Phase modulation time dynamics of the liquid-crystal spatial light modulator
Abstract In this paper, liquid-crystal spatial light modulators are presented for precise dynamic manipulation of coherent light fields in space, which are used in diffractive optoelectronic and optical data processing systems. In addition, this paper presents the results of the temporal dynamics st...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Minikhanov, T. Z. [verfasserIn] Zlokazov, E. Yu. [verfasserIn] Starikov, R. S. [verfasserIn] Cheremkhin, P. A. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2024 |
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| Schlagwörter: |
Liquid-crystal spatial light modulator Coherent optical diffractive processor |
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| Anmerkung: |
© Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
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| Übergeordnetes Werk: |
Enthalten in: Measurement techniques - Springer US, 1958, 66(2024), 12 vom: März, Seite 935-939 |
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| Übergeordnetes Werk: |
volume:66 ; year:2024 ; number:12 ; month:03 ; pages:935-939 |
| Links: |
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| DOI / URN: |
10.1007/s11018-024-02309-x |
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SPR056203799 |
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| 520 | |a Abstract In this paper, liquid-crystal spatial light modulators are presented for precise dynamic manipulation of coherent light fields in space, which are used in diffractive optoelectronic and optical data processing systems. In addition, this paper presents the results of the temporal dynamics study of the HoloEye PLUTO‑2 VIS-016 liquid-crystal spatial light modulator for light field rate modulation analysis. Experiments using binary phase computer-generated holograms and binary focusing phase diffractive optical elements are performed. The time characteristics of the modulator response are determined from the experimental data. Displaying the diffraction structure model on the screen of the spatial light modulator results in a rise time of the diffraction efficiency of 146 ms, and switching to a new model leads to a decay time of 97 ms. The obtained results allow implementing the dynamic generation of an alternating diffraction field at 2 Hz update frequency with −16 dB interference level. Increasing the frequency of updating diffraction structure models increases the level of interframe noise in the generated diffraction field, and when updating with the frequency indicated in the specification, separating the generated distributions is virtually impossible. From the presented results, the studied modulator model can be applied for high-precision formation of complex diffraction fields with a frame update rate lower than stated. Determining the actual frame rate from the rise and decay times of diffraction efficiency allows correctly determining the minimum operating time of an information optical system with a liquid-crystal spatial light modulator. | ||
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| 700 | 1 | |a Cheremkhin, P. A. |e verfasserin |0 (orcid)0000-0003-3556-2663 |4 aut | |
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10.1007/s11018-024-02309-x doi (DE-627)SPR056203799 (SPR)s11018-024-02309-x-e DE-627 ger DE-627 rakwb eng 620 VZ 50.21 bkl 33.00 bkl Minikhanov, T. Z. verfasserin (orcid)0000-0002-2246-9729 aut Phase modulation time dynamics of the liquid-crystal spatial light modulator 2024 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In this paper, liquid-crystal spatial light modulators are presented for precise dynamic manipulation of coherent light fields in space, which are used in diffractive optoelectronic and optical data processing systems. In addition, this paper presents the results of the temporal dynamics study of the HoloEye PLUTO‑2 VIS-016 liquid-crystal spatial light modulator for light field rate modulation analysis. Experiments using binary phase computer-generated holograms and binary focusing phase diffractive optical elements are performed. The time characteristics of the modulator response are determined from the experimental data. Displaying the diffraction structure model on the screen of the spatial light modulator results in a rise time of the diffraction efficiency of 146 ms, and switching to a new model leads to a decay time of 97 ms. The obtained results allow implementing the dynamic generation of an alternating diffraction field at 2 Hz update frequency with −16 dB interference level. Increasing the frequency of updating diffraction structure models increases the level of interframe noise in the generated diffraction field, and when updating with the frequency indicated in the specification, separating the generated distributions is virtually impossible. From the presented results, the studied modulator model can be applied for high-precision formation of complex diffraction fields with a frame update rate