Polarization-independent nonreciprocal radiation in polar dielectric-Weyl semimetal planar heterostructure

The polarization-independent nonreciprocal radiation is highly demanded for controlling light-matter interactions in tailoring and enhancing radiative heat transfer. An obvious violation of Kirchhoff’s law and strong nonreciprocity ( η ) has been achieved in a form of...
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Gespeichert in:

Autor*in:	Li, Hongjing [verfasserIn] Zheng, Gaige [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2023

Schlagwörter:	Nonreciprocal radiation Weyl semimetal Polarization-independent Polar dielectric

Übergeordnetes Werk:	Enthalten in: Optics communications - Amsterdam, 1969, 550
Übergeordnetes Werk:	volume:550

DOI / URN:	10.1016/j.optcom.2023.130002

Katalog-ID:	ELV065275403

Internformat


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245	1	0	\|a Polarization-independent nonreciprocal radiation in polar dielectric-Weyl semimetal planar heterostructure
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520			\|a The polarization-independent nonreciprocal radiation is highly demanded for controlling light-matter interactions in tailoring and enhancing radiative heat transfer. An obvious violation of Kirchhoff’s law and strong nonreciprocity ( η ) has been achieved in a form of heterostructure composed of polar dielectric, Weyl semimetals (WSMs) and silver (Ag) substrate. By manipulating the structural parameters, a remarkable result of nonreciprocal radiation is realized under both transverse electric (TE) and transverse magnetic (TM) wave incidence. The peak value of η is 0.53 and 0.37 for TM and TE polarizations, respectively, at the resonance wavelength of 8.7 μ m . By changing the azimuthal angle of incidence, η spectra can be effectively manipulated. The distribution map of η is symmetrical with ϕ = 90 ° , and η = 0 for both TM and TE polarizations. Our results provide a much simpler way to prove the violation of Kirchhoff’s law and could lead to the advancement of high efficiency nonreciprocal thermal radiation.
650		4	\|a Nonreciprocal radiation
650		4	\|a Weyl semimetal
650		4	\|a Polarization-independent
650		4	\|a Polar dielectric
700	1		\|a Zheng, Gaige \|e verfasserin \|0 (orcid)0000-0002-7794-5534 \|4 aut
773	0	8	\|i Enthalten in \|t Optics communications \|d Amsterdam, 1969 \|g 550 \|h Online-Ressource \|w (DE-627)266889247 \|w (DE-600)1468811-6 \|w (DE-576)07596239X \|x 1873-0310 \|7 nnns
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bklnumber	33.18 33.38 50.37
publishDate	2023
allfields	10.1016/j.optcom.2023.130002 doi (DE-627)ELV065275403 (ELSEVIER)S0030-4018(23)00750-2 DE-627 ger DE-627 rda eng 530 VZ 33.18 bkl 33.38 bkl 50.37 bkl Li, Hongjing verfasserin aut Polarization-independent nonreciprocal radiation in polar dielectric-Weyl semimetal planar heterostructure 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The polarization-independent nonreciprocal radiation is highly demanded for controlling light-matter interactions in tailoring and enhancing radiative heat transfer. An obvious violation of Kirchhoff’s law and strong nonreciprocity ( η ) has been achieved in a form of heterostructure composed of polar dielectric, Weyl semimetals (WSMs) and silver (Ag) substrate. By manipulating the structural parameters, a remarkable result of nonreciprocal radiation is realized under both transverse electric (TE) and transverse magnetic (TM) wave incidence. The peak value of η is 0.53 and 0.37 for TM and TE polarizations, respectively, at the resonance wavelength of 8.7 μ m . By changing the azimuthal angle of incidence, η spectra can be effectively manipulated. The distribution map of η is symmetrical with ϕ = 90 ° , and η = 0 for both TM and TE polarizations. Our results provide a much simpler way to prove the violation of Kirchhoff’s law and could lead to the advancement of high efficiency nonreciprocal thermal radiation. Nonreciprocal radiation Weyl semimetal Polarization-independent Polar dielectric Zheng, Gaige verfasserin (orcid)0000-0002-7794-5534 aut Enthalten in Optics communications Amsterdam, 1969 550 Online-Ressource (DE-627)266889247 (DE-600)1468811-6 (DE-576)07596239X 1873-0310 nnns volume:550 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2007 GBV_ILN_2008 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 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_4338 GBV_ILN_4393 GBV_ILN_4700 33.18 Optik VZ 33.38 Quantenoptik nichtlineare Optik VZ 50.37 Technische Optik VZ AR 550
