Lasing modes of a microdisk with a ring gain area and of an active microring
Microcavity lasers shaped as thin circular disks are famous for the ultra-low thresholds of their whispering-gallery modes. We considered a two-dimensional model of such a laser in free space with a ring-like active region and compared the characteristics of its modes with the modes of an active mic...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Zolotukhina, Anna S [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2015 |
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| Rechteinformationen: |
Nutzungsrecht: © Springer Science+Business Media New York 2015 |
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| Schlagwörter: |
Computer Communication Networks |
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| Übergeordnetes Werk: |
Enthalten in: Optical and quantum electronics - Dordrecht : Kluwer, 1975, 47(2015), 12, Seite 3883-3891 |
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| Übergeordnetes Werk: |
volume:47 ; year:2015 ; number:12 ; pages:3883-3891 |
| Links: |
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| DOI / URN: |
10.1007/s11082-015-0240-0 |
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| Katalog-ID: |
OLC1963257324 |
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| 100 | 1 | |a Zolotukhina, Anna S |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Lasing modes of a microdisk with a ring gain area and of an active microring |
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| 520 | |a Microcavity lasers shaped as thin circular disks are famous for the ultra-low thresholds of their whispering-gallery modes. We considered a two-dimensional model of such a laser in free space with a ring-like active region and compared the characteristics of its modes with the modes of an active microring, i.e. a similar disk with a concentric hole. The comparison showed that a microring has considerable rarefaction effect in terms of emission thresholds, accompanied by the blue-shift of emission spectra. If the ring becomes narrower than a half-wavelength in material, then all lasing modes obtain catastrophically high thresholds. | ||
| 540 | |a Nutzungsrecht: © Springer Science+Business Media New York 2015 | ||
| 650 | 4 | |a Microdisk | |
| 650 | 4 | |a Physics | |
| 650 | 4 | |a Microring | |
| 650 | 4 | |a Computer Communication Networks | |
| 650 | 4 | |a Optics, Optoelectronics, Plasmonics and Optical Devices | |
| 650 | 4 | |a Lasing modes | |
| 650 | 4 | |a Electrical Engineering | |
| 650 | 4 | |a Lasers | |
| 650 | 4 | |a Threshold of lasing | |
| 650 | 4 | |a Laser resonators | |
| 650 | 4 | |a Characterization and Evaluation of Materials | |
| 700 | 1 | |a Spiridonov, Alexander O |4 oth | |
| 700 | 1 | |a Karchevskii, Evgenii M |4 oth | |
| 700 | 1 | |a Nosich, Alexander I |4 oth | |
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10.1007/s11082-015-0240-0 doi PQ20160430 (DE-627)OLC1963257324 (DE-599)GBVOLC1963257324 (PRQ)c1399-fb0f2d18e0590f74471014b6cb7193a469e44f79dce593e0ec9a0f6c7e60a6070 (KEY)0014969120150000047001203883lasingmodesofamicrodiskwitharinggainareaandofanact DE-627 ger DE-627 rakwb eng 500 620 DE-600 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 bkl Zolotukhina, Anna S verfasserin aut Lasing modes of a microdisk with a ring gain area and of an active microring 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Microcavity lasers shaped as thin circular disks are famous for the ultra-low thresholds of their whispering-gallery modes. We considered a two-dimensional model of such a laser in free space with a ring-like active region and compared the characteristics of its modes with the modes of an active microring, i.e. a similar disk with a concentric hole. The comparison showed that a microring has considerable rarefaction effect in terms of emission thresholds, accompanied by the blue-shift of emission spectra. If the ring becomes narrower than a half-wavelength in material, then all lasing modes obtain catastrophically high thresholds. Nutzungsrecht: © Springer Science+Business Media New York 2015 Microdisk Physics Microring Computer Communication Networks Optics, Optoelectronics, Plasmonics and Optical Devices Lasing modes Electrical Engineering Lasers Threshold of lasing Laser resonators Characterization and Evaluation of Materials Spiridonov, Alexander O oth Karchevskii, Evgenii M oth Nosich, Alexander I oth Enthalten in Optical and quantum electronics Dordrecht : Kluwer, 1975 47(2015), 12, Seite 3883-3891 (DE-627)129419540 (DE-600)189950-8 (DE-576)014796139 0306-8919 nnns volume:47 year:2015 number:12 pages:3883-3891 http://dx.doi.org/10.1007/s11082-015-0240-0 Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 GBV_ILN_150 33.38 AVZ 33.18 AVZ 33.23 AVZ 53.54 AVZ 52.88 AVZ 33.72 AVZ AR 47 2015 12 3883-3891 |
