Allotropic effects on the energy loss of swift H+ and He+ ion beams through thin foils

Author(s):  
Rafael Garcia-Molina ◽  
Isabel Abril ◽  
Cristian D. Denton ◽  
Santiago Heredia-Avalos
Keyword(s):  
1976 ◽  
Vol 132 ◽  
pp. 75-77 ◽  
Author(s):  
J.W. Tape ◽  
W.M. Gibson ◽  
J. Remillieux ◽  
R. Laubert ◽  
H.E. Wegner

2006 ◽  
Vol 24 (3) ◽  
pp. 421-425 ◽  
Author(s):  
CLAUDE DEUTSCH ◽  
ROMAIN POPOFF

We have focused our attention on the stopping mechanisms involved in the recently proposed ion beam-target US program. This mechanism emphasizes out production of warm dense matter through pulsed ion beams, linearly accelerated, and interacting with thin foils in Bragg peak conditions. We reviewed the relevant energy loss mechanisms involved at moderate and low velocity ion projectile. Small velocities close to zero are given some attention.


1995 ◽  
Vol 52 (3) ◽  
pp. 3010-3014 ◽  
Author(s):  
E. M. Bringa ◽  
N. R. Arista

1967 ◽  
Vol 45 (12) ◽  
pp. 4039-4051 ◽  
Author(s):  
L. Hastings ◽  
A. van Wijngaarden

Local regions on the surface of ZnO:Zn phosphor samples were deteriorated by a large number of low-energy ions. In this manner thin films which did not luminesce under ion bombardment were prepared. The phosphor samples were then scanned across energetic ion beams with sufficient energy to traverse the thin phosphor films. By comparing the luminescent response to this ion excitation in the damaged and undamaged portions of the phosphor surface, the total average energy losses of 1H, 4He, 14N, 40Ar, and 84Kr in passing through the films were determined. It was found that the energy losses for the heavier projectiles, when compared with the energy loss of hydrogen, are appreciably smaller than the energy losses predicted by the Lindhard and Scharff theory.The deterioration depth of the phosphor under prolonged bombardment is proportional to the speed of the damaging projectiles.


1968 ◽  
Vol 23 (12) ◽  
pp. 1988-1994
Author(s):  
H. Zeidl ◽  
H. Baier

The Monte Carlo method is applied to investigate the penetration of fast electron through thin foils of matter. The “step by step method” is used. Energy loss and secondary electron emission are taken into account. As an example for the possible application of the computational program we calculated “refraction” and “reflection” of relativistic electrons on thin Al-foils. Scattering and reflection depends significantly on the energy loss of the electrons in the foil. The “mean scattering angle” of the electron beam (with respect to the foil normal) has been shown to be smaller than the angle of incidence (with respect to the foil normal). Possible experimental methods to test the predictions on mean scattering and reflection angles (as defined in this paper) are discussed.


1984 ◽  
Vol 2 (1) ◽  
pp. 13-26 ◽  
Author(s):  
P. C. Thompson ◽  
P. D. Roberts

The shock pressures generated in the interaction of lasers and light ion beams with thin foils are calculated using a two-dimensional, axisymmetric hydrodynamic code. For lasers, finite spot sizes produce a significant decrease in the pressure generated, compared to previous 1-D estimates. The effect is closely related to the coupling of the critical density with the ablation surface and is less important at shorter wavelengths, the appropriate parameter being Iλ2. For 0·5 TW red light and a 100 μm radius spot pressures are limited to 30 Mb. Perturbations across the beam profile are discussed and it is demonstrated that beam uniformity of 30% (25% for green light) is required to achieve velocity modulation of less than 2%, such as would be necessary for an equation of state measurement.For the larger targets used with light ion beams, two-dimensional effects prove to be less of a problem, and for high-Z materials the initial 1-D estimates of peak pressure are adequate. In order to obtain the shock planarity requisite for equation of state measurements in a high-Z target an intensity uniformity of ±15% would be required. However, use of a composite target enables this to be relaxed to ±25% whilst obtaining slightly higher pressures.


2011 ◽  
Vol 175 (2) ◽  
pp. 247-255 ◽  
Author(s):  
Isabel Abril ◽  
Rafael Garcia-Molina ◽  
Cristian D. Denton ◽  
Ioanna Kyriakou ◽  
Dimitris Emfietzoglou

Author(s):  
O. L. Krivanek

The structure of bulk surfaces can be studied by reflection electron microscopy and the structure of interfaces in thin foils by TEM. Both methods are capable of nearly atomic-level resolution. This paper explores whether the structural information can be supplemented with chemical and electronic information by the use of electron energy loss spectroscopy.Energy loss spectra from the surface of bulk Be have been obtained at 35kV primary energy by Klein, and spectra of the Si surface at 14.2kV have been obtained by Schilling, who also demonstrated that the relative strength of the volume and the surface plasmon can be altered by changing the reflection geometry.Fig. 1 contains two energy loss spectra obtained in surface reflection from (100) Si at 100kV in a standard TEM (Philips 400) with a magnetic sector energy analyzer (Gatan 607), and a diagram showing the geometry of the incident beam and the beam admitted into the spectrometer relative to the surface.


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