Signatures of the Carrier Envelope Phase in Nonlinear Thomson Scattering

High-energy radiation can be generated by colliding a relativistic electron bunch with a high-intensity laser pulse—a process known as Thomson scattering. In the nonlinear regime the emitted radiation contains harmonics. For a laser pulse whose length is comparable to its wavelength, the carrier env...
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Autor*in:	Marcel Ruijter [verfasserIn] Vittoria Petrillo [verfasserIn] Thomas C. Teter [verfasserIn] Maksim Valialshchikov [verfasserIn] Sergey Rykovanov [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2021

Schlagwörter:	Thomson scattering carrier envelope phase high-intensity laser relativistic electron

Übergeordnetes Werk:	In: Crystals - MDPI AG, 2011, 11(2021), 5, p 528
Übergeordnetes Werk:	volume:11 ; year:2021 ; number:5, p 528

Links:	Link aufrufen Link aufrufen Link aufrufen Journal toc

DOI / URN:	10.3390/cryst11050528

Katalog-ID:	DOAJ085528978

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520			\|a High-energy radiation can be generated by colliding a relativistic electron bunch with a high-intensity laser pulse—a process known as Thomson scattering. In the nonlinear regime the emitted radiation contains harmonics. For a laser pulse whose length is comparable to its wavelength, the carrier envelope phase changes the behavior of the motion of the electron and therefore the radiation spectrum. Here we show theoretically and numerically the dependency of the spectrum on the intensity of the laser and the carrier envelope phase. Additionally, we also discuss what experimental parameters are required to measure the effects for a beamed pulse.
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spelling	10.3390/cryst11050528 doi (DE-627)DOAJ085528978 (DE-599)DOAJ1f364a907b1c4fc3b8276b6ef9f8e6fd DE-627 ger DE-627 rakwb eng QD901-999 Marcel Ruijter verfasserin aut Signatures of the Carrier Envelope Phase in Nonlinear Thomson Scattering 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier High-energy radiation can be generated by colliding a relativistic electron bunch with a high-intensity laser pulse—a process known as Thomson scattering. In the nonlinear regime the emitted radiation contains harmonics. For a laser pulse whose length is comparable to its wavelength, the carrier envelope phase changes the behavior of the motion of the electron and therefore the radiation spectrum. Here we show theoretically and numerically the dependency of the spectrum on the intensity of the laser and the carrier envelope phase. Additionally, we also discuss what experimental parameters are required to measure the effects for a beamed pulse. Thomson scattering carrier envelope phase high-intensity laser relativistic electron Crystallography Vittoria Petrillo verfasserin aut Thomas C. Teter verfasserin aut Maksim Valialshchikov verfasserin aut Sergey Rykovanov verfasserin aut In Crystals MDPI AG, 2011 11(2021), 5, p 528 (DE-627)718303067 (DE-600)2661516-2 20734352 nnns volume:11 year:2021 number:5, p 528 https://doi.org/10.3390/cryst11050528 kostenfrei https://doaj.org/article/1f364a907b1c4fc3b8276b6ef9f8e6fd kostenfrei https://www.mdpi.com/2073-4352/11/5/528 kostenfrei https://doaj.org/toc/2073-4352 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 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_602 GBV_ILN_2014 GBV_ILN_2055 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 11 2021 5, p 528
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language	English
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callnumber-first	Q - Science
author	Marcel Ruijter
spellingShingle	Marcel Ruijter misc QD901-999 misc Thomson scattering misc carrier envelope phase misc high-intensity laser misc relativistic electron misc Crystallography Signatures of the Carrier Envelope Phase in Nonlinear Thomson Scattering
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topic_title	QD901-999 Signatures of the Carrier Envelope Phase in Nonlinear Thomson Scattering Thomson scattering carrier envelope phase high-intensity laser relativistic electron
topic	misc QD901-999 misc Thomson scattering misc carrier envelope phase misc high-intensity laser misc relativistic electron misc Crystallography
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title	Signatures of the Carrier Envelope Phase in Nonlinear Thomson Scattering
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title_full	Signatures of the Carrier Envelope Phase in Nonlinear Thomson Scattering
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title_sort	signatures of the carrier envelope phase in nonlinear thomson scattering
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title_auth	Signatures of the Carrier Envelope Phase in Nonlinear Thomson Scattering
abstract	High-energy radiation can be generated by colliding a relativistic electron bunch with a high-intensity laser pulse—a process known as Thomson scattering. In the nonlinear regime the emitted radiation contains harmonics. For a laser pulse whose length is comparable to its wavelength, the carrier envelope phase changes the behavior of the motion of the electron and therefore the radiation spectrum. Here we show theoretically and numerically the dependency of the spectrum on the intensity of the laser and the carrier envelope phase. Additionally, we also discuss what experimental parameters are required to measure the effects for a beamed pulse.
abstractGer	High-energy radiation can be generated by colliding a relativistic electron bunch with a high-intensity laser pulse—a process known as Thomson scattering. In the nonlinear regime the emitted radiation contains harmonics. For a laser pulse whose length is comparable to its wavelength, the carrier envelope phase changes the behavior of the motion of the electron and therefore the radiation spectrum. Here we show theoretically and numerically the dependency of the spectrum on the intensity of the laser and the carrier envelope phase. Additionally, we also discuss what experimental parameters are required to measure the effects for a beamed pulse.
abstract_unstemmed	High-energy radiation can be generated by colliding a relativistic electron bunch with a high-intensity laser pulse—a process known as Thomson scattering. In the nonlinear regime the emitted radiation contains harmonics. For a laser pulse whose length is comparable to its wavelength, the carrier envelope phase changes the behavior of the motion of the electron and therefore the radiation spectrum. Here we show theoretically and numerically the dependency of the spectrum on the intensity of the laser and the carrier envelope phase. Additionally, we also discuss what experimental parameters are required to measure the effects for a beamed pulse.
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title_short	Signatures of the Carrier Envelope Phase in Nonlinear Thomson Scattering
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author2	Vittoria Petrillo Thomas C. Teter Maksim Valialshchikov Sergey Rykovanov
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