Progress of magneto-optical ceramics

The magneto-optical effect (Faraday effect) was discovered in the middle of the 19th century. In the latter half of the 20th century, the practical use of isolators using single crystals (Faraday rotators) using the melt growth method began. One century after Faraday's discovery of the magneto-...
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Gespeichert in:

Autor*in:	Ikesue, A. [verfasserIn] Aung, Y.L. [verfasserIn] Wang, J. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2022

Schlagwörter:	Ceramics Isolator Magneto-optics Faraday Verdet constant Insertion loss Extinction Ratio Optical homogeneity Laser damage Paramagnetic Ferrimagnetic

Übergeordnetes Werk:	Enthalten in: Progress in quantum electronics - Amsterdam [u.a.] : Elsevier Science, 1969, 86
Übergeordnetes Werk:	volume:86

DOI / URN:	10.1016/j.pquantelec.2022.100416

Katalog-ID:	ELV008885192

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520			\|a The magneto-optical effect (Faraday effect) was discovered in the middle of the 19th century. In the latter half of the 20th century, the practical use of isolators using single crystals (Faraday rotators) using the melt growth method began. One century after Faraday's discovery of the magneto-optic effect, R.L. Coble proved translucency of polycrystalline ceramics. Ceramics may have many scattering sources due to their polycrystalline microstructure, and even from the viewpoint of scattering theory, it was considered impossible to apply them to the generation of coherent light (laser). However, 40 years later, A. Ikesue demonstrated laser ceramics for the first time with performance comparable to that of optical single crystal counterparts. The possibility of laser application of polycrystalline ceramics also makes it possible to apply it to Faraday rotators (optical isolators) that utilize coherence light. A magneto-optical single crystal composed of a single crystal orientation was considered to be superior in that it provided excellent optical performance and an accurate Faraday rotation angle. However, polycrystalline ceramics composed of random crystal orientations can not only provide accurate Faraday rotation angle but can also have a higher extinction ratio than single crystal isolators. A ceramic medium with extremely low scattering and extremely low insertion loss, which cannot be achieved with a single crystal material, has been developed. In addition, new materials, which have Verdet constants several times higher than those of main commercial crystal for isolator, have made it possible to reduce the size of isolator devices. However, these materials cannot be synthesized by the conventional melt-growth method. In the 21st century, polycrystalline ceramics are paradigms for Faraday rotating elements, and are about to enter a period of change from single crystals to polycrystalline ceramics.
650		4	\|a Ceramics
650		4	\|a Isolator
650		4	\|a Magneto-optics
650		4	\|a Faraday
650		4	\|a Verdet constant
650		4	\|a Insertion loss
650		4	\|a Extinction Ratio
650		4	\|a Optical homogeneity
650		4	\|a Laser damage
650		4	\|a Paramagnetic
650		4	\|a Ferrimagnetic
700	1		\|a Aung, Y.L. \|e verfasserin \|4 aut
700	1		\|a Wang, J. \|e verfasserin \|4 aut
773	0	8	\|i Enthalten in \|t Progress in quantum electronics \|d Amsterdam [u.a.] : Elsevier Science, 1969 \|g 86 \|h Online-Ressource \|w (DE-627)320405915 \|w (DE-600)2000674-3 \|w (DE-576)25526674X \|x 0079-6727 \|7 nnns
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936	b	k	\|a 33.23 \|j Quantenphysik
936	b	k	\|a 33.24 \|j Quantenfeldtheorie
936	b	k	\|a 33.38 \|j Quantenoptik \|j nichtlineare Optik
936	b	k	\|a 33.50 \|j Physik der Elementarteilchen und Felder: Allgemeines
936	b	k	\|a 33.72 \|j Halbleiterphysik
951			\|a AR
952			\|d 86

Indexfelder

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bklnumber	33.23 33.24 33.38 33.50 33.72
publishDate	2022
allfields	10.1016/j.pquantelec.2022.100416 doi (DE-627)ELV008885192 (ELSEVIER)S0079-6727(22)00041-6 DE-627 ger DE-627 rda eng 530 DE-600 33.23 bkl 33.24 bkl 33.38 bkl 33.50 bkl 33.72 bkl Ikesue, A. verfasserin aut Progress of magneto-optical ceramics 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The magneto-optical effect (Faraday effect) was discovered in the middle of the 19th century. In the latter half of the 20th century, the practical use of isolators using single crystals (Faraday rotators) using the melt growth method began. One century after Faraday's discovery of the magneto-optic effect, R.L. Coble proved translucency of polycrystalline ceramics. Ceramics may have many scattering sources due to their polycrystalline microstructure, and