Topological Silicon Photonics
The field of topological photonics has seen tremendous and wide‐ranging developments in recent years. Evolving from the broader field of topological insulators, topological photonics systems today harness a variety topological phases. These include the Su–Schreifer–Heeger, quantum Hall, quantum vall...
Ausführliche Beschreibung
Autor*in: |
Dawn T. H. Tan [verfasserIn] |
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E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2021 |
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Übergeordnetes Werk: |
In: Advanced Photonics Research - Wiley-VCH, 2021, 2(2021), 9, Seite n/a-n/a |
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Übergeordnetes Werk: |
volume:2 ; year:2021 ; number:9 ; pages:n/a-n/a |
Links: |
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DOI / URN: |
10.1002/adpr.202100010 |
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Katalog-ID: |
DOAJ062873741 |
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520 | |a The field of topological photonics has seen tremendous and wide‐ranging developments in recent years. Evolving from the broader field of topological insulators, topological photonics systems today harness a variety topological phases. These include the Su–Schreifer–Heeger, quantum Hall, quantum valley Hall and quantum spin Hall topologies. Importantly, the latter two generate edge states with opposite group velocities and opposite spin, respectively, allowing unidirectional light propagation and advanced photonic routing to occur. Amongst these exciting developments is a subset of advancements made in topological silicon photonics, which could potentially lend its appeal to complementary metal–oxide–semiconductor (CMOS) photonics applications, including telecommunications, data communications, quantum photonics, future exascale supercomputers, photonic neuromorphic computing, and infrared sensing. The fundamental underpinnings of these topological phases lead to interesting features, including chirality, scatter‐free light propagation around sharp bends, and importantly topological protection against defects, disorder, and scattering. This topological protection may be harnessed toward tunable light propagation, photon‐pair generation, quantum spatial entanglement, robust photonic routing, and beyond. Herein, the recent advancements made in the burgeoning field of topological silicon photonics are discussed. | ||
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10.1002/adpr.202100010 doi (DE-627)DOAJ062873741 (DE-599)DOAJ6daca1feac444139b7fb69b5816141b8 DE-627 ger DE-627 rakwb eng TA1501-1820 QC350-467 Dawn T. H. Tan verfasserin aut Topological Silicon Photonics 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The field of topological photonics has seen tremendous and wide‐ranging developments in recent years. Evolving from the broader field of topological insulators, topological photonics systems today harness a variety topological phases. These include the Su–Schreifer–Heeger, quantum Hall, quantum valley Hall and quantum spin Hall topologies. Importantly, the latter two generate edge states with opposite group velocities and opposite spin, respectively, allowing unidirectional light propagation and advanced photonic routing to occur. Amongst these exciting developments is a subset of advancements made in topological silicon photonics, which could potentially lend its appeal to complementary metal–oxide–semiconductor (CMOS) photonics applications, including telecommunications, data communications, quantum photonics, future exascale supercomputers, photonic neuromorphic computing, and infrared sensing. The fundamental underpinnings of these topological phases lead to interesting features, including chirality, scatter‐free light propagation around sharp bends, and importantly topological protection against defects, disorder, and scattering. This topological protection may be harnessed toward tunable light propagation, photon‐pair generation, quantum spatial entanglement, robust photonic routing, and beyond. Herein, the recent advancements made in the burgeoning field of topological silicon photonics are discussed. quantum spin Hall quantum valley Hall silicon photonics Su–Schrieffer–Heeger topological photonics topological silicon photonics Applied optics. Photonics Optics. Light In Advanced Photonics Research Wiley-VCH, 2021 2(2021), 9, Seite n/a-n/a (DE-627)1691163821 (DE-600)3009932-8 26999293 nnns volume:2 year:2021 number:9 pages:n/a-n/a https://doi.org/10.1002/adpr.202100010 kostenfrei https://doaj.org/article/6daca1feac444139b7fb69b5816141b8 kostenfrei https://doi.org/10.1002/adpr.202100010 kostenfrei https://doaj.org/toc/2699-9293 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 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_2068 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2 2021 9 n/a-n/a |
