Neutron-proton charge exchange at high energies. A crucial reaction

1975 ◽  
Vol 28 (2) ◽  
pp. 137-154 ◽  
Author(s):  
B. Diu ◽  
E. Leader
Keyword(s):  
Charge Exchange ◽  
High Energies ◽  
Proton Charge

Non-regge and hyper-regge effects in pion-nucleon charge exchange scattering at high energies

1975 ◽  
Vol 30 (3) ◽  
pp. 345-384 ◽  
Author(s):  
D. Joynson ◽  
E. Leader ◽  
B. Nicolescu ◽  
C. Lopez
Keyword(s):  
Charge Exchange ◽  
High Energies ◽  
Pion Nucleon ◽  
Exchange Scattering

scholarly journals Pion Charge-Exchange Scattering at High Energies

1976 ◽  
Vol 37 (2) ◽  
pp. 76-79 ◽  
Author(s):  
A. V. Barnes ◽  
D. J. Mellema ◽  
A. V. Tollestrup ◽  
R. L. Walker ◽  
O. I. Dahl ◽  
...  
Keyword(s):  
Charge Exchange ◽  
High Energies ◽  
Exchange Scattering

Charge Exchange Cross Sections of Hydrogen Particles in Gases at High Energies

1958 ◽  
Vol 109 (2) ◽  
pp. 355-359 ◽  
Author(s):  
C. F. Barnett ◽  
H. K. Reynolds
Keyword(s):  
Charge Exchange ◽  
Cross Sections ◽  
High Energies

scholarly journals Effects of oblique incidence and colliding pulses on laser-driven proton acceleration from relativistically transparent ultrathin targets

2020 ◽  
Vol 86 (5) ◽  
Author(s):  
J. Ferri ◽  
E. Siminos ◽  
L. Gremillet ◽  
T. Fülöp
Keyword(s):  
Oblique Incidence ◽  
Laser Pulses ◽  
High Energy ◽  
Femtosecond Laser Pulses ◽  
Reference Case ◽  
Proton Acceleration ◽  
Ion Energy ◽  
High Energies ◽  
Proton Charge ◽  
Induced Transparency

The use of ultrathin solid foils offers optimal conditions for accelerating protons to high energies from laser–matter interactions. When the target is thin enough that relativistic self-induced transparency sets in, all of the target electrons get heated to high energies by the laser, which maximizes the accelerating electric field and therefore the final ion energy. In this work, we first investigate how ion acceleration by ultraintense femtosecond laser pulses in transparent CH $_2$ solid foils is modified when turning from normal to oblique ( $45^\circ$ ) incidence. Due to stronger electron heating, we find that higher proton energies can be obtained at oblique incidence but in thinner optimum targets. We then show that proton acceleration can be further improved by splitting the laser pulse into two half-pulses focused at opposite incidence angles. An increase by ${\sim }30\,\%$ in the maximum proton energy and by a factor of ${\sim }4$ in the high-energy proton charge is reported compared to the reference case of a single normally incident pulse.

Inclusive Kaon Charge Exchange in the Triple-Regge Region at High Energies

1981 ◽  
Vol 46 (21) ◽  
pp. 1358-1361 ◽  
Author(s):  
P. M. Yager ◽  
H. G. E. Kobrak ◽  
R. E. Pitt ◽  
R. A. Swanson ◽  
K. W. Edwards ◽  
...  
Keyword(s):  
Charge Exchange ◽  
High Energies ◽  
Regge Region

Neutron-proton charge exchange scattering between 190 MeV and 590 MeV

1980 ◽  
Vol 90 (4) ◽  
pp. 367-370 ◽  
Author(s):  
W. Hürster ◽  
Th. Fischer ◽  
G. Hammel ◽  
K. Kern ◽  
M. Kleinschmidt ◽  
...  
Keyword(s):  
Charge Exchange ◽  
Proton Charge ◽  
Exchange Scattering

Antiproton-proton charge exchange between 1 and 3 GeV/c

1978 ◽  
Vol 17 (1) ◽  
pp. 16-23 ◽  
Author(s):  
D. Cutts ◽  
M. L. Good ◽  
P. D. Grannis ◽  
D. Green ◽  
Y. Y. Lee ◽  
...  
Keyword(s):  
Charge Exchange ◽  
Proton Charge
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