even from the viewpoint of scattering theory, it was considered impossible to apply them to the generation of coherent light (laser). However, 40 years later, A. Ikesue demonstrated laser ceramics for the first time with performance comparable to that of optical single crystal counterparts. The possibility of laser application of polycrystalline ceramics also makes it possible to apply it to Faraday rotators (optical isolators) that utilize coherence light. A magneto-optical single crystal composed of a single crystal orientation was considered to be superior in that it provided excellent optical performance and an accurate Faraday rotation angle. However, polycrystalline ceramics composed of random crystal orientations can not only provide accurate Faraday rotation angle but can also have a higher extinction ratio than single crystal isolators. A ceramic medium with extremely low scattering and extremely low insertion loss, which cannot be achieved with a single crystal material, has been developed. In addition, new materials, which have Verdet constants several times higher than those of main commercial crystal for isolator, have made it possible to reduce the size of isolator devices. However, these materials cannot be synthesized by the conventional melt-growth method. In the 21st century, polycrystalline ceramics are paradigms for Faraday rotating elements, and are about to enter a period of change from single crystals to polycrystalline ceramics. Ceramics Isolator Magneto-optics Faraday Verdet constant Insertion loss Extinction Ratio Optical homogeneity Laser damage Paramagnetic Ferrimagnetic Aung, Y.L. verfasserin aut Wang, J. verfasserin aut Enthalten in Progress in quantum electronics Amsterdam [u.a.] : Elsevier Science, 1969 86 Online-Ressource (DE-627)320405915 (DE-600)2000674-3 (DE-576)25526674X 0079-6727 nnns volume:86 GBV_USEFLAG_U SYSFLAG_U GBV_ELV 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_63 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_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.23 Quantenphysik 33.24 Quantenfeldtheorie 33.38 Quantenoptik nichtlineare Optik 33.50 Physik der Elementarteilchen und Felder: Allgemeines 33.72 Halbleiterphysik AR 86
spelling	10.1016/j.pquantelec.2022.100416 doi (DE-627)ELV008885192 (ELSEVIER)S0079-6727(22)00041-6 DE-627 ger DE-627 rda eng 530 DE-600 33.23 bkl 33.24 bkl 33.38 bkl 33.50 bkl 33.72 bkl Ikesue, A. verfasserin aut Progress of magneto-optical ceramics 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The magneto-optical effect (Faraday effect) was discovered in the middle of the 19th century. In the latter half of the 20th century, the practical use of isolators using single crystals (Faraday rotators) using the melt growth method began. One century after Faraday's discovery of the magneto-optic effect, R.L. Coble proved translucency of polycrystalline ceramics. Ceramics may have many scattering sources due to their polycrystalline microstructure, and even from the viewpoint of scattering theory, it was considered impossible to apply them to the generation of coherent light (laser). However, 40 years later, A. Ikesue demonstrated laser ceramics for the first time with performance comparable to that of optical single crystal counterparts. The possibility of laser application of polycrystalline ceramics also makes it possible to apply it to Faraday rotators (optical isolators) that utilize coherence light. A magneto-optical single crystal composed of a single crystal orientation was considered to be superior in that it provided excellent optical performance and an accurate Faraday rotation angle. However, polycrystalline ceramics composed of random crystal orientations can not only provide accurate Faraday rotation angle but can also have a higher extinction ratio than single crystal isolators. A ceramic medium with extremely low scattering and extremely low insertion loss, which cannot be achieved with a single crystal material, has been developed. In addition, new materials, which have Verdet constants several times higher than those of main commercial crystal for isolator, have made it possible to reduce the size of isolator devices. However, these materials cannot be synthesized by the conventional melt-growth method. In the 21st century, polycrystalline ceramics are paradigms for Faraday rotating elements, and are about to enter a period of change from single crystals to polycrystalline ceramics. Ceramics Isolator Magneto-optics Faraday Verdet constant Insertion loss Extinction Ratio Optical homogeneity Laser damage Paramagnetic Ferrimagnetic Aung, Y.L. verfasserin aut Wang, J. verfasserin aut Enthalten in Progress in quantum electronics Amsterdam [u.a.] : Elsevier Science, 1969 86 Online-Ressource (DE-627)320405915 (DE-600)2000674-3 (DE-576)25526674X 0079-6727 nnns volume:86 GBV_USEFLAG_U SYSFLAG_U GBV_ELV 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_63 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_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.23 Quantenphysik 33.24 Quantenfeldtheorie 33.38 Quantenoptik nichtlineare Optik 33.50 Physik der Elementarteilchen und Felder: Allgemeines 33.72 Halbleiterphysik AR 86
