OPTICAL SUM GENERATION OF THE TWO‐FREQUENCY OUTPUT OF A GIANT PULSE RUBY LASER

1967 ◽  
Vol 11 (2) ◽  
pp. 51-53 ◽  
Author(s):  
Daniel J. Bradley ◽  
George Magyar ◽  
Martin C. Richardson
1966 ◽  
Vol 9 (4) ◽  
pp. 150-152 ◽  
Author(s):  
Daniel J. Bradley ◽  
Malcolm S. Engwell ◽  
A. W. McCullough ◽  
George Magyar ◽  
Martin C. Richardson

1968 ◽  
Vol 39 (8) ◽  
pp. 4043-4044 ◽  
Author(s):  
J. E. Bjorkholm ◽  
R. H. Stolen
Keyword(s):  

1969 ◽  
Vol 1 (5) ◽  
pp. 245-247 ◽  
Author(s):  
D.J. Bradley ◽  
C.J. Mitchell ◽  
M.S. Petty

1968 ◽  
Vol 21 (3) ◽  
pp. 168-180
Author(s):  
Kiyoshi HAYASE ◽  
Kenro MIYAMOTO ◽  
Junji FUJITA ◽  
Taijiro UCHIDA

1968 ◽  
Vol 11 (6) ◽  
pp. 546-548
Author(s):  
A. M. Leontovich ◽  
M. N. Popova ◽  
M. Ya. Shchelev

1968 ◽  
Vol 72 (7) ◽  
pp. 2684-2686 ◽  
Author(s):  
Ikuzo Tanaka ◽  
Yuji Mori ◽  
Toshisato Minagawa ◽  
Eiichi Okutsu

1976 ◽  
Vol 24 (5) ◽  
pp. 552-558
Author(s):  
L. A. Lavrovskii ◽  
A. V. Milinkevich ◽  
Y. F. Morgun ◽  
M. A. Muravitskii ◽  
V. A. Savva ◽  
...  

1970 ◽  
Vol 25 (4) ◽  
pp. 488-503 ◽  
Author(s):  
R. Sigel

Abstract Foils of solid hydrogen were irradiated with a giant pulse ruby laser. The formation and ex-pansion of the plasma produced this way was investigated by time-resolved absorption measure-ments, by streak and framing photography, by holographic interferometry and by time-off-flight and charge collection measurements. The measurements yield a fairly complete picture of this process: After the initial breakdown in the solid a plasma is produced at the surface of the foil facing the laser. Owing to the high pressure of the plasma the solid hydrogen is compressed by a shock wave. This allows the layer in which the plasma is produced to penetrate into the interior of the foil with a velocity of 3 × 106 cm/sec. Thus under the action of the focused beam foils up to 1 mm thickness are pierced by the light before the end of the pulse. The plasma cloud, ejected towards the laser, contains 4 × 1016 ions with a mean kinetic energy of 200 eV this corresponding to about half of the absorbed energy. The observations are compared with the well known results obtained in a plane, one-dimensional geometry. If allowance is made for the influence of the focusing of the laser beam on the structure of the shock front, the observations are readily understood.


Sign in / Sign up

Export Citation Format

Share Document