Thermal, quantum antibunching and lasing thresholds from single emitters to macroscopic devices
Starting from a fully quantized Hamiltonian for an ensemble of identical emitters coupled to the modes of an optical cavity, we determine analytically regimes of thermal, collective anti-bunching and laser emission that depend explicitly on the number of emitters. The lasing regime is reached for a...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Carroll, Mark Anthony [verfasserIn] D'Alessandro, Giampaolo [verfasserIn] Lippi, Gian Luca [verfasserIn] Oppo, Gian-Luca [verfasserIn] Papoff, Francesco [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2021 |
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| Ausgabe: |
Published 10 February 2021 |
| Anmerkung: |
Last seen: 23.03.2022 |
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| Übergeordnetes Werk: |
Enthalten in: Physical review letters - College Park, Md. : APS, 1958, Volume 126(2021), Issue 6, Article 063902 |
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| Übergeordnetes Werk: |
volume:126 ; year:2021 ; number:6 ; elocationid:063902 |
| Links: |
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| DOI / URN: |
10.1103/PhysRevLett.126.063902 |
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| Katalog-ID: |
1796376221 |
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| 520 | |a Starting from a fully quantized Hamiltonian for an ensemble of identical emitters coupled to the modes of an optical cavity, we determine analytically regimes of thermal, collective anti-bunching and laser emission that depend explicitly on the number of emitters. The lasing regime is reached for a number of emitters above a critical number-which depends on the light-matter coupling, detuning, and the dissipation rates-via a universal transition from thermal emission to collective anti-bunching to lasing as the pump increases. Cases where the second order intensity correlation fails to predict laser action are also presented. | ||
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10.1103/PhysRevLett.126.063902 doi (DE-627)1796376221 (DE-599)KXP1796376221 DE-627 ger DE-627 rda eng Carroll, Mark Anthony verfasserin (DE-588)1253955514 (DE-627)1796376981 aut Thermal, quantum antibunching and lasing thresholds from single emitters to macroscopic devices Published 10 February 2021 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Last seen: 23.03.2022 Starting from a fully quantized Hamiltonian for an ensemble of identical emitters coupled to the modes of an optical cavity, we determine analytically regimes of thermal, collective anti-bunching and laser emission that depend explicitly on the number of emitters. The lasing regime is reached for a number of emitters above a critical number-which depends on the light-matter coupling, detuning, and the dissipation rates-via a universal transition from thermal emission to collective anti-bunching to lasing as the pump increases. Cases where the second order intensity correlation fails to predict laser action are also presented. D'Alessandro, Giampaolo verfasserin (DE-588)1249695236 (DE-627)1786229307 aut Lippi, Gian Luca verfasserin (DE-588)1253955816 (DE-627)1796377473 aut Oppo, Gian-Luca verfasserin (DE-588)125395593X (DE-627)1796377716 aut Papoff, Francesco verfasserin (DE-588)125395612X (DE-627)1796378089 aut Enthalten in Physical review letters College Park, Md. : APS, 1958 Volume 126(2021), Issue 6, Article 063902 Online-Ressource (DE-627)268756899 (DE-600)1472655-5 (DE-576)077609441 1079-7114 nnns volume:126 year:2021 number:6 elocationid:063902 https://doi.org/10.1103/PhysRevLett.126.063902 Resolving-System Full Text at Publisher lizenzpflichtig GBV_USEFLAG_U GBV_ILN_2088 ISIL_DE-Frei3c SYSFLAG_1 GBV_KXP GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_266 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2027 GBV_ILN_2110 GBV_ILN_2190 GBV_ILN_2336 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_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 126 2021 6 063902 Volume 126(2021), Issue 6, Article 063902 2088 01 DE-Frei3c 4098085674 00 --%%-- APS --%%-- n APS Funding text: G. D. and F. P. wish to thank the Mathematisches Forschungsinstitut Oberwolfach for support. l01 23-03-22 2088 01 DE-Frei3c APS |
| spelling |
