scholarly journals The Photoneutron Cross Section of 9Be in the Intermediate Energy Range

1959 ◽  
Vol 12 (1) ◽  
pp. 21 ◽  
Author(s):  
HH Thies ◽  
BM Spicer ◽  
JEE Baglln
Keyword(s):  
Energy Range ◽  
Cross Section ◽  
Level Scheme ◽  
Complex Shape ◽  
Intermediate Energy ◽  
Bremsstrahlung Radiation ◽  
Integrated Cross Section ◽  
The Cross

The photoneutron cross section of DBe has been measured in the region from 6�5 to 18 MeV, using filtered bremsstrahlung radiation from an 18 MeV synchrotron. The integrated cross section is in agreement with an earlier experiment, but increased resolution has shown a more complex shape, with sharp maxima at 1l�25�O�2 and 13� 25 � 0�2 MeV. The significant features of the cross section are discussed and compared with the level scheme as it is known at present.

Integrated Cross Section for a Velocity-Dependent Potential

1961 ◽  
Vol 123 (6) ◽  
pp. 2177-2179 ◽  
Author(s):  
O. Rojo ◽  
J. S. Levinger
Keyword(s):  
Cross Section ◽  
Dependent Potential ◽  
Integrated Cross Section

INCLUSIVE TRITIUM STRIPPING REACTION THEORY

1996 ◽  
Vol 05 (01) ◽  
pp. 107-119 ◽  
Author(s):  
A.I. AKHIEZER ◽  
A.P. SOZNIK ◽  
YU. A. BEREZHNOY
Keyword(s):  
Cross Section ◽  
Transfer Reaction ◽  
Energy Distributions ◽  
Nucleon Transfer ◽  
Intermediate Energies ◽  
Reaction Theory ◽  
Integrated Cross Section

The angular and energy distributions and the integrated cross-section of the inclusive two-nucleon transfer reaction with the participation of three-nucleon nucleus were calculated at intermediate energies.

PHOTONEUTRON THRESHOLD AND CROSS SECTION FOR 71Lu175

1958 ◽  
Vol 36 (4) ◽  
pp. 415-418 ◽  
Author(s):  
H. J. King ◽  
L. Katz
Keyword(s):  
Cross Section ◽  
Neutron Yield ◽  
Giant Resonance ◽  
Threshold Energy ◽  
Half Width ◽  
Bremsstrahlung Energy ◽  
Resonance Cross Section ◽  
Integrated Cross Section ◽  
Peak Value

The neutron yield resulting from photoneutron reactions in Lu175 has been measured as a function of peak bremsstrahlung energy up to 23 Mev. The threshold energy for this reaction was found to be 7.77 ± 0.05 Mev. The giant resonance cross section has a peak value of 225 millibarns at 16 Mev., a half-width of 8.4 Mev., and an integrated cross section to 23 Mev. of 1.9 Mev-barns.

Fluctuations in the integrated cross section of the reaction 45Sc(p, n)45Ti

1967 ◽  
Vol 96 (3) ◽  
pp. 521-528 ◽  
Author(s):  
K.V.K. Iyengar ◽  
S.K. Gupta ◽  
K.K. Sekharan ◽  
M.K. Mehta ◽  
A.S. Divatia
Keyword(s):  
Cross Section ◽  
Integrated Cross Section

Differential and Angle-Integrated Cross-Section Measurement for the6Li(n,t)4He Reaction atEn= 1.05, 1.54, and 2.25 MeV

2006 ◽  
Vol 153 (1) ◽  
pp. 41-45 ◽  
Author(s):  
Guohui Zhang ◽  
Rongtai Cao ◽  
Jinxiang Chen ◽  
Guoyou Tang ◽  
Yu. M. Gledenov ◽  
...  
Keyword(s):  
Cross Section ◽  
Cross Section Measurement ◽  
Section Measurement ◽  
Integrated Cross Section

Photoneutron Cross Sections in 14N

1972 ◽  
Vol 50 (15) ◽  
pp. 1689-1696 ◽  
Author(s):  
R. W. Gellie ◽  
K. H. Lokan ◽  
N. K. Sherman ◽  
R. G. Johnson ◽  
J. I. Lodge
Keyword(s):  
Excited States ◽  
Cross Section ◽  
Cross Sections ◽  
Neutron Emission ◽  
Giant Resonance ◽  
Sequential Decay ◽  
Dipole Resonance ◽  
Intermediate States ◽  
Integrated Cross Section ◽  
High Degree

Photoneutron distributions from 14N have been obtained by time-of-flight methods, for bremsstrahlung end-point energies increasing in 2 MeV steps from 15.5 to 29.5 MeV. A large part of the neutron yield is associated with the sequential decay of 14N to 12C, through well-defined intermediate states of 13C, at 7.55, 8.86, and 11.80 MeV, which are unstable against neutron emission. The (γ,n0) cross section for neutron emission to the ground state of 13N is found to agree very closely with the corresponding (γ,p0) cross section, implying a high degree of isospin purity for the giant dipole resonance of 14N. It is observed that the decay of the giant resonance proceeds freely through those odd-parity excited states of the A = 13 nuclei which are single hole states formed by the removal of a p-shell nucleon from the parent 14N.The integrated cross section for all neutron-producing interactions is found to be 88 ± 5 MeV mb.

scholarly journals Evaluation of the 239Pu(n,2n) Integrated Cross Section

2001 ◽  
Author(s):  
D P McNabb ◽  
J D Anderson ◽  
R W Bauer ◽  
J A Becker ◽  
F Dietrich ◽  
...  
Keyword(s):  
Cross Section ◽  
Integrated Cross Section

scholarly journals EXPERIMENTAL TESTS ON THE LIFETIME ASYMMETRY

2011 ◽  
Vol 26 (13) ◽  
pp. 987-998 ◽  
Author(s):  
ZHI-QIANG SHI ◽  
GUANG-JIONG NI
Keyword(s):  
Cross Section ◽  
Z Boson ◽  
Particle Physics ◽  
Test Problem ◽  
Precise Measurement ◽  
Experimental Tests ◽  
Moller Scattering ◽  
The Standard Model ◽  
Integrated Cross Section ◽  
Important Significance

The experimental test problem of the left–right polarization-dependent lifetime asymmetry is discussed. It shows that the existing experiments cannot demonstrate the lifetime asymmetry to be right or wrong after analyzing the measurements on the neutron, the muon and the tau lifetime, as well as the g-2 experiment. However, it is pointed out emphatically that the SLD and the E158 experiments, the measurements of the left–right integrated cross section asymmetry in Z boson production by e+e- collisions and by electron–electron Møller scattering, can indirectly demonstrate the lifetime asymmetry. In order to directly demonstrate the lifetime asymmetry, we propose some possible experiments on the decays of polarized muons. The precise measurement of the lifetime asymmetry could have important significance for building a muon collider, also in cosmology and astrophysics. It would provide a sensitive test of the standard model in particle physics and allow for exploration of the possible V+A interactions.

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