Charge-changing contribution to energy loss of 32 MeV 3He+ in the charge state non-equilibrium region

1991 ◽  
Vol 160 (1) ◽  
pp. 77-80 ◽  
Author(s):  
H. Ogawa ◽  
I. Katayama ◽  
H. Ikegami ◽  
Y. Haruyama ◽  
A. Aoki ◽  
...  
1992 ◽  
Vol 167 (5-6) ◽  
pp. 487-492 ◽  
Author(s):  
H. Ogawa ◽  
I. Katayama ◽  
I. Sugai ◽  
Y. Haruyama ◽  
M. Tosaki ◽  
...  

1981 ◽  
Vol 23 (3) ◽  
pp. 957-966 ◽  
Author(s):  
J. A. Golovchenko ◽  
A. N. Goland ◽  
J. S. Rosner ◽  
C. E. Thorn ◽  
H. E. Wegner ◽  
...  

2014 ◽  
Vol 744 ◽  
pp. 5-37 ◽  
Author(s):  
P. C. Valente ◽  
J. C. Vassilicos

AbstractThe previously reported non-equilibrium dissipation law is investigated in turbulent flows generated by various regular and fractal square grids. The flows are documented in terms of various turbulent profiles which reveal their differences. In spite of significant inhomogeneity and anisotropy differences, the new non-equilibrium dissipation law is observed in all of these flows. Various transverse and longitudinal integral scales are measured and used to define the dissipation coefficient $C_{\varepsilon }$. It is found that the new non-equilibrium dissipation law is not an artefact of a particular choice of the integral scale and that the usual equilibrium dissipation law can actually coexist with the non-equilibrium law in different regions of the same flow.


1995 ◽  
Vol 13 (2) ◽  
pp. 281-292 ◽  
Author(s):  
P. Sigmund ◽  
A. Närmann

A general and powerful formalism has been developed for computation of energy-loss spectra of penetrating charged particles in the presence of charge exchange. Options on the input side are the cross sections for electron capture and loss, transition rates for radiative and nonradiative spontaneous processes and their associated energy losses or gains, and finally, cross sections for all processes that contribute to particle stopping but are not associated with charge exchange. The formalism generates an n × n transfer matrix, where n is the number of states needed for an adequate description of the projectile under consideration. This matrix delivers the joint distribution of energy loss and exit charge state for a given incident charge state and energy.The formalism can be used in principle as an alternative for Monte Carlo simulation, but until now we have concentrated on direct evaluation of key experimental parameters related to the energy-loss spectrum integrated over all exit charge states, in particular, mean energy loss, straggling, and skewness. Generally, valid analytic expressions have been found for these quantities, each of which can be separated into a stationary term representing chargestate equilibrium and a transient depending on the incident charge state. A brief survey is given of current analytic and numerical efforts addressing other experimental parameters.


1997 ◽  
Vol 79 (11) ◽  
pp. 2030-2033 ◽  
Author(s):  
T. Schenkel ◽  
M. A. Briere ◽  
A. V. Barnes ◽  
A. V. Hamza ◽  
K. Bethge ◽  
...  

2016 ◽  
Vol 93 (5) ◽  
Author(s):  
Richard A. Wilhelm ◽  
Elisabeth Gruber ◽  
Valerie Smejkal ◽  
Stefan Facsko ◽  
Friedrich Aumayr

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