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10.1007/s11082-015-0240-0 doi PQ20160430 (DE-627)OLC1963257324 (DE-599)GBVOLC1963257324 (PRQ)c1399-fb0f2d18e0590f74471014b6cb7193a469e44f79dce593e0ec9a0f6c7e60a6070 (KEY)0014969120150000047001203883lasingmodesofamicrodiskwitharinggainareaandofanact DE-627 ger DE-627 rakwb eng 500 620 DE-600 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 bkl Zolotukhina, Anna S verfasserin aut Lasing modes of a microdisk with a ring gain area and of an active microring 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Microcavity lasers shaped as thin circular disks are famous for the ultra-low thresholds of their whispering-gallery modes. We considered a two-dimensional model of such a laser in free space with a ring-like active region and compared the characteristics of its modes with the modes of an active microring, i.e. a similar disk with a concentric hole. The comparison showed that a microring has considerable rarefaction effect in terms of emission thresholds, accompanied by the blue-shift of emission spectra. If the ring becomes narrower than a half-wavelength in material, then all lasing modes obtain catastrophically high thresholds. Nutzungsrecht: © Springer Science+Business Media New York 2015 Microdisk Physics Microring Computer Communication Networks Optics, Optoelectronics, Plasmonics and Optical Devices Lasing modes Electrical Engineering Lasers Threshold of lasing Laser resonators Characterization and Evaluation of Materials Spiridonov, Alexander O oth Karchevskii, Evgenii M oth Nosich, Alexander I oth Enthalten in Optical and quantum electronics Dordrecht : Kluwer, 1975 47(2015), 12, Seite 3883-3891 (DE-627)129419540 (DE-600)189950-8 (DE-576)014796139 0306-8919 nnns volume:47 year:2015 number:12 pages:3883-3891 http://dx.doi.org/10.1007/s11082-015-0240-0 Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 GBV_ILN_150 33.38 AVZ 33.18 AVZ 33.23 AVZ 53.54 AVZ 52.88 AVZ 33.72 AVZ AR 47 2015 12 3883-3891 |
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10.1007/s11082-015-0240-0 doi PQ20160430 (DE-627)OLC1963257324 (DE-599)GBVOLC1963257324 (PRQ)c1399-fb0f2d18e0590f74471014b6cb7193a469e44f79dce593e0ec9a0f6c7e60a6070 (KEY)0014969120150000047001203883lasingmodesofamicrodiskwitharinggainareaandofanact DE-627 ger DE-627 rakwb eng 500 620 DE-600 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 bkl Zolotukhina, Anna S verfasserin aut Lasing modes of a microdisk with a ring gain area and of an active microring 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Microcavity lasers shaped as thin circular disks are famous for the ultra-low thresholds of their whispering-gallery modes. We considered a two-dimensional model of such a laser in free space with a ring-like active region and compared the characteristics of its modes with the modes of an active microring, i.e. a similar disk with a concentric hole. The comparison showed that a microring has considerable rarefaction effect in terms of emission thresholds, accompanied by the blue-shift of emission spectra. If the ring becomes narrower than a half-wavelength in material, then all lasing modes obtain catastrophically high thresholds. Nutzungsrecht: © Springer Science+Business Media New York 2015 Microdisk Physics Microring Computer Communication Networks Optics, Optoelectronics, Plasmonics and Optical Devices Lasing modes Electrical Engineering Lasers Threshold of lasing Laser resonators Characterization and Evaluation of Materials Spiridonov, Alexander O oth Karchevskii, Evgenii M oth Nosich, Alexander I oth Enthalten in Optical and quantum electronics Dordrecht : Kluwer, 1975 47(2015), 12, Seite 3883-3891 (DE-627)129419540 (DE-600)189950-8 (DE-576)014796139 0306-8919 nnns volume:47 year:2015 number:12 pages:3883-3891 http://dx.doi.org/10.1007/s11082-015-0240-0 Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 GBV_ILN_150 33.38 AVZ 33.18 AVZ 33.23 AVZ 53.54 AVZ 52.88 AVZ 33.72 AVZ AR 47 2015 12 3883-3891 |
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10.1007/s11082-015-0240-0 doi PQ20160430 (DE-627)OLC1963257324 (DE-599)GBVOLC1963257324 (PRQ)c1399-fb0f2d18e0590f74471014b6cb7193a469e44f79dce593e0ec9a0f6c7e60a6070 (KEY)0014969120150000047001203883lasingmodesofamicrodiskwitharinggainareaandofanact DE-627 ger DE-627 rakwb eng 500 620 DE-600 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 bkl Zolotukhina, Anna S verfasserin aut Lasing modes of a microdisk with a ring gain area and of an active microring 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Microcavity lasers shaped as thin circular disks are famous for the ultra-low thresholds of their whispering-gallery modes. We considered a two-dimensional model of such a laser in free space with a ring-like active region and compared the characteristics of its modes with the modes of an active microring, i.e. a similar disk with a concentric hole. The comparison showed that a microring has considerable rarefaction effect in terms of emission thresholds, accompanied by the blue-shift of emission spectra. If the ring becomes narrower than a half-wavelength in material, then all lasing modes obtain catastrophically high thresholds. Nutzungsrecht: © Springer Science+Business Media New York 2015 Microdisk Physics Microring Computer Communication Networks Optics, Optoelectronics, Plasmonics and Optical Devices Lasing modes Electrical Engineering Lasers Threshold of lasing Laser resonators Characterization and Evaluation of Materials Spiridonov, Alexander O oth Karchevskii, Evgenii M oth Nosich, Alexander I oth Enthalten in Optical and quantum electronics Dordrecht : Kluwer, 1975 47(2015), 12, Seite 3883-3891 (DE-627)129419540 (DE-600)189950-8 (DE-576)014796139 0306-8919 nnns volume:47 year:2015 number:12 pages:3883-3891 http://dx.doi.org/10.1007/s11082-015-0240-0 Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 GBV_ILN_150 33.38 AVZ 33.18 AVZ 33.23 AVZ 53.54 AVZ 52.88 AVZ 33.72 AVZ AR 47 2015 12 3883-3891 |