lower than stated. Determining the actual frame rate from the rise and decay times of diffraction efficiency allows correctly determining the minimum operating time of an information optical system with a liquid-crystal spatial light modulator. Computer-generated holography (dpeaa)DE-He213 Liquid-crystal spatial light modulator (dpeaa)DE-He213 Coherent optical diffractive processor (dpeaa)DE-He213 Diffractive optical neural networks (dpeaa)DE-He213 Diffractive optical element (dpeaa)DE-He213 Zlokazov, E. Yu. verfasserin (orcid)0000-0003-1340-7734 aut Starikov, R. S. verfasserin (orcid)0000-0002-7369-1565 aut Cheremkhin, P. A. verfasserin (orcid)0000-0003-3556-2663 aut Enthalten in Measurement techniques Springer US, 1958 66(2024), 12 vom: März, Seite 935-939 (DE-627)325573468 (DE-600)2037682-0 1573-8906 nnns volume:66 year:2024 number:12 month:03 pages:935-939 https://dx.doi.org/10.1007/s11018-024-02309-x X:SPRINGER Resolving-System lizenzpflichtig Volltext SYSFLAG_0 GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 50.21 VZ 33.00 VZ AR 66 2024 12 03 935-939 |
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10.1007/s11018-024-02309-x doi (DE-627)SPR056203799 (SPR)s11018-024-02309-x-e DE-627 ger DE-627 rakwb eng 620 VZ 50.21 bkl 33.00 bkl Minikhanov, T. Z. verfasserin (orcid)0000-0002-2246-9729 aut Phase modulation time dynamics of the liquid-crystal spatial light modulator 2024 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In this paper, liquid-crystal spatial light modulators are presented for precise dynamic manipulation of coherent light fields in space, which are used in diffractive optoelectronic and optical data processing systems. In addition, this paper presents the results of the temporal dynamics study of the HoloEye PLUTO‑2 VIS-016 liquid-crystal spatial light modulator for light field rate modulation analysis. Experiments using binary phase computer-generated holograms and binary focusing phase diffractive optical elements are performed. The time characteristics of the modulator response are determined from the experimental data. Displaying the diffraction structure model on the screen of the spatial light modulator results in a rise time of the diffraction efficiency of 146 ms, and switching to a new model leads to a decay time of 97 ms. The obtained results allow implementing the dynamic generation of an alternating diffraction field at 2 Hz update frequency with −16 dB interference level. Increasing the frequency of updating diffraction structure models increases the level of interframe noise in the generated diffraction field, and when updating with the frequency indicated in the specification, separating the generated distributions is virtually impossible. From the presented results, the studied modulator model can be applied for high-precision formation of complex diffraction fields with a frame update rate lower than stated. Determining the actual frame rate from the rise and decay times of diffraction efficiency allows correctly determining the minimum operating time of an information optical system with a liquid-crystal spatial light modulator. Computer-generated holography (dpeaa)DE-He213 Liquid-crystal spatial light modulator (dpeaa)DE-He213 Coherent optical diffractive processor (dpeaa)DE-He213 Diffractive optical neural networks (dpeaa)DE-He213 Diffractive optical element (dpeaa)DE-He213 Zlokazov, E. Yu. verfasserin (orcid)0000-0003-1340-7734 aut Starikov, R. S. verfasserin (orcid)0000-0002-7369-1565 aut Cheremkhin, P. A. verfasserin (orcid)0000-0003-3556-2663 aut Enthalten in Measurement techniques Springer US, 1958 66(2024), 12 vom: März, Seite 935-939 (DE-627)325573468 (DE-600)2037682-0 1573-8906 nnns volume:66 year:2024 number:12 month:03 pages:935-939 https://dx.doi.org/10.1007/s11018-024-02309-x X:SPRINGER Resolving-System lizenzpflichtig Volltext SYSFLAG_0 GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 50.21 VZ 33.00 VZ AR 66 2024 12 03 935-939 |
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10.1007/s11018-024-02309-x doi (DE-627)SPR056203799 (SPR)s11018-024-02309-x-e DE-627 ger DE-627 rakwb eng 620 VZ 50.21 bkl 33.00 bkl Minikhanov, T. Z. verfasserin (orcid)0000-0002-2246-9729 aut Phase modulation time dynamics of the liquid-crystal spatial light modulator 2024 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In this paper, liquid-crystal spatial light modulators are presented for precise dynamic manipulation of coherent light fields in space, which are used in diffractive optoelectronic and optical data processing systems. In addition, this paper presents the results of the temporal dynamics study of the HoloEye PLUTO‑2 VIS-016 liquid-crystal spatial light modulator for light field rate modulation analysis. Experiments using binary phase computer-generated holograms and binary focusing phase diffractive optical elements are performed. The time characteristics of the modulator response are determined from the experimental data. Displaying the diffraction structure model on the screen of the spatial light modulator results