scholarly journals Dynamics of the super pinch electron beam and fusion energy perspective

Author(s):  
D. R. Welch ◽  
D. V. Rose ◽  
D. V. Novikov ◽  
M. E. Weller ◽  
A. A. Esaulov ◽  
...  
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2009 ◽  
Vol 56 (1) ◽  
pp. 346-351 ◽  
Author(s):  
P. M. Burns ◽  
M. Myers ◽  
J. D. Sethian ◽  
M. F. Wolford ◽  
J. L. Giuliani ◽  
...  

Author(s):  
S. P. Obenschain ◽  
A. J. Schmitt ◽  
J. W. Bates ◽  
M. F. Wolford ◽  
M. C. Myers ◽  
...  

Argon fluoride (ArF) is currently the shortest wavelength laser that can credibly scale to the energy and power required for high gain inertial fusion. ArF's deep ultraviolet light and capability to provide much wider bandwidth than other contemporary inertial confinement fusion (ICF) laser drivers would drastically improve the laser target coupling efficiency and enable substantially higher pressures to drive an implosion. Our radiation hydrodynamics simulations indicate gains greater than 100 are feasible with a sub-megajoule ArF driver. Our laser kinetics simulations indicate that the electron beam-pumped ArF laser can have intrinsic efficiencies of more than 16%, versus about 12% for the next most efficient krypton fluoride excimer laser. We expect at least 10% ‘wall plug' efficiency for delivering ArF light to target should be achievable using solid-state pulsed power and efficient electron beam transport to the laser gas that was demonstrated with the U.S. Naval Research Laboratory's Electra facility. These advantages could enable the development of modest size and lower cost fusion power plant modules. This would drastically change the present view on inertial fusion energy as being too expensive and the power plant size too large. This article is part of a discussion meeting issue ‘Prospects for high gain inertial fusion energy (part 1)'.


2001 ◽  
Vol 40 (Part 1, No. 2B) ◽  
pp. 1152-1155 ◽  
Author(s):  
Isao Okuda ◽  
Eiichi Takahashi ◽  
Isao Matsushima ◽  
Yuji Matsumoto ◽  
Susumu Kato ◽  
...  

2007 ◽  
Vol 52 (3) ◽  
pp. 445-453 ◽  
Author(s):  
P. M. Burns ◽  
M. Myers ◽  
J. D. Sethian ◽  
M. F. Wolford ◽  
J. L. Giuliani ◽  
...  
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2004 ◽  
Vol 92 (7) ◽  
pp. 1043-1056 ◽  
Author(s):  
J.D. Sethian ◽  
R.V. Smilgys ◽  
S.B. Swanekamp ◽  
D. Weidenheimer ◽  
D. Giorgi ◽  
...  

2003 ◽  
Vol 10 (5) ◽  
pp. 2142-2146 ◽  
Author(s):  
J. D. Sethian ◽  
M. Friedman ◽  
J. L. Giuliani ◽  
R. H. Lehmberg ◽  
S. P. Obenschain ◽  
...  
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Author(s):  
G. G. Shaw

The morphology and composition of the fiber-matrix interface can best be studied by transmission electron microscopy and electron diffraction. For some composites satisfactory samples can be prepared by electropolishing. For others such as aluminum alloy-boron composites ion erosion is necessary.When one wishes to examine a specimen with the electron beam perpendicular to the fiber, preparation is as follows: A 1/8 in. disk is cut from the sample with a cylindrical tool by spark machining. Thin slices, 5 mils thick, containing one row of fibers, are then, spark-machined from the disk. After spark machining, the slice is carefully polished with diamond paste until the row of fibers is exposed on each side, as shown in Figure 1.In the case where examination is desired with the electron beam parallel to the fiber, preparation is as follows: Experimental composites are usually 50 mils or less in thickness so an auxiliary holder is necessary during ion milling and for easy transfer to the electron microscope. This holder is pure aluminum sheet, 3 mils thick.


Author(s):  
Kenneth H. Downing ◽  
Robert M. Glaeser

The structural damage of molecules irradiated by electrons is generally considered to occur in two steps. The direct result of inelastic scattering events is the disruption of covalent bonds. Following changes in bond structure, movement of the constituent atoms produces permanent distortions of the molecules. Since at least the second step should show a strong temperature dependence, it was to be expected that cooling a specimen should extend its lifetime in the electron beam. This result has been found in a large number of experiments, but the degree to which cooling the specimen enhances its resistance to radiation damage has been found to vary widely with specimen types.


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