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Laser Wakefield Acceleration in a Plasma Channel. / Dorozhkina, M. S.; Baluev, K. V.; Kutergin, D. D. и др.

в: Bulletin of the Lebedev Physics Institute, Том 50, 10.2023, стр. S715-S723.

Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование

Harvard

Dorozhkina, MS, Baluev, KV, Kutergin, DD, Lotov, IK, Minakov, VA, Spitsyn, RI, Tuev, PV & Lotov, KV 2023, 'Laser Wakefield Acceleration in a Plasma Channel', Bulletin of the Lebedev Physics Institute, Том. 50, стр. S715-S723. https://doi.org/10.3103/S1068335623180057

APA

Dorozhkina, M. S., Baluev, K. V., Kutergin, D. D., Lotov, I. K., Minakov, V. A., Spitsyn, R. I., Tuev, P. V., & Lotov, K. V. (2023). Laser Wakefield Acceleration in a Plasma Channel. Bulletin of the Lebedev Physics Institute, 50, S715-S723. https://doi.org/10.3103/S1068335623180057

Vancouver

Dorozhkina MS, Baluev KV, Kutergin DD, Lotov IK, Minakov VA, Spitsyn RI и др. Laser Wakefield Acceleration in a Plasma Channel. Bulletin of the Lebedev Physics Institute. 2023 окт.;50:S715-S723. doi: 10.3103/S1068335623180057

Author

Dorozhkina, M. S. ; Baluev, K. V. ; Kutergin, D. D. и др. / Laser Wakefield Acceleration in a Plasma Channel. в: Bulletin of the Lebedev Physics Institute. 2023 ; Том 50. стр. S715-S723.

BibTeX

@article{d6297f946d21494c964f331338137f36,
title = "Laser Wakefield Acceleration in a Plasma Channel",
abstract = "It is shown by numerical simulations that, if a laser pulse from the eXawatt Center for Extreme Light Studies (Sarov) is used as a driver for a laser wakefield accelerator, an electron bunch with a charge of 50 pC can be accelerated to energy of 100 GeV with an energy spread of less than 1%. To this end, it is necessary to form a plasma channel 70 m long with a characteristic radius of 200 μm and a plasma density of 3 × 1015 cm–3 on the axis. In a denser plasma, the acceleration rate is higher, but the acceleration length and the resulting energy are smaller. The accelerator parameters can be numerically optimized using a quasistatic model describing the laser pulse in terms of its envelope, which reduces the computation time by several orders of magnitude as compared to complete models.",
keywords = "laser acceleration, numerical simulations, plasma acceleration, plasma channel",
author = "Dorozhkina, {M. S.} and Baluev, {K. V.} and Kutergin, {D. D.} and Lotov, {I. K.} and Minakov, {V. A.} and Spitsyn, {R. I.} and Tuev, {P. V.} and Lotov, {K. V.}",
note = "This study was supported by a scientific program of the National Center for Physics and Mathematics. Публикация для корректировки.",
year = "2023",
month = oct,
doi = "10.3103/S1068335623180057",
language = "English",
volume = "50",
pages = "S715--S723",
journal = "Bulletin of the Lebedev Physics Institute",
issn = "1068-3356",
publisher = "Springer Science + Business Media",

}

RIS

TY - JOUR

T1 - Laser Wakefield Acceleration in a Plasma Channel

AU - Dorozhkina, M. S.

AU - Baluev, K. V.

AU - Kutergin, D. D.

AU - Lotov, I. K.

AU - Minakov, V. A.

AU - Spitsyn, R. I.

AU - Tuev, P. V.

AU - Lotov, K. V.

N1 - This study was supported by a scientific program of the National Center for Physics and Mathematics. Публикация для корректировки.

PY - 2023/10

Y1 - 2023/10

N2 - It is shown by numerical simulations that, if a laser pulse from the eXawatt Center for Extreme Light Studies (Sarov) is used as a driver for a laser wakefield accelerator, an electron bunch with a charge of 50 pC can be accelerated to energy of 100 GeV with an energy spread of less than 1%. To this end, it is necessary to form a plasma channel 70 m long with a characteristic radius of 200 μm and a plasma density of 3 × 1015 cm–3 on the axis. In a denser plasma, the acceleration rate is higher, but the acceleration length and the resulting energy are smaller. The accelerator parameters can be numerically optimized using a quasistatic model describing the laser pulse in terms of its envelope, which reduces the computation time by several orders of magnitude as compared to complete models.

AB - It is shown by numerical simulations that, if a laser pulse from the eXawatt Center for Extreme Light Studies (Sarov) is used as a driver for a laser wakefield accelerator, an electron bunch with a charge of 50 pC can be accelerated to energy of 100 GeV with an energy spread of less than 1%. To this end, it is necessary to form a plasma channel 70 m long with a characteristic radius of 200 μm and a plasma density of 3 × 1015 cm–3 on the axis. In a denser plasma, the acceleration rate is higher, but the acceleration length and the resulting energy are smaller. The accelerator parameters can be numerically optimized using a quasistatic model describing the laser pulse in terms of its envelope, which reduces the computation time by several orders of magnitude as compared to complete models.

KW - laser acceleration

KW - numerical simulations

KW - plasma acceleration

KW - plasma channel

UR - https://www.scopus.com/record/display.uri?eid=2-s2.0-85173703276&origin=inward&txGid=9e642ec24efe86f790cfa02996ecab48

UR - https://www.mendeley.com/catalogue/256d5383-e01c-3133-a9f1-eee87e341884/

U2 - 10.3103/S1068335623180057

DO - 10.3103/S1068335623180057

M3 - Article

VL - 50

SP - S715-S723

JO - Bulletin of the Lebedev Physics Institute

JF - Bulletin of the Lebedev Physics Institute

SN - 1068-3356

ER -

ID: 59548767