scholarly journals The Yield of Neutral Mesons from Proton Bombardment of Light Nuclei

1952 ◽  
Vol 85 (2) ◽  
pp. 373-374 ◽  
Author(s):  
R. W. Hales ◽  
R. H. Hildebrand ◽  
N. Knable ◽  
B. J. Moyer
Keyword(s):  
Light Nuclei ◽  
Proton Bombardment ◽  
Neutral Mesons

scholarly journals Gamma-Radiation from Light Nuclei under Proton Bombardment

1948 ◽  
Vol 73 (2) ◽  
pp. 181-182 ◽  
Author(s):  
W. A. Fowler ◽  
C. C. Lauritsen ◽  
T. Lauritsen
Keyword(s):  
Gamma Radiation ◽  
Light Nuclei ◽  
Proton Bombardment

Alpha particles from the proton bombardment of light nuclei

Physica ◽  
1963 ◽  
Vol 29 (12) ◽  
pp. 1281-1295 ◽  
Author(s):  
J. Kuperus ◽  
P.W.M. Glaudemans ◽  
P.M. Endt
Keyword(s):  
Alpha Particles ◽  
Light Nuclei ◽  
Proton Bombardment

The angular distribution of γ-radiation from light nuclei I. Experimental

1949 ◽  
Vol 199 (1056) ◽  
pp. 56-73 ◽  
Keyword(s):  
Angular Distribution ◽  
Proton Energy ◽  
The Other ◽  
Light Nuclei ◽  
Proton Bombardment ◽  
Proton Capture ◽  
Γ Radiation ◽  
Experimental Procedure

The experimental procedure used in studying the angular distribution of γ-radiation produced by the proton bombardment of some light nuclei is described. Results are given for the radiation following proton capture by the nuclei Li 7 , Be 9 , C 12 , C 13 and for the radiation from the residual O 16* nucleus produced in the reaction F 19 ( p , α) O 16* . Proton energies between 300 and 1000 keV were available. The distribution of the radiation from Li 7 was investigated over the whole range of energies; in the other cases the distribution was measured at energies corresponding to resonance maxima for the processes. The main results are: reaction Li 7 ( p , γ) Be 8 Be 9 ( p , γ) B 10 C 12 ( p , γ) N 13 C 13 ( p , γ) N 14 F 19 ( p , α) O 16* proton energy (keV) 440 960 450 550 330, 470 and 670 590 870 angular distribution 1+ 0.05 cosθ 1 + 0.09 sin 2 θ isotropic isotropic isotropic 1 + 0.2 cos 2 θ 1 + 0.1 cos 2 θ

COMBINATIONAL APPROACH AND A LOOK INTO THE PARTICLE PRODUCTION DATA AT 530 and 800 GeV/c

2005 ◽  
Vol 20 (29) ◽  
pp. 2227-2244 ◽  
Author(s):  
BHASKAR DE ◽  
S. K. BISWAS ◽  
S. BHATTACHARYYA
Keyword(s):  
Particle Production ◽  
High Energy ◽  
Light Nuclei ◽  
Production Data ◽  
Proton Proton ◽  
Nuclear Collisions ◽  
Neutral Mesons

In the light of the combinational approach that has been recently utilized to accommodate data from high energy nuclear collisions, we attempt here to interpret the nature of the latest data obtained by E706 collaboration of FERMILAB on neutral mesons produced in both proton–proton (PP) and proton–beryllium (P Be ) collisions. The study demonstrates that the approach can be useful for analyzing data on particle production in collisions involving both heavy and relatively much light nuclei such as beryllium.

scholarly journals Gamma-Radiation from Light Nuclei under Proton Bombardment

1949 ◽  
Vol 76 (2) ◽  
pp. 314-315 ◽  
Author(s):  
W. A. Fowler ◽  
C. C. Lauritsen
Keyword(s):  
Gamma Radiation ◽  
Light Nuclei ◽  
Proton Bombardment

Production of Light Neutral Mesons in Ultrarelativistic Cu + Au and U + U Collisions in the Region of Mean Velocities

2020 ◽  
Vol 84 (10) ◽  
pp. 1269-1274
Author(s):  
A. Berdnikov ◽  
Y. Berdnikov ◽  
S. Zharko ◽  
D. Kotov ◽  
P. Radzevich
Keyword(s):  
Neutral Mesons

Proposed Solutions to Achieve Nuclear Fusion

Engevista ◽  
2017 ◽  
Vol 19 (5) ◽  
pp. 1496
Author(s):  
Relly Victoria Virgil Petrescu ◽  
Raffaella Aversa ◽  
Antonio Apicella ◽  
Florian Ion Petrescu
Keyword(s):  
Nuclear Reactor ◽  
Nuclear Reactions ◽  
Nuclear Fusion ◽  
Nuclear Fission ◽  
Light Nuclei ◽  
Fast Neutrons ◽  
Fusion Reactions ◽  
Nuclear Fusion Reactions ◽  
The Masses ◽  
Fusion Products

Despite research carried out around the world since the 1950s, no industrial application of fusion to energy production has yet succeeded, apart from nuclear weapons with the H-bomb, since this application does not aims at containing and controlling the reaction produced. There are, however, some other less mediated uses, such as neutron generators. The fusion of light nuclei releases enormous amounts of energy from the attraction between the nucleons due to the strong interaction (nuclear binding energy). Fusion it is with nuclear fission one of the two main types of nuclear reactions applied. The mass of the new atom obtained by the fusion is less than the sum of the masses of the two light atoms. In the process of fusion, part of the mass is transformed into energy in its simplest form: heat. This loss is explained by the Einstein known formula E=mc2. Unlike nuclear fission, the fusion products themselves (mainly helium 4) are not radioactive, but when the reaction is used to emit fast neutrons, they can transform the nuclei that capture them into isotopes that some of them can be radioactive. In order to be able to start and to be maintained with the success the nuclear fusion reactions, it is first necessary to know all this reactions very well. This means that it is necessary to know both the main reactions that may take place in a nuclear reactor and their sense and effects. The main aim is to choose and coupling the most convenient reactions, forcing by technical means for their production in the reactor. Taking into account that there are a multitude of possible variants, it is necessary to consider in advance the solutions that we consider them optimal. The paper takes into account both variants of nuclear fusion, and cold and hot. For each variant will be mentioned the minimum necessary specifications.

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