allfields_unstemmed	10.1016/j.pquantelec.2022.100416 doi (DE-627)ELV008885192 (ELSEVIER)S0079-6727(22)00041-6 DE-627 ger DE-627 rda eng 530 DE-600 33.23 bkl 33.24 bkl 33.38 bkl 33.50 bkl 33.72 bkl Ikesue, A. verfasserin aut Progress of magneto-optical ceramics 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The magneto-optical effect (Faraday effect) was discovered in the middle of the 19th century. In the latter half of the 20th century, the practical use of isolators using single crystals (Faraday rotators) using the melt growth method began. One century after Faraday's discovery of the magneto-optic effect, R.L. Coble proved translucency of polycrystalline ceramics. Ceramics may have many scattering sources due to their polycrystalline microstructure, and even from the viewpoint of scattering theory, it was considered impossible to apply them to the generation of coherent light (laser). However, 40 years later, A. Ikesue demonstrated laser ceramics for the first time with performance comparable to that of optical single crystal counterparts. The possibility of laser application of polycrystalline ceramics also makes it possible to apply it to Faraday rotators (optical isolators) that utilize coherence light. A magneto-optical single crystal composed of a single crystal orientation was considered to be superior in that it provided excellent optical performance and an accurate Faraday rotation angle. However, polycrystalline ceramics composed of random crystal orientations can not only provide accurate Faraday rotation angle but can also have a higher extinction ratio than single crystal isolators. A ceramic medium with extremely low scattering and extremely low insertion loss, which cannot be achieved with a single crystal material, has been developed. In addition, new materials, which have Verdet constants several times higher than those of main commercial crystal for isolator, have made it possible to reduce the size of isolator devices. However, these materials cannot be synthesized by the conventional melt-growth method. In the 21st century, polycrystalline ceramics are paradigms for Faraday rotating elements, and are about to enter a period of change from single crystals to polycrystalline ceramics. Ceramics Isolator Magneto-optics Faraday Verdet constant Insertion loss Extinction Ratio Optical homogeneity Laser damage Paramagnetic Ferrimagnetic Aung, Y.L. verfasserin aut Wang, J. verfasserin aut Enthalten in Progress in quantum electronics Amsterdam [u.a.] : Elsevier Science, 1969 86 Online-Ressource (DE-627)320405915 (DE-600)2000674-3 (DE-576)25526674X 0079-6727 nnns volume:86 GBV_USEFLAG_U SYSFLAG_U GBV_ELV 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_63 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_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.23 Quantenphysik 33.24 Quantenfeldtheorie 33.38 Quantenoptik nichtlineare Optik 33.50 Physik der Elementarteilchen und Felder: Allgemeines 33.72 Halbleiterphysik AR 86
allfieldsGer	10.1016/j.pquantelec.2022.100416 doi (DE-627)ELV008885192 (ELSEVIER)S0079-6727(22)00041-6 DE-627 ger DE-627 rda eng 530 DE-600 33.23 bkl 33.24 bkl 33.38 bkl 33.50 bkl 33.72 bkl Ikesue, A. verfasserin aut Progress of magneto-optical ceramics 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The magneto-optical effect (Faraday effect) was discovered in the middle of the 19th century. In the latter half of the 20th century, the practical use of isolators using single crystals (Faraday rotators) using the melt growth method began. One century after Faraday's discovery of the magneto-optic effect, R.L. Coble proved translucency of polycrystalline ceramics. Ceramics may have many scattering sources due to their polycrystalline microstructure, and even from the viewpoint of scattering theory, it was considered impossible to apply them to the generation of coherent light (laser). However, 40 years later, A. Ikesue demonstrated laser ceramics for the first time with performance comparable to that of optical single crystal counterparts. The possibility of laser application of polycrystalline ceramics also makes it possible to apply it to Faraday rotators (optical isolators) that