in a rise time of the diffraction efficiency of 146 ms, and switching to a new model leads to a decay time of 97 ms. The obtained results allow implementing the dynamic generation of an alternating diffraction field at 2 Hz update frequency with −16 dB interference level. Increasing the frequency of updating diffraction structure models increases the level of interframe noise in the generated diffraction field, and when updating with the frequency indicated in the specification, separating the generated distributions is virtually impossible. From the presented results, the studied modulator model can be applied for high-precision formation of complex diffraction fields with a frame update rate lower than stated. Determining the actual frame rate from the rise and decay times of diffraction efficiency allows correctly determining the minimum operating time of an information optical system with a liquid-crystal spatial light modulator. Computer-generated holography (dpeaa)DE-He213 Liquid-crystal spatial light modulator (dpeaa)DE-He213 Coherent optical diffractive processor (dpeaa)DE-He213 Diffractive optical neural networks (dpeaa)DE-He213 Diffractive optical element (dpeaa)DE-He213 Zlokazov, E. Yu. verfasserin (orcid)0000-0003-1340-7734 aut Starikov, R. S. verfasserin (orcid)0000-0002-7369-1565 aut Cheremkhin, P. A. verfasserin (orcid)0000-0003-3556-2663 aut Enthalten in Measurement techniques Springer US, 1958 66(2024), 12 vom: März, Seite 935-939 (DE-627)325573468 (DE-600)2037682-0 1573-8906 nnns volume:66 year:2024 number:12 month:03 pages:935-939 https://dx.doi.org/10.1007/s11018-024-02309-x X:SPRINGER Resolving-System lizenzpflichtig Volltext SYSFLAG_0 GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 50.21 VZ 33.00 VZ AR 66 2024 12 03 935-939 |
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10.1007/s11018-024-02309-x doi (DE-627)SPR056203799 (SPR)s11018-024-02309-x-e DE-627 ger DE-627 rakwb eng 620 VZ 50.21 bkl 33.00 bkl Minikhanov, T. Z. verfasserin (orcid)0000-0002-2246-9729 aut Phase modulation time dynamics of the liquid-crystal spatial light modulator 2024 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In this paper, liquid-crystal spatial light modulators are presented for precise dynamic manipulation of coherent light fields in space, which are used in diffractive optoelectronic and optical data processing systems. In addition, this paper presents the results of the temporal dynamics study of the HoloEye PLUTO‑2 VIS-016 liquid-crystal spatial light modulator for light field rate modulation analysis. Experiments using binary phase computer-generated holograms and binary focusing phase diffractive optical elements are performed. The time characteristics of the modulator response are determined from the experimental data. Displaying the diffraction structure model on the screen of the spatial light modulator results in a rise time of the diffraction efficiency of 146 ms, and switching to a new model leads to a decay time of 97 ms. The obtained results allow implementing the dynamic generation of an alternating diffraction field at 2 Hz update frequency with −16 dB interference level. Increasing the frequency of updating diffraction structure models increases the level of interframe noise in the generated diffraction field, and when updating with the frequency indicated in the specification, separating the generated distributions is virtually impossible. From the presented results, the studied modulator model can be applied for high-precision formation of complex diffraction fields with a frame update rate lower than stated. Determining the actual frame rate from the rise and decay times of diffraction efficiency allows correctly determining the minimum operating time of an information optical system with a liquid-crystal spatial light modulator. Computer-generated holography (dpeaa)DE-He213 Liquid-crystal spatial light modulator (dpeaa)DE-He213 Coherent optical diffractive processor (dpeaa)DE-He213 Diffractive optical neural networks (dpeaa)DE-He213 Diffractive optical element (dpeaa)DE-He213 Zlokazov, E. Yu. verfasserin (orcid)0000-0003-1340-7734 aut Starikov, R. S. verfasserin (orcid)0000-0002-7369-1565 aut Cheremkhin, P. A. verfasserin (orcid)0000-0003-3556-2663 aut Enthalten in Measurement techniques Springer US, 1958 66(2024), 12 vom: März, Seite 935-939 (DE-627)325573468 (DE-600)2037682-0 1573-8906 nnns volume:66 year:2024 number:12 month:03 pages:935-939 https://dx.doi.org/10.1007/s11018-024-02309-x X:SPRINGER Resolving-System lizenzpflichtig Volltext SYSFLAG_0 GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 50.21 VZ 33.00 VZ AR 66 2024 12 03 935-939 |