spelling	10.1016/j.optcom.2023.130002 doi (DE-627)ELV065275403 (ELSEVIER)S0030-4018(23)00750-2 DE-627 ger DE-627 rda eng 530 VZ 33.18 bkl 33.38 bkl 50.37 bkl Li, Hongjing verfasserin aut Polarization-independent nonreciprocal radiation in polar dielectric-Weyl semimetal planar heterostructure 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The polarization-independent nonreciprocal radiation is highly demanded for controlling light-matter interactions in tailoring and enhancing radiative heat transfer. An obvious violation of Kirchhoff’s law and strong nonreciprocity ( η ) has been achieved in a form of heterostructure composed of polar dielectric, Weyl semimetals (WSMs) and silver (Ag) substrate. By manipulating the structural parameters, a remarkable result of nonreciprocal radiation is realized under both transverse electric (TE) and transverse magnetic (TM) wave incidence. The peak value of η is 0.53 and 0.37 for TM and TE polarizations, respectively, at the resonance wavelength of 8.7 μ m . By changing the azimuthal angle of incidence, η spectra can be effectively manipulated. The distribution map of η is symmetrical with ϕ = 90 ° , and η = 0 for both TM and TE polarizations. Our results provide a much simpler way to prove the violation of Kirchhoff’s law and could lead to the advancement of high efficiency nonreciprocal thermal radiation. Nonreciprocal radiation Weyl semimetal Polarization-independent Polar dielectric Zheng, Gaige verfasserin (orcid)0000-0002-7794-5534 aut Enthalten in Optics communications Amsterdam, 1969 550 Online-Ressource (DE-627)266889247 (DE-600)1468811-6 (DE-576)07596239X 1873-0310 nnns volume:550 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2007 GBV_ILN_2008 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 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_4338 GBV_ILN_4393 GBV_ILN_4700 33.18 Optik VZ 33.38 Quantenoptik nichtlineare Optik VZ 50.37 Technische Optik VZ AR 550
allfields_unstemmed	10.1016/j.optcom.2023.130002 doi (DE-627)ELV065275403 (ELSEVIER)S0030-4018(23)00750-2 DE-627 ger DE-627 rda eng 530 VZ 33.18 bkl 33.38 bkl 50.37 bkl Li, Hongjing verfasserin aut Polarization-independent nonreciprocal radiation in polar dielectric-Weyl semimetal planar heterostructure 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The polarization-independent nonreciprocal radiation is highly demanded for controlling light-matter interactions in tailoring and enhancing radiative heat transfer. An obvious violation of Kirchhoff’s law and strong nonreciprocity ( η ) has been achieved in a form of heterostructure composed of polar dielectric, Weyl semimetals (WSMs) and silver (Ag) substrate. By manipulating the structural parameters, a remarkable result of nonreciprocal radiation is realized under both transverse electric (TE) and transverse magnetic (TM) wave incidence. The peak value of η is 0.53 and 0.37 for TM and TE polarizations, respectively, at the resonance wavelength of 8.7 μ m . By changing the azimuthal angle of incidence, η spectra can be effectively manipulated. The distribution map of η is symmetrical with ϕ = 90 ° , and η = 0 for both TM and TE polarizations. Our results provide a much simpler way to prove the violation of Kirchhoff’s law and could lead to the advancement of high efficiency nonreciprocal thermal radiation. Nonreciprocal radiation Weyl semimetal Polarization-independent Polar dielectric Zheng, Gaige verfasserin (orcid)0000-0002-7794-5534 aut Enthalten in Optics communications Amsterdam, 1969 550 Online-Ressource (DE-627)266889247 (DE-600)1468811-6 (DE-576)07596239X 1873-0310 nnns volume:550 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2007 GBV_ILN_2008 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 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_4338 GBV_ILN_4393 GBV_ILN_4700 33.18 Optik VZ 33.38 Quantenoptik nichtlineare Optik VZ 50.37 Technische Optik VZ AR 550
