CA2059553A1 - Birefringent polarizing device - Google Patents
Birefringent polarizing deviceInfo
- Publication number
- CA2059553A1 CA2059553A1 CA002059553A CA2059553A CA2059553A1 CA 2059553 A1 CA2059553 A1 CA 2059553A1 CA 002059553 A CA002059553 A CA 002059553A CA 2059553 A CA2059553 A CA 2059553A CA 2059553 A1 CA2059553 A1 CA 2059553A1
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- Prior art keywords
- birefringent
- elements
- beams
- prism
- space
- Prior art date
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Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/28—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for polarising
- G02B27/283—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for polarising used for beam splitting or combining
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/10—Beam splitting or combining systems
- G02B27/12—Beam splitting or combining systems operating by refraction only
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- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Polarising Elements (AREA)
- Optical Elements Other Than Lenses (AREA)
Abstract
A birefringent polarizing device which separates a beam (1) into polarized component beams (9) and (10) by transmitting both components through plane parallel element (3). Separation occurs since one or both of plane parallel element (3) and element (2) is birefringent. Elements (2) and (4) are of the same refractive index or indices so that beams (9) and (10) emerge parallel to one another. Plane parallel element (3) may also be a space (3) which allows the device to be used with high powered lasers. Many variants are described.
Description
W O 90/15357 2 ~ ~ 9 ~ ~ 3: PCT/~U9o/00223 BIREFRINGENT POLARIZING DEVICE
Technical Field This invention relates to birefringent polarizers and polarizing beam-splitters and particularly to birefringent polarizers and polarizing beam-splitters which separate polarization components by transmitting both components through an interface.
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3ack~;roun~ Art : Many polarizers and polarizing beam-splitters are known to the art, each having disadvantages.
The Glan-Thompson polarizer, which is a block of birefringent material cut into pr sms and then cemented together acts by reflecting one polarization component at the cement interface and by transmitting the other. The device requires a considerable amount of birefringent material, generally calcite, which is scarce and expensive, and is unable to work with high powered lasers and ultraviolet light, since the light destroys or clouds cement.
- The Glan-Thompson polarizing beam-splitter, which makes use of the reflected polari7ation component, suffers from the added disadvantage that polarized beams exit said device at inconvenient angles, for example ~5 degrees, when it is often useful that beams are parallel, o-thogonal or otherwise oriented.
The Glan-Taylor polarizer which is similar to the Glan-Thompson polarizer but uses an air space instead of cement to separate polarization componen~s can work with many light sources but suffers from reflection loss and ghosting caused by the air gap.
The Wollaston, Rochon and Senarmont beam-splitters, which separate polarization components by transmitting said components through an interface, ?ermit optical contacting for use with most light sources, but ?roduce beams which also exit . .
- ' . . ~ ' ' '.` ~ ,..................................... .
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WO90/15~ 2 - PCT/AU9~/002^~3 at inconvenient angles, with one or both polarization components suffering from chromatism and distortion. . -The doubie refracting element (beam displacer), which produces accurately parallel polarized beams of light, achieves . small beam separation and limited field. Also, since the beams - may pass through a considerable amount of material before - achieving useful separation, then wavefront distortion can occur in the extraordinary beam, due to imperfections in the crystal's structure. See, for example, "Birefringence of Quartz and Calcite," Journal of the Optical Society of America, volume 99, number 7, July 1959, pages 710-712). Beam separation can be ru-ther limited by the smaii size and high cost of suitable crystals.
Polarizing prisms and tneir various defects are described in deLail by H. E. Benne_t and J. ;-. Bennett, "Polarization," in Handbook of Optics, W. G. Driscoll and W.
Vaughan, Editors, ~cGraw-Hill, New York, 197~.
.
. Disclosure Of The Invention '..
It is an object of this invention to provide a birefringent polarizing beam-splitter in which polarized beams :~
of electromagnetic radiation may emerge from the device being - free from chromatism and distortion and such that angular .~ separation may be greater than for a double refracting element.
; It is also an object of the invention to provide a polarizing beam-splitter in which polarized beams of ; electromagnetic radiation may emerge from said device being oriented at convenient angles.
. It is another object of the invention to provide a polarizing beam-splitter which may be conservative in the use of birefringent material.
It is a further object of the invention to provide a beam displacer which may causes less wavefront distortion in the extraordinary beam than a known birefringent beam displacer.
It is a still further object of tr.e invention to provide an improved polarizer.
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: To this end, in accordance wit~ a~9 ~ ~ tion, the birefringent polarizing device is characterised by a space or an element which is all or in part plane parallel, situated between at least two optical elements, wherein polarization components are separated by the transmission of said components ~ through an interface, with at least one element forming said - interface being birerringent.
Isotropic elements on either side of said element which is all or in part plane parallel have the same refractive index, birefringent elements on either side of said space or element which is all or in part plane parallel have the same optic axis orienLations, and when elements on either side of said space or element which is all or in parL plane parallel are at least one isolropic and at least one Di-efringent, then the refractive indices or said isotropic elemer._ or elements match an index or indices o_ said birefringent element or elements.
Birefringent elements on either side of a space may be Brewster prisms with different optic ax.is orientations, as -in the two elements of a Wollaston, Rochon or Senarmont prism, so that said prisms may permit the transmission of one polarization component without Fresnel reflection. These .- prisms may be in physical contact without being in optical contact, thus having air between them, eliminating stress - birefringence between elements and removing the accurate polishing requirement. One Brewster prism may also be isotropic.
In the case of a polarizer, the unused polarization component may be reflected as well as transmitted at an interface so as to provide a large acceptance angle.
Also reflecting surfaces or Brewster windows may be included in said device to translate a polarization component . or components.
.~
W090/15357 ~ - 4 - PCT/AU~0/00223 Brlef Description Of Drawin~s Fig. 1 represents an embodiment in accordance with the invention describlng the metnod in which a beam-splitter with a plane parallel element operates.
Fig. 2 represents a particular embodiment in accordance with the invention being a beam splitter which uses the Wollaston prism beam-splitting method to obtain polarized components.