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10.1007/s11018-024-02309-x doi (DE-627)SPR056203799 (SPR)s11018-024-02309-x-e DE-627 ger DE-627 rakwb eng 620 VZ 50.21 bkl 33.00 bkl Minikhanov, T. Z. verfasserin (orcid)0000-0002-2246-9729 aut Phase modulation time dynamics of the liquid-crystal spatial light modulator 2024 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In this paper, liquid-crystal spatial light modulators are presented for precise dynamic manipulation of coherent light fields in space, which are used in diffractive optoelectronic and optical data processing systems. In addition, this paper presents the results of the temporal dynamics study of the HoloEye PLUTO‑2 VIS-016 liquid-crystal spatial light modulator for light field rate modulation analysis. Experiments using binary phase computer-generated holograms and binary focusing phase diffractive optical elements are performed. The time characteristics of the modulator response are determined from the experimental data. Displaying the diffraction structure model on the screen of the spatial light modulator results in a rise time of the diffraction efficiency of 146 ms, and switching to a new model leads to a decay time of 97 ms. The obtained results allow implementing the dynamic generation of an alternating diffraction field at 2 Hz update frequency with −16 dB interference level. Increasing the frequency of updating diffraction structure models increases the level of interframe noise in the generated diffraction field, and when updating with the frequency indicated in the specification, separating the generated distributions is virtually impossible. From the presented results, the studied modulator model can be applied for high-precision formation of complex diffraction fields with a frame update rate lower than stated. Determining the actual frame rate from the rise and decay times of diffraction efficiency allows correctly determining the minimum operating time of an information optical system with a liquid-crystal spatial light modulator. Computer-generated holography (dpeaa)DE-He213 Liquid-crystal spatial light modulator (dpeaa)DE-He213 Coherent optical diffractive processor (dpeaa)DE-He213 Diffractive optical neural networks (dpeaa)DE-He213 Diffractive optical element (dpeaa)DE-He213 Zlokazov, E. Yu. verfasserin (orcid)0000-0003-1340-7734 aut Starikov, R. S. verfasserin (orcid)0000-0002-7369-1565 aut Cheremkhin, P. A. verfasserin (orcid)0000-0003-3556-2663 aut Enthalten in Measurement techniques Springer US, 1958 66(2024), 12 vom: März, Seite 935-939 (DE-627)325573468 (DE-600)2037682-0 1573-8906 nnns volume:66 year:2024 number:12 month:03 pages:935-939 https://dx.doi.org/10.1007/s11018-024-02309-x X:SPRINGER Resolving-System lizenzpflichtig Volltext SYSFLAG_0 GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 50.21 VZ 33.00 VZ AR 66 2024 12 03 935-939 |
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Z.</subfield><subfield code="e">verfasserin</subfield><subfield code="0">(orcid)0000-0002-2246-9729</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Phase modulation time dynamics of the liquid-crystal spatial light modulator</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2024</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract In this paper, liquid-crystal spatial light modulators are presented for precise dynamic manipulation of coherent light fields in space, which are used in diffractive optoelectronic and optical data processing systems. In addition, this paper presents the results of the temporal dynamics study of the HoloEye PLUTO‑2 VIS-016 liquid-crystal spatial light modulator for light field rate modulation analysis. Experiments using binary phase computer-generated holograms and binary focusing phase diffractive optical elements are performed. The time characteristics of the modulator response are determined from the experimental data. Displaying the diffraction structure model on the screen of the spatial light modulator results in a rise time of the diffraction efficiency of 146 ms, and switching to a new model leads to a decay time of 97 ms. The obtained results allow implementing the dynamic generation of an alternating diffraction field at 2 Hz update frequency with −16 dB interference level. Increasing the frequency of updating diffraction structure models increases the level of interframe noise in the generated diffraction field, and when updating with the frequency indicated in the specification, separating the generated distributions is virtually impossible. From the presented results, the studied modulator model can be applied for high-precision formation of complex diffraction fields with a frame update rate lower than stated. 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Minikhanov, T. Z. |
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phase modulation time dynamics of the liquid-crystal spatial light modulator |
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Phase modulation time dynamics of the liquid-crystal spatial light modulator |
| abstract |
