Pump Frequency Resonances for Light-Induced Incipient Superconductivity in YBa_{2}Cu_{3}O_{6.5}
Optical excitation in the cuprates has been shown to induce transient superconducting correlations above the thermodynamic transition temperature T_{C}, as evidenced by the terahertz-frequency optical properties in the nonequilibrium state. In YBa_{2}Cu_{3}O_{6+x}, this phenomenon has so far been as...
Ausführliche Beschreibung
Autor*in: |
B. Liu [verfasserIn] M. Först [verfasserIn] M. Fechner [verfasserIn] D. Nicoletti [verfasserIn] J. Porras [verfasserIn] T. Loew [verfasserIn] B. Keimer [verfasserIn] A. Cavalleri [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2020 |
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Übergeordnetes Werk: |
In: Physical Review X - American Physical Society, 2011, 10(2020), 1, p 011053 |
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Übergeordnetes Werk: |
volume:10 ; year:2020 ; number:1, p 011053 |
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DOI / URN: |
10.1103/PhysRevX.10.011053 |
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DOAJ062372564 |
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10.1103/PhysRevX.10.011053 doi (DE-627)DOAJ062372564 (DE-599)DOAJ84377c5b2c5e438a8165afec27b466c2 DE-627 ger DE-627 rakwb eng QC1-999 B. Liu verfasserin aut Pump Frequency Resonances for Light-Induced Incipient Superconductivity in YBa_{2}Cu_{3}O_{6.5} 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Optical excitation in the cuprates has been shown to induce transient superconducting correlations above the thermodynamic transition temperature T_{C}, as evidenced by the terahertz-frequency optical properties in the nonequilibrium state. In YBa_{2}Cu_{3}O_{6+x}, this phenomenon has so far been associated with the nonlinear excitation of certain lattice modes and the creation of new crystal structures. In other compounds, like La_{2−x}Ba_{x}CuO_{4}, similar effects were reported also for excitation at near-infrared frequencies, and were interpreted as a signature of the melting of competing orders. However, to date, it has not been possible to systematically tune the pump frequency widely in any one compound, to comprehensively compare the frequency-dependent photosusceptibility for this phenomenon. Here, we make use of a newly developed nonlinear optical device, which generates widely tunable high-intensity femtosecond pulses, to excite YBa_{2}Cu_{3}O_{6.5} throughout the entire optical spectrum (3–750 THz). In the far-infrared region (3–24 THz), signatures of nonequilibrium superconductivity are induced only for excitation of the 16.4- and 19.2-THz vibrational modes that drive c-axis apical oxygen atomic positions. For higher driving frequencies (25–750 THz), a second resonance is observed around the charge transfer band edge at approximately 350 THz. These findings highlight the importance of coupling to the electronic structure of the CuO_{2} planes, mediated either by a phonon or by charge transfer. Physics M. Först verfasserin aut M. Fechner verfasserin aut D. Nicoletti verfasserin aut J. Porras verfasserin aut T. Loew verfasserin aut B. Keimer verfasserin aut A. Cavalleri verfasserin aut In Physical Review X American Physical Society, 2011 10(2020), 1, p 011053 (DE-627)666214115 (DE-600)2622565-7 21603308 nnns volume:10 year:2020 number:1, p 011053 https://doi.org/10.1103/PhysRevX.10.011053 kostenfrei https://doaj.org/article/84377c5b2c5e438a8165afec27b466c2 kostenfrei http://doi.org/10.1103/PhysRevX.10.011053 kostenfrei http://doi.org/10.1103/PhysRevX.10.011053 kostenfrei https://doaj.org/toc/2160-3308 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ 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_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 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 10 2020 1, p 011053 |
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10.1103/PhysRevX.10.011053 doi (DE-627)DOAJ062372564 (DE-599)DOAJ84377c5b2c5e438a8165afec27b466c2 DE-627 ger DE-627 rakwb eng QC1-999 B. Liu verfasserin aut Pump Frequency Resonances for Light-Induced Incipient Superconductivity in YBa_{2}Cu_{3}O_{6.5} 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Optical excitation in the cuprates has been shown to induce transient superconducting correlations above the thermodynamic transition temperature T_{C}, as evidenced by the terahertz-frequency optical properties in the nonequilibrium state. In YBa_{2}Cu_{3}O_{6+x}, this phenomenon has so far been associated with the nonlinear excitation of certain lattice modes and the creation of new crystal structures. In other compounds, like La_{2−x}Ba_{x}CuO_{4}, similar effects were reported also for excitation at