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10.1002/adpr.202100010 doi (DE-627)DOAJ062873741 (DE-599)DOAJ6daca1feac444139b7fb69b5816141b8 DE-627 ger DE-627 rakwb eng TA1501-1820 QC350-467 Dawn T. H. Tan verfasserin aut Topological Silicon Photonics 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The field of topological photonics has seen tremendous and wide‐ranging developments in recent years. Evolving from the broader field of topological insulators, topological photonics systems today harness a variety topological phases. These include the Su–Schreifer–Heeger, quantum Hall, quantum valley Hall and quantum spin Hall topologies. Importantly, the latter two generate edge states with opposite group velocities and opposite spin, respectively, allowing unidirectional light propagation and advanced photonic routing to occur. Amongst these exciting developments is a subset of advancements made in topological silicon photonics, which could potentially lend its appeal to complementary metal–oxide–semiconductor (CMOS) photonics applications, including telecommunications, data communications, quantum photonics, future exascale supercomputers, photonic neuromorphic computing, and infrared sensing. The fundamental underpinnings of these topological phases lead to interesting features, including chirality, scatter‐free light propagation around sharp bends, and importantly topological protection against defects, disorder, and scattering. This topological protection may be harnessed toward tunable light propagation, photon‐pair generation, quantum spatial entanglement, robust photonic routing, and beyond. Herein, the recent advancements made in the burgeoning field of topological silicon photonics are discussed. quantum spin Hall quantum valley Hall silicon photonics Su–Schrieffer–Heeger topological photonics topological silicon photonics Applied optics. Photonics Optics. Light In Advanced Photonics Research Wiley-VCH, 2021 2(2021), 9, Seite n/a-n/a (DE-627)1691163821 (DE-600)3009932-8 26999293 nnns volume:2 year:2021 number:9 pages:n/a-n/a https://doi.org/10.1002/adpr.202100010 kostenfrei https://doaj.org/article/6daca1feac444139b7fb69b5816141b8 kostenfrei https://doi.org/10.1002/adpr.202100010 kostenfrei https://doaj.org/toc/2699-9293 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 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_2068 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2 2021 9 n/a-n/a |
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10.1002/adpr.202100010 doi (DE-627)DOAJ062873741 (DE-599)DOAJ6daca1feac444139b7fb69b5816141b8 DE-627 ger DE-627 rakwb eng TA1501-1820 QC350-467 Dawn T. H. Tan verfasserin aut Topological Silicon Photonics 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The field of topological photonics has seen tremendous and wide‐ranging developments in recent years. Evolving from the broader field of topological insulators, topological photonics systems today harness a variety topological phases. These include the Su–Schreifer–Heeger, quantum Hall, quantum valley Hall and quantum spin Hall topologies. Importantly, the latter two generate edge states with opposite group velocities and opposite spin, respectively, allowing unidirectional light propagation and advanced photonic routing to occur. Amongst these exciting developments is a subset of advancements made in topological silicon photonics, which could potentially lend its appeal to complementary metal–oxide–semiconductor (CMOS) photonics applications, including telecommunications, data communications, quantum photonics, future exascale supercomputers, photonic neuromorphic computing, and infrared sensing. The fundamental underpinnings of these topological phases lead to interesting features, including chirality, scatter‐free light propagation around sharp bends, and importantly topological protection against defects, disorder, and scattering. This topological protection may be harnessed toward tunable light propagation, photon‐pair generation, quantum spatial entanglement, robust photonic routing, and beyond. Herein, the recent advancements made in the burgeoning field of topological silicon photonics are discussed. quantum spin Hall quantum valley Hall silicon photonics Su–Schrieffer–Heeger topological photonics topological silicon photonics Applied optics. Photonics Optics. Light In Advanced Photonics Research Wiley-VCH, 2021 2(2021), 9, Seite n/a-n/a (DE-627)1691163821 (DE-600)3009932-8 26999293 nnns volume:2 year:2021 number:9 pages:n/a-n/a https://doi.org/10.1002/adpr.202100010 kostenfrei https://doaj.org/article/6daca1feac444139b7fb69b5816141b8 kostenfrei https://doi.org/10.1002/adpr.202100010 kostenfrei https://doaj.org/toc/2699-9293 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 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_2068 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2 2021 9 n/a-n/a |