utilize coherence light. A magneto-optical single crystal composed of a single crystal orientation was considered to be superior in that it provided excellent optical performance and an accurate Faraday rotation angle. However, polycrystalline ceramics composed of random crystal orientations can not only provide accurate Faraday rotation angle but can also have a higher extinction ratio than single crystal isolators. A ceramic medium with extremely low scattering and extremely low insertion loss, which cannot be achieved with a single crystal material, has been developed. In addition, new materials, which have Verdet constants several times higher than those of main commercial crystal for isolator, have made it possible to reduce the size of isolator devices. However, these materials cannot be synthesized by the conventional melt-growth method. In the 21st century, polycrystalline ceramics are paradigms for Faraday rotating elements, and are about to enter a period of change from single crystals to polycrystalline ceramics. Ceramics Isolator Magneto-optics Faraday Verdet constant Insertion loss Extinction Ratio Optical homogeneity Laser damage Paramagnetic Ferrimagnetic Aung, Y.L. verfasserin aut Wang, J. verfasserin aut Enthalten in Progress in quantum electronics Amsterdam [u.a.] : Elsevier Science, 1969 86 Online-Ressource (DE-627)320405915 (DE-600)2000674-3 (DE-576)25526674X 0079-6727 nnns volume:86 GBV_USEFLAG_U SYSFLAG_U GBV_ELV 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_63 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_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.23 Quantenphysik 33.24 Quantenfeldtheorie 33.38 Quantenoptik nichtlineare Optik 33.50 Physik der Elementarteilchen und Felder: Allgemeines 33.72 Halbleiterphysik AR 86
allfieldsSound	10.1016/j.pquantelec.2022.100416 doi (DE-627)ELV008885192 (ELSEVIER)S0079-6727(22)00041-6 DE-627 ger DE-627 rda eng 530 DE-600 33.23 bkl 33.24 bkl 33.38 bkl 33.50 bkl 33.72 bkl Ikesue, A. verfasserin aut Progress of magneto-optical ceramics 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The magneto-optical effect (Faraday effect) was discovered in the middle of the 19th century. In the latter half of the 20th century, the practical use of isolators using single crystals (Faraday rotators) using the melt growth method began. One century after Faraday's discovery of the magneto-optic effect, R.L. Coble proved translucency of polycrystalline ceramics. Ceramics may have many scattering sources due to their polycrystalline microstructure, and even from the viewpoint of scattering theory, it was considered impossible to apply them to the generation of coherent light (laser). However, 40 years later, A. Ikesue demonstrated laser ceramics for the first time with performance comparable to that of optical single crystal counterparts. The possibility of laser application of polycrystalline ceramics also makes it possible to apply it to Faraday rotators (optical isolators) that utilize coherence light. A magneto-optical single crystal composed of a single crystal orientation was considered to be superior in that it provided excellent optical performance and an accurate Faraday rotation angle. However, polycrystalline ceramics composed of random crystal orientations can not only provide accurate Faraday rotation angle but can also have a higher extinction ratio than single crystal isolators. A ceramic medium with extremely low scattering and extremely low insertion loss, which cannot be achieved with a single crystal material, has been developed. In addition, new materials, which have Verdet constants several times higher than those of main commercial crystal for isolator, have made it possible to reduce the size of isolator devices. However, these materials cannot be synthesized by the conventional melt-growth method. In the 21st century, polycrystalline ceramics are paradigms for Faraday rotating elements, and are about to enter a period of change from single crystals to polycrystalline ceramics. Ceramics Isolator Magneto-optics Faraday Verdet constant Insertion loss Extinction Ratio Optical homogeneity Laser damage Paramagnetic Ferrimagnetic Aung, Y.L. verfasserin aut Wang, J. verfasserin aut Enthalten in Progress in quantum electronics Amsterdam [u.a.] : Elsevier Science, 1969 86 Online-Ressource (DE-627)320405915 (DE-600)2000674-3 (DE-576)25526674X 0079-6727 nnns volume:86 GBV_USEFLAG_U SYSFLAG_U GBV_ELV 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_63 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_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.23 Quantenphysik 33.24 Quantenfeldtheorie 33.38 Quantenoptik nichtlineare Optik 33.50 Physik der Elementarteilchen und Felder: Allgemeines 33.72 Halbleiterphysik AR 86
