components Implementations are also possible that are arranged and provide a compact optical device for measuring the relative position change of the encoder scale in N dimensions.
Available in a minimalistic optical design for an optical encoder head are multiple retroreflective elements, which can be any single cubic, cuboid (rectangular surface) Hexagons), right angle prisms (eg, prisms having 45, 45, 90, or 30, 60, 90) included angles, or a plurality of retroreflecting optical surfaces With any other monolithic part having a combination. Embodiments disclosed herein can be used to capture and evaluate two or four diffraction orders of a 1D or 2D grating, respectively, and therefore capture less than two or four diffraction orders Compared with the configuration, the efficiency can be improved. In addition, each of the embodiments described herein can be used with both homodyne and heterodyne light sources.
In an exemplary embodiment, four diffractive measurement beams can be controlled using a single monolithic glass cube and encoder scale (eg, a 2D diffraction grating). When the input measurement beam is supplied to a glass cube, the input measurement beam passes through the cube and strikes the encoder scale at a non-littrow angle, and at least four first order diffraction orders (eg, + 1st order and -1st order in the first plane and + 1st order and -1st order in the second orthogonal plane). The four diffracted beams reenter the cube and are retroreflected near the four corners of the cube, returning to the encoder scale, where the beam is again diffracted at a non-Littrow angle and out of the diffracted beams Are spatially separated and propagate in the opposite direction to the initial input beam. The twice diffracted beam passes through the cube and is ready to interfere with one or more reference beams. The above arrangement provides four phase measurement results, so the position of the encoder head or encoder scale can be calculated with some redundancy in all three dimensions.
FIG. 2A is a schematic cross-sectional view of an exemplary monolithic optical component 200 for use in an encoder head of an interferometric encoder system, similar to the exemplary embodiment described above. Optical component 200 is configured to receive a plurality of one-time diffracted beams from encoder scale 105 and to redirect these one-time diffracted beams back to the encoder scale. Other parts of the interferometric encoder system are omitted from the figure for clarity. The optical component 200 includes a monolithic cube having an upper facet 202, a lower facet 204, and four side facets 206. The encoder scale 105 includes a 2D grid.
During operation of the interferometric encoder system, the measurement beam 201 acquired from the light source is incident on the top facet 202 of the optical component 200, where the measurement beam 201 is perpendicular to the facet 202 surface. The measurement beam 201 passes through the upper facet 202 and the lower facet 204 and reaches the encoder scale 105 at a non-Littrow angle. Due to the diffraction characteristics of the encoder scale 105, the measurement beam 201 is diffracted into a plurality of diffraction orders. The diffracted beam is, for example, one or more first beams obtained from the positive diffraction order of the encoder scale and one or more second beams obtained from the negative diffraction order from the encoder scale 105. Correspond. For example, the encoder scale 105 has two beams propagating the measurement beam 201 in the XY plane (for example, + 1st order diffraction and −1st order diffraction) and two beams (for example, +1) propagating in the YZ plane. Diffracted into second order diffraction and first order diffraction).
The one-time diffracted beam 203 returns to the optical component 200, and the beam enters the optical component 200 again from the lower facet 204. The one-time diffracted beam 203 is then reflected by the side facet 206 and the top facet 202 of the optical component 200 and returned to the bottom facet 204. The one-time diffracted beam 203 passes through the lower facet 204 toward the encoder scale 105, and the encoder beam 105 diffracts the second time under non-retrow conditions. The twice diffracted beam 205 then returns toward the optical component 200 in a direction substantially opposite to the direction of the incident beam 201. After passing through the optical component 200, each of the two-time diffracted beams 205 is combined with a corresponding reference beam (omitted for clarity) to form a corresponding output beam, which is then detected by the detection module ( For example, a polarizer and a photodetector). An electronic processor coupled to the detector analyzes the interference signal from each detector to extract phase information regarding the relative position of the encoder scale and / or encoder head.
In the example shown in FIG. 2A, the top facet 202 transmits radiation incident normal to the surface of the facet 202, while radiation incident on the facet 202 surface at an angle of inclination with respect to the facet surface. Is configured to reflect. This property of the top facet 202 can be established using a multilayer coating on the facet (eg, multiple alternating layers of different thin film materials). By manipulating the thickness and composition of each layer in the multilayer stack, the reflection characteristics can be tailored to a specific angle of incidence. That is, the coating has anti-reflective properties for radiation that is normal incidence radiation and has high reflectivity for radiation incident at one or more tilt angles with respect to the facet 202 surface. Can be optimized. For example, if all tilted beams impinging on the top facet 202 have the same angle of incidence with respect to the facet surface, the layer thickness of the multilayer coating at a certain angle of incidence and wavelength can be expressed as a reflective quarter for that tilted beam. It can be configured to exhibit behavior similar to that of a single wavelength stack and to exhibit behavior similar to that of a transmissive half-wave stack for normally incident light. The angle dependence of surface reflection is due to the change in the optical path length difference between reflections from various interlayer interfaces.
For coatings configured to maximize transmission of the normal incident beam, the incident beam angle tolerance of this coating can be up to about +/− 10 ° from normal. For coatings configured to maximize the reflectivity of tilted beams (ie, beams that are non-perpendicular and non-parallel to the incident surface), the incident beam angle tolerance of this coating is approximately + / -2 ° to about +/− 5 °. In the case of a coating that substantially transmits the incident beam at a particular angle, the coating is at least 75% of the incident beam (eg, at least 80%, at least 85%, at least 90%, at least 95%, at least 98%, or At least 99%). In the case of a coating that substantially reflects an incident beam at a certain angle, the coating is at least 75% (eg, at least 80%, at least 85%, at least 90%, at least 95%, At least 98%, or at least 99%). Materials for such coatings can include, for example, zinc sulfide, titanium dioxide, magnesium fluoride, and / or silicon dioxide. An example of a multilayer coating that reflects only about 1.2% of the vertical beam and 95.2% of the tilted beam at 27.82 ° in BK7 glass is a stack of ABCBCBCBA, where A is a 57 nm magnesium fluoride layer , B is a 942 nm zinc sulfide layer, and C is a 1149 nm magnesium fluoride layer. Other guidelines regarding such multilayer film design methods are described in, for example, E.I. E. Hecht, “Optics”, 4th edition, Addison Wesley, 2003, the entire contents of which are incorporated herein by reference. Multi-layer coatings can also be used among other embodiments, including the following examples.
Unlike top facet 202, bottom facet 204 is configured to transmit incident radiation that is perpendicular or oblique to the surface of the bottom facet. In some implementations, to facilitate transmission from the bottom facet 204, the facet 204 is configured to include a multilayer coating for a wide angle of incidence. Alternatively, the bottom facet 204 can be configured to include a multilayer coating that is optimized for a particular angle of incidence (eg, normal incidence and incidence at one tilt angle) and a particular wavelength or wavelength range. The side facets 206 are naturally reflective due to total internal reflection (ie, the area outside the part 200 has a lower refractive index than the area inside the part 200). However, the side facets 206 can also be configured to include a highly reflective coating.