10.1103/PhysRevLett.126.063902 doi (DE-627)1796376221 (DE-599)KXP1796376221 DE-627 ger DE-627 rda eng Carroll, Mark Anthony verfasserin (DE-588)1253955514 (DE-627)1796376981 aut Thermal, quantum antibunching and lasing thresholds from single emitters to macroscopic devices Published 10 February 2021 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Last seen: 23.03.2022 Starting from a fully quantized Hamiltonian for an ensemble of identical emitters coupled to the modes of an optical cavity, we determine analytically regimes of thermal, collective anti-bunching and laser emission that depend explicitly on the number of emitters. The lasing regime is reached for a number of emitters above a critical number-which depends on the light-matter coupling, detuning, and the dissipation rates-via a universal transition from thermal emission to collective anti-bunching to lasing as the pump increases. Cases where the second order intensity correlation fails to predict laser action are also presented. D'Alessandro, Giampaolo verfasserin (DE-588)1249695236 (DE-627)1786229307 aut Lippi, Gian Luca verfasserin (DE-588)1253955816 (DE-627)1796377473 aut Oppo, Gian-Luca verfasserin (DE-588)125395593X (DE-627)1796377716 aut Papoff, Francesco verfasserin (DE-588)125395612X (DE-627)1796378089 aut Enthalten in Physical review letters College Park, Md. : APS, 1958 Volume 126(2021), Issue 6, Article 063902 Online-Ressource (DE-627)268756899 (DE-600)1472655-5 (DE-576)077609441 1079-7114 nnns volume:126 year:2021 number:6 elocationid:063902 https://doi.org/10.1103/PhysRevLett.126.063902 Resolving-System Full Text at Publisher lizenzpflichtig GBV_USEFLAG_U GBV_ILN_2088 ISIL_DE-Frei3c SYSFLAG_1 GBV_KXP GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_266 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2027 GBV_ILN_2110 GBV_ILN_2190 GBV_ILN_2336 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_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 126 2021 6 063902 Volume 126(2021), Issue 6, Article 063902 2088 01 DE-Frei3c 4098085674 00 --%%-- APS --%%-- n APS Funding text: G. D. and F. P. wish to thank the Mathematisches Forschungsinstitut Oberwolfach for support. l01 23-03-22 2088 01 DE-Frei3c APS |
| allfields_unstemmed |
10.1103/PhysRevLett.126.063902 doi (DE-627)1796376221 (DE-599)KXP1796376221 DE-627 ger DE-627 rda eng Carroll, Mark Anthony verfasserin (DE-588)1253955514 (DE-627)1796376981 aut Thermal, quantum antibunching and lasing thresholds from single emitters to macroscopic devices Published 10 February 2021 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Last seen: 23.03.2022 Starting from a fully quantized Hamiltonian for an ensemble of identical emitters coupled to the modes of an optical cavity, we determine analytically regimes of thermal, collective anti-bunching and laser emission that depend explicitly on the number of emitters. The lasing regime is reached for a number of emitters above a critical number-which depends on the light-matter coupling, detuning, and the dissipation rates-via a universal transition from thermal emission to collective anti-bunching to lasing as the pump increases. Cases where the second order intensity correlation fails to predict laser action are also presented. D'Alessandro, Giampaolo verfasserin (DE-588)1249695236 (DE-627)1786229307 aut Lippi, Gian Luca verfasserin (DE-588)1253955816 (DE-627)1796377473 aut Oppo, Gian-Luca verfasserin (DE-588)125395593X (DE-627)1796377716 aut Papoff, Francesco verfasserin (DE-588)125395612X (DE-627)1796378089 aut Enthalten in Physical review letters College Park, Md. : APS, 1958 Volume 126(2021), Issue 6, Article 063902 Online-Ressource (DE-627)268756899 (DE-600)1472655-5 (DE-576)077609441 1079-7114 nnns volume:126 year:2021 number:6 elocationid:063902 https://doi.org/10.1103/PhysRevLett.126.063902 Resolving-System Full Text at Publisher lizenzpflichtig GBV_USEFLAG_U GBV_ILN_2088 ISIL_DE-Frei3c SYSFLAG_1 GBV_KXP GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_266 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2027 GBV_ILN_2110 GBV_ILN_2190 GBV_ILN_2336 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_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 126 2021 6 063902 Volume 126(2021), Issue 6, Article 063902 2088 01 DE-Frei3c 4098085674 00 --%%-- APS --%%-- n APS Funding text: G. D. and F. P. wish to thank the Mathematisches Forschungsinstitut Oberwolfach for support. l01 23-03-22 2088 01 DE-Frei3c APS |
| allfieldsGer |