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10.1002/adpr.202100010 doi (DE-627)DOAJ062873741 (DE-599)DOAJ6daca1feac444139b7fb69b5816141b8 DE-627 ger DE-627 rakwb eng TA1501-1820 QC350-467 Dawn T. H. Tan verfasserin aut Topological Silicon Photonics 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The field of topological photonics has seen tremendous and wide‐ranging developments in recent years. Evolving from the broader field of topological insulators, topological photonics systems today harness a variety topological phases. These include the Su–Schreifer–Heeger, quantum Hall, quantum valley Hall and quantum spin Hall topologies. Importantly, the latter two generate edge states with opposite group velocities and opposite spin, respectively, allowing unidirectional light propagation and advanced photonic routing to occur. Amongst these exciting developments is a subset of advancements made in topological silicon photonics, which could potentially lend its appeal to complementary metal–oxide–semiconductor (CMOS) photonics applications, including telecommunications, data communications, quantum photonics, future exascale supercomputers, photonic neuromorphic computing, and infrared sensing. The fundamental underpinnings of these topological phases lead to interesting features, including chirality, scatter‐free light propagation around sharp bends, and importantly topological protection against defects, disorder, and scattering. This topological protection may be harnessed toward tunable light propagation, photon‐pair generation, quantum spatial entanglement, robust photonic routing, and beyond. Herein, the recent advancements made in the burgeoning field of topological silicon photonics are discussed. quantum spin Hall quantum valley Hall silicon photonics Su–Schrieffer–Heeger topological photonics topological silicon photonics Applied optics. Photonics Optics. Light In Advanced Photonics Research Wiley-VCH, 2021 2(2021), 9, Seite n/a-n/a (DE-627)1691163821 (DE-600)3009932-8 26999293 nnns volume:2 year:2021 number:9 pages:n/a-n/a https://doi.org/10.1002/adpr.202100010 kostenfrei https://doaj.org/article/6daca1feac444139b7fb69b5816141b8 kostenfrei https://doi.org/10.1002/adpr.202100010 kostenfrei https://doaj.org/toc/2699-9293 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 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_2068 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2 2021 9 n/a-n/a |
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10.1002/adpr.202100010 doi (DE-627)DOAJ062873741 (DE-599)DOAJ6daca1feac444139b7fb69b5816141b8 DE-627 ger DE-627 rakwb eng TA1501-1820 QC350-467 Dawn T. H. Tan verfasserin aut Topological Silicon Photonics 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The field of topological photonics has seen tremendous and wide‐ranging developments in recent years. Evolving from the broader field of topological insulators, topological photonics systems today harness a variety topological phases. These include the Su–Schreifer–Heeger, quantum Hall, quantum valley Hall and quantum spin Hall topologies. Importantly, the latter two generate edge states with opposite group velocities and opposite spin, respectively, allowing unidirectional light propagation and advanced photonic routing to occur. Amongst these exciting developments is a subset of advancements made in topological silicon photonics, which could potentially lend its appeal to complementary metal–oxide–semiconductor (CMOS) photonics applications, including telecommunications, data communications, quantum photonics, future exascale supercomputers, photonic neuromorphic computing, and infrared sensing. The fundamental underpinnings of these topological phases lead to interesting features, including chirality, scatter‐free light propagation around sharp bends, and importantly topological protection against defects, disorder, and scattering. This topological protection may be harnessed toward tunable light propagation, photon‐pair generation, quantum spatial entanglement, robust photonic routing, and beyond. Herein, the recent advancements made in the burgeoning field of topological silicon photonics are discussed. quantum spin Hall quantum valley Hall silicon photonics Su–Schrieffer–Heeger topological photonics topological silicon photonics Applied optics. Photonics Optics. Light In Advanced Photonics Research Wiley-VCH, 2021 2(2021), 9, Seite n/a-n/a (DE-627)1691163821 (DE-600)3009932-8 26999293 nnns volume:2 year:2021 number:9 pages:n/a-n/a https://doi.org/10.1002/adpr.202100010 kostenfrei https://doaj.org/article/6daca1feac444139b7fb69b5816141b8 kostenfrei https://doi.org/10.1002/adpr.202100010 kostenfrei https://doaj.org/toc/2699-9293 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 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_2068 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2 2021 9 n/a-n/a |