language	English
source	Enthalten in Progress in quantum electronics 86 volume:86
sourceStr	Enthalten in Progress in quantum electronics 86 volume:86
format_phy_str_mv	Article
bklname	Quantenphysik Quantenfeldtheorie Quantenoptik nichtlineare Optik Physik der Elementarteilchen und Felder: Allgemeines Halbleiterphysik
institution	findex.gbv.de
topic_facet	Ceramics Isolator Magneto-optics Faraday Verdet constant Insertion loss Extinction Ratio Optical homogeneity Laser damage Paramagnetic Ferrimagnetic
dewey-raw	530
isfreeaccess_bool	false
container_title	Progress in quantum electronics
authorswithroles_txt_mv	Ikesue, A. @@aut@@ Aung, Y.L. @@aut@@ Wang, J. @@aut@@
publishDateDaySort_date	2022-01-01T00:00:00Z
hierarchy_top_id	320405915
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language_de	englisch
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author	Ikesue, A.
spellingShingle	Ikesue, A. ddc 530 bkl 33.23 bkl 33.24 bkl 33.38 bkl 33.50 bkl 33.72 misc Ceramics misc Isolator misc Magneto-optics misc Faraday misc Verdet constant misc Insertion loss misc Extinction Ratio misc Optical homogeneity misc Laser damage misc Paramagnetic misc Ferrimagnetic Progress of magneto-optical ceramics
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topic_title	530 DE-600 33.23 bkl 33.24 bkl 33.38 bkl 33.50 bkl 33.72 bkl Progress of magneto-optical ceramics Ceramics Isolator Magneto-optics Faraday Verdet constant Insertion loss Extinction Ratio Optical homogeneity Laser damage Paramagnetic Ferrimagnetic
topic	ddc 530 bkl 33.23 bkl 33.24 bkl 33.38 bkl 33.50 bkl 33.72 misc Ceramics misc Isolator misc Magneto-optics misc Faraday misc Verdet constant misc Insertion loss misc Extinction Ratio misc Optical homogeneity misc Laser damage misc Paramagnetic misc Ferrimagnetic
topic_unstemmed	ddc 530 bkl 33.23 bkl 33.24 bkl 33.38 bkl 33.50 bkl 33.72 misc Ceramics misc Isolator misc Magneto-optics misc Faraday misc Verdet constant misc Insertion loss misc Extinction Ratio misc Optical homogeneity misc Laser damage misc Paramagnetic misc Ferrimagnetic
topic_browse	ddc 530 bkl 33.23 bkl 33.24 bkl 33.38 bkl 33.50 bkl 33.72 misc Ceramics misc Isolator misc Magneto-optics misc Faraday misc Verdet constant misc Insertion loss misc Extinction Ratio misc Optical homogeneity misc Laser damage misc Paramagnetic misc Ferrimagnetic
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title	Progress of magneto-optical ceramics
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title_full	Progress of magneto-optical ceramics
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title_sort	progress of magneto-optical ceramics
title_auth	Progress of magneto-optical ceramics
abstract	The magneto-optical effect (Faraday effect) was discovered in the middle of the 19th century. In the latter half of the 20th century, the practical use of isolators using single crystals (Faraday rotators) using the melt growth method began. One century after Faraday's discovery of the magneto-optic effect, R.L. Coble proved translucency of polycrystalline ceramics. Ceramics may have many scattering sources due to their polycrystalline microstructure, and even from the viewpoint of scattering theory, it was considered impossible to apply them to the generation of coherent light (laser). However, 40 years later, A. Ikesue demonstrated laser ceramics for the first time with performance comparable to that of optical single crystal counterparts. The possibility of laser application of polycrystalline ceramics also makes it possible to apply it to Faraday rotators (optical isolators) that utilize coherence light. A magneto-optical single crystal composed of a single crystal orientation was considered to be superior in that it provided excellent optical performance and an accurate Faraday rotation angle. However, polycrystalline ceramics composed of random crystal orientations can not only provide accurate Faraday rotation angle but can also have a higher extinction ratio than single crystal isolators. A ceramic medium with extremely low scattering and extremely low insertion loss, which cannot be achieved with a single crystal material, has been developed. In addition, new materials, which have Verdet constants several times higher than those of main commercial crystal for isolator, have made it possible to reduce the size of isolator devices. However, these materials cannot be synthesized by the conventional melt-growth method. In the 21st century, polycrystalline ceramics are paradigms for Faraday rotating elements, and are about to enter a period of change from single crystals to polycrystalline ceramics.
