Measurement of gamma-ray production cross sections for nuclear reactions 14N(d,pγ)15N and 28Si(d,pγ) 29Si

L. Csedreki, I. Uzonyi, Z. Szikszai, G. Gyürky, G. Á Szíki, A. Kiss

Research output: Contribution to journalArticle

12 Citations (Scopus)

Abstract

In this work the differential cross sections for gamma-ray emission from the 14N(d,pγ)15N (Eγ = 1885, 2297, 7299 and 8310 keV) and from the 28Si(d,pγ)29Si (Eγ = 1273, 2028, 2426 and 4934 keV) were measured simultaneously with the 14N(d,p4,5,6,7)15N differential cross sections and 14N(d,d)14N elastic scattering cross section using a HPGe detector at 55 and an ion implanted Si detector at 135 with respect to the beam direction in the deuteron energy range 0.65-2.0 MeV. The target was a thin silicon-nitride film. Gamma-ray angular distribution measurements were performed to determine the possible anisotropy of the gamma-ray emission, and the measured cross section values were converted into total gamma-ray producing cross sections for most of the gamma-ray emissions. The average uncertainties of nitrogen and silicon gamma-ray production cross sections are 5% and 12%, respectively and 8% concerning the particle production cross section of natN(d,d0)natN and 14N(d,p 4,5,6,7)15N reactions.

Original languageEnglish
Pages (from-to)20-26
Number of pages7
JournalNuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms
Volume328
DOIs
Publication statusPublished - Jun 1 2014

Fingerprint

Gamma ray production
Nuclear reactions
nuclear reactions
Gamma rays
gamma rays
cross sections
Detectors
Elastic scattering
Angular distribution
Silicon nitride
detectors
particle production
silicon nitrides
Anisotropy
scattering cross sections
deuterons
elastic scattering
Nitrogen
angular distribution
Silicon

Keywords

  • DIGE
  • Silicon-nitride film, Cross sections for gamma-ray and particles

ASJC Scopus subject areas

  • Instrumentation
  • Nuclear and High Energy Physics

Cite this

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title = "Measurement of gamma-ray production cross sections for nuclear reactions 14N(d,pγ)15N and 28Si(d,pγ) 29Si",
abstract = "In this work the differential cross sections for gamma-ray emission from the 14N(d,pγ)15N (Eγ = 1885, 2297, 7299 and 8310 keV) and from the 28Si(d,pγ)29Si (Eγ = 1273, 2028, 2426 and 4934 keV) were measured simultaneously with the 14N(d,p4,5,6,7)15N differential cross sections and 14N(d,d)14N elastic scattering cross section using a HPGe detector at 55 and an ion implanted Si detector at 135 with respect to the beam direction in the deuteron energy range 0.65-2.0 MeV. The target was a thin silicon-nitride film. Gamma-ray angular distribution measurements were performed to determine the possible anisotropy of the gamma-ray emission, and the measured cross section values were converted into total gamma-ray producing cross sections for most of the gamma-ray emissions. The average uncertainties of nitrogen and silicon gamma-ray production cross sections are 5{\%} and 12{\%}, respectively and 8{\%} concerning the particle production cross section of natN(d,d0)natN and 14N(d,p 4,5,6,7)15N reactions.",
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author = "L. Csedreki and I. Uzonyi and Z. Szikszai and G. Gy{\"u}rky and Sz{\'i}ki, {G. {\'A}} and A. Kiss",
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TY - JOUR

T1 - Measurement of gamma-ray production cross sections for nuclear reactions 14N(d,pγ)15N and 28Si(d,pγ) 29Si

AU - Csedreki, L.

AU - Uzonyi, I.

AU - Szikszai, Z.

AU - Gyürky, G.

AU - Szíki, G. Á

AU - Kiss, A.

PY - 2014/6/1

Y1 - 2014/6/1

N2 - In this work the differential cross sections for gamma-ray emission from the 14N(d,pγ)15N (Eγ = 1885, 2297, 7299 and 8310 keV) and from the 28Si(d,pγ)29Si (Eγ = 1273, 2028, 2426 and 4934 keV) were measured simultaneously with the 14N(d,p4,5,6,7)15N differential cross sections and 14N(d,d)14N elastic scattering cross section using a HPGe detector at 55 and an ion implanted Si detector at 135 with respect to the beam direction in the deuteron energy range 0.65-2.0 MeV. The target was a thin silicon-nitride film. Gamma-ray angular distribution measurements were performed to determine the possible anisotropy of the gamma-ray emission, and the measured cross section values were converted into total gamma-ray producing cross sections for most of the gamma-ray emissions. The average uncertainties of nitrogen and silicon gamma-ray production cross sections are 5% and 12%, respectively and 8% concerning the particle production cross section of natN(d,d0)natN and 14N(d,p 4,5,6,7)15N reactions.

AB - In this work the differential cross sections for gamma-ray emission from the 14N(d,pγ)15N (Eγ = 1885, 2297, 7299 and 8310 keV) and from the 28Si(d,pγ)29Si (Eγ = 1273, 2028, 2426 and 4934 keV) were measured simultaneously with the 14N(d,p4,5,6,7)15N differential cross sections and 14N(d,d)14N elastic scattering cross section using a HPGe detector at 55 and an ion implanted Si detector at 135 with respect to the beam direction in the deuteron energy range 0.65-2.0 MeV. The target was a thin silicon-nitride film. Gamma-ray angular distribution measurements were performed to determine the possible anisotropy of the gamma-ray emission, and the measured cross section values were converted into total gamma-ray producing cross sections for most of the gamma-ray emissions. The average uncertainties of nitrogen and silicon gamma-ray production cross sections are 5% and 12%, respectively and 8% concerning the particle production cross section of natN(d,d0)natN and 14N(d,p 4,5,6,7)15N reactions.

KW - DIGE

KW - Silicon-nitride film, Cross sections for gamma-ray and particles

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