Fig. 3 represents an embodiment in accordance with the invention being a beam-splitter in which at least one element is isotropic, being an e~bodiment which is economical in its use of birefringent materi21.
Fig. 9 represents an embodiment in accordance with the invention being a beam-splitler in which the second element is plane parallel only in part.
Fig. 5 represents an e~.~odiment in accordance with the invention being a polarizer which provides a large acceptance field.
Fig. 6 represents an embodiment in accordance with :~
the invention, being an extension of the three element Wollaston, producing output beams which are parallel and free from chromatism and distortion.
Fig. 7 represents an embodiment in accordance with the invention being a beam-splitter in which polarizatio~
components exit at orthogonal angies.
Fig. 8 represents an embodiment in accordance with the invention being a beam-splitter which includes an air space.
Fig. 9 represents an embodiment in accordance with the invention being a beam-splitter wherein Brewster prisms are used to reduce reflection loss for one polarization component.
Fig. 10 represents an embodiment in accordance with the invention being a plain polarizer which includes Brewster prisms.
Fig. 11 represents an embodiment in accordance with the invention being a polarizer similar to the previous '"';
.
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., ~ WO90/153~7 ~ 5 ~ 2 ~ ~ 9 ~ ~ 3 PC~/AUgo/00223 embodiment in which beams are reflected from a mirror to counter displacement.
Fig. 12 represents an embodiment in accordance with the invention being a polarizer in which two mirrors are employed to counter image inversion.
Fig. 13 represents an embodiment in accordance with the invention being a polarizer which employs the Rochon prism beam-splitting method and includes Brewster prisms.
Fig. 14 represents an embodiment in accordance with the invention similar to the previous embodiment, in which both polarization components are transmitted through the last face of the second prism.
Fig. 15 represents a beam displacer, similar to a known beam displacer made of calcite, in which the amount of calcite is reduced by replacing a substantial section of said beam displacer with isotropic ma~erial.
Figure 16 represents an embodiment using 45 degree calcite prisms, wherein beams eme-ge orthogonal to one and other.
Figure 17 represents an embodiment similar to the embodiment in figure 16, wherein beams exit at an angle of 120 degrees.
Descri~tion Of Preferred Embodiments Fig. 1 represents an embodiment in accordance with the invention describing how a beam-splitter which includes a plane parallel element operates, in which a beam of electromagnetic radiation 1 enters first element 2 and passes into second element 3, which in this case is the plane parallel element, so that beam 1 separates into orthogonally polarized : beams 5 and 6.
- Since at least element 2 or element 3 is double refracting, the beams will separate by encountering different refractive indices as known, for example, in the Wollaston prism (Bennett and Bennett, page 10-60). Similar separation also occurs when one of said elemen~s is isotropic.
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w~ s7~ 3 - 6 - PCT/AU90/00223 The refractive indices of elements on either side of element ~ are the same for the same polarization components, and so once beams 5 and 6 have passed through element 3, with faces 7 and 8 parallel, said beams will pass into element 4 parallel to related components in 2.
After leaving element 4 component beams become beams 9 and 10 which are parallel to each other and parallel to input beam 1, being free from chromatism and distortion.
Figure 2 represents a particular embodiment in accordance with the invention being a beam-splitter based on the Wollaston prism beam-splitting method.
Beam 21 enters double re racting prism 22 with its optic axis 25 in the plane of the drawing and ?arallel to inpu, face 30. Beam 21 becomes beam 26 in prism 22 where said beam then passes into plane parallel element 2', being a double refracting element with its optic axis 27 normal to the plane of the drawing. Said beam 26 then becomes orthogonally polarized beams 28 and 29, as known.
Now, beams 28 and 29 continue through interface 32 and into double refracting prism 24, with its optic axis 33 in the same direction as optic axis 25, such that beams refract to become parallel to related beams in 22. As beams 28 and 29 are parallel to component beams 26, and given that faces 30 and 31 are plane parallel, then beams 37 and 38 exit eiement 24 parallel to input beam 21.
Block 34, formed by extending the dotted lines, can represent a Wollaston prism. Since Wollaston prisms are commonly manufactured with extinction ratios in excess of 105:1, and since beams in the described embodiment exit as if from a Wollaston prism, then extinction ratios should be similar to those of the Wollaston prism or better. Note, beams travel through the equivalent of two Wollaston prisms in sequence.
By covering surfaces 35 and 36 with an absorbing material, as is done with the Glan-~hompson prism, reflected light can be removed from the device.
Calcite, which is generally the double refracting material used in constructing Wollaston prisms, has a larae .. : , - : ' -:' ~' ' ' ' , '' : .
W090/15357 2 ~ 3 PCT/AUgo/00223 positive coefficient of expansion parallel to the optic axis and a smaller negative coefficient of expansion perpendicular to the optic axis. When the two parts of a Wollaston prism are then joined together a considerable amount of strain may generate in each prism when the temperature changes. This strain, which can produce strain birefringence, still permits excellent extinction in output component beams. The same event should thus occur in the described embodiment.
Similar embodiments may be constructed based upon Rochon and Senarmont prism beam-splitting methods. Further embodiments may also be constructed based upon known three beam-splitting methods with optic axes reversed as, for example, in said described embodiment wherein elements 22 and 24 have optic axes normal to the plane of the paper, and element 23 has its optic axis ln the plane G~ the drawing parallel to input face 30. Other optic axis orientations may also be used to advantage.
Calcite is a scarce and expensive material, hence polarizing devices which reduce the amount OL calcite or other -birefringent material required are desirable.
In figure 3 elements 41, 43 and 44 may be isotropic while element 42 is birefringent, or 42 may be isotropic while 41, ~ and 44 are birefringent, reducing the amount of birefringent material employed. Also element 41 may be double refracting while elements 42, 43 and 44 may be isotropic, with refractive indices of elements 43 and 44 matching those of element 41. In this last case chromatism and distortion could appear in one of the output beams ard so its use would be appropriate where imaging is not required. Other variations which include designs in figures l and 2 will also be obvious.
