DEPENDENCE OF RATE OF 13N AND 15O RADIONUCLIDES PRODUCTION IN AIR FROM THE MAXIMAL ENERGY AND THE SPECTRUM OF BREMSSTRAHLUNG

被引:0
|
作者
Gann, A. V. [1 ]
Gann, V. V. [1 ]
Pugachev, G. D. [1 ]
Shapoval, I. I. [1 ]
Shapoval, I. A. [1 ]
Shestakova, V. S. [1 ]
机构
[1] Kharkiv Inst Phys & Technol, Natl Sci Ctr, Kharkov, Ukraine
关键词
D O I
暂无
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
While using electron beams in physical experiments, medicine and industry their converting in bremsstrahlung takes place which leads to air radiolysis practically in all accelerating chamber (ACH). Forbidden period of an entrance to ACH at energy of accelerated electrons above 30 MeV is determined by the concentration of N-13 and O-15 in ACH air. However, now in the literature and normative documentation there is no data for concentration calculation of radioactive gases in ACH in an operational mode of accelerating setup with bremsstrahlung. By means of GEANT 4 package spectra of bremsstrahlung and neutron radiations are calculated, which are formed at interaction of an electron beam with a thick target. Also the dependence of constant rate for N-13 and O-15 radionuclides production in air are estimated at the energy of accelerated electrons from 25 up to 100 MeV. Obtained results can be used for calculation of concentration of radioactive gases in ACH and in atmospheric emissions.
引用
收藏
页码:178 / 180
页数:3
相关论文
共 23 条
  • [1] Time-dependent chemical compositions of 13N and 15O induced in air by the operation of a high energy electron accelerator
    Endo, A
    Henshaw, J
    Mignanelli, MA
    HEALTH PHYSICS, 1998, 74 (04): : 456 - 464
  • [2] CALIBRATION OF A GM DETECTOR TO MEASURE 15O AND 13N IN AIR BY IMMERSION IN A STANDARDIZED 32P SOLUTION
    HOLEMAN, GR
    HEALTH PHYSICS, 1969, 17 (01): : 158 - +
  • [3] The Evaluation and Calculation of Production Cross Sections for 11C, 13N and 15O from 11B, 13C, 15N(p,n) and 16O(p,x)13N Reactions up to 80 MeV
    Zhuang Youxiang ( China Nuclear Data Center
    中国核科技报告, 1996, (S2) : 64 - 73
  • [4] Production of 11C, 13N and 15O in proton-induced nuclear reactions up to 200 MeV
    Rodriguez-Gonzalez, T.
    Guerrero, C.
    Baecker, C. M.
    Bauer, J.
    Baeumer, C.
    Brons, S.
    Jentzen, W.
    Jimenez-Ramos, M. C.
    Millan-Callado, M. A.
    Schoemers, C.
    Timmermann, B.
    Quesada, J. M.
    Capote, R.
    NUCLEAR DATA SHEETS, 2023, 187 : 579 - 596
  • [5] PRODUCTION OF RADIOISOTOPES 11C 13N AND 15O USING DEUTERON BEAM FROM A 3 MEV VAN DE GRAAFF ACCELERATOR
    RITCHIE, AIM
    NUCLEAR INSTRUMENTS & METHODS, 1968, 64 (02): : 181 - &
  • [6] LEVELS OF 15O SEEN FROM REACTION 13C(3HE,N)15O
    HINDERLI.HF
    LOCHSTET, WA
    BULLETIN OF THE AMERICAN PHYSICAL SOCIETY, 1968, 13 (04): : 606 - &
  • [7] Synthesis of 11C, 18F, 15O, and 13N Radiolabels for Positron Emission Tomography
    Miller, Philip W.
    Long, Nicholas J.
    Vilar, Ramon
    Gee, Antony D.
    ANGEWANDTE CHEMIE-INTERNATIONAL EDITION, 2008, 47 (47) : 8998 - 9033
  • [8] Excitation Functions of 14N(d,t)13N and 14N(d,an)11C Reactions from Threshold to 12.3 MeV: Radionuclidic Purity of 15O Produced via the 14N(d,n)15O Reaction
    Szucs, Z.
    Hamkens, W.
    Takacs, S.
    Tarkanyi, F.
    Radiochimica Acta, 80 (02):
  • [9] Excitation functions of 14N(d,t)13N and 14N(d,αn)11C reactions from threshold to 12.3 MeV:: Radionuclidic purity of 15O produced via the 14N(d,n)15O reaction
    Szucs, Z
    Hamkens, W
    Takacs, S
    Tarkanyi, F
    Coenen, HH
    Qaim, SM
    RADIOCHIMICA ACTA, 1998, 80 (02) : 59 - 63
  • [10] Imaging plate characteristics of positron emitters:: 11C, 13N, 15O, 18F and 38K
    Noguchi, J
    Suzuki, K
    RADIOCHIMICA ACTA, 2001, 89 (07) : 433 - 437