2B and 2C are three-dimensional (3D) schematic diagrams of the optical component 200 shown in FIG. 2A. As shown in FIGS. 2B and 2C, the optical component 200 is oriented such that the bottom edge of the side facet 206 does not align with the edge of the encoder scale 105. In this example, the encoder scale 105 includes a grating composed of a set of grooves extending along a direction parallel to at least two edges of the portion of the encoder scale 105 shown in the figure. If the optical component 200 is rotated so that the lower edge of the side facet 206 is inclined with respect to the edge of the encoder scale, and therefore inclined with respect to the direction in which the groove extends, the diffracted beam is ensured once. Roughly, it can propagate toward the corner of the optical component 200, and retroreflection occurs due to the corner of the optical component 200. FIG. 2B shows a more general case of the angle at which the optical component 200 can be rotated relative to the encoder grid lines, but in FIG. 2C the angle is just 45 °. That is, the one-time diffracted beam 203 propagates toward the edge formed by the intersection of the side facets 206 after passing through the lower facet 204. As a result, it is possible to maintain a certain degree of symmetry between the polarization characteristics and the beam path between the various beams.
In some embodiments, the optical component prevents the one-time diffracted beam from colliding on the edge formed by the intersection of the side facets, while at least some one-time diffracted beams are It can comprise so that it may inject into such an edge. FIG. 3A is a 3D schematic diagram of an exemplary monolithic optic 300 that prevents the diffracted beam from impinging on the edge formed by the intersection of the side facets 306. In order to realize this effect, the optical component 300 is configured to be a rectangular parallelepiped oriented at 45 ° with respect to the grating direction of the encoder scale 105 (that is, the direction in which the elongated portion of the grating extends). Yes. FIG. 3B is a 3D schematic diagram of a cube rotated 30 ° relative to the grating direction to prevent a single diffracted beam from hitting the facet edge.
For clarity, the other components of the interferometric system and the reference beam are omitted in FIG. Similar to optical component 200 of FIG. 2, optical component 300 can be formed of glass and include multilayer coatings on different facets to increase transmission of incident radiation at a specified angle and / or at another specified angle. The reflection of incident radiation can be increased. In some implementations, component 300 or component 200 can alternatively be configured to increase the spatial separation between beams incident on the facet surface. Each separated beam can then be directed toward a different region of optical component 300 or 200 (eg, toward the facet or side of optical component 300 or 200). Physical separation allows the facets or surfaces on which each separated beam is incident to include a corresponding local reflective or transmissive coating for that beam. By widening the spatial separation between the beams, the spacing between the local anti-reflective / transparent coatings formed on the optical component can be further increased, and thus the complexity of manufacturing different coatings close to each other Is reduced. Various parameters can be adjusted to obtain the spacing between the beams to allow the formation of a local coating, such as the aspect ratio of the optical component, between the encoder scale 105 and the optical component 300 or 200. , The pitch between the grooves of the grating of the encoder scale 105, and / or the rotation of the encoder scale 105 in the grating direction relative to the optical component.
In some embodiments, it is advantageous to provide and detect the measurement beam along a direction parallel to the plane containing the encoder scale 105. 4A receives a measurement beam 401 propagating along a direction parallel to a plane containing the encoder scale 105, redirects the measurement beam 401 toward the encoder scale, and follows a direction parallel to the plane containing the encoder scale 105. 2 is a schematic cross-sectional view of an optical component 400 according to an example for outputting a plurality of two-time diffraction measurement beams 405. FIG. The shape of the optical component 400 corresponds to a monolithic triangular prism. For clarity, the other optical elements of the interferometric system are omitted in FIG. 4A and only one two-time diffracted beam is shown. However, the optical component 400 can redirect a plurality of two-time diffracted beams, the two-time diffracted beams being one or more first beams derived from the positive diffraction order from the encoder scale 105; One or more second beams obtained from negative diffraction orders from encoder scale 105 are included. As shown in FIG. 4, the measurement beam incident on the encoder scale 105 does not satisfy the Littrow condition.
The optical component 400 can be formed of any suitable material that is substantially transparent to the wavelength of the measurement beam (eg, glass for light in the visible wavelength range) and receives the incident measurement beam 401 and 2 A first facet 402 is included for transmitting the diffraction diffraction measurement beam 405. The first facet 402 can also include a thin film multilayer coating (not shown) configured to reflect radiation incident at an oblique angle relative to the facet surface. The second facet 404 can include a thin film multilayer coating configured to allow transmission or reflection of incident radiation depending on the angle of incidence. For example, as shown in FIG. 4A, the second facet 404 is a thin film multilayer coating (not shown) that maximizes the transmission of radiation that is incident on the surface of the second facet 404 perpendicularly and at a first tilt angle. May be included. However, the second facet 404 reflects radiation incident on the facet surface at a second tilt angle different from the first, which is possible either by a multilayer coating or a total internal reflection phenomenon. The third facet 406 includes a thin film coating (not shown) configured to substantially reflect radiation at any angle to its surface. For example, the thin film coating of the third facet 406 can include a thin film layer of silver or gold.
FIG. 4B is a 3D schematic diagram of the optical component 400. In some implementations, the component 400 is rotated relative to the grid direction of the encoder scale 105. For example, the lower edge of the part 400 formed by the intersection of the side facet 406 and the facet 404 is non-parallel to the grating groove direction (eg, non-parallel to the direction in which the elongated portion of the groove extends). Can be rotated. By rotating the optical component 400 non-parallel to the groove, in some implementations it can be ensured that the diffracted beam propagates once roughly toward the corner of the optical component 400.
In some embodiments, the monolithic optic can be configured to work with an encoder scale having a one-dimensional (1D) pattern, eg, a 1D grating. FIG. 5 is a 3D schematic diagram of an optical component 500 used in an encoder head of an interferometric encoder system, which receives a plurality of one-time diffracted beams from an encoder scale 105 having a 1D grating. Arranged to redirect the diffracted beam back to the encoder scale 105. In the implementation shown in FIG. 5, the one-time diffracted beam 503 received by the component 500 includes beams obtained from both positive and negative diffraction orders along the same plane. The optical component 500 is a monolithic regular hexagonal prism and can be formed of a material that is substantially transparent to the wavelength of the measurement beam (eg, glass for a measurement beam in the visible wavelength range). Basically, the prism shape shown in FIG. 5 depends on the plane of the cuboid prism that is passed by and / or reflects the measurement beam (including the incident measurement beam and the one and two diffraction measurement beams). The portion of the cuboid that is defined and not passed by the measurement beam or does not reflect the measurement beam has been removed.