allfieldsGer	10.1016/j.optcom.2023.130002 doi (DE-627)ELV065275403 (ELSEVIER)S0030-4018(23)00750-2 DE-627 ger DE-627 rda eng 530 VZ 33.18 bkl 33.38 bkl 50.37 bkl Li, Hongjing verfasserin aut Polarization-independent nonreciprocal radiation in polar dielectric-Weyl semimetal planar heterostructure 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The polarization-independent nonreciprocal radiation is highly demanded for controlling light-matter interactions in tailoring and enhancing radiative heat transfer. An obvious violation of Kirchhoff’s law and strong nonreciprocity ( η ) has been achieved in a form of heterostructure composed of polar dielectric, Weyl semimetals (WSMs) and silver (Ag) substrate. By manipulating the structural parameters, a remarkable result of nonreciprocal radiation is realized under both transverse electric (TE) and transverse magnetic (TM) wave incidence. The peak value of η is 0.53 and 0.37 for TM and TE polarizations, respectively, at the resonance wavelength of 8.7 μ m . By changing the azimuthal angle of incidence, η spectra can be effectively manipulated. The distribution map of η is symmetrical with ϕ = 90 ° , and η = 0 for both TM and TE polarizations. Our results provide a much simpler way to prove the violation of Kirchhoff’s law and could lead to the advancement of high efficiency nonreciprocal thermal radiation. Nonreciprocal radiation Weyl semimetal Polarization-independent Polar dielectric Zheng, Gaige verfasserin (orcid)0000-0002-7794-5534 aut Enthalten in Optics communications Amsterdam, 1969 550 Online-Ressource (DE-627)266889247 (DE-600)1468811-6 (DE-576)07596239X 1873-0310 nnns volume:550 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2007 GBV_ILN_2008 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 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_4338 GBV_ILN_4393 GBV_ILN_4700 33.18 Optik VZ 33.38 Quantenoptik nichtlineare Optik VZ 50.37 Technische Optik VZ AR 550
allfieldsSound	10.1016/j.optcom.2023.130002 doi (DE-627)ELV065275403 (ELSEVIER)S0030-4018(23)00750-2 DE-627 ger DE-627 rda eng 530 VZ 33.18 bkl 33.38 bkl 50.37 bkl Li, Hongjing verfasserin aut Polarization-independent nonreciprocal radiation in polar dielectric-Weyl semimetal planar heterostructure 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The polarization-independent nonreciprocal radiation is highly demanded for controlling light-matter interactions in tailoring and enhancing radiative heat transfer. An obvious violation of Kirchhoff’s law and strong nonreciprocity ( η ) has been achieved in a form of heterostructure composed of polar dielectric, Weyl semimetals (WSMs) and silver (Ag) substrate. By manipulating the structural parameters, a remarkable result of nonreciprocal radiation is realized under both transverse electric (TE) and transverse magnetic (TM) wave incidence. The peak value of η is 0.53 and 0.37 for TM and TE polarizations, respectively, at the resonance wavelength of 8.7 μ m . By changing the azimuthal angle of incidence, η spectra can be effectively manipulated. The distribution map of η is symmetrical with ϕ = 90 ° , and η = 0 for both TM and TE polarizations. Our results provide a much simpler way to prove the violation of Kirchhoff’s law and could lead to the advancement of high efficiency nonreciprocal thermal radiation. Nonreciprocal radiation Weyl semimetal Polarization-independent Polar dielectric Zheng, Gaige verfasserin (orcid)0000-0002-7794-5534 aut Enthalten in Optics communications Amsterdam, 1969 550 Online-Ressource (DE-627)266889247 (DE-600)1468811-6 (DE-576)07596239X 1873-0310 nnns volume:550 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2007 GBV_ILN_2008 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 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_4338 GBV_ILN_4393 GBV_ILN_4700 33.18 Optik VZ 33.38 Quantenoptik nichtlineare Optik VZ 50.37 Technische Optik VZ AR 550
language	English
source	Enthalten in Optics communications 550 volume:550
sourceStr	Enthalten in Optics communications 550 volume:550
format_phy_str_mv	Article
bklname	Optik Quantenoptik nichtlineare Optik Technische Optik
institution	findex.gbv.de
topic_facet	Nonreciprocal radiation Weyl semimetal Polarization-independent Polar dielectric
dewey-raw	530
isfreeaccess_bool	false
container_title	Optics communications
authorswithroles_txt_mv	Li, Hongjing @@aut@@ Zheng, Gaige @@aut@@
publishDateDaySort_date	2023-01-01T00:00:00Z
hierarchy_top_id	266889247
dewey-sort	3530
id	ELV065275403
language_de	englisch
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author	Li, Hongjing
spellingShingle	Li, Hongjing ddc 530 bkl 33.18 bkl 33.38 bkl 50.37 misc Nonreciprocal radiation misc Weyl semimetal misc Polarization-independent misc Polar dielectric Polarization-independent nonreciprocal radiation in polar dielectric-Weyl semimetal planar heterostructure
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topic_title	530 VZ 33.18 bkl 33.38 bkl 50.37 bkl Polarization-independent nonreciprocal radiation in polar dielectric-Weyl semimetal planar heterostructure Nonreciprocal radiation Weyl semimetal Polarization-independent Polar dielectric
topic	ddc 530 bkl 33.18 bkl 33.38 bkl 50.37 misc Nonreciprocal radiation misc Weyl semimetal misc Polarization-independent misc Polar dielectric
