Standard

Commissioning of the linear accelerator of the SRF SKIF injector. / Nikiforov, Danila; Levichev, A. E.; Fedorov, Vyacheslav и др.

в: Radiation Detection Technology and Methods, 19.05.2026.

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

Harvard

Nikiforov, D, Levichev, AE, Fedorov, V, Reva, S, Sinyatkin, SV, Abed, N, Smirnov, K, Arsentyeva, MV, Barnyakov, A, Batrakov, A, Chekmenev, D, Dorokhov, V, Fomin, L, Kondakov, A, Meshkov, O, Pavlenko, A, Pavlov, O, Pivovarov, I, Samoilov, S, Semenov, A, Sibiryakova, K, Sudnik, A, Tur, A, Vizitiu, I & Volkov, V 2026, 'Commissioning of the linear accelerator of the SRF SKIF injector', Radiation Detection Technology and Methods. https://doi.org/10.1007/s41605-026-00659-4

APA

Nikiforov, D., Levichev, A. E., Fedorov, V., Reva, S., Sinyatkin, S. V., Abed, N., Smirnov, K., Arsentyeva, M. V., Barnyakov, A., Batrakov, A., Chekmenev, D., Dorokhov, V., Fomin, L., Kondakov, A., Meshkov, O., Pavlenko, A., Pavlov, O., Pivovarov, I., Samoilov, S., ... Volkov, V. (2026). Commissioning of the linear accelerator of the SRF SKIF injector. Radiation Detection Technology and Methods. https://doi.org/10.1007/s41605-026-00659-4

Vancouver

Nikiforov D, Levichev AE, Fedorov V, Reva S, Sinyatkin SV, Abed N и др. Commissioning of the linear accelerator of the SRF SKIF injector. Radiation Detection Technology and Methods. 2026 май 19. doi: 10.1007/s41605-026-00659-4

Author

Nikiforov, Danila ; Levichev, A. E. ; Fedorov, Vyacheslav и др. / Commissioning of the linear accelerator of the SRF SKIF injector. в: Radiation Detection Technology and Methods. 2026.

BibTeX

@article{3dda7cb18b0e453fac2b258a735db89a,
title = "Commissioning of the linear accelerator of the SRF SKIF injector",
abstract = "Purpose: Linear accelerator of the injector of the synchrotron radiation facility SKIF (SRF SKIF) was assembled in Koltsovo in the end 2024. It is the beginning part of the accelerator complex where the electron beam is formed. After the acceleration up to the energy of 200 MeV the beam is transported to the booster synchrotron. Methods: The linear accelerator (linac) consists of the electron source based on the radiofrequency (RF) gun, the bunching channel with the bunching preaccelerator and five regular accelerating structures. Three 50 MW klystrons with the operating frequency of 2856 MHz feed the accelerating structures. Two of the klystrons were developed and manufactured at the Budker Institute of Nuclear Physics of Siberian Branch of Russian Academy of Sciences (BINP SB RAS) in house, while the remaining one was purchased. Results: During the linac operation, maximum values of the RF power in waveguides were achieved. The transverse dynamics of the bunched electron beam was tuned in a single-bunch mode. Using the mechanical waveguide phase shifters, the accelerating field phases were chosen, which provided the required beam energy. Conclusion: Achieved parameters of the linac beam allowed us to proceed to the work with the linac–booster transport channel and the booster synchrotron itself. The article describes the linac launching process together with its current operation status and the achieved beam parameters.",
keywords = "Accelerating structures, Beam diagnostics, Electron beam, Linear accelerator, RF power, Линейный ускоритель, Мощность ВЧ, Электронный пучок, Диагностика пучка, Ускоряющие структуры",
author = "Danila Nikiforov and Levichev, {A. E.} and Vyacheslav Fedorov and Stanislav Reva and Sinyatkin, {S. V.} and N. Abed and Kirill Smirnov and Arsentyeva, {M. V.} and Alexey Barnyakov and Alexander Batrakov and Dmitry Chekmenev and Viktor Dorokhov and Lev Fomin and Alexey Kondakov and Oleg Meshkov and Anton Pavlenko and Oleg Pavlov and Ilya Pivovarov and Sergey Samoilov and Alexey Semenov and Kristina Sibiryakova and Anastasia Sudnik and Alexander Tur and Ilya Vizitiu and Vladimir Volkov",
note = "Nikiforov, D., Levichev, A.E., Fedorov, V. et al. Commissioning of the linear accelerator of the SRF SKIF injector. Radiat Detect Technol Methods (2026). https://doi.org/10.1007/s41605-026-00659-4 This work was partially supported by the Ministry of Science and Higher Education of the Russian Federation within the governmental order for SRF SKIF Boreskov Institute of Catalysis (project FWUR-2026-0004).",
year = "2026",
month = may,
day = "19",
doi = "10.1007/s41605-026-00659-4",
language = "English",
journal = "Radiation Detection Technology and Methods",
issn = "2509-9930",
publisher = "Springer Singapore",

}

RIS

TY - JOUR

T1 - Commissioning of the linear accelerator of the SRF SKIF injector

AU - Nikiforov, Danila

AU - Levichev, A. E.