In the example shown in FIGS. 2-5, the incident measurement beam and the twice diffracted beam travel through the monolithic optic. However, in some embodiments, these beams may propagate to and from the encoder scale 105 without propagating through the optical components. FIG. 6 is a 3D schematic diagram of an optical component 600 in which neither the incident measurement beam 601 nor the twice-diffracted measurement beam propagates through the component 600. For clarity, other parts of the interferometric encoder system and the reference beam have been omitted.
As shown in FIG. 6, the incident measurement beam 601 propagates toward the encoder scale 105 outside the part 600. The one-time diffracted beam obtained from the diffraction of each measurement beam at the encoder scale 105 then propagates into the part 600, where the one-time diffracted beam is reflected at the facets of the part 600 by the encoder scale 105. The direction is changed so as to return to (2), and the second diffraction is performed without satisfying the Littrow condition. The twice diffracted beam 605 then propagates in the opposite direction substantially parallel to the incident measurement beam 601 without passing through the optical component 600. The advantage of a configuration in which the incident and diffracted beam does not pass through the monolithic optical component, such as the component 600 shown in FIG. It is a point which can be comprised so that it may have a high reflectance. Since it is not necessary to pass the beam through these surfaces, these surfaces can be formed with a highly reflective coating, thus improving the efficiency of reflecting light. Increasing the amount of reflected light may improve the signal that is ultimately detected by the photodetector module.
In some embodiments, the monolithic optic with transmissive / reflective facets deviates from the shape of a cuboid or right-angle prism. An optical component 700 described later is an example of such a component. In some cases, such other shapes can also be used to extract phase difference information. That is, the optical component can be configured to cause multiple measurement beams to interfere with each other, thus eliminating the need to obtain another reference beam from the light source. The encoder position information is then based on the phase of the interference beam, which is related to the optical path difference (OPD) between the measurement beams.
FIG. 7 is a 3D schematic diagram of an exemplary monolithic optic 700 that combines multiple measurement beams and interferes to generate an output beam, phase information from the output beam, and hence The position information related to the encoder scale can be extracted. For clarity, the other components of the interferometric system are omitted in FIG. In this example, the optical component 700 has a shape corresponding to a regular pentagonal prism and can be formed of glass.
In operation, incident measurement beam 701 propagating along a direction perpendicular to the surface of upper facet 702 travels through upper facet 702 and lower facet 704 of component 700. The incident beam 701 is diffracted by the encoder scale (including diffraction grating lines) at the first position 720 without satisfying the Littrow condition to generate a plurality of diffracted beams corresponding to different diffraction orders of the incident measurement beam 701. For example, the encoder scale diffracts the measurement beam 701 into two beams propagating in the first plane and two beams propagating in the second orthogonal plane. For clarity, only two of the diffracted beams generated at the first location 720 are shown, and each one-time diffracted beam propagates in a different plane. The single diffracted beam is redirected by the facets of the optical component 700, and both redirected single diffracted beams are incident on a second position 730 of the encoder scale, the second position 730 being a first position. Is different. At the second position 730, the one-time diffracted measurement beam does not satisfy the Littrow condition and is diffracted again, so that the two-time diffracted beam 705 propagates along the opposite direction parallel to the direction of the incident measurement beam 701. The double diffracted beam 705 is also collinear to interfere when the double diffracted beam 705 reaches the detector module (not shown) of the interferometric system. Upon receiving the interfering two-time diffracted beam 705, the detector module can generate an electronic interference signal. An electronic processor connected to the detector module can analyze the interference signal to extract phase information and determine the position of the encoder scale relative to the encoder head (ie, monolithic optical component) from the phase information.
Various embodiments of an interferometric encoder system utilizing monolithic optical components are possible. For example, in some embodiments, an interferometric encoder system includes a beam separating component (eg, polarized and unpolarized beam splitter) and a beam steering component (eg, mirror, lens, prism, retroreflective). Body) and / or polarization control components in addition to monolithic optical components. The additional beam separation element and / or beam steering element provides a fixed number of reference beams at specified positions, which are combined with the diffractive measurement beam obtained using monolithic optics. For example, in some embodiments, a beam combining component can be used to combine one or more double diffracted measurement beams with one or more reference beams, respectively, which are combined with the detector module. Interfere with. In some embodiments, the beam separation component and / or the beam steering component are arranged such that the measurement and reference beams remain parallel to each other even if there is a poor angular alignment of the initial source input beam. it can. In some embodiments, one or more other diffraction gratings on the encoder scale can be used to diffract the reference beam back to the monolithic optic. The use of additional gratings can provide a compact interferometric encoder system configuration in some implementations, which is generally very space efficient for generating multiple beams from one beam. It is because it is a high means (for example, refer FIG. 9).
The beam-splitting combining component disclosed herein can also include a beam separation element such as, for example, a polarized or non-polarized beam separation prism. Other beam separation elements can also be used, such as half mirrors or dichroic mirror prisms. The beam steering components disclosed herein include retroreflectors, such as corner cube reflectors, and / or prisms, such as right triangular prisms. Examples of polarization state changing elements disclosed herein include, but are not limited to, linear polarizers, quarter wave plates, and half wave plates.
FIG. 8 illustrates an embodiment of an interferometric encoder system that includes a beam steering component and a beam combining component in addition to a monolithic optic component to obtain a twice diffracted measurement beam. In particular, FIG. 8 is a schematic cross-sectional view of an interferometric encoder head 810 that includes a monolithic optical component 800 for receiving a plurality of diffracted beams from an encoder scale, a first beam splitter / It includes a combiner component 812, a second beam separation component 814, a third beam separation component 816, and a retroreflector 818. In some implementations, the encoder head also includes a polarization control component 820 (eg, a quarter wave-plate (QWP), half-wave plate, or polarization rotator).
In certain embodiments, the polarization state of the beam is typically diffracted twice by the grating, passed multiple times through the air glass interface, and uncoated with monolithic optics or other optical elements in the interferometer system. It may be generally elliptical after multiple internal reflections from the surface and the coated surface. In some cases, changing the polarization state in this way may ultimately result in less light reaching the detector module, reducing the overall efficiency of the interferometer system, and / or position detection. The accuracy can be reduced. Polarization elements such as polarization control component 820 can be added to the encoder head device and positioned to compensate for changes in polarization state. The compensator can be placed between the monolithic optic (eg, cuboid or right-angle prism) and the encoder scale (and / or reference grating) and / or on the surface that is part of the retroreflector. For example, as shown in FIG. 8, the encoder head 810 includes a first QWP 820a on the first surface of the beam separation component 812 and a second QWP 820b on the second surface of the beam splitter 812. . The first QWP 820a is disposed between the beam separation component 812 and the retroreflector 818, while the second QWP 820b is disposed between the beam separation component 812 and the monolithic optical component 800.
