Standard

Photon Collider for Energy of 1–2 TeV. / Ginzburg, I. F.; Kotkin, G. L.

в: Physics of Particles and Nuclei, Том 52, № 5, 09.2021, стр. 899-912.

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

Harvard

Ginzburg, IF & Kotkin, GL 2021, 'Photon Collider for Energy of 1–2 TeV', Physics of Particles and Nuclei, Том. 52, № 5, стр. 899-912. https://doi.org/10.1134/S1063779621050038

APA

Ginzburg, I. F., & Kotkin, G. L. (2021). Photon Collider for Energy of 1–2 TeV. Physics of Particles and Nuclei, 52(5), 899-912. https://doi.org/10.1134/S1063779621050038

Vancouver

Ginzburg IF, Kotkin GL. Photon Collider for Energy of 1–2 TeV. Physics of Particles and Nuclei. 2021 сент.;52(5):899-912. doi: 10.1134/S1063779621050038

Author

Ginzburg, I. F. ; Kotkin, G. L. / Photon Collider for Energy of 1–2 TeV. в: Physics of Particles and Nuclei. 2021 ; Том 52, № 5. стр. 899-912.

BibTeX

@article{fd3662cc3f7e40e58b8a90fdc7e1481b,
title = "Photon Collider for Energy of 1–2 TeV",
abstract = "We discuss a photon collider based on the ee linear collider with energy 2E = 1 - 2 TeV in cms (ILC, CLIC, …), TeV PLC. Earlier, this energy range was considered hopeless for the experiment in the foreseeable future. We discuss a realization TeV PLC based on modern lasers. A small modification of the laser-optical system constructed for the photon collider with energy E ≈ 250 GeV will be sufficient if the parameters are chosen optimally. The high-energy part of the photon spectrum does not depend on design details and is well separated from the low-energy part. That is a narrow band near the upper boundary, about 5% wide. The high-energy integrated γγ luminosity is about 1/5 and the maximum differential luminosity is about 1/4 of the corresponding values for the photon collider with E ≈ 250 GeV.",
author = "Ginzburg, {I. F.} and Kotkin, {G. L.}",
note = "Funding Information: This work was supported by the SB RAS program of fundamental scientific research no. II.15.1., project no. 0314-2019-00, and the HARMONIA project (contract UMO-2015/18/M/ST2/00518 (2016-2020)). Publisher Copyright: {\textcopyright} 2021, Pleiades Publishing, Ltd.",
year = "2021",
month = sep,
doi = "10.1134/S1063779621050038",
language = "English",
volume = "52",
pages = "899--912",
journal = "Physics of Particles and Nuclei",
issn = "1063-7796",
publisher = "Maik Nauka-Interperiodica Publishing",
number = "5",

}

RIS

TY - JOUR

T1 - Photon Collider for Energy of 1–2 TeV

AU - Ginzburg, I. F.

AU - Kotkin, G. L.

N1 - Funding Information: This work was supported by the SB RAS program of fundamental scientific research no. II.15.1., project no. 0314-2019-00, and the HARMONIA project (contract UMO-2015/18/M/ST2/00518 (2016-2020)). Publisher Copyright: © 2021, Pleiades Publishing, Ltd.

PY - 2021/9

Y1 - 2021/9

N2 - We discuss a photon collider based on the ee linear collider with energy 2E = 1 - 2 TeV in cms (ILC, CLIC, …), TeV PLC. Earlier, this energy range was considered hopeless for the experiment in the foreseeable future. We discuss a realization TeV PLC based on modern lasers. A small modification of the laser-optical system constructed for the photon collider with energy E ≈ 250 GeV will be sufficient if the parameters are chosen optimally. The high-energy part of the photon spectrum does not depend on design details and is well separated from the low-energy part. That is a narrow band near the upper boundary, about 5% wide. The high-energy integrated γγ luminosity is about 1/5 and the maximum differential luminosity is about 1/4 of the corresponding values for the photon collider with E ≈ 250 GeV.

AB - We discuss a photon collider based on the ee linear collider with energy 2E = 1 - 2 TeV in cms (ILC, CLIC, …), TeV PLC. Earlier, this energy range was considered hopeless for the experiment in the foreseeable future. We discuss a realization TeV PLC based on modern lasers. A small modification of the laser-optical system constructed for the photon collider with energy E ≈ 250 GeV will be sufficient if the parameters are chosen optimally. The high-energy part of the photon spectrum does not depend on design details and is well separated from the low-energy part. That is a narrow band near the upper boundary, about 5% wide. The high-energy integrated γγ luminosity is about 1/5 and the maximum differential luminosity is about 1/4 of the corresponding values for the photon collider with E ≈ 250 GeV.

UR - http://www.scopus.com/inward/record.url?scp=85116112417&partnerID=8YFLogxK

U2 - 10.1134/S1063779621050038

DO - 10.1134/S1063779621050038

M3 - Article

AN - SCOPUS:85116112417

VL - 52

SP - 899

EP - 912

JO - Physics of Particles and Nuclei

JF - Physics of Particles and Nuclei

SN - 1063-7796

IS - 5

ER -

ID: 34358695