Scaling laws for temperature and reflectivity of plasma generated by a short neodymium laser pulse

1980 ◽  
Vol 13 (7) ◽  
pp. 1221-1233 ◽  
Author(s):  
T P Donaldson ◽  
J E Balmer ◽  
J A Zimmermann
2009 ◽  
Vol 79 (3) ◽  
Author(s):  
Yongsheng Huang ◽  
Yuanjie Bi ◽  
Yijin Shi ◽  
Naiyan Wang ◽  
Xiuzhang Tang ◽  
...  

2005 ◽  
Vol 23 (4) ◽  
pp. 401-409 ◽  
Author(s):  
J. BADZIAK ◽  
S. GŁOWACZ ◽  
S. JABŁOŃSKI ◽  
P. PARYS ◽  
J. WOŁOWSKI ◽  
...  

Basic properties of generation of high-current ion beams using the skin-layer ponderomotive acceleration (S-LPA) mechanism, induced by a short laser pulse interacting with a solid target are studied. Simplified scaling laws for the ion energies, the ion current densities, the ion beam intensities, and the efficiency of ions' production are derived for the cases of subrelativistic and relativistic laser-plasma interactions. The results of the time-of-flight measurements performed for both backward-accelerated ion beams from a massive target and forward-accelerated beams from a thin foil target irradiated by 1-ps laser pulse of intensity up to ∼ 1017 W/cm2 are presented. The ion current densities and the ion beam intensities at the source obtained from these measurements are compared to the ones achieved in recent short-pulse experiments using the target normal sheath acceleration (TNSA) mechanism at relativistic (>1019 W/cm2) laser intensities. The possibility of application of high-current ion beams produced by S-LPA at relativistic intensities for fast ignition of fusion target is considered. Using the derived scaling laws for the ion beam parameters, the achievement conditions for ignition of compressed DT fuel with ion beams driven by ps laser pulses of total energy ≤ 100 kJ is shown.


2005 ◽  
Vol 71 (11) ◽  
Author(s):  
M. Mero ◽  
J. Liu ◽  
W. Rudolph ◽  
D. Ristau ◽  
K. Starke

2007 ◽  
Vol 89 (4) ◽  
pp. 549-552 ◽  
Author(s):  
D. Lin ◽  
Q. Kong ◽  
Z. Chen ◽  
P.X. Wang ◽  
J.J. Xu ◽  
...  

1989 ◽  
Vol 7 (2) ◽  
pp. 249-258 ◽  
Author(s):  
K. Mima ◽  
H. Takabe ◽  
S. Nakai

The conventional implosion scheme for high gain and high density compression depends upon the piston action of an accelerated heavy pusher. However, the contact surface between the pusher and the fuel layer is very unstable in the stagnation phase. In this paper, the laser pulse tailoring and the scaling laws for pellet gain, fuel ρR, etc. are discussed under the condition of very weak piston action of the pusher. The scaling laws indicate that the fuel will be ignited by 100 kJ, 0·35 μm wavelength laser irradiation.


1972 ◽  
Vol 14 ◽  
pp. 561-562 ◽  
Author(s):  
F. E. Irons ◽  
N. J. Peacock

The technique for absolute calibration using the branching ratio of two transitions which have a common upper level but widely separated energies has been employed and described by Griffin and McWhirter (1961).Using the plasma produced by irradiation of a carbon target with a 1 GW, 6 nsec duration, neodymium laser pulse, we have been able to calibrate a grazing incidence spectrograph at the wavelength (25.83 Å) of the 7–1 transition in C VI by direct comparison with the intensity of the 7–6 (3434 Å) transition emitted from the same ions in the plasma. The spectrum from a similar carbon plasma has been described by Boland et al. (1968) and in several ways is ideal for this type of measurement.


Author(s):  
Zhuoran Ma ◽  
Zhe Wang ◽  
Feichao Fu ◽  
Rui Wang ◽  
Dao Xiang

We propose a proof-of-principle experiment to test a new scheme to produce a single-cycle radiation pulse in free-electron lasers (FELs). Here, a few ${\it\alpha}$ -BBO crystals will be first used to produce an equally spaced laser pulse train. Then, the laser pulse train illuminates the cathode to produce a frequency-chirped electron bunch train in a photocathode rf gun. Finally, the frequency-chirped electron bunch train passes through a tapered undulator to produce a quasi-single-cycle THz pulse. This experiment should allow comparison and confirmation of predictive models and scaling laws, and the preliminary experimental results will also be discussed.


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