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10.1007/s11082-015-0240-0 doi PQ20160430 (DE-627)OLC1963257324 (DE-599)GBVOLC1963257324 (PRQ)c1399-fb0f2d18e0590f74471014b6cb7193a469e44f79dce593e0ec9a0f6c7e60a6070 (KEY)0014969120150000047001203883lasingmodesofamicrodiskwitharinggainareaandofanact DE-627 ger DE-627 rakwb eng 500 620 DE-600 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 bkl Zolotukhina, Anna S verfasserin aut Lasing modes of a microdisk with a ring gain area and of an active microring 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Microcavity lasers shaped as thin circular disks are famous for the ultra-low thresholds of their whispering-gallery modes. We considered a two-dimensional model of such a laser in free space with a ring-like active region and compared the characteristics of its modes with the modes of an active microring, i.e. a similar disk with a concentric hole. The comparison showed that a microring has considerable rarefaction effect in terms of emission thresholds, accompanied by the blue-shift of emission spectra. If the ring becomes narrower than a half-wavelength in material, then all lasing modes obtain catastrophically high thresholds. Nutzungsrecht: © Springer Science+Business Media New York 2015 Microdisk Physics Microring Computer Communication Networks Optics, Optoelectronics, Plasmonics and Optical Devices Lasing modes Electrical Engineering Lasers Threshold of lasing Laser resonators Characterization and Evaluation of Materials Spiridonov, Alexander O oth Karchevskii, Evgenii M oth Nosich, Alexander I oth Enthalten in Optical and quantum electronics Dordrecht : Kluwer, 1975 47(2015), 12, Seite 3883-3891 (DE-627)129419540 (DE-600)189950-8 (DE-576)014796139 0306-8919 nnns volume:47 year:2015 number:12 pages:3883-3891 http://dx.doi.org/10.1007/s11082-015-0240-0 Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 GBV_ILN_150 33.38 AVZ 33.18 AVZ 33.23 AVZ 53.54 AVZ 52.88 AVZ 33.72 AVZ AR 47 2015 12 3883-3891 |
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Enthalten in Optical and quantum electronics 47(2015), 12, Seite 3883-3891 volume:47 year:2015 number:12 pages:3883-3891 |
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Enthalten in Optical and quantum electronics 47(2015), 12, Seite 3883-3891 volume:47 year:2015 number:12 pages:3883-3891 |
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Microdisk Physics Microring Computer Communication Networks Optics, Optoelectronics, Plasmonics and Optical Devices Lasing modes Electrical Engineering Lasers Threshold of lasing Laser resonators Characterization and Evaluation of Materials |
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Zolotukhina, Anna S @@aut@@ Spiridonov, Alexander O @@oth@@ Karchevskii, Evgenii M @@oth@@ Nosich, Alexander I @@oth@@ |
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lasing modes of a microdisk with a ring gain area and of an active microring |
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Lasing modes of a microdisk with a ring gain area and of an active microring |
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Microcavity lasers shaped as thin circular disks are famous for the ultra-low thresholds of their whispering-gallery modes. We considered a two-dimensional model of such a laser in free space with a ring-like active region and compared the characteristics of its modes with the modes of an active microring, i.e. a similar disk with a concentric hole. The comparison showed that a microring has considerable rarefaction effect in terms of emission thresholds, accompanied by the blue-shift of emission spectra. If the ring becomes narrower than a half-wavelength in material, then all lasing modes obtain catastrophically high thresholds. |
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Microcavity lasers shaped as thin circular disks are famous for the ultra-low thresholds of their whispering-gallery modes. We considered a two-dimensional model of such a laser in free space with a ring-like active region and compared the characteristics of its modes with the modes of an active microring, i.e. a similar disk with a concentric hole. The comparison showed that a microring has considerable rarefaction effect in terms of emission thresholds, accompanied by the blue-shift of emission spectra. If the ring becomes narrower than a half-wavelength in material, then all lasing modes obtain catastrophically high thresholds. |
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Microcavity lasers shaped as thin circular disks are famous for the ultra-low thresholds of their whispering-gallery modes. We considered a two-dimensional model of such a laser in free space with a ring-like active region and compared the characteristics of its modes with the modes of an active microring, i.e. a similar disk with a concentric hole. The comparison showed that a microring has considerable rarefaction effect in terms of emission thresholds, accompanied by the blue-shift of emission spectra. If the ring becomes narrower than a half-wavelength in material, then all lasing modes obtain catastrophically high thresholds. |
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Lasing modes of a microdisk with a ring gain area and of an active microring |
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