Abstract In this paper, liquid-crystal spatial light modulators are presented for precise dynamic manipulation of coherent light fields in space, which are used in diffractive optoelectronic and optical data processing systems. In addition, this paper presents the results of the temporal dynamics study of the HoloEye PLUTO‑2 VIS-016 liquid-crystal spatial light modulator for light field rate modulation analysis. Experiments using binary phase computer-generated holograms and binary focusing phase diffractive optical elements are performed. The time characteristics of the modulator response are determined from the experimental data. Displaying the diffraction structure model on the screen of the spatial light modulator results in a rise time of the diffraction efficiency of 146 ms, and switching to a new model leads to a decay time of 97 ms. The obtained results allow implementing the dynamic generation of an alternating diffraction field at 2 Hz update frequency with −16 dB interference level. Increasing the frequency of updating diffraction structure models increases the level of interframe noise in the generated diffraction field, and when updating with the frequency indicated in the specification, separating the generated distributions is virtually impossible. From the presented results, the studied modulator model can be applied for high-precision formation of complex diffraction fields with a frame update rate lower than stated. Determining the actual frame rate from the rise and decay times of diffraction efficiency allows correctly determining the minimum operating time of an information optical system with a liquid-crystal spatial light modulator. © Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
| abstractGer |
Abstract In this paper, liquid-crystal spatial light modulators are presented for precise dynamic manipulation of coherent light fields in space, which are used in diffractive optoelectronic and optical data processing systems. In addition, this paper presents the results of the temporal dynamics study of the HoloEye PLUTO‑2 VIS-016 liquid-crystal spatial light modulator for light field rate modulation analysis. Experiments using binary phase computer-generated holograms and binary focusing phase diffractive optical elements are performed. The time characteristics of the modulator response are determined from the experimental data. Displaying the diffraction structure model on the screen of the spatial light modulator results in a rise time of the diffraction efficiency of 146 ms, and switching to a new model leads to a decay time of 97 ms. The obtained results allow implementing the dynamic generation of an alternating diffraction field at 2 Hz update frequency with −16 dB interference level. Increasing the frequency of updating diffraction structure models increases the level of interframe noise in the generated diffraction field, and when updating with the frequency indicated in the specification, separating the generated distributions is virtually impossible. From the presented results, the studied modulator model can be applied for high-precision formation of complex diffraction fields with a frame update rate lower than stated. Determining the actual frame rate from the rise and decay times of diffraction efficiency allows correctly determining the minimum operating time of an information optical system with a liquid-crystal spatial light modulator. © Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
| abstract_unstemmed |
Abstract In this paper, liquid-crystal spatial light modulators are presented for precise dynamic manipulation of coherent light fields in space, which are used in diffractive optoelectronic and optical data processing systems. In addition, this paper presents the results of the temporal dynamics study of the HoloEye PLUTO‑2 VIS-016 liquid-crystal spatial light modulator for light field rate modulation analysis. Experiments using binary phase computer-generated holograms and binary focusing phase diffractive optical elements are performed. The time characteristics of the modulator response are determined from the experimental data. Displaying the diffraction structure model on the screen of the spatial light modulator results in a rise time of the diffraction efficiency of 146 ms, and switching to a new model leads to a decay time of 97 ms. The obtained results allow implementing the dynamic generation of an alternating diffraction field at 2 Hz update frequency with −16 dB interference level. Increasing the frequency of updating diffraction structure models increases the level of interframe noise in the generated diffraction field, and when updating with the frequency indicated in the specification, separating the generated distributions is virtually impossible. From the presented results, the studied modulator model can be applied for high-precision formation of complex diffraction fields with a frame update rate lower than stated. Determining the actual frame rate from the rise and decay times of diffraction efficiency allows correctly determining the minimum operating time of an information optical system with a liquid-crystal spatial light modulator. © Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
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Phase modulation time dynamics of the liquid-crystal spatial light modulator |
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| score |
7.4014626 |