Figure 4 represents an embodiment in accordance with the invention in which beams 53 and 54 leave said embodiment at different angles. Element 51 is double refracting and elements 52 and 53 are isotropic, with refrac~ive indices of elements 52 and 53 matching those of element 51. Element 52 could be, for example, injection moulded.
Figure 5 represents an emoodiment in accordance with the invention being a po-larizer onl~, constructed so that .: : : ' : : ','. ' : :
WO 90/1~3~7 ~ 5 ~ 8 - PCT/AU90/00223 unwanted components may be transmitted as well as reflected at interface 74.
Beam 75 passes through prism 71 so that unwanted component 76 is reflected from surface 74 and wanted component 77 is transmitted through surface 74. Transmitted beam 77 then passes into element 73 leaving the device as beam 78.
; For beam 79, in which both polarization components are transmitted, unwanted component 80 passes through element 72 so as to separate from wanted component 81. Wanted component 81 passes into element 73 and out of the polarizer as beam 82.
As unwanted components may be transr..itted as well as reflected, the described device will permit a larger optical acceptance angle than is obtained with the Glan-Thompson polarizing prism.
Figure 6 represents an embodiment in accordance with the invention which operates such ,hat beams are separated in element 91, and further separated in plane parallel element 92;
the embodiment being an extension of the three element Wollaston prism (Bennett and Bennett, page 10-61). Parallel beams are produced which are free from chromatism and distortion.
Fig. 7 represents an embodiment in accordance with - the invention in which polarization components exit said . embodiment at orthogonal angles. In this embodiment the Rochon beam splitting method is employed. Beam 99 is reflected from face 95 so as to exit the device as beam 96 being orthogonal to . beam 97.
If a quarter waveplate is placed at position 98 then . beam 96, when passed through said device in the reverse direction, will pass through waveplate 98. On being reflected back through said waveplate said beam will return through said embodiment as beam 97.
Glan-Taylor and Glan-Focault polarizers, which consist of birefringent prisms separated by an air gap, work by transmitting one polarization component at said gap and by reflecting the other component. A problem with this type of - polarizer is that reflection loss occurs at the air gap along . . - ............................. , - . , ::
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W090il5357 _ 9 _ 2 ~ 3PCT/AU90/00223 with ghosting. By allowing both polarization components to be transmitted it is possible to reduce this reflection loss and also to provide a polarizing beam-splitter whic~ has the advantages of an air spaced polarizer.
Fig. 8 represents an embodiment in accordance with the invention comprising two birefringent prisms and an air space. As shown, beam 100 enters prism 101 and is split at face 102 into orthogonally polarized beams 103 and 104. Said beams, after travelling through the air space, pass into prism 105. In this embodiment prisms 101 and 105 have the same optic axis orientations and faces 102 and 106 are parallel, so beams 103 and 104 will enter p-lsm 105 and exit said ?rism as parallel beams 107 and 108. Thus in passing th.ough the two prisms input beam 100 will be sepa-ated into pa-allel, orthogonally polarized output beams 107 and 108.
I' the optic axes of the elements are normal to the plane of the drawing, as with a Glan-Focault p-ism, then, in the drawing, the upper beam will suffer smaller reflection loss than the lower beam. This is because the electric field of the upper beam is parallel to the plane of incidence, being P
polarization, which in this case passes through the interface close to or at Brewster's angle. By also coating hypotenuse faces with antireflection films, reflection loss at said faces can be reduced for the other polarization component.
Fig. 9 represen~s an embodiment in accordance with the invention being a polarizer in which reflection loss at every faces, as calculated from Fresnel's equalion, is reduced to zero for one polarization component. In this embodiment beam 112 enters prism 110 and is split into orthogonally polarized components 113 and 114. These components then pass into prism 111. If the optic axes of said prisms 110 and 111 are oriented normal to the plane of the drawing, beam 112 will become parallel beams 115 and 116 with beam 116 being the ordinary beam which passes through each prism at Brewster's angle.
Other enbodiments coul~ transmit the extraordinary -beam.
W090/153~7 ~ 3 1 o - PCT/AU90/00223 Fig. 10 represents an embodiment in accordance with the invention, simllar to the previous embodiment, bei~g a polarizer which uses Brewster prisms.
Beam 120 passes through prism 121 with the P polarized component passing through prism 122 at Brewster's angle. The S polarized component meets stop 123.
Fig. 11 represents an embodiment ln accordance with the invention being a polarizer wherein component beams are reflected from mirror 130 so as to counter displacement which occurs in the preceding embodiment. This is the previous embodiment with prism 1~ reflected about said mirror.
Fig. 12 represents an em~odiment in accordance with the invention being a polarizer in which a further reflection occurs at second mirror 190 so as to prevent the image from being inverted and to keep output beam 142 parallel to input beam 141.
Fig. 13 represents an embodiment in accordance with the invention belng a polarizing device simil~r to the Rochon prism, which includes Brewster prisms.
In this embodiment beam 150 is separated into orthogonally polarized beams 153 and 154, with the P polarized component 154 passing through both prisms at Brewster's angle and the S polarized component 153 being totally reflected at last face 155. Here the optic axis orientation of the first element 151 is normal to the plane of the drawing so that beam 154 is the ordinary beam. The optic axis of the second element 152 is in the plane of the drawing parallel to the P polarized beam in the element. Prism 152 could be replaced with a glass prism having an index of refraction matching that of the ordinary ray in prism 151. Some glasses of said index are described by E. O. Ammann and G. A. Massey, Journal of the Optical Society of America, volume 58, number 11, 1968, pages 1472-1433.
Fig. 14 represents an embodiment in accordance with the invention similar to the previous embodiment but wherein the S polarized component is transmitted through the last face instead of being reflected from said face.
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., , . " : :' ' ': ' ' ' , ~ ~ ', WO90/15357 ~ 2 ~ ~ 9 ~ ~ 3 In the embodiment second prism 161 has its optic axis normal to the plane of the drawing and the first prism 160 may be glass. The S polarized beam is transmitted through face 162.
Since prisrns i~ the previous two embodiments are not cemented or optically contacted then strain between elements is removed. Note, these prisms could be in physica1 contact and still be considered air spaced.