During operation of an interferometric encoder system that utilizes encoder head 810, input beam 825 is provided from a light source to a third beam separation component 816. The third beam splitter 816 separates the incident beam 825 into a measurement beam (solid line) and a reference beam (dashed line). For example, the beam splitter 816 can include a polarizing beam splitter, which converts the input beam composed of orthogonally polarized beam components (eg, s and p polarized beam components) to the polarization of the reference and measurement beams. Based on the difference, separate into reference and measurement beams. Both the reference beam and the measurement beam pass through the second beam separation component 814.
The measurement beam passes through the second beam separation component 814 without changing the first beam separation component 812, and the measurement beam is then redirected toward the monolithic optical component 800 and the encoder scale 105 at the beam separation interface. Is done. Using optical component 800, the measurement beam is diffracted multiple times with a non-Littrow angle to produce two or more two-time diffracted measurement beams.
In contrast, the reference beam interacts with the beam separation interface of the second beam separation component 814 and is split into two separate reference beams. Both reference beams generated by the component 814 pass through the first beam separating component 812 and reflect little or no toward the retroreflector 818. The retroreflector 818 redirects each reference beam back toward the first beam separation component 812, where each reference beam is combined with the corresponding two-time diffractometry beam. Separate output beams 807 and 809 are generated. As shown in FIG. 8, the two output beams 807, 809 exit from the first beam separation component 812. If the encoder scale 105 includes a 2D grating, the encoder head apparatus shown in FIG. 8 may be used to generate an additional output beam that propagates out of the plane of the figure. In this case, an additional beam separation element would also have to be used to create an additional reference beam. The advantage of the configuration shown in FIG. 8 is that the measurement and reference beams remain parallel to each other in each output beam, even if the initial input beam has poor angular alignment. This is because the measurement beam and the reference beam are retro-reflected by each of component 800 and component 818, resulting in all output beam angles changing by the same amount as the input beam angle.
FIG. 9 is a schematic diagram of an exemplary interferometric encoder head 910 that includes a monolithic optical component 900 and a reference grating 950. The optical component 900 can include, for example, a polarization beam separation component configured to obtain a measurement beam 901 and a reference beam 911 from an input beam 925 supplied from a light source, where the input beam 925 is derived from orthogonal polarization beam components. Become. When reflected from the beam separation interface 902, the measurement beam 901 propagates to the encoder scale 105, and the beam 901 has a plurality of diffraction orders (eg, +1) at a first position 903 of the encoder scale 105 at a non-Letrow angle. Next, minus 1st order diffraction). For clarity, only one diffracted beam is shown in the first position 903 of FIG.
A plurality of single diffraction measurement beams (eg, 901 ′) then propagate back to the monolithic optical component 900. In the optical component 900, the one-time diffractometer beam is reflected at the central facet 902 and one or more side facets of the component 900, after which the one-time diffractometer beam is in a non-Littrow condition at the second position 904 Further, the direction is changed so as to return to the encoder scale 105 at an inclination angle with respect to the encoder scale 105. When the measurement beam reaches the encoder scale, a second diffraction is performed at a plurality of diffraction orders. Again, for clarity, only one diffracted beam is shown in the second position 904 in FIG. A twice diffracted measurement beam (eg, 901 ″) propagates back to the optical component 900 and is then reflected by the central facet 902 and propagates along a direction opposite and parallel to the direction of the input beam 925.
The central facet 902 is also used to acquire a reference beam 911. Reference beam 911 (dashed line in FIG. 9) propagates through component 900 to reference grating 950, and the reference beam has a plurality of diffraction orders (eg, +1) at a non-Littrow angle at a first position 906 of reference grating 950. Next, minus 1st order diffraction). For clarity, only one diffracted beam 911 'is shown at position 906 of the reference grating 950 in FIG. One or more of the one-time diffracted reference beams return to part 900. In optical component 900, the one-time diffracted reference beam is reflected at the central facet 902 and one or more side facets of component 900, after which the one-time diffracted measurement beam is a reference grating at a non-Littrow angle at a second location 907. The direction is changed back to 950.
The measurement beam is diffracted a second time at one or more diffraction orders (eg, + 1st order, −1st order diffraction) at a second position 907 of the reflective grating 950. Again, for clarity, only one double diffracted reference beam 911 ″ is shown in FIG. Each twice diffracted reference beam then propagates through beam separating component 900 and is combined with a corresponding twice diffracted measurement beam to form a corresponding output beam. The output beam is then received by a detector module (not shown), and an exemplary output beam is shown as beam 960 in FIG. To ensure that the reference and measurement beams are properly reflected or transmitted at the component facets, the facets include a multilayer coating to reflect and / or transmit incident radiation at a specified angle of incidence. Can be configured. In the example shown in FIG. 9, the central facet 902 is configured to function as a beam splitter for radiation incident at 45 ° to the surface of the facet 902 and to reflect incident radiation at other angles. An example of a multi-layer coating that reflects only 3.2% of the 45 ° beam (relative to the interface normal) and 96.8% of the 20 ° beam at the beam separation plane between the two blocks of BK7 glass. , ABCBCBCBA stack, A is a 78 nm magnesium fluoride layer, B is a 756 nm zinc sulfide layer, and C is a 365 nm magnesium fluoride layer.
FIG. 10 shows another embodiment of an encoder head that can use a reference grid. In particular, FIG. 10 is a 3D schematic diagram illustrating an example of an interferometric encoder head 1010, which includes a beam splitter 1002, a reference grating 1050, a measurement block 1060, and a reference block 1070. The measurement block 1060 and the reference block 1070 include optical elements such as a right triangular prism, and are fixed to the beam splitter 1002 by using, for example, an optical adhesive. The beam splitter 1002 can include, for example, a non-polarizing beam splitter or a polarizing beam splitter. Measurement block 1060 is positioned to direct the measurement beam toward encoder scale 105 and receive the one-time and two-time diffraction measurement beams from encoder scale 105. The reference block 1070 is similarly positioned to send a reference beam toward the reference grating 1050 and receive a one-time and two-time diffracted reference beam from the reference grating 1050. A beam splitter 1002 receives an input beam 1001 having orthogonally polarized beam components from a light source (not shown) and separates the input beam 1001 into both a reference beam and a measurement beam. The reference beam and measurement beam are then redirected by beam splitter 1002 towards reference block 1070 and measurement block 1060, respectively. The beam splitter 1002 is also configured to combine the twice diffracted reference beam and the twice reference measurement beam into four separate output beams 1007, and the four separate output beams 1007 are transmitted to the detector module. Interference signals are obtained from four separate output beams 1007, and the relative position of the encoder scale and / or encoder head is determined (eg, based on phase information from the interference signals).
FIG. 11 is an example of another embodiment of an encoder head that includes a reference grating. In particular, FIG. 11 is a schematic diagram illustrating a cross-sectional view of an interferometric encoder head 1110. The interferometric encoder head 1110 includes a measurement block 1160 (eg, a cuboid), a reference block 1170 (eg, a cuboid), and a polarized beam. It includes a splitter 1102, a reference grating 1150, and two quarter wave plates (QWP) 1180.