near-infrared frequencies, and were interpreted as a signature of the melting of competing orders. However, to date, it has not been possible to systematically tune the pump frequency widely in any one compound, to comprehensively compare the frequency-dependent photosusceptibility for this phenomenon. Here, we make use of a newly developed nonlinear optical device, which generates widely tunable high-intensity femtosecond pulses, to excite YBa_{2}Cu_{3}O_{6.5} throughout the entire optical spectrum (3–750 THz). In the far-infrared region (3–24 THz), signatures of nonequilibrium superconductivity are induced only for excitation of the 16.4- and 19.2-THz vibrational modes that drive c-axis apical oxygen atomic positions. For higher driving frequencies (25–750 THz), a second resonance is observed around the charge transfer band edge at approximately 350 THz. These findings highlight the importance of coupling to the electronic structure of the CuO_{2} planes, mediated either by a phonon or by charge transfer. Physics M. Först verfasserin aut M. Fechner verfasserin aut D. Nicoletti verfasserin aut J. Porras verfasserin aut T. Loew verfasserin aut B. Keimer verfasserin aut A. Cavalleri verfasserin aut In Physical Review X American Physical Society, 2011 10(2020), 1, p 011053 (DE-627)666214115 (DE-600)2622565-7 21603308 nnns volume:10 year:2020 number:1, p 011053 https://doi.org/10.1103/PhysRevX.10.011053 kostenfrei https://doaj.org/article/84377c5b2c5e438a8165afec27b466c2 kostenfrei http://doi.org/10.1103/PhysRevX.10.011053 kostenfrei http://doi.org/10.1103/PhysRevX.10.011053 kostenfrei https://doaj.org/toc/2160-3308 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ 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_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 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 10 2020 1, p 011053 |
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10.1103/PhysRevX.10.011053 doi (DE-627)DOAJ062372564 (DE-599)DOAJ84377c5b2c5e438a8165afec27b466c2 DE-627 ger DE-627 rakwb eng QC1-999 B. Liu verfasserin aut Pump Frequency Resonances for Light-Induced Incipient Superconductivity in YBa_{2}Cu_{3}O_{6.5} 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Optical excitation in the cuprates has been shown to induce transient superconducting correlations above the thermodynamic transition temperature T_{C}, as evidenced by the terahertz-frequency optical properties in the nonequilibrium state. In YBa_{2}Cu_{3}O_{6+x}, this phenomenon has so far been associated with the nonlinear excitation of certain lattice modes and the creation of new crystal structures. In other compounds, like La_{2−x}Ba_{x}CuO_{4}, similar effects were reported also for excitation at near-infrared frequencies, and were interpreted as a signature of the melting of competing orders. However, to date, it has not been possible to systematically tune the pump frequency widely in any one compound, to comprehensively compare the frequency-dependent photosusceptibility for this phenomenon. Here, we make use of a newly developed nonlinear optical device, which generates widely tunable high-intensity femtosecond pulses, to excite YBa_{2}Cu_{3}O_{6.5} throughout the entire optical spectrum (3–750 THz). In the far-infrared region (3–24 THz), signatures of nonequilibrium superconductivity are induced only for excitation of the 16.4- and 19.2-THz vibrational modes that drive c-axis apical oxygen atomic positions. For higher driving frequencies (25–750 THz), a second resonance is observed around the charge transfer band edge at approximately 350 THz. These findings highlight the importance of coupling to the electronic structure of the CuO_{2} planes, mediated either by a phonon or by charge transfer. Physics M. Först verfasserin aut M. Fechner verfasserin aut D. Nicoletti verfasserin aut J. Porras verfasserin aut T. Loew verfasserin aut B. Keimer verfasserin aut A. Cavalleri verfasserin aut In Physical Review X American Physical Society, 2011 10(2020), 1, p 011053 (DE-627)666214115 (DE-600)2622565-7 21603308 nnns volume:10 year:2020 number:1, p 011053 https://doi.org/10.1103/PhysRevX.10.011053 kostenfrei https://doaj.org/article/84377c5b2c5e438a8165afec27b466c2 kostenfrei http://doi.org/10.1103/PhysRevX.10.011053 kostenfrei http://doi.org/10.1103/PhysRevX.10.011053 kostenfrei https://doaj.org/toc/2160-3308 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ 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_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 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 10 2020 1, p 011053 |
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Pump Frequency Resonances for Light-Induced Incipient Superconductivity in YBa_{2}Cu_{3}O_{6.5} |