Fig. 15 represents a beam displacer, similar to a known calcite beam displacer, wherein the amount of calcite is reduced by replacing a substantial section of said beam displacer with isotropic material.
In the embodiment elements 170 and 172 are 45 degree calcite prisms with optic axes orientec normal t^ the plane of the drawing, and element 171 is ar. iso.-o~ic pla^.e parallel element with a refractive index sir.ilâ- to ~hat o the extraordinary beam in calcite.
In said known beam displace- beam sepe-ation is 6.2 degrees. In this embodiment beam sep2ration is ,.1 degrees. If elements 170 and 172 are optically con~acted to element 171, Fresnel reflection at surface 173 will be less than 0.03 percent for the P polarized component and zero for the S
polarized component. This is because the P polarized component passes through the interface at an angle close to Brewster's angle.
For said embodiment, wave~ront distor~ion in the extraordinary beam can be reduced by aDout ~0 percent, as can the amount calcite. This permits the construction of large beam displacers. Note, calcite can be further reduced as shown in figure 3.
Figure 16 represents an embodiment using 45 degree calcite prisms, wherein beams emerge orthogonal to one and other.
Prisms 180 and 1~ have opt-c axes normal to the plane of the drawing and element 181 ~s isotropic with a refractive index similar to that o~ the extraordinary ray in calcite, as in the previous embodimen=. Section 183, shown by dotted lines, which would normally be the upper section of the previously described beam displacer, -s here th.e section below ' .
- , . .
WO 9Q/1~357 ~ ~ 5 ~ ~ ~ 3 - 12 - PCT/A~'90/00223 reflec.ing surface 184. Beam 186 will leave prism 182 as if from said section 183, being free from chromatism and distortion.
This embodiment can be used with high powered light sources if optical contacting is employed and the amount of calcite and wavefront distortion in the extraordinary beam can be further reduced.
Figure 17 represents an embodiment similar to embodiment 16, wherein beams exit at an angle of 120 degrees to one and other.
In this embodiment prism 190 is a 60 degree right prlsm, and element 19? is modified so that poiarization component 195 may leave said element free fro~ chromatism and distortion.
The orientation of face 193 is dete-mined by reflecting the supposed upper section of a beam displacer about reflecting surface 194, reflecting sur ace 194 being orthogonal to faces of plane parallel element 19'.
Elements 190, 191 and 192 may be calcite, or said elements may be combinations of calcite and other material, for example synthetic fused silica or Schott optical glass BK 7.
Further embodiments using other birefringent materials will be evident.
In each embodiment which includes a plane parallel element, little restriction is placed upon cements which may be used and optical contacting may also be employed. Steel, Smartt and Giovanelli have successfully contacted glass and calcite (Au~tralian Journal of Phvsics, volume 14, 1961, page 209), and since it is difficult to produce surfaces of the required flatness in prisms (F. Twyman, "Prism and Lens Making," second edition, Hilger & Watts, London, 1952) then in these embodiments the first and third elements could be polished to required flatness as plane parallel sections, later being divided to provide separate elements.
Many modifications and varia_ions to the described embodiments will be apparent to those skilled in the art and all such modifications and variations should be considered as within the scope of the present invent-on.
: .
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: :
-:
Technical Field This invention relates to birefringent polarizers and polarizing beam-splitters and particularly to birefringent polarizers and polarizing beam-splitters which separate polarization components by transmitting both components through an interface.
.
3ack~;roun~ Art : Many polarizers and polarizing beam-splitters are known to the art, each having disadvantages.
The Glan-Thompson polarizer, which is a block of birefringent material cut into pr sms and then cemented together acts by reflecting one polarization component at the cement interface and by transmitting the other. The device requires a considerable amount of birefringent material, generally calcite, which is scarce and expensive, and is unable to work with high powered lasers and ultraviolet light, since the light destroys or clouds cement.
- The Glan-Thompson polarizing beam-splitter, which makes use of the reflected polari7ation component, suffers from the added disadvantage that polarized beams exit said device at inconvenient angles, for example ~5 degrees, when it is often useful that beams are parallel, o-thogonal or otherwise oriented.
The Glan-Taylor polarizer which is similar to the Glan-Thompson polarizer but uses an air space instead of cement to separate polarization componen~s can work with many light sources but suffers from reflection loss and ghosting caused by the air gap.
The Wollaston, Rochon and Senarmont beam-splitters, which separate polarization components by transmitting said components through an interface, ?ermit optical contacting for use with most light sources, but ?roduce beams which also exit . .
- ' . . ~ ' ' '.` ~ ,..................................... .
.
WO90/15~ 2 - PCT/AU9~/002^~3 at inconvenient angles, with one or both polarization components suffering from chromatism and distortion. . -The doubie refracting element (beam displacer), which produces accurately parallel polarized beams of light, achieves . small beam separation and limited field. Also, since the beams - may pass through a considerable amount of material before - achieving useful separation, then wavefront distortion can occur in the extraordinary beam, due to imperfections in the crystal's structure. See, for example, "Birefringence of Quartz and Calcite," Journal of the Optical Society of America, volume 99, number 7, July 1959, pages 710-712). Beam separation can be ru-ther limited by the smaii size and high cost of suitable crystals.
Polarizing prisms and tneir various defects are described in deLail by H. E. Benne_t and J. ;-. Bennett, "Polarization," in Handbook of Optics, W. G. Driscoll and W.
Vaughan, Editors, ~cGraw-Hill, New York, 197~.
.
. Disclosure Of The Invention '..
It is an object of this invention to provide a birefringent polarizing beam-splitter in which polarized beams :~
of electromagnetic radiation may emerge from the device being - free from chromatism and distortion and such that angular .~ separation may be greater than for a double refracting element.
; It is also an object of the invention to provide a polarizing beam-splitter in which polarized beams of ; electromagnetic radiation may emerge from said device being oriented at convenient angles.
. It is another object of the invention to provide a polarizing beam-splitter which may be conservative in the use of birefringent material.
It is a further object of the invention to provide a beam displacer which may causes less wavefront distortion in the extraordinary beam than a known birefringent beam displacer.
It is a still further object of tr.e invention to provide an improved polarizer.
