Reaction rates of residual nuclei produced in 59Co at the target QUINTA

M. Zeman; J. Adam; K. Katovsky; A. A. Baldin; W. I. Furman; Yu Kish; J. Khushvaktov; A. A. Solnyshkin; V. M. Tsoupko-Sitnikov; S. I. Tyutyunnikov; J. Vrzalova; L. Zavorka; M. Suchopar; V. Wagner; P. Zhivkov

Reaction rates of residual nuclei produced in ⁵⁹Co at the target QUINTA

M. Zeman, J. Adam, K. Katovsky, A. A. Baldin, W. I. Furman, Yu Kish, J. Khushvaktov, A. A. Solnyshkin, V. M. Tsoupko-Sitnikov, S. I. Tyutyunnikov, J. Vrzalova, L. Zavorka, M. Suchopar, V. Wagner, P. Zhivkov

Research output: Contribution to journal › Conference article › peer-review

Abstract

In December 2013, an experiment with the natural uranium spallation target QUINTA was performed at the Joint Institute for Nuclear Research (JINR). The mass of the QUINTA setup is 512 kg. It consist of five hexagonal sections. The experimental samples of 59Co have been irradiated in the field of secondary neutrons generated by the deuteron beam at the Nuclotron accelerator at JINR. Energy of the deuteron beam was 4 AGeV. During the experiment, samples were situated in different positions inside the assembly and after irradiation they were measured at the high-purity germanium semiconductor detectors. Experimental reaction rates of residual nuclei were determined and compared with reaction rates calculated with the MCNPX code.

Original language	English
Journal	Proceedings of Science
State	Published - 2014
Externally published	Yes
Event	22nd International Baldin Seminar on High Energy Physics Problems "Relativistic Nuclear Physics and Quantum Chromodynamics", Baldin ISHEPP 2014 - Dubna, Russian Federation Duration: Sep 15 2014 → Sep 20 2014

Cite this

@article{d0ea80939b8a43619db2fb6203c62078,

title = "Reaction rates of residual nuclei produced in 59Co at the target QUINTA",

abstract = "In December 2013, an experiment with the natural uranium spallation target QUINTA was performed at the Joint Institute for Nuclear Research (JINR). The mass of the QUINTA setup is 512 kg. It consist of five hexagonal sections. The experimental samples of 59Co have been irradiated in the field of secondary neutrons generated by the deuteron beam at the Nuclotron accelerator at JINR. Energy of the deuteron beam was 4 AGeV. During the experiment, samples were situated in different positions inside the assembly and after irradiation they were measured at the high-purity germanium semiconductor detectors. Experimental reaction rates of residual nuclei were determined and compared with reaction rates calculated with the MCNPX code.",

author = "M. Zeman and J. Adam and K. Katovsky and Baldin, {A. A.} and Furman, {W. I.} and Yu Kish and J. Khushvaktov and Solnyshkin, {A. A.} and Tsoupko-Sitnikov, {V. M.} and Tyutyunnikov, {S. I.} and J. Vrzalova and L. Zavorka and M. Suchopar and V. Wagner and P. Zhivkov",

note = "Publisher Copyright: {\textcopyright} Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike Licence.; 22nd International Baldin Seminar on High Energy Physics Problems {"}Relativistic Nuclear Physics and Quantum Chromodynamics{"}, Baldin ISHEPP 2014 ; Conference date: 15-09-2014 Through 20-09-2014",

year = "2014",

language = "English",

journal = "Proceedings of Science",

issn = "1824-8039",

publisher = "Sissa Medialab",

}

TY - JOUR

T1 - Reaction rates of residual nuclei produced in 59Co at the target QUINTA

AU - Zeman, M.

AU - Adam, J.

AU - Katovsky, K.

AU - Baldin, A. A.

AU - Furman, W. I.

AU - Kish, Yu

AU - Khushvaktov, J.

AU - Solnyshkin, A. A.

AU - Tsoupko-Sitnikov, V. M.

AU - Tyutyunnikov, S. I.

AU - Vrzalova, J.

AU - Zavorka, L.

AU - Suchopar, M.

AU - Wagner, V.

AU - Zhivkov, P.

N1 - Publisher Copyright: © Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike Licence.

PY - 2014

Y1 - 2014

N2 - In December 2013, an experiment with the natural uranium spallation target QUINTA was performed at the Joint Institute for Nuclear Research (JINR). The mass of the QUINTA setup is 512 kg. It consist of five hexagonal sections. The experimental samples of 59Co have been irradiated in the field of secondary neutrons generated by the deuteron beam at the Nuclotron accelerator at JINR. Energy of the deuteron beam was 4 AGeV. During the experiment, samples were situated in different positions inside the assembly and after irradiation they were measured at the high-purity germanium semiconductor detectors. Experimental reaction rates of residual nuclei were determined and compared with reaction rates calculated with the MCNPX code.

AB - In December 2013, an experiment with the natural uranium spallation target QUINTA was performed at the Joint Institute for Nuclear Research (JINR). The mass of the QUINTA setup is 512 kg. It consist of five hexagonal sections. The experimental samples of 59Co have been irradiated in the field of secondary neutrons generated by the deuteron beam at the Nuclotron accelerator at JINR. Energy of the deuteron beam was 4 AGeV. During the experiment, samples were situated in different positions inside the assembly and after irradiation they were measured at the high-purity germanium semiconductor detectors. Experimental reaction rates of residual nuclei were determined and compared with reaction rates calculated with the MCNPX code.

UR - http://www.scopus.com/inward/record.url?scp=85051053919&partnerID=8YFLogxK

M3 - Conference article

AN - SCOPUS:85051053919

SN - 1824-8039

JO - Proceedings of Science

JF - Proceedings of Science

T2 - 22nd International Baldin Seminar on High Energy Physics Problems "Relativistic Nuclear Physics and Quantum Chromodynamics", Baldin ISHEPP 2014

Y2 - 15 September 2014 through 20 September 2014

ER -

Reaction rates of residual nuclei produced in ⁵⁹Co at the target QUINTA

Abstract

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