The operation of the encoder head 1110 is the same as the operation of the encoder head 1010 shown in FIG. That is, the beam splitter 1102 receives an input beam 1125 having orthogonal polarization components and separates the input beam 1125 into a reference beam (dashed line) and a measurement beam (solid line), after which the reference beam and the measurement beam are respectively referred to as a reference block 1170. Propagate towards measurement block 1160.
Initially, the measurement beam passes through measurement block 1160 and QWP 1180, is reflected little or not at all, and one or more diffraction orders (eg, + 1st order, −1st order diffraction) at non-Littrow angles by encoder scale 105. Is diffracted into The one-time diffracted measurement beam returns to the measurement block 1160 and the one-time diffracted measurement beam is reflected by the side facets of the measurement block 1160 and returns to the encoder scale 105. As with the other embodiments described above, the measurement block 1160 can include a local thin film coating configured to reflect the diffracted measurement beam once based on the angle of incidence. The one-time diffraction measurement beam returns to the encoder scale 105, and the encoder scale 105 performs a second diffraction on the beam to one or more diffraction orders at a non-Littrow angle. At least some of the twice diffracted measurement beams propagate back to measurement block 1160 along a direction parallel to the incident measurement beam.
Similarly, the incident reference beam passes through reference block 1170 and QWP 1180, is reflected little or not, and is diffracted by reference grating 1150 to one or more diffraction orders (eg, + 1st order, −1st order diffraction). The The one-time diffracted reference beam returns to reference block 1170, is reflected by the side facets of block 1170, and returns to reference grating 1150. In other embodiments described above, the reference block 1170 can include a local thin film multilayer coating configured to reflect the diffracted reference beam once based on the angle of incidence. The one-time diffracted reference beam returns to the reference grating 1150 where it is diffracted a second time to one or more diffraction orders. At least some of the twice diffracted reference beams propagate back to the reference block 1170 along a direction parallel to the incident reference beam. The twice diffracted reference beam and the twice diffracted measurement beam are then combined in a beam splitter 1102 to form an output beam 1107, which relates to the optical path length difference between the measurement beam and the reference beam. Contains phase information. A detector module and electronic processor (not shown) can be used to calculate information regarding one or more relative degrees of freedom of encoder scale 105 and / or encoder head 1110.
Measurement block 1160 and reference block 1170 are arranged identically (ie, from beam splitter 1102 so that they overlap when the twice diffracted reference beam and twice diffracted measurement beam are combined in beam splitter 1102). The same distance and the same distance from each grid). For example, in some implementations, the distance between reference block 1170 and reference grid 1150 can be different from the distance between measurement block 1160 and encoder scale 105. In some implementations, the grid pitch on encoder scale 105 can be different from the pitch on reference grid 1150. In some implementations, the dimensions of the measurement block 1160 can be different from the dimensions of the reference block 1170. For example, it may be preferable to minimize the effects of fluctuations by bringing the reference grid 1150 into contact with the reference block 1170 or at least in very close proximity. In order to make the offset between the input and output beams the same as in the measurement path, the dimensions and / or grating pitch of the reference block 1170 should be different from those used in the measurement path. . In addition, in the configuration shown in FIG. 11, the beam supply and the beam pickup are spatially separated by guiding the output beam 1107 along a direction different from that of the input beam 1125.
As described in the above embodiments, one surface of the monolithic optic should be configured to transmit the beam, while the other surface of the monolithic optic is configured to reflect the beam. Should do. One surface of the optical component can reflect or transmit one or more angles of the incident beam by providing a thin film multilayer coating on the surface.
In some embodiments, monolithic optical components (eg, cubes, cuboids, and right-angle prisms) can be formed with a slight offset from the perfect geometric shape. Loss of symmetry as a result of angular misalignment can help reduce errors in encoder scale position detection associated with spurious reflection. That is, spurious reflections tend to follow different paths from the measurement beam and therefore do not mismodulate the detected interference signal. For example, the edges on either side of an originally symmetric monolithic optic may be, for example, greater than 0 ° but greater than about 10 ° from the condition that they are parallel to each other and / or the plane of the encoder scale, subject to manufacturing tolerances. It can be shifted by a small amount (eg, about 0.5 °, about 1 °, about 5 °, or about 7 °). One such case is shown schematically in FIG. 12, in which the surface 1211 of the glass monolithic optic 1210 facing the encoder scale is an amount relative to the encoder scale 105, for example 1 °. Only intentionally tilted. The solid line shows the intended path of the measurement beam and two diffraction events. In contrast, the dashed line indicates an unintended spurious beam, which is first diffracted with zero order diffraction, reflected by an inclined surface 1211, diffracted by first order diffraction, including retroreflection, and glass monolithic optical component 1210. After roughly following the intended measurement path, a third diffraction is finally performed on the grating. Since the direction and position of the spurious beam is different from the desired beam direction and position, measurement errors that may otherwise be caused by the presence of the spurious beam at the detector can be substantially reduced. In contrast, if the lower surface of the glass monolithic optic is parallel to the encoder scale, the spurious beam will be at the same angle and at the same position as the desired measurement beam, which will cause further errors in position measurement. .
In some embodiments, the encoder head is configured to propagate the measurement and reference beams within the encoder head optics with a small separation angle from each other. For example, inclusion of one or more polarizing optics in the beam path of the measurement and reference beam can provide a small separation angle (eg, between about 0.05 mrad and 20 mrad) between the measurement and reference beams. . By having a small separation angle between the measurement and reference beams, these beams can be distinguished not only by their polarization but also by their propagation angle, resulting in a large periodic error in the mixing of polarizations in the encoder head. Is reduced. This is illustrated in FIG. 13, where box 1310 shows an encoder head that includes monolithic optics and / or beam splitting optics and retroreflective optics. The two input beams 1301, 1302, each intended to be a reference and measurement beam, are orthogonally polarized with respect to each other and separated by a small angle. The output beams 1303, 1304 from the encoder head still have the same separation angle and are mutually orthogonally polarized, but the desired output in either direction or polarization depending on the possibility of polarizer leakage in the encoder head. There may be another unintended output beam 1305, 1306 (ie, a ghost beam) that is different from the beams 1303, 1304. A birefringent beam combiner 1320 can redirect the intended output beams 1303, 1304 so that the beams 1303, 1304 are parallel, whereas the unintended beams 1305, 1306 are beam combiners 1320. Are deflected along substantially different directions. Thus, the desired output beams 1303, 1304 can reach the detector module 130 (eg, including the photodetector and polarizer) at the same angle, while the unwanted beams are more powerful desired beams. Depending on the angle, the detector module 130 is not reached or the interference fringe contrast is substantially reduced. Thus, measurement errors due to the presence of unwanted beams at the detector can be eliminated.