. .
. .
.;
.. - ~ - - - ~ . :
: To this end, in accordance wit~ a~9 ~ ~ tion, the birefringent polarizing device is characterised by a space or an element which is all or in part plane parallel, situated between at least two optical elements, wherein polarization components are separated by the transmission of said components ~ through an interface, with at least one element forming said - interface being birerringent.
Isotropic elements on either side of said element which is all or in part plane parallel have the same refractive index, birefringent elements on either side of said space or element which is all or in part plane parallel have the same optic axis orienLations, and when elements on either side of said space or element which is all or in parL plane parallel are at least one isolropic and at least one Di-efringent, then the refractive indices or said isotropic elemer._ or elements match an index or indices o_ said birefringent element or elements.
Birefringent elements on either side of a space may be Brewster prisms with different optic ax.is orientations, as -in the two elements of a Wollaston, Rochon or Senarmont prism, so that said prisms may permit the transmission of one polarization component without Fresnel reflection. These .- prisms may be in physical contact without being in optical contact, thus having air between them, eliminating stress - birefringence between elements and removing the accurate polishing requirement. One Brewster prism may also be isotropic.
In the case of a polarizer, the unused polarization component may be reflected as well as transmitted at an interface so as to provide a large acceptance angle.
Also reflecting surfaces or Brewster windows may be included in said device to translate a polarization component . or components.
.~
W090/15357 ~ - 4 - PCT/AU~0/00223 Brlef Description Of Drawin~s Fig. 1 represents an embodiment in accordance with the invention describlng the metnod in which a beam-splitter with a plane parallel element operates.
Fig. 2 represents a particular embodiment in accordance with the invention being a beam splitter which uses the Wollaston prism beam-splitting method to obtain polarized components.
Fig. 3 represents an embodiment in accordance with the invention being a beam-splitter in which at least one element is isotropic, being an e~bodiment which is economical in its use of birefringent materi21.
Fig. 9 represents an embodiment in accordance with the invention being a beam-splitler in which the second element is plane parallel only in part.
Fig. 5 represents an e~.~odiment in accordance with the invention being a polarizer which provides a large acceptance field.
Fig. 6 represents an embodiment in accordance with :~
the invention, being an extension of the three element Wollaston, producing output beams which are parallel and free from chromatism and distortion.
Fig. 7 represents an embodiment in accordance with the invention being a beam-splitter in which polarizatio~
components exit at orthogonal angies.
Fig. 8 represents an embodiment in accordance with the invention being a beam-splitter which includes an air space.
Fig. 9 represents an embodiment in accordance with the invention being a beam-splitter wherein Brewster prisms are used to reduce reflection loss for one polarization component.
Fig. 10 represents an embodiment in accordance with the invention being a plain polarizer which includes Brewster prisms.
Fig. 11 represents an embodiment in accordance with the invention being a polarizer similar to the previous '"';
.
. .
., ~ WO90/153~7 ~ 5 ~ 2 ~ ~ 9 ~ ~ 3 PC~/AUgo/00223 embodiment in which beams are reflected from a mirror to counter displacement.
Fig. 12 represents an embodiment in accordance with the invention being a polarizer in which two mirrors are employed to counter image inversion.
Fig. 13 represents an embodiment in accordance with the invention being a polarizer which employs the Rochon prism beam-splitting method and includes Brewster prisms.
Fig. 14 represents an embodiment in accordance with the invention similar to the previous embodiment, in which both polarization components are transmitted through the last face of the second prism.
Fig. 15 represents a beam displacer, similar to a known beam displacer made of calcite, in which the amount of calcite is reduced by replacing a substantial section of said beam displacer with isotropic ma~erial.
Figure 16 represents an embodiment using 45 degree calcite prisms, wherein beams eme-ge orthogonal to one and other.
Figure 17 represents an embodiment similar to the embodiment in figure 16, wherein beams exit at an angle of 120 degrees.
Descri~tion Of Preferred Embodiments Fig. 1 represents an embodiment in accordance with the invention describing how a beam-splitter which includes a plane parallel element operates, in which a beam of electromagnetic radiation 1 enters first element 2 and passes into second element 3, which in this case is the plane parallel element, so that beam 1 separates into orthogonally polarized : beams 5 and 6.
- Since at least element 2 or element 3 is double refracting, the beams will separate by encountering different refractive indices as known, for example, in the Wollaston prism (Bennett and Bennett, page 10-60). Similar separation also occurs when one of said elemen~s is isotropic.
: -,,, , . , : , .: , . . .
w~ s7~ 3 - 6 - PCT/AU90/00223 The refractive indices of elements on either side of element ~ are the same for the same polarization components, and so once beams 5 and 6 have passed through element 3, with faces 7 and 8 parallel, said beams will pass into element 4 parallel to related components in 2.
After leaving element 4 component beams become beams 9 and 10 which are parallel to each other and parallel to input beam 1, being free from chromatism and distortion.
Figure 2 represents a particular embodiment in accordance with the invention being a beam-splitter based on the Wollaston prism beam-splitting method.
Beam 21 enters double re racting prism 22 with its optic axis 25 in the plane of the drawing and ?arallel to inpu, face 30. Beam 21 becomes beam 26 in prism 22 where said beam then passes into plane parallel element 2', being a double refracting element with its optic axis 27 normal to the plane of the drawing. Said beam 26 then becomes orthogonally polarized beams 28 and 29, as known.
Now, beams 28 and 29 continue through interface 32 and into double refracting prism 24, with its optic axis 33 in the same direction as optic axis 25, such that beams refract to become parallel to related beams in 22. As beams 28 and 29 are parallel to component beams 26, and given that faces 30 and 31 are plane parallel, then beams 37 and 38 exit eiement 24 parallel to input beam 21.
Block 34, formed by extending the dotted lines, can represent a Wollaston prism. Since Wollaston prisms are commonly manufactured with extinction ratios in excess of 105:1, and since beams in the described embodiment exit as if from a Wollaston prism, then extinction ratios should be similar to those of the Wollaston prism or better. Note, beams travel through the equivalent of two Wollaston prisms in sequence.
