Relativistic theory of atom-laser interactions at very high laser intensities

2000 ◽  
Vol 63 (4) ◽  
pp. 642-647
Author(s):  
A. M. Ermolaev
1995 ◽  
Vol 388 ◽  
Author(s):  
Rand R. Biggers. ◽  
M. Grant Norton ◽  
I. Maartense ◽  
T.L. Peterson ◽  
E. K. Moser ◽  
...  

AbstractThe pulsed-laser deposition (PLD) technique utilizes one of the most energetic beams available to form thin films of the superconducting oxide YBa2Cu3O7 (YBCO). IN this study we examine the growth of YBCO at very high laser fluences (25 to 40 J/cm2); a more typical fluence for PLD would be nearer to 3 J/cm2. the use of high fluences leads to unique film microstructures which, in some cases, appear to be related to the correspondingly higher moveabilities of the adatoms. Films grown on vicinal substrates, using high laser fluences, exhibited well-defined elongated granular morphologies (with excellent transition temperature, Tc, and critical current density, Jc). Films grown on vicinal substrates using off-axis magnetron sputtering, plasma-enhanced metal organic chemical vapor deposition (PE-MOCVD), or PLD at more typical laser fluences showed some similar morphologies, but less well-defined. Under certain growth conditions, using high laser fluences with (001) oriented substrates, the YBCO films can exhibit a mixture of a- and c-axis growth where both crystallographic orientations nucleate on the substrate surface at the same time, and grow in concert. the ratio of a-axis oriented to c-axis oriented grains is strongly affected by the pulse repetition rate of the laser.


1999 ◽  
Vol 61 (2) ◽  
pp. 263-273 ◽  
Author(s):  
FREDERICK OSMAN ◽  
REYNALDO CASTILLO ◽  
HEINRICH HORA

The nonlinear plasma dielectric function due to relativistic electron motion is derived. From this, one can obtain the nonlinear refractive index of the plasma and estimate the importance of relativistic self-focusing in comparison with ponderomotive non-relativistic self-focusing at very high laser intensities. When the laser intensity is very high, ponderomotive self-focusing will be dominant. However, at some point, when the oscillating velocity of the plasma electrons becomes very large, relativistic effects will also play a role in self-focusing.


1976 ◽  
Vol 36 (16) ◽  
pp. 949-952 ◽  
Author(s):  
L. A. Lompre ◽  
G. Mainfray ◽  
C. Manus ◽  
S. Repoux ◽  
J. Thebault

1998 ◽  
Vol 81 (14) ◽  
pp. 2882-2885 ◽  
Author(s):  
Richard Taïeb ◽  
Valérie Véniard ◽  
Alfred Maquet

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