In general, any of the analysis methods described above can be implemented in computer hardware or software, or a combination of both, including determining phase information and encoder scale freedom information from detected interference signals. For example, in some embodiments, the electronic processor 150 can be installed in a computer and connected to one or more encoder systems and configured to perform analysis of signals from the encoder system. The analysis can be implemented in a computer program using standard programming techniques according to the methods described herein. The program code is applied to input data (eg, interference phase information) and the functions described herein are executed to generate output information (eg, degree of freedom information). The output information is applied to one or more output devices such as a display monitor. Each program may be implemented in a high-level procedural or object-oriented programming language to communicate with a computer system. However, the program can be implemented in assembly or machine language as desired. In either case, the language can be a compiled or interpreted language. Furthermore, the program can be executed on a dedicated integrated circuit preprogrammed for that purpose.
Each such computer program is preferably stored on a storage medium or device (eg, ROM or magnetic diskette) readable by a general purpose or special purpose programmable computer to store the computer on the storage medium or device. When the computer reads, it is configured or operated to perform the procedures described herein. Computer programs can also be stored in cache or main memory during program execution. The analysis method can also be implemented as a computer-readable storage medium configured with a computer program, which is described herein in a computer-specific, predetermined manner. Execute the function.
Lithography tool applications Lithography tools are particularly useful in lithography applications used in the manufacture of large scale integrated circuits such as computer chips. Lithography is a key technology driver for the semiconductor manufacturing industry. Overlay improvement is one of the five major challenges for the realization of line widths (design rules) of 22 nm or less, for example, International Technology Roadmap for Semiconductors p. 58-59 (2009).
Overlay is directly dependent on the performance, ie accuracy and precision, of the metrology system used to position the wafer and reticle (or mask) stage. The annual output of lithography tools can be as high as $ 50-500 million, and the economic value of metrology system improvements is great. Every 1% increase in lithography tool production yields an economic benefit of approximately $ 1 million per year for integrated circuit manufacturers, significantly increasing the competitive advantage of lithography tool suppliers.
The function of the lithography tool is to direct spatially patterned radiation onto the wafer with the photoresist coating. This process involves determining which position on the wafer receives radiation (alignment) and irradiating the photoresist at that position (exposure).
During exposure, the radiation source illuminates the patterned reticle, which scatters the radiation and produces spatially patterned radiation. A reticle is also referred to as a mask, and these terms are used interchangeably below. In the case of reduced projection lithography, the reduced projection lens collects the scattered radiation and forms a reduced image of the reticle pattern. Alternatively, in the case of proximity printing, the scattered radiation propagates a short distance (usually on the order of micrometers) and then contacts the wafer to produce a 1: 1 image of the reticle pattern. Radiation initiates a photochemical process in the resist that converts the radiation pattern into a latent image in the resist.
In order to properly position the wafer, the wafer includes an alignment mark on the wafer surface, which can be measured by a dedicated sensor. The position of the measured alignment mark defines the position of the wafer in the tool. This information, along with the desired patterning specifications for the wafer surface, guides the wafer alignment for spatially patterned radiation. Based on such information, a translatable stage that supports the photoresist-coated wafer moves the wafer so that the radiation exposes the correct position of the wafer. In certain lithography tools, such as lithography scanners, a mask is also placed on a translatable stage that is moved with the wafer during exposure.
Encoder systems such as those described above are important components of a positioning mechanism that controls the position of the wafer and reticle and aligns the reticle image on the wafer. If such an encoder system includes the features described above, the accuracy of the distance measured by the system can be improved and / or the period of time maintained without off-line maintenance can be increased, and as a result, Throughput increases with increased production and reduced tool downtime.
In general, a lithography tool, also called an exposure system, typically includes an illumination system and a wafer positioning system. The illumination system includes a radiation source that provides radiation, such as ultraviolet, visible, x-ray, electron or ion radiation, and a reticle or mask that imparts a pattern to the radiation, thereby producing spatially patterned radiation. Is done. In addition, for reduced projection lithography, the illumination system can include a lens assembly for imaging the spatially patterned radiation onto the wafer. The imaged radiation exposes the resist coated on the wafer. The illumination system also includes a mask stage that supports the mask and a positioning system for adjusting the position of the mask stage relative to the radiation directed through the mask. The wafer positioning system includes a wafer stage that supports the wafer and a positioning system for adjusting the position of the wafer stage relative to the imaged radiation. Integrated circuit fabrication can include multiple exposure steps. As general reference materials relating to lithography, for example, J. Org. R. Sheets (J.R. W. See B.W.Smith, Microlithography: Science and Technology (Marcel Dekker, Inc. New York, 1998). The contents of which are incorporated herein by reference.
The encoder system described above can be used to accurately measure the position of each of the wafer stage and mask stage relative to other components of the exposure system, such as a lens assembly, radiation source or support structure. In such cases, the optical assembly of the encoder system can be attached to a stationary structure and the encoder scale can be attached to a movable element such as one of a mask and a wafer stage. Alternatively, this situation can be reversed, with the optical assembly attached to a movable object and the encoder scale attached to a stationary object.
More generally, such an encoder system can also be used to measure the position of any one component in the exposure system with respect to any other component in the exposure system, where The optical assembly is attached to or supported by one of the parts, and the encoder scale is attached or supported by the other of the parts.
An example of a lithography tool 1400 using an interferometric system 1426 is shown in FIG. The encoder system is used to accurately measure the position of a wafer (not shown) within the exposure system. Here, stage 1422 is used to position and support the wafer relative to the exposure station. The scanner 1400 includes a frame 1402, which carries other support structures and various parts carried on these support structures. The exposure base 1404 is attached to the lens housing 1406 on the upper surface, and a reticle or mask stage 1416 used to support the reticle or mask is attached on the lens housing 1406. A positioning system for positioning the mask relative to the exposure station is indicated schematically by element 1417. The positioning system 1417 can include, for example, a piezoelectric transducer element and corresponding control electronics. Alternatively, although not shown in the embodiments described herein, a mask stage that uses one or more of the encoder systems described above and whose position needs to be accurately monitored during the lithographic structure manufacturing process And the position of other movable elements can also be measured accurately (see above-mentioned Sheets and Smith, Microlithography: Science and Technology).
A support base 1413 is suspended under the exposure base 1404, and the support base 1413 supports the wafer stage 1422. Stage 1422 includes a device under test 1428 that allows measurement beam 1454 to be diffracted by optical assembly 1426 into the stage. A positioning system for positioning the stage 1422 relative to the optical assembly 1426 is indicated schematically by element 1419. The positioning system 1419 can include, for example, a piezoelectric transducer element and corresponding control electronics. The object to be measured diffracts the reflection of the measurement beam and returns it to the optical assembly attached to the exposure base 1404. The encoder system can be any of the previous embodiments.