By covering surfaces 35 and 36 with an absorbing material, as is done with the Glan-~hompson prism, reflected light can be removed from the device.
Calcite, which is generally the double refracting material used in constructing Wollaston prisms, has a larae .. : , - : ' -:' ~' ' ' ' , '' : .
W090/15357 2 ~ 3 PCT/AUgo/00223 positive coefficient of expansion parallel to the optic axis and a smaller negative coefficient of expansion perpendicular to the optic axis. When the two parts of a Wollaston prism are then joined together a considerable amount of strain may generate in each prism when the temperature changes. This strain, which can produce strain birefringence, still permits excellent extinction in output component beams. The same event should thus occur in the described embodiment.
Similar embodiments may be constructed based upon Rochon and Senarmont prism beam-splitting methods. Further embodiments may also be constructed based upon known three beam-splitting methods with optic axes reversed as, for example, in said described embodiment wherein elements 22 and 24 have optic axes normal to the plane of the paper, and element 23 has its optic axis ln the plane G~ the drawing parallel to input face 30. Other optic axis orientations may also be used to advantage.
Calcite is a scarce and expensive material, hence polarizing devices which reduce the amount OL calcite or other -birefringent material required are desirable.
In figure 3 elements 41, 43 and 44 may be isotropic while element 42 is birefringent, or 42 may be isotropic while 41, ~ and 44 are birefringent, reducing the amount of birefringent material employed. Also element 41 may be double refracting while elements 42, 43 and 44 may be isotropic, with refractive indices of elements 43 and 44 matching those of element 41. In this last case chromatism and distortion could appear in one of the output beams ard so its use would be appropriate where imaging is not required. Other variations which include designs in figures l and 2 will also be obvious.
Figure 4 represents an embodiment in accordance with the invention in which beams 53 and 54 leave said embodiment at different angles. Element 51 is double refracting and elements 52 and 53 are isotropic, with refrac~ive indices of elements 52 and 53 matching those of element 51. Element 52 could be, for example, injection moulded.
Figure 5 represents an emoodiment in accordance with the invention being a po-larizer onl~, constructed so that .: : : ' : : ','. ' : :
WO 90/1~3~7 ~ 5 ~ 8 - PCT/AU90/00223 unwanted components may be transmitted as well as reflected at interface 74.
Beam 75 passes through prism 71 so that unwanted component 76 is reflected from surface 74 and wanted component 77 is transmitted through surface 74. Transmitted beam 77 then passes into element 73 leaving the device as beam 78.
; For beam 79, in which both polarization components are transmitted, unwanted component 80 passes through element 72 so as to separate from wanted component 81. Wanted component 81 passes into element 73 and out of the polarizer as beam 82.
As unwanted components may be transr..itted as well as reflected, the described device will permit a larger optical acceptance angle than is obtained with the Glan-Thompson polarizing prism.
Figure 6 represents an embodiment in accordance with the invention which operates such ,hat beams are separated in element 91, and further separated in plane parallel element 92;
the embodiment being an extension of the three element Wollaston prism (Bennett and Bennett, page 10-61). Parallel beams are produced which are free from chromatism and distortion.
Fig. 7 represents an embodiment in accordance with - the invention in which polarization components exit said . embodiment at orthogonal angles. In this embodiment the Rochon beam splitting method is employed. Beam 99 is reflected from face 95 so as to exit the device as beam 96 being orthogonal to . beam 97.
If a quarter waveplate is placed at position 98 then . beam 96, when passed through said device in the reverse direction, will pass through waveplate 98. On being reflected back through said waveplate said beam will return through said embodiment as beam 97.
Glan-Taylor and Glan-Focault polarizers, which consist of birefringent prisms separated by an air gap, work by transmitting one polarization component at said gap and by reflecting the other component. A problem with this type of - polarizer is that reflection loss occurs at the air gap along . . - ............................. , - . , ::
-' , ,.- , . . ..
'' . ' ~ : . ~ '. :
. . - .
, ~, .
W090il5357 _ 9 _ 2 ~ 3PCT/AU90/00223 with ghosting. By allowing both polarization components to be transmitted it is possible to reduce this reflection loss and also to provide a polarizing beam-splitter whic~ has the advantages of an air spaced polarizer.
Fig. 8 represents an embodiment in accordance with the invention comprising two birefringent prisms and an air space. As shown, beam 100 enters prism 101 and is split at face 102 into orthogonally polarized beams 103 and 104. Said beams, after travelling through the air space, pass into prism 105. In this embodiment prisms 101 and 105 have the same optic axis orientations and faces 102 and 106 are parallel, so beams 103 and 104 will enter p-lsm 105 and exit said ?rism as parallel beams 107 and 108. Thus in passing th.ough the two prisms input beam 100 will be sepa-ated into pa-allel, orthogonally polarized output beams 107 and 108.
I' the optic axes of the elements are normal to the plane of the drawing, as with a Glan-Focault p-ism, then, in the drawing, the upper beam will suffer smaller reflection loss than the lower beam. This is because the electric field of the upper beam is parallel to the plane of incidence, being P
polarization, which in this case passes through the interface close to or at Brewster's angle. By also coating hypotenuse faces with antireflection films, reflection loss at said faces can be reduced for the other polarization component.
Fig. 9 represen~s an embodiment in accordance with the invention being a polarizer in which reflection loss at every faces, as calculated from Fresnel's equalion, is reduced to zero for one polarization component. In this embodiment beam 112 enters prism 110 and is split into orthogonally polarized components 113 and 114. These components then pass into prism 111. If the optic axes of said prisms 110 and 111 are oriented normal to the plane of the drawing, beam 112 will become parallel beams 115 and 116 with beam 116 being the ordinary beam which passes through each prism at Brewster's angle.
Other enbodiments coul~ transmit the extraordinary -beam.
W090/153~7 ~ 3 1 o - PCT/AU90/00223 Fig. 10 represents an embodiment in accordance with the invention, simllar to the previous embodiment, bei~g a polarizer which uses Brewster prisms.
Beam 120 passes through prism 121 with the P polarized component passing through prism 122 at Brewster's angle. The S polarized component meets stop 123.