AU - Fedorov, Vyacheslav

AU - Reva, Stanislav

AU - Sinyatkin, S. V.

AU - Abed, N.

AU - Smirnov, Kirill

AU - Arsentyeva, M. V.

AU - Barnyakov, Alexey

AU - Batrakov, Alexander

AU - Chekmenev, Dmitry

AU - Dorokhov, Viktor

AU - Fomin, Lev

AU - Kondakov, Alexey

AU - Meshkov, Oleg

AU - Pavlenko, Anton

AU - Pavlov, Oleg

AU - Pivovarov, Ilya

AU - Samoilov, Sergey

AU - Semenov, Alexey

AU - Sibiryakova, Kristina

AU - Sudnik, Anastasia

AU - Tur, Alexander

AU - Vizitiu, Ilya

AU - Volkov, Vladimir

N1 - Nikiforov, D., Levichev, A.E., Fedorov, V. et al. Commissioning of the linear accelerator of the SRF SKIF injector. Radiat Detect Technol Methods (2026). https://doi.org/10.1007/s41605-026-00659-4 This work was partially supported by the Ministry of Science and Higher Education of the Russian Federation within the governmental order for SRF SKIF Boreskov Institute of Catalysis (project FWUR-2026-0004).

PY - 2026/5/19

Y1 - 2026/5/19

N2 - Purpose: Linear accelerator of the injector of the synchrotron radiation facility SKIF (SRF SKIF) was assembled in Koltsovo in the end 2024. It is the beginning part of the accelerator complex where the electron beam is formed. After the acceleration up to the energy of 200 MeV the beam is transported to the booster synchrotron. Methods: The linear accelerator (linac) consists of the electron source based on the radiofrequency (RF) gun, the bunching channel with the bunching preaccelerator and five regular accelerating structures. Three 50 MW klystrons with the operating frequency of 2856 MHz feed the accelerating structures. Two of the klystrons were developed and manufactured at the Budker Institute of Nuclear Physics of Siberian Branch of Russian Academy of Sciences (BINP SB RAS) in house, while the remaining one was purchased. Results: During the linac operation, maximum values of the RF power in waveguides were achieved. The transverse dynamics of the bunched electron beam was tuned in a single-bunch mode. Using the mechanical waveguide phase shifters, the accelerating field phases were chosen, which provided the required beam energy. Conclusion: Achieved parameters of the linac beam allowed us to proceed to the work with the linac–booster transport channel and the booster synchrotron itself. The article describes the linac launching process together with its current operation status and the achieved beam parameters.

AB - Purpose: Linear accelerator of the injector of the synchrotron radiation facility SKIF (SRF SKIF) was assembled in Koltsovo in the end 2024. It is the beginning part of the accelerator complex where the electron beam is formed. After the acceleration up to the energy of 200 MeV the beam is transported to the booster synchrotron. Methods: The linear accelerator (linac) consists of the electron source based on the radiofrequency (RF) gun, the bunching channel with the bunching preaccelerator and five regular accelerating structures. Three 50 MW klystrons with the operating frequency of 2856 MHz feed the accelerating structures. Two of the klystrons were developed and manufactured at the Budker Institute of Nuclear Physics of Siberian Branch of Russian Academy of Sciences (BINP SB RAS) in house, while the remaining one was purchased. Results: During the linac operation, maximum values of the RF power in waveguides were achieved. The transverse dynamics of the bunched electron beam was tuned in a single-bunch mode. Using the mechanical waveguide phase shifters, the accelerating field phases were chosen, which provided the required beam energy. Conclusion: Achieved parameters of the linac beam allowed us to proceed to the work with the linac–booster transport channel and the booster synchrotron itself. The article describes the linac launching process together with its current operation status and the achieved beam parameters.

KW - Accelerating structures

KW - Beam diagnostics

KW - Electron beam

KW - Linear accelerator

KW - RF power

KW - Линейный ускоритель

KW - Мощность ВЧ

KW - Электронный пучок

KW - Диагностика пучка

KW - Ускоряющие структуры

UR - https://www.mendeley.com/catalogue/04161206-3952-3fce-8225-5802ee362c67/

UR - https://www.scopus.com/pages/publications/105039552546

U2 - 10.1007/s41605-026-00659-4

DO - 10.1007/s41605-026-00659-4

M3 - Article

JO - Radiation Detection Technology and Methods

JF - Radiation Detection Technology and Methods

SN - 2509-9930

ER -

ID: 83337480