Excitation functions of nuclear reactions producing11C

Anders, B.; Herges, P.; Scobel, W.

doi:10.1007/bf01421701

Cited by 24 publications

(9 citation statements)

References 46 publications

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“…1 that the cross sections from the present experiment fall along high side of the upper curve previously set by the measurements of Anders et al [6] and Welch et al [7] and calculations of Dimbylow [5]. The predictions of Dimbylow [5] are within our error bars, as are, for the most part, the measurements from Anders et al [6] and Welch et al [7]. …”

Section: Discussion Of Experimental Resultssupporting

confidence: 87%

“…The empty symbols are previously published data: Brolley et al (blue circles) [8], Brill et al (pink circles) [9], Anders et al (green circles) [6], Welch et al (blue triangles) [7], Soewarsono et al (pink triangles) [10], Uno et al (green triangles) [11], and optical model calcualtions of Dimbylow (blue diamonds) [5]. The solid red symbols are from this experiment using the polyethylene target and both NaI detectors in coincidence; the larger of the associated error bars indicates the increase in overall uncertainty when the uncertainty in incident neutron energy is included.…”

Section: Figmentioning

confidence: 99%

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C12(n, 2n)C11 cross section from threshold to 26.5 M

et al. 2018

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The 12C(n, 2n)11C cross section was measured from just below threshold to 26.5 MeV using the Pelletron accelerator at Ohio University. Monoenergetic neutrons, produced via the 3H(d,n)4He reaction, were allowed to strike targets of polyethylene and graphite. Activation of both targets was measured by counting positron annihilations resulting from the β+ decay of 11C. Annihilation gamma rays were detected, both in coincidence and singly, using back-to-back NaI detectors. The incident neutron flux was determined indirectly via 1H(n,p) protons elastically scattered from the polyethylene target. Previous measurements fall into upper and lower bands; the results of the present measurement are consistent with the upper band.

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Section: Discussion Of Experimental Resultssupporting

confidence: 87%

Section: Figmentioning

confidence: 99%

C12(n, 2n)C11 cross section from threshold to 26.5 M

et al. 2018

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“…For example, the excitation function for the 12 C(n,2n) n C reaction in SCINFUL is shown in Figure 7. It agrees with the recent data of Anders et al 30 up to 34 MeV, cross section data being somewhat larger than earlier data. 31 For E n > 34 MeV one can only "evaluate" the excitation function by a "best estimate" smooth curve which intersects 22 mb at E" = 90 MeV, i.e., the value quoted (but not measured) by Kellogg.…”

Section: Cross Sections As Needed To Obtain a Better Representation Osupporting

confidence: 93%

SCINFUL: A Monte Carlo based computer program to determine a scintillator full energy response to neutron detection for E/sub n/ between 0. 1 and 80 MeV: Program development and comparisons of program predictions with experimental data

Dickens¹

1988

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A major purpose of the Techni cal Information Center is to provide the broadest dissemination possi ble of-information contained in DOE's Research and Development Reports to business, industry, the academic community, and federal, state and local governments. Although a small portion of this report is not reproducible, it is being made available to expedite the availability of information on the research discussed herein.

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“…1 , and have a constant value of about 20 mb, though there can be seen some discrepancy between results measured at TIARA and RIKEN. The ENDFIB-VI data I) which are evaluated according to the values of Anders et al 12) are more than 50 % higher than ours below 40 Me V, however above 40 MeV the ENDFIB-VI data rapidly decrease with energy and give much lower values than our data. 21O-x Bi (x = 3,12) reactions.…”

Section: C(n2n)llc Reactionmentioning

confidence: 81%

“…As clearly seen in Fig.l, the existent cross section data below 40 Me V are clearly divided into two groups, high values by Anders et aI. 12 ) and lower values by Brill et al 13 ) Our data below 40Me V 4 ) agree with the lower values and our data above 40 Me V7) are smoothly connected to our data below 40 MeV in Fig. 1 , and have a constant value of about 20 mb, though there can be seen some discrepancy between results measured at TIARA and RIKEN.…”

Section: C(n2n)llc Reactionmentioning

confidence: 91%

High Energy Neutron Activation Cross Sections

Nakamura

Kim

Uwamino

et al. 2002

Journal of Nuclear Science and Technology

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A systematic study on neutron activation cross-section measurements in the energy from 20 MeV to 150 MeV has been performed over several years. For this study, we have developed the quasi-monoenergetic neutron fields using 7U(p,n) reaction at three AVF cyclotron facilities; 1) Institute for Nuclear Study, University of Tokyo for 20 to 40 MeV protons, 2) Takasaki Institute of Advanced Radiation Applications(TIARA) of Japan Atomic Energy Research Institute(JAERI) for 40 to 90 MeV protons, 3) Institute of Physical and Chemical Research(RIKEN) for 70 to 210 MeV protons. By using these neutron fields, we have measured the activation cross sections of 30Si(n,np), 47Ti(n,np), 48TI(n,np), 52Cr(n,2n), 58Ni(n,2n) in the energy range of 15 to 40 MeV, and of 12qn,2n), 59Co(n,xn) and (n,xnp), natCu(n,xn) and (n,xnp), 209Bi(n,xn) in the energy range of 15 to 80 or 150 MeV. We are now developing a new p-Li quasi-monoenergetic neutron field in the energy range of 20 to 90 MeV using a new AVF cyclotron installed in the Cyclotron and Radioisotope Center, Tohoku University, for measurements of neutron activation cross sections of light elements such as 0 and N which are included in air, water and soil.

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Excitation functions of nuclear reactions producing11C

Cited by 24 publications

References 46 publications

C12(n, 2n)C11 cross section from threshold to 26.5 M

C12(n, 2n)C11 cross section from threshold to 26.5 M

SCINFUL: A Monte Carlo based computer program to determine a scintillator full energy response to neutron detection for E/sub n/ between 0. 1 and 80 MeV: Program development and comparisons of program predictions with experimental data

High Energy Neutron Activation Cross Sections

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