Fig. 11 represents an embodiment ln accordance with the invention being a polarizer wherein component beams are reflected from mirror 130 so as to counter displacement which occurs in the preceding embodiment. This is the previous embodiment with prism 1~ reflected about said mirror.
Fig. 12 represents an em~odiment in accordance with the invention being a polarizer in which a further reflection occurs at second mirror 190 so as to prevent the image from being inverted and to keep output beam 142 parallel to input beam 141.
Fig. 13 represents an embodiment in accordance with the invention belng a polarizing device simil~r to the Rochon prism, which includes Brewster prisms.
In this embodiment beam 150 is separated into orthogonally polarized beams 153 and 154, with the P polarized component 154 passing through both prisms at Brewster's angle and the S polarized component 153 being totally reflected at last face 155. Here the optic axis orientation of the first element 151 is normal to the plane of the drawing so that beam 154 is the ordinary beam. The optic axis of the second element 152 is in the plane of the drawing parallel to the P polarized beam in the element. Prism 152 could be replaced with a glass prism having an index of refraction matching that of the ordinary ray in prism 151. Some glasses of said index are described by E. O. Ammann and G. A. Massey, Journal of the Optical Society of America, volume 58, number 11, 1968, pages 1472-1433.
Fig. 14 represents an embodiment in accordance with the invention similar to the previous embodiment but wherein the S polarized component is transmitted through the last face instead of being reflected from said face.
, : ! ~, ~:
,, ~,~, .
., , . " : :' ' ': ' ' ' , ~ ~ ', WO90/15357 ~ 2 ~ ~ 9 ~ ~ 3 In the embodiment second prism 161 has its optic axis normal to the plane of the drawing and the first prism 160 may be glass. The S polarized beam is transmitted through face 162.
Since prisrns i~ the previous two embodiments are not cemented or optically contacted then strain between elements is removed. Note, these prisms could be in physica1 contact and still be considered air spaced.
Fig. 15 represents a beam displacer, similar to a known calcite beam displacer, wherein the amount of calcite is reduced by replacing a substantial section of said beam displacer with isotropic material.
In the embodiment elements 170 and 172 are 45 degree calcite prisms with optic axes orientec normal t^ the plane of the drawing, and element 171 is ar. iso.-o~ic pla^.e parallel element with a refractive index sir.ilâ- to ~hat o the extraordinary beam in calcite.
In said known beam displace- beam sepe-ation is 6.2 degrees. In this embodiment beam sep2ration is ,.1 degrees. If elements 170 and 172 are optically con~acted to element 171, Fresnel reflection at surface 173 will be less than 0.03 percent for the P polarized component and zero for the S
polarized component. This is because the P polarized component passes through the interface at an angle close to Brewster's angle.
For said embodiment, wave~ront distor~ion in the extraordinary beam can be reduced by aDout ~0 percent, as can the amount calcite. This permits the construction of large beam displacers. Note, calcite can be further reduced as shown in figure 3.
Figure 16 represents an embodiment using 45 degree calcite prisms, wherein beams emerge orthogonal to one and other.
Prisms 180 and 1~ have opt-c axes normal to the plane of the drawing and element 181 ~s isotropic with a refractive index similar to that o~ the extraordinary ray in calcite, as in the previous embodimen=. Section 183, shown by dotted lines, which would normally be the upper section of the previously described beam displacer, -s here th.e section below ' .
- , . .
WO 9Q/1~357 ~ ~ 5 ~ ~ ~ 3 - 12 - PCT/A~'90/00223 reflec.ing surface 184. Beam 186 will leave prism 182 as if from said section 183, being free from chromatism and distortion.
This embodiment can be used with high powered light sources if optical contacting is employed and the amount of calcite and wavefront distortion in the extraordinary beam can be further reduced.
Figure 17 represents an embodiment similar to embodiment 16, wherein beams exit at an angle of 120 degrees to one and other.
In this embodiment prism 190 is a 60 degree right prlsm, and element 19? is modified so that poiarization component 195 may leave said element free fro~ chromatism and distortion.
The orientation of face 193 is dete-mined by reflecting the supposed upper section of a beam displacer about reflecting surface 194, reflecting sur ace 194 being orthogonal to faces of plane parallel element 19'.
Elements 190, 191 and 192 may be calcite, or said elements may be combinations of calcite and other material, for example synthetic fused silica or Schott optical glass BK 7.
Further embodiments using other birefringent materials will be evident.
In each embodiment which includes a plane parallel element, little restriction is placed upon cements which may be used and optical contacting may also be employed. Steel, Smartt and Giovanelli have successfully contacted glass and calcite (Au~tralian Journal of Phvsics, volume 14, 1961, page 209), and since it is difficult to produce surfaces of the required flatness in prisms (F. Twyman, "Prism and Lens Making," second edition, Hilger & Watts, London, 1952) then in these embodiments the first and third elements could be polished to required flatness as plane parallel sections, later being divided to provide separate elements.
Many modifications and varia_ions to the described embodiments will be apparent to those skilled in the art and all such modifications and variations should be considered as within the scope of the present invent-on.
: .
:; . , - . . . .
: . . . .
, , ~
. ' ':
: :
-:
Claims (7)
1. A birefringent device for polarizing light which separates polarization components by transmitting said components through an interface, characterised by:
a space or an element which is all or in part plane parallel situated between at least two optical elements wherein;
isotropic elements on sides of said element which is all or in part plane parallel have the same refractive index and wherein;
birefringent elements on sides of said space or element which is all or in part plane parallel have the same optic axis orientations and wherein;
isotropic and birefringent elements on sides of said space or element which is all or in part plane parallel have an isotropic element or elements which match an index or indices of said birefringent element or elements and wherein;
birefringent Brewster prisms on sides of said space may have different optic axis orientations so that said prisms may permit the transmission of one polarization component without Fresnel reflection and wherein;
a birefringent Brewster prism on one side of said space and an isotropic Brewster prism on the other side of said space may permit the transmission of one polarization component without Fresnel reflection.
a space or an element which is all or in part plane parallel situated between at least two optical elements wherein;
isotropic elements on sides of said element which is all or in part plane parallel have the same refractive index and wherein;
birefringent elements on sides of said space or element which is all or in part plane parallel have the same optic axis orientations and wherein;
isotropic and birefringent elements on sides of said space or element which is all or in part plane parallel have an isotropic element or elements which match an index or indices of said birefringent element or elements and wherein;
birefringent Brewster prisms on sides of said space may have different optic axis orientations so that said prisms may permit the transmission of one polarization component without Fresnel reflection and wherein;
a birefringent Brewster prism on one side of said space and an isotropic Brewster prism on the other side of said space may permit the transmission of one polarization component without Fresnel reflection.
