Neutron-proton Bremsstrahlung Inclusive Photon Measurements from 100 to 280 MeV

Neutron-proton Bremsstrahlung Inclusive Photon Measurements from 100 to 280 MeV PDF Author: Douglas Ray Mayo
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ISBN:
Category :
Languages : en
Pages : 494

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Neutron-proton Bremsstrahlung Inclusive Photon Measurements from 100 to 280 MeV

Neutron-proton Bremsstrahlung Inclusive Photon Measurements from 100 to 280 MeV PDF Author: Douglas Ray Mayo
Publisher:
ISBN:
Category :
Languages : en
Pages : 494

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A Measurement of Neutron-proton Bremsstrahlung Near 130 MeV

A Measurement of Neutron-proton Bremsstrahlung Near 130 MeV PDF Author: J.A. Edgington
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ISBN:
Category :
Languages : en
Pages : 26

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Neutron-proton Bremsstrahlung Measurements at 208 MeV.

Neutron-proton Bremsstrahlung Measurements at 208 MeV. PDF Author: John Chancellor Young
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ISBN:
Category :
Languages : en
Pages : 290

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Neutron-proton Bremsstrahlung Experiments

Neutron-proton Bremsstrahlung Experiments PDF Author:
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Category :
Languages : en
Pages : 8

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It is well known that charged particles emit bremsstrahlung radiation when they are accelerated. Classical electron bremsstrahlung occurs when a photon is emitted by an electron accelerated in the field of a nucleus. The bremsstrahlung process also occurs in the scattering of nucleons, for which it is the lowest energy inelastic process that can occur. Like electron bremsstrahlung, nucleon-nucleon bremsstrahlung also requires the exchange of a virtual particle to conserve energy and momentum. In electron bremsstrahlung a virtual photon is exchanged but with two nucleons a meson can be exchanged. Unlike electron bremsstrahlung, in nucleon-nucleon bremsstrahlung the photon can originate from the exchanged meson. This exchange contribution has been shown in calculations to be a significant fraction of bremsstrahlung events. Thus bremsstrahlung serves as a probe of exchange currents in the nucleon-nucleon interaction. Because of a lack of a free neutron target or an intense neutron beam, few measurements of neutron-proton bremsstrahlung exist, each having poor statistical accuracy and poor energy resolution. The white neutron source at the Weapons Neutron Research (WNR) target area at the Los Alamos Meson Physics Facility (LAMPF) produces neutrons with energies from below 50 to above 400 MeV. Using time-of-flight techniques and a liquid hydrogen target, we are measuring the outgoing photons of energies up to 250 MeV at gamma ray angles of around 90[degree] relative to the incident beam. Protons scattered at very forward angles are also detected in coincidence with the gamma rays.

Neutron- Proton Bremsstrahlung

Neutron- Proton Bremsstrahlung PDF Author: Yaşar Safkan
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ISBN:
Category :
Languages : en
Pages : 240

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The triply-differential cross section for neutron-proton bremsstrahlung (np -+ np[gamma]) was measured at the WNR facility of Los Alamos National Laboratory. A liquid hydrogen target was exposed to the pulsed neutron beam, and the scattered neutrons and recoil protons were observed in coincidence at angles of 20°, 28°, and 36° on opposite sides of the beam. Measuring the proton and neutron energies allows the reconstruction of the full kinematics for each event. Events with incident neutron energies between 175 and 275 MeV are included in the data analysis so as to remain below the pion production threshold. The resulting photon angular distributions for each of the nine angle pairs are presented, and are compared with theoretical predictions.

Nuclear Science Abstracts

Nuclear Science Abstracts PDF Author:
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Category : Nuclear energy
Languages : en
Pages : 612

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Dose Measurements of Bremsstrahlung-Produced Neutrons at the Advanced Photon Source

Dose Measurements of Bremsstrahlung-Produced Neutrons at the Advanced Photon Source PDF Author:
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Category :
Languages : en
Pages : 42

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Bremsstrahlung is generated in the storage rings of the synchrotron radiation facilities by the radiative interaction of the circulating particle beam with both the residual gas molecules and storage ring components. These bremsstrahlung photons, having an energy range of zero to the maximum energy of the particle beam, interact with beamline components like beam stops and collimators generating photoneutrons of varying energies. There are three main processes by which photoneutrons may be produced by the high energy bremsstrahlung photons: giant nuclear dipole resonance and decay (10 MeV E{sub {gamma}} 30 MeV), quasi-deuteron production and decay (50 MeV

Neutron-proton Bremsstrahlung at 4.8 MeV.

Neutron-proton Bremsstrahlung at 4.8 MeV. PDF Author: John Whittaker
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ISBN:
Category : Physics
Languages : en
Pages : 222

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ASYMMETRIC NEUTRON--PROTON BREMSSTRAHLUNG AT 130 MeV.

ASYMMETRIC NEUTRON--PROTON BREMSSTRAHLUNG AT 130 MeV. PDF Author:
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Category :
Languages : en
Pages :

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Coincident Neutron/proton Pairs from 6̳Li Photodisintegration with 40-100 MeV Photons

Coincident Neutron/proton Pairs from 6̳Li Photodisintegration with 40-100 MeV Photons PDF Author: Buddy Boyce Ritchie
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ISBN:
Category :
Languages : en
Pages : 362

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