In operation, a radiation beam 1410, eg, a UV beam from an ultraviolet (UV) laser (not shown), passes through the beam shaping optics assembly 1412 and travels downward after being reflected by the mirror 1414. The radiation beam then passes through a mask (not shown) carried by mask stage 1416. A mask (not shown) is imaged onto a wafer (not shown) on wafer stage 1422 through lens assembly 1408 carried by lens housing 1406. Base 1404 and the various components supported thereby are isolated from environmental vibrations by a damping system depicted as spring 1420.
In some embodiments, one or more of the encoder systems described above can be used to measure displacement along multiple axes and angles associated with, for example, but not limited to, a wafer and a reticle (mask) stage. . In addition, the wafer can be exposed using another beam instead of the UV laser beam, for example, an X-ray beam, an electron beam, an ion beam, a visible ray, or the like.
In certain embodiments, the optical assembly 1426 may be positioned to measure changes in the position of the reticle (or mask) stage 1416 or other movable parts such as a scanner system. Finally, the encoder system can be used in a similar manner for lithography systems that include steppers in addition to or instead of scanners.
As is well known in the art, lithography is an important part of a manufacturing method for fabricating semiconductor devices. For example, US Pat. No. 5,483,343 outlines the steps of such a manufacturing method. These steps are described below with reference to FIGS. 15A and 15B. FIG. 15A is a flowchart of a manufacturing sequence of a semiconductor device such as a semiconductor chip (for example, IC or LSI), a liquid crystal panel, or a CCD. Step 1951 is a design process for designing a circuit of the semiconductor device. Step 1952 is a process for manufacturing a mask based on the circuit pattern design. Step 1953 is a process for manufacturing a wafer by using a material such as silicon.
Step 1954 is a wafer process called a pre-process, in which a circuit is formed on the wafer through lithography using the mask and wafer thus prepared. In order to form a circuit on the wafer corresponding to these patterns on the mask with sufficient spatial resolution, positioning of the lithography tool wafer with respect to the wafer is required. The interferometric methods and systems described herein can be particularly beneficial for improving the effectiveness of lithography used in wafer processes.
Step 1955 is an assembly step, which is called a post-process, and the wafer processed in step 1954 is formed into semiconductor chips. This step includes assembly (dicing and bonding) and packaging (chip encapsulation). Step 1956 is an inspection step. In the inspection step, operability check, durability check, etc. of the semiconductor device produced in step 1955 are executed. Through these steps, the semiconductor device is completed and shipped (step 1957).
FIG. 15B is a flowchart showing details of the wafer process. Step 1961 is an oxidation process for oxidizing the wafer surface. Step 1962 is a CVD process for forming an insulating film on the wafer surface. Step 1963 is an electrode formation process for forming electrodes on the wafer by vapor deposition. Step 1964 is an ion implantation process for implanting ions into the wafer. Step 1965 is a resist process for applying a resist (photosensitive material) to the wafer. Step 1966 is an exposure process for printing the circuit pattern of the mask on the wafer through exposure (ie, lithography) using the exposure apparatus described above. Even in the exposure process, as described above, the accuracy and resolution of such lithography steps is improved by the use of the interferometric systems and methods described herein.
Step 1967 is a developing process for developing the exposed wafer. Step 1968 is an etching process for removing portions other than the developed resist image. Step 1969 is a resist separation process for separating the resist material remaining on the wafer after execution of the etching process. By repeating these processes, circuit patterns are formed and superimposed on the wafer.
The encoder system described above can also be used in other applications where the relative position of an object needs to be accurately measured. For example, in applications where a writing beam, such as a laser, x-ray, ion, or electron beam, marks a pattern on the substrate while moving either the substrate or the beam, an encoder system is used to align the substrate and the writing beam. Relative movement can be measured.
A number of embodiments have been described. Nevertheless, of course, various changes can be made. For example, in some embodiments, the monolithic optical component includes another beam steering element (eg, a grating and / or refractive wedge) integrally formed with the component, which makes the beam more desirable. The flexibility to orient to the position is further increased. Alternatively, or in addition, other beam steering elements that are integrated with the monolithic optic allow beam shapes that make the interferometric encoder system less sensitive to changes in encoder scale position. It can be.
FIG. 16 shows an example of an encoder head that uses a transmissive and reflective grating patch integrally formed with a monolithic optic to provide a beam shape that is less susceptible to variations in encoder scale position.
FIG. 16A illustrates only one measurement beam 1601 of up to four measurement beams guided by a monolithic optical component 1610a (eg, a cuboid) toward a two-dimensional (2D) encoder scale (eg, 2D grating) 105. It is the schematic of the cross section which shows a beam path | route. The beam 1601 re-enters the part 1610 after being diffracted by the encoder scale 105, is retroreflected by the two side facets and the top face of the part 1610a, and then a patch of the transmission grating 1605 integrally formed in the part 1610a. Reach (patch). The grating 1605 redirects the once-diffracted beam to the encoder scale 105 at a substantially right angle. A second diffraction from the encoder scale 105 is performed on the measurement beam. The twice diffracted measurement beam can be of the same diffraction order (eg, + 1st order diffraction) as the one-time diffracted beam, for example, along the direction opposite the initial incident beam (beam 1611) by the transmission grating patch 1605. Converted.
FIG. 16B is an encoder head configuration similar to FIG. 16A, in which a reflective grating 1606 on the top facet of a monolithic optic 1610b (eg, cuboid) provides retroreflection of the single diffracted measurement beam, thereby The diffraction diffraction measurement beam is directed to the encoder scale 105. As shown in FIG. 16B, the reflective grating 1606 is offset laterally from the transmissive grating 1605 so that the one-time diffracted measurement beam can pass through the bottom facet of the component 1610b without changing the beam path. The twice diffracted beam is then redirected by the transmission grating 1605 along a path parallel to the incident measurement beam 1601 and opposite to the incident measurement beam 1601 (eg, beam 1611).
FIG. 16C is a 3D view of the encoder shown in FIG. 16B, again showing only one measurement beam path. As shown in FIG. 16C, the edges of the part 1610b are not oriented parallel to the grooves of the encoder grid. This configuration allows the diffracted beam to be incident on the intersection of the two side facets and the top facet of the part 1610b.
An encoder system,
An encoder scale,
Directing light to the encoder scale to generate a plurality of twice diffracted measurement beams, and combining each of the plurality of twice diffracted measurement beams with a corresponding reference beam to form a plurality of output beams. A configured encoder head, comprising:
The encoder head includes a monolithic optical component having a plurality of facets;
The plurality of facets is
Receiving a plurality of single diffraction measurement beams from the surface of the encoder scale;
Configured to redirect the plurality of one-time diffraction measurement beams back to the surface of the encoder scale;
The encoder scale is positioned in the path of the one diffraction beam, to generate the two diffraction beams,
The two-time diffraction measurement beam does not satisfy a Littrow condition for the encoder scale ;
A plurality of detector elements, each detector being positioned to detect a corresponding output beam; and
Receiving an interference signal from each of the detection elements, each interference signal including a phase related to an optical path difference between one of the two-time diffracted measurement beams and the corresponding reference beam; Receiving a signal,
An encoder system comprising: the electronic processor configured to perform determining information regarding degrees of freedom of the encoder scale based on the phase for each interference signal.
