Free Electron Laser Measurement of Liquid Carbon Reflectivity in the Extreme Ultraviolet

Ultrafast time-resolved extreme ultraviolet (EUV) reflectivity measurements of optically pumped amorphous carbon (a-C) have been performed with the FERMI free electron laser (FEL). This work extends the energy range used in previous reflectivity studies and adds polarization dependence. The EUV prob...

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Main Authors: Sumana L. Raj, Shane W. Devlin, Riccardo Mincigrucci, Craig P. Schwartz, Emiliano Principi, Filippo Bencivenga, Laura Foglia, Alessandro Gessini, Alberto Simoncig, Gabor Kurdi, Claudio Masciovecchio, Richard J. Saykally
Format: Article
Language:English
Published: MDPI AG 2020-05-01
Series:Photonics
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Online Access:https://www.mdpi.com/2304-6732/7/2/35
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author Sumana L. Raj
Shane W. Devlin
Riccardo Mincigrucci
Craig P. Schwartz
Emiliano Principi
Filippo Bencivenga
Laura Foglia
Alessandro Gessini
Alberto Simoncig
Gabor Kurdi
Claudio Masciovecchio
Richard J. Saykally
author_facet Sumana L. Raj
Shane W. Devlin
Riccardo Mincigrucci
Craig P. Schwartz
Emiliano Principi
Filippo Bencivenga
Laura Foglia
Alessandro Gessini
Alberto Simoncig
Gabor Kurdi
Claudio Masciovecchio
Richard J. Saykally
author_sort Sumana L. Raj
collection DOAJ
description Ultrafast time-resolved extreme ultraviolet (EUV) reflectivity measurements of optically pumped amorphous carbon (a-C) have been performed with the FERMI free electron laser (FEL). This work extends the energy range used in previous reflectivity studies and adds polarization dependence. The EUV probe is known to be sensitive to lattice dynamics, since in this range the reflectivity is essentially unaffected by the photo-excited surface plasma. The exploitation of both s- and p-polarized EUV radiation permits variation of the penetration depth of the probe; a significant increase in the characteristic time is observed upon increasing the probing depth (1 vs. 5 ps) due to hydrodynamic expansion and consequent destruction of the excited region, implying that there is only a short window during which the probed region is in the isochoric regime. A weak wavelength dependence of the reflectivity is found, consistent with previous measurements and implying a maximum electronic temperature of 0.8 eV ± 0.4.
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spelling doaj.art-16a7e635e92c41cd81a4f7bcfa69e61b2023-11-20T01:29:51ZengMDPI AGPhotonics2304-67322020-05-01723510.3390/photonics7020035Free Electron Laser Measurement of Liquid Carbon Reflectivity in the Extreme UltravioletSumana L. Raj0Shane W. Devlin1Riccardo Mincigrucci2Craig P. Schwartz3Emiliano Principi4Filippo Bencivenga5Laura Foglia6Alessandro Gessini7Alberto Simoncig8Gabor Kurdi9Claudio Masciovecchio10Richard J. Saykally11Department of Chemistry, University of California, Berkeley, CA 94720, USADepartment of Chemistry, University of California, Berkeley, CA 94720, USAElettra Sincrotrone Trieste SCpA, Basovizza, 34149 Trieste, ItalyMolecular Foundry, Lawrence Berkeley National Lab, Berkeley, CA 94720, USAElettra Sincrotrone Trieste SCpA, Basovizza, 34149 Trieste, ItalyElettra Sincrotrone Trieste SCpA, Basovizza, 34149 Trieste, ItalyElettra Sincrotrone Trieste SCpA, Basovizza, 34149 Trieste, ItalyElettra Sincrotrone Trieste SCpA, Basovizza, 34149 Trieste, ItalyElettra Sincrotrone Trieste SCpA, Basovizza, 34149 Trieste, ItalyElettra Sincrotrone Trieste SCpA, Basovizza, 34149 Trieste, ItalyElettra Sincrotrone Trieste SCpA, Basovizza, 34149 Trieste, ItalyDepartment of Chemistry, University of California, Berkeley, CA 94720, USAUltrafast time-resolved extreme ultraviolet (EUV) reflectivity measurements of optically pumped amorphous carbon (a-C) have been performed with the FERMI free electron laser (FEL). This work extends the energy range used in previous reflectivity studies and adds polarization dependence. The EUV probe is known to be sensitive to lattice dynamics, since in this range the reflectivity is essentially unaffected by the photo-excited surface plasma. The exploitation of both s- and p-polarized EUV radiation permits variation of the penetration depth of the probe; a significant increase in the characteristic time is observed upon increasing the probing depth (1 vs. 5 ps) due to hydrodynamic expansion and consequent destruction of the excited region, implying that there is only a short window during which the probed region is in the isochoric regime. A weak wavelength dependence of the reflectivity is found, consistent with previous measurements and implying a maximum electronic temperature of 0.8 eV ± 0.4.https://www.mdpi.com/2304-6732/7/2/35liquid carbonEUVfree electron laserreflectivitypump-probepolarization
spellingShingle Sumana L. Raj
Shane W. Devlin
Riccardo Mincigrucci
Craig P. Schwartz
Emiliano Principi
Filippo Bencivenga
Laura Foglia
Alessandro Gessini
Alberto Simoncig
Gabor Kurdi
Claudio Masciovecchio
Richard J. Saykally
Free Electron Laser Measurement of Liquid Carbon Reflectivity in the Extreme Ultraviolet
Photonics
liquid carbon
EUV
free electron laser
reflectivity
pump-probe
polarization
title Free Electron Laser Measurement of Liquid Carbon Reflectivity in the Extreme Ultraviolet
title_full Free Electron Laser Measurement of Liquid Carbon Reflectivity in the Extreme Ultraviolet
title_fullStr Free Electron Laser Measurement of Liquid Carbon Reflectivity in the Extreme Ultraviolet
title_full_unstemmed Free Electron Laser Measurement of Liquid Carbon Reflectivity in the Extreme Ultraviolet
title_short Free Electron Laser Measurement of Liquid Carbon Reflectivity in the Extreme Ultraviolet
title_sort free electron laser measurement of liquid carbon reflectivity in the extreme ultraviolet
topic liquid carbon
EUV
free electron laser
reflectivity
pump-probe
polarization
url https://www.mdpi.com/2304-6732/7/2/35
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