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The field of topological photonics has seen tremendous and wide‐ranging developments in recent years. Evolving from the broader field of topological insulators, topological photonics systems today harness a variety topological phases. These include the Su–Schreifer–Heeger, quantum Hall, quantum valley Hall and quantum spin Hall topologies. Importantly, the latter two generate edge states with opposite group velocities and opposite spin, respectively, allowing unidirectional light propagation and advanced photonic routing to occur. Amongst these exciting developments is a subset of advancements made in topological silicon photonics, which could potentially lend its appeal to complementary metal–oxide–semiconductor (CMOS) photonics applications, including telecommunications, data communications, quantum photonics, future exascale supercomputers, photonic neuromorphic computing, and infrared sensing. The fundamental underpinnings of these topological phases lead to interesting features, including chirality, scatter‐free light propagation around sharp bends, and importantly topological protection against defects, disorder, and scattering. This topological protection may be harnessed toward tunable light propagation, photon‐pair generation, quantum spatial entanglement, robust photonic routing, and beyond. Herein, the recent advancements made in the burgeoning field of topological silicon photonics are discussed. |
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The field of topological photonics has seen tremendous and wide‐ranging developments in recent years. Evolving from the broader field of topological insulators, topological photonics systems today harness a variety topological phases. These include the Su–Schreifer–Heeger, quantum Hall, quantum valley Hall and quantum spin Hall topologies. Importantly, the latter two generate edge states with opposite group velocities and opposite spin, respectively, allowing unidirectional light propagation and advanced photonic routing to occur. Amongst these exciting developments is a subset of advancements made in topological silicon photonics, which could potentially lend its appeal to complementary metal–oxide–semiconductor (CMOS) photonics applications, including telecommunications, data communications, quantum photonics, future exascale supercomputers, photonic neuromorphic computing, and infrared sensing. The fundamental underpinnings of these topological phases lead to interesting features, including chirality, scatter‐free light propagation around sharp bends, and importantly topological protection against defects, disorder, and scattering. This topological protection may be harnessed toward tunable light propagation, photon‐pair generation, quantum spatial entanglement, robust photonic routing, and beyond. Herein, the recent advancements made in the burgeoning field of topological silicon photonics are discussed. |
abstract_unstemmed |
The field of topological photonics has seen tremendous and wide‐ranging developments in recent years. Evolving from the broader field of topological insulators, topological photonics systems today harness a variety topological phases. These include the Su–Schreifer–Heeger, quantum Hall, quantum valley Hall and quantum spin Hall topologies. Importantly, the latter two generate edge states with opposite group velocities and opposite spin, respectively, allowing unidirectional light propagation and advanced photonic routing to occur. Amongst these exciting developments is a subset of advancements made in topological silicon photonics, which could potentially lend its appeal to complementary metal–oxide–semiconductor (CMOS) photonics applications, including telecommunications, data communications, quantum photonics, future exascale supercomputers, photonic neuromorphic computing, and infrared sensing. The fundamental underpinnings of these topological phases lead to interesting features, including chirality, scatter‐free light propagation around sharp bends, and importantly topological protection against defects, disorder, and scattering. This topological protection may be harnessed toward tunable light propagation, photon‐pair generation, quantum spatial entanglement, robust photonic routing, and beyond. Herein, the recent advancements made in the burgeoning field of topological silicon photonics are discussed. |
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