The encoder system of claim 1, wherein the monolithic optical component has a cubic shape.
The encoder system according to claim 1, wherein the monolithic optical component has a rectangular parallelepiped shape.
The monolithic optical component includes a first facet arranged to receive a non-diffracting measurement beam and emit the double diffracting measurement beam;
The first facet, the cause bulk permeability of the radiation propagating in a direction perpendicular to the first facet and morphism anti the incident radiation at an oblique angle relative to the first facet of claim 1 Encoder system.
The monolithic optic includes a second facet arranged to receive a one-time diffractometer beam or a two-time diffractometer beam from the encoder scale;
Said second facet causes bulk permeability of the radiation propagating in a direction perpendicular to said second facet, the encoder system according to claim 4.
The encoder system according to claim 5, wherein the second facet is disposed in front of the first facet so as to face the first facet.
The encoder system of claim 5, wherein the second facet is disposed perpendicular to the first facet.
The second facet is
Reflecting radiation incident on the second facet in a first tilt angle range relative to the second facet;
The encoder system of claim 7, configured to transmit radiation incident on the second facet at a second different tilt angle range relative to the second facet.
The side facet of the monolithic optical component, to morphism anti incident radiation at an oblique angle to the side facet, the encoder system according to claim 4.
The encoder scale comprises a 1D grating or a 2D grating;
The encoder system according to claim 1, wherein the 1D grating or the 2D grating is configured by a groove extending along a first direction.
11. An encoder system according to claim 10, wherein the plane containing the side facets of the monolithic optic is oriented at an angle of inclination with respect to the first direction.
The encoder system according to claim 1, wherein the monolithic optical component is a regular hexagonal prism.
The encoder head is configured to direct a non-diffracting measurement beam along a first beam path to the encoder scale;
The encoder system of claim 1, wherein the first beam path of the non-diffracting measurement beam is outside the monolithic optical component.
The encoder scale is positioned to diffract the incident beam along a second beam path relative to the monolithic optical component;
The encoder system of claim 13, wherein the second beam path of the diffracted incident beam is outside the monolithic optic.
The encoder system of claim 14, wherein the incident beam comprises one of the one-time diffraction measurement beams.
The encoder system of claim 1, wherein the monolithic optical component includes a regular pentagonal prism.
The one-time diffraction measurement beam is
A first one-time diffraction measurement beam obtained from a positive diffraction order from the encoder scale;
The encoder system according to claim 1, comprising a second one-time diffraction measurement beam obtained from a negative diffraction order from the encoder scale.
The first one-time diffractive measurement beam and the second one-time diffractive measurement beam are obtained from positive and negative diffraction orders along a first plane;
A third one-diffractive measurement beam and a fourth one obtained from the positive and negative orders of diffraction from the encoder scale, respectively, along a second orthogonal direction. The encoder system of claim 17 further comprising a diffraction diffraction measurement beam.
A plurality of optical elements configured to receive an input beam and to obtain from the input beam (1) the corresponding reference beam for each two-time diffracted measurement beam; and (2) an incident measurement beam. The encoder system according to claim 1, comprising:
The plurality of optical elements are:
Multiple beam splitters,
The encoder system according to claim 19, comprising a retroreflector.
The monolithic optical component is
Receive the input beam,
The encoder system of claim 1, configured to obtain (1) the corresponding reference beam for each two-time diffracted measurement beam and (2) an incident measurement beam from the input beam.
The monolithic optical component includes a beam separation facet;
The beam separation facet is
Separating the input beam based on the polarization of the input beam and a specified angle of incidence with respect to the beam separation facet;
The encoder system of claim 21, configured to reflect a beam incident on the beam separation facet at an incident angle other than the specified incident angle.
23. The encoder system of claim 22, further comprising a reference grating positioned to receive the reference beam from the monolithic optic and redirect a diffractive reference beam to the monolithic optic.
A movable stage; and the encoder system according to claim 1,
A system in which either the encoder system or the device under test is attached to the movable stage.
An encoder system according to claim 1;
A movable stage to which either the encoder system or the device under test is attached;
An illumination system coupled to the encoder system, the illumination system including a radiation source, the radiation source directing radiation to the encoder system during operation of the lithography system;
A detector for detecting an output beam from the encoder system during operation of the lithography system;
A lithography system coupled to the electronic processor and configured to adjust a position of the stage based on information regarding displacement of the encoder system.
An encoder head for use with an encoder scale,
The encoder head is configured to combine each of a plurality of twice diffracted measurement beams with a corresponding reference beam to form a plurality of output beams;
i) receiving a plurality of single diffraction measurement beams from the surface of the encoder scale;
ii) configured to redirect the plurality of one-time diffraction measurement beams back toward the surface of the encoder scale;
The encoder scale is positioned in the path of one diffracted beam to generate the two diffraction beams,
The encoder head , wherein the two-time diffraction measurement beam does not satisfy a Littrow condition with respect to the encoder scale .
The encoder system of claim 1, wherein a first edge of the monolithic optic and a second edge opposite the monolithic optic deviate from an angle by less than about 10 degrees.
The encoder system of claim 1, wherein the plurality of one-time diffracted measurement beams are obtained from a single non-diffracted measurement beam.
27. The encoder head of claim 26, wherein the plurality of single diffracted measurement beams are obtained from a single non-diffracted measurement beam.
The encoder system according to claim 1, wherein the plurality of one-time diffraction measurement beams do not satisfy a Littrow condition with respect to the encoder scale.
27. The encoder head of claim 26, wherein the plurality of one-time diffraction measurement beams do not satisfy a Littrow condition for the encoder scale.
The first facet transmits at least 75% of radiation propagating in a direction perpendicular to the first facet and reflects at least 75% of radiation incident at an angle of inclination with respect to the first facet The encoder system according to claim 4.
6. The encoder system of claim 5, wherein the second facet transmits at least 75% of radiation propagating in a direction perpendicular to the second facet.
The encoder system of claim 9, wherein the side facets of the monolithic optic reflect at least 75% of radiation incident at an angle of inclination with respect to the side facets.
JP2014541271A 2011-11-09 2012-11-08 Small encoder head for interferometric encoder systems Active JP5890531B2 (en)
US201161557776P true 2011-11-09 2011-11-09
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US61/557,776 2011-11-09
US61/557,755 2011-11-09
PCT/US2012/064211 WO2013070957A1 (en) 2011-11-09 2012-11-08 Compact encoder head for interferometric encoder system
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JP2014541271A Active JP5890531B2 (en) 2011-11-09 2012-11-08 Small encoder head for interferometric encoder systems
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