abstract |
Optical excitation in the cuprates has been shown to induce transient superconducting correlations above the thermodynamic transition temperature T_{C}, as evidenced by the terahertz-frequency optical properties in the nonequilibrium state. In YBa_{2}Cu_{3}O_{6+x}, this phenomenon has so far been associated with the nonlinear excitation of certain lattice modes and the creation of new crystal structures. In other compounds, like La_{2−x}Ba_{x}CuO_{4}, similar effects were reported also for excitation at near-infrared frequencies, and were interpreted as a signature of the melting of competing orders. However, to date, it has not been possible to systematically tune the pump frequency widely in any one compound, to comprehensively compare the frequency-dependent photosusceptibility for this phenomenon. Here, we make use of a newly developed nonlinear optical device, which generates widely tunable high-intensity femtosecond pulses, to excite YBa_{2}Cu_{3}O_{6.5} throughout the entire optical spectrum (3–750 THz). In the far-infrared region (3–24 THz), signatures of nonequilibrium superconductivity are induced only for excitation of the 16.4- and 19.2-THz vibrational modes that drive c-axis apical oxygen atomic positions. For higher driving frequencies (25–750 THz), a second resonance is observed around the charge transfer band edge at approximately 350 THz. These findings highlight the importance of coupling to the electronic structure of the CuO_{2} planes, mediated either by a phonon or by charge transfer. |
abstractGer |
Optical excitation in the cuprates has been shown to induce transient superconducting correlations above the thermodynamic transition temperature T_{C}, as evidenced by the terahertz-frequency optical properties in the nonequilibrium state. In YBa_{2}Cu_{3}O_{6+x}, this phenomenon has so far been associated with the nonlinear excitation of certain lattice modes and the creation of new crystal structures. In other compounds, like La_{2−x}Ba_{x}CuO_{4}, similar effects were reported also for excitation at near-infrared frequencies, and were interpreted as a signature of the melting of competing orders. However, to date, it has not been possible to systematically tune the pump frequency widely in any one compound, to comprehensively compare the frequency-dependent photosusceptibility for this phenomenon. Here, we make use of a newly developed nonlinear optical device, which generates widely tunable high-intensity femtosecond pulses, to excite YBa_{2}Cu_{3}O_{6.5} throughout the entire optical spectrum (3–750 THz). In the far-infrared region (3–24 THz), signatures of nonequilibrium superconductivity are induced only for excitation of the 16.4- and 19.2-THz vibrational modes that drive c-axis apical oxygen atomic positions. For higher driving frequencies (25–750 THz), a second resonance is observed around the charge transfer band edge at approximately 350 THz. These findings highlight the importance of coupling to the electronic structure of the CuO_{2} planes, mediated either by a phonon or by charge transfer. |
abstract_unstemmed |
Optical excitation in the cuprates has been shown to induce transient superconducting correlations above the thermodynamic transition temperature T_{C}, as evidenced by the terahertz-frequency optical properties in the nonequilibrium state. In YBa_{2}Cu_{3}O_{6+x}, this phenomenon has so far been associated with the nonlinear excitation of certain lattice modes and the creation of new crystal structures. In other compounds, like La_{2−x}Ba_{x}CuO_{4}, similar effects were reported also for excitation at near-infrared frequencies, and were interpreted as a signature of the melting of competing orders. However, to date, it has not been possible to systematically tune the pump frequency widely in any one compound, to comprehensively compare the frequency-dependent photosusceptibility for this phenomenon. Here, we make use of a newly developed nonlinear optical device, which generates widely tunable high-intensity femtosecond pulses, to excite YBa_{2}Cu_{3}O_{6.5} throughout the entire optical spectrum (3–750 THz). In the far-infrared region (3–24 THz), signatures of nonequilibrium superconductivity are induced only for excitation of the 16.4- and 19.2-THz vibrational modes that drive c-axis apical oxygen atomic positions. For higher driving frequencies (25–750 THz), a second resonance is observed around the charge transfer band edge at approximately 350 THz. These findings highlight the importance of coupling to the electronic structure of the CuO_{2} planes, mediated either by a phonon or by charge transfer. |
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