abstractGer	The magneto-optical effect (Faraday effect) was discovered in the middle of the 19th century. In the latter half of the 20th century, the practical use of isolators using single crystals (Faraday rotators) using the melt growth method began. One century after Faraday's discovery of the magneto-optic effect, R.L. Coble proved translucency of polycrystalline ceramics. Ceramics may have many scattering sources due to their polycrystalline microstructure, and even from the viewpoint of scattering theory, it was considered impossible to apply them to the generation of coherent light (laser). However, 40 years later, A. Ikesue demonstrated laser ceramics for the first time with performance comparable to that of optical single crystal counterparts. The possibility of laser application of polycrystalline ceramics also makes it possible to apply it to Faraday rotators (optical isolators) that utilize coherence light. A magneto-optical single crystal composed of a single crystal orientation was considered to be superior in that it provided excellent optical performance and an accurate Faraday rotation angle. However, polycrystalline ceramics composed of random crystal orientations can not only provide accurate Faraday rotation angle but can also have a higher extinction ratio than single crystal isolators. A ceramic medium with extremely low scattering and extremely low insertion loss, which cannot be achieved with a single crystal material, has been developed. In addition, new materials, which have Verdet constants several times higher than those of main commercial crystal for isolator, have made it possible to reduce the size of isolator devices. However, these materials cannot be synthesized by the conventional melt-growth method. In the 21st century, polycrystalline ceramics are paradigms for Faraday rotating elements, and are about to enter a period of change from single crystals to polycrystalline ceramics.
abstract_unstemmed	The magneto-optical effect (Faraday effect) was discovered in the middle of the 19th century. In the latter half of the 20th century, the practical use of isolators using single crystals (Faraday rotators) using the melt growth method began. One century after Faraday's discovery of the magneto-optic effect, R.L. Coble proved translucency of polycrystalline ceramics. Ceramics may have many scattering sources due to their polycrystalline microstructure, and even from the viewpoint of scattering theory, it was considered impossible to apply them to the generation of coherent light (laser). However, 40 years later, A. Ikesue demonstrated laser ceramics for the first time with performance comparable to that of optical single crystal counterparts. The possibility of laser application of polycrystalline ceramics also makes it possible to apply it to Faraday rotators (optical isolators) that utilize coherence light. A magneto-optical single crystal composed of a single crystal orientation was considered to be superior in that it provided excellent optical performance and an accurate Faraday rotation angle. However, polycrystalline ceramics composed of random crystal orientations can not only provide accurate Faraday rotation angle but can also have a higher extinction ratio than single crystal isolators. A ceramic medium with extremely low scattering and extremely low insertion loss, which cannot be achieved with a single crystal material, has been developed. In addition, new materials, which have Verdet constants several times higher than those of main commercial crystal for isolator, have made it possible to reduce the size of isolator devices. However, these materials cannot be synthesized by the conventional melt-growth method. In the 21st century, polycrystalline ceramics are paradigms for Faraday rotating elements, and are about to enter a period of change from single crystals to polycrystalline ceramics.
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title_short	Progress of magneto-optical ceramics
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