2. A device as claimed in claim 1, wherein an unwanted polarization component may be reflected as well as transmitted at an interface.
3. A device as claimed in claims 1 and 2, characterised in that reflecting surfaces or Brewster windows are included to translate a polarization component or components.
4. A device as claimed in claims 1, 2 and 3, wherein additional elements are added to advantage.
5. A device as claimed in claims 1, 2, 3 and 9 characterised in that said device is employed for a purpose other than polarizing light or beam-splitting such as, for example, combining beams.
6. An optical instrument which includes a birefringent polarizing device characterized in that it further includes a device as claimed in claims 1, 2, 3, 4 or 5.
7. Any feature or step or combination of features or steps described herein.
Applications Claiming Priority (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| AUPJ4465 | 1989-05-30 | ||
| AUPJ446589 | 1989-05-30 | ||
| AUPJ5850 | 1989-08-17 | ||
| AUPJ585089 | 1989-08-17 | ||
| US08/220,716 US5724184A (en) | 1989-05-30 | 1994-03-14 | Polarizer with birefringent plate |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CA2059553A1 true CA2059553A1 (en) | 1990-12-01 |
Family
ID=27157504
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA002059553A Abandoned CA2059553A1 (en) | 1989-05-30 | 1990-05-29 | Birefringent polarizing device |
Country Status (2)
| Country | Link |
|---|---|
| CA (1) | CA2059553A1 (en) |
| WO (1) | WO1990015357A1 (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN111947892A (en) * | 2020-07-17 | 2020-11-17 | 中国科学院上海光学精密机械研究所 | Deep ultraviolet depolarizer detection device and detection method |
| WO2021228287A1 (en) | 2020-05-14 | 2021-11-18 | Univerzita Palackého v Olomouci | Polarizing optical separator for stellar intensity interferometry |
Families Citing this family (9)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5172186A (en) * | 1990-07-03 | 1992-12-15 | Konica Corporation | Laser interferometry length measuring an apparatus employing a beam slitter |
| US6175448B1 (en) * | 1998-08-17 | 2001-01-16 | New Focus, Inc. | Optical circulators using beam angle turners |
| US6049426A (en) | 1998-08-17 | 2000-04-11 | New Focus, Inc. | Compact polarization insensitive circulators with simplified structure and low polarization mode dispersion |
| US6282025B1 (en) | 1999-08-02 | 2001-08-28 | New Focus, Inc. | Optical polarization beam combiner/splitter |
| US6342981B1 (en) | 1999-09-21 | 2002-01-29 | Rose Research, Llc | Zero-displacement phase retarder device and method |
| US6822793B2 (en) | 1999-10-29 | 2004-11-23 | Finisar Corporation | Compact polarization insensitive circulators with simplified structure and low polarization mode dispersion |
| US6690514B2 (en) * | 2001-04-27 | 2004-02-10 | Solid Optics, Inc. | Single crystal polarizing prism and method of manufacturing thereof |
| DE102013103282A1 (en) | 2013-04-02 | 2014-10-02 | Carl Zeiss Laser Optics Gmbh | Polarizer arrangement for spatially separating polarization states of a light beam |
| JP6334218B2 (en) * | 2014-03-17 | 2018-05-30 | 株式会社光学技研 | Total reflection type polarizer |
Family Cites Families (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3868168A (en) * | 1973-01-16 | 1975-02-25 | American Optical Corp | Combination of birefringent elements for polarizing interferential systems |
| SU570003A1 (en) * | 1976-04-12 | 1977-08-25 | Горьковский ордена Трудового Красного Знамени научно-исследовательский радиофизический институт | Modulator |
| SU809025A1 (en) * | 1979-05-03 | 1981-02-28 | Горьковский Ордена Трудового Крас-Ного Знамени Научно-Исследователь-Ский Радиофизический Институт | Modulated beam phase control assembly for multi-channel optical spectrum analyzer |
| JPH01113626A (en) * | 1987-10-27 | 1989-05-02 | Toyo Commun Equip Co Ltd | Measuring method for optical wavelength |
| JPH01233418A (en) * | 1988-03-14 | 1989-09-19 | Nippon Telegr & Teleph Corp <Ntt> | Optical isolator |
| JPH01241502A (en) * | 1988-03-23 | 1989-09-26 | Namiki Precision Jewel Co Ltd | Polarizing element for optical isolator |
| JP2572627B2 (en) * | 1988-05-13 | 1997-01-16 | ティーディーケイ株式会社 | Optical isolator and optical circulator |
| JP2651701B2 (en) * | 1988-05-18 | 1997-09-10 | 並木精密宝石株式会社 | Laser module with optical isolator |
-
1990
- 1990-05-29 WO PCT/AU1990/000223 patent/WO1990015357A1/en active Application Filing
- 1990-05-29 CA CA002059553A patent/CA2059553A1/en not_active Abandoned
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2021228287A1 (en) | 2020-05-14 | 2021-11-18 | Univerzita Palackého v Olomouci | Polarizing optical separator for stellar intensity interferometry |
| CN111947892A (en) * | 2020-07-17 | 2020-11-17 | 中国科学院上海光学精密机械研究所 | Deep ultraviolet depolarizer detection device and detection method |
| CN111947892B (en) * | 2020-07-17 | 2022-03-08 | 中国科学院上海光学精密机械研究所 | Deep ultraviolet depolarizer detection device and detection method |
Also Published As
| Publication number | Publication date |
|---|---|
| WO1990015357A1 (en) | 1990-12-13 |
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