10.1103/PhysRevLett.126.063902 doi (DE-627)1796376221 (DE-599)KXP1796376221 DE-627 ger DE-627 rda eng Carroll, Mark Anthony verfasserin (DE-588)1253955514 (DE-627)1796376981 aut Thermal, quantum antibunching and lasing thresholds from single emitters to macroscopic devices Published 10 February 2021 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Last seen: 23.03.2022 Starting from a fully quantized Hamiltonian for an ensemble of identical emitters coupled to the modes of an optical cavity, we determine analytically regimes of thermal, collective anti-bunching and laser emission that depend explicitly on the number of emitters. The lasing regime is reached for a number of emitters above a critical number-which depends on the light-matter coupling, detuning, and the dissipation rates-via a universal transition from thermal emission to collective anti-bunching to lasing as the pump increases. Cases where the second order intensity correlation fails to predict laser action are also presented. D'Alessandro, Giampaolo verfasserin (DE-588)1249695236 (DE-627)1786229307 aut Lippi, Gian Luca verfasserin (DE-588)1253955816 (DE-627)1796377473 aut Oppo, Gian-Luca verfasserin (DE-588)125395593X (DE-627)1796377716 aut Papoff, Francesco verfasserin (DE-588)125395612X (DE-627)1796378089 aut Enthalten in Physical review letters College Park, Md. : APS, 1958 Volume 126(2021), Issue 6, Article 063902 Online-Ressource (DE-627)268756899 (DE-600)1472655-5 (DE-576)077609441 1079-7114 nnns volume:126 year:2021 number:6 elocationid:063902 https://doi.org/10.1103/PhysRevLett.126.063902 Resolving-System Full Text at Publisher lizenzpflichtig GBV_USEFLAG_U GBV_ILN_2088 ISIL_DE-Frei3c SYSFLAG_1 GBV_KXP GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_266 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2027 GBV_ILN_2110 GBV_ILN_2190 GBV_ILN_2336 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_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 126 2021 6 063902 Volume 126(2021), Issue 6, Article 063902 2088 01 DE-Frei3c 4098085674 00 --%%-- APS --%%-- n APS Funding text: G. D. and F. P. wish to thank the Mathematisches Forschungsinstitut Oberwolfach for support. l01 23-03-22 2088 01 DE-Frei3c APS |
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Thermal, quantum antibunching and lasing thresholds from single emitters to macroscopic devices |
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Thermal, quantum antibunching and lasing thresholds from single emitters to macroscopic devices |
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thermal, quantum antibunching and lasing thresholds from single emitters to macroscopic devices |
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Thermal, quantum antibunching and lasing thresholds from single emitters to macroscopic devices |
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Starting from a fully quantized Hamiltonian for an ensemble of identical emitters coupled to the modes of an optical cavity, we determine analytically regimes of thermal, collective anti-bunching and laser emission that depend explicitly on the number of emitters. The lasing regime is reached for a number of emitters above a critical number-which depends on the light-matter coupling, detuning, and the dissipation rates-via a universal transition from thermal emission to collective anti-bunching to lasing as the pump increases. Cases where the second order intensity correlation fails to predict laser action are also presented. Last seen: 23.03.2022 |
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Starting from a fully quantized Hamiltonian for an ensemble of identical emitters coupled to the modes of an optical cavity, we determine analytically regimes of thermal, collective anti-bunching and laser emission that depend explicitly on the number of emitters. The lasing regime is reached for a number of emitters above a critical number-which depends on the light-matter coupling, detuning, and the dissipation rates-via a universal transition from thermal emission to collective anti-bunching to lasing as the pump increases. Cases where the second order intensity correlation fails to predict laser action are also presented. Last seen: 23.03.2022 |
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Starting from a fully quantized Hamiltonian for an ensemble of identical emitters coupled to the modes of an optical cavity, we determine analytically regimes of thermal, collective anti-bunching and laser emission that depend explicitly on the number of emitters. The lasing regime is reached for a number of emitters above a critical number-which depends on the light-matter coupling, detuning, and the dissipation rates-via a universal transition from thermal emission to collective anti-bunching to lasing as the pump increases. Cases where the second order intensity correlation fails to predict laser action are also presented. Last seen: 23.03.2022 |
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