topic_unstemmed	ddc 530 bkl 33.18 bkl 33.38 bkl 50.37 misc Nonreciprocal radiation misc Weyl semimetal misc Polarization-independent misc Polar dielectric
topic_browse	ddc 530 bkl 33.18 bkl 33.38 bkl 50.37 misc Nonreciprocal radiation misc Weyl semimetal misc Polarization-independent misc Polar dielectric
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title	Polarization-independent nonreciprocal radiation in polar dielectric-Weyl semimetal planar heterostructure
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title_full	Polarization-independent nonreciprocal radiation in polar dielectric-Weyl semimetal planar heterostructure
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title_sort	polarization-independent nonreciprocal radiation in polar dielectric-weyl semimetal planar heterostructure
title_auth	Polarization-independent nonreciprocal radiation in polar dielectric-Weyl semimetal planar heterostructure
abstract	The polarization-independent nonreciprocal radiation is highly demanded for controlling light-matter interactions in tailoring and enhancing radiative heat transfer. An obvious violation of Kirchhoff’s law and strong nonreciprocity ( η ) has been achieved in a form of heterostructure composed of polar dielectric, Weyl semimetals (WSMs) and silver (Ag) substrate. By manipulating the structural parameters, a remarkable result of nonreciprocal radiation is realized under both transverse electric (TE) and transverse magnetic (TM) wave incidence. The peak value of η is 0.53 and 0.37 for TM and TE polarizations, respectively, at the resonance wavelength of 8.7 μ m . By changing the azimuthal angle of incidence, η spectra can be effectively manipulated. The distribution map of η is symmetrical with ϕ = 90 ° , and η = 0 for both TM and TE polarizations. Our results provide a much simpler way to prove the violation of Kirchhoff’s law and could lead to the advancement of high efficiency nonreciprocal thermal radiation.
abstractGer	The polarization-independent nonreciprocal radiation is highly demanded for controlling light-matter interactions in tailoring and enhancing radiative heat transfer. An obvious violation of Kirchhoff’s law and strong nonreciprocity ( η ) has been achieved in a form of heterostructure composed of polar dielectric, Weyl semimetals (WSMs) and silver (Ag) substrate. By manipulating the structural parameters, a remarkable result of nonreciprocal radiation is realized under both transverse electric (TE) and transverse magnetic (TM) wave incidence. The peak value of η is 0.53 and 0.37 for TM and TE polarizations, respectively, at the resonance wavelength of 8.7 μ m . By changing the azimuthal angle of incidence, η spectra can be effectively manipulated. The distribution map of η is symmetrical with ϕ = 90 ° , and η = 0 for both TM and TE polarizations. Our results provide a much simpler way to prove the violation of Kirchhoff’s law and could lead to the advancement of high efficiency nonreciprocal thermal radiation.
abstract_unstemmed	The polarization-independent nonreciprocal radiation is highly demanded for controlling light-matter interactions in tailoring and enhancing radiative heat transfer. An obvious violation of Kirchhoff’s law and strong nonreciprocity ( η ) has been achieved in a form of heterostructure composed of polar dielectric, Weyl semimetals (WSMs) and silver (Ag) substrate. By manipulating the structural parameters, a remarkable result of nonreciprocal radiation is realized under both transverse electric (TE) and transverse magnetic (TM) wave incidence. The peak value of η is 0.53 and 0.37 for TM and TE polarizations, respectively, at the resonance wavelength of 8.7 μ m . By changing the azimuthal angle of incidence, η spectra can be effectively manipulated. The distribution map of η is symmetrical with ϕ = 90 ° , and η = 0 for both TM and TE polarizations. Our results provide a much simpler way to prove the violation of Kirchhoff’s law and could lead to the advancement of high efficiency nonreciprocal thermal radiation.
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title_short	Polarization-independent nonreciprocal radiation in polar dielectric-Weyl semimetal planar heterostructure
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doi_str	10.1016/j.optcom.2023.130002
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Polarization-independent nonreciprocal radiation in polar dielectric-Weyl semimetal planar heterostructure

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