fast-ignition fuel-assembly: theory and experiments r. betti, c.d. zhou, w. theobald k. anderson, a....
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Fast-Ignition Fuel-Assembly:Theory and Experiments
R. Betti, C.D. Zhou, W. TheobaldK. Anderson, A. Solodov
Laboratory for Laser Energetics5th Fusion Science Center Meeting
February 28, Chicago, IL
FSC
C. Zhou, W. Theobald, R. Betti, P.B. Radha, V. Smalyuk, C.K.Li et al, Phys. Rev. Lett. 98: 025004 (2007)
Arb
itra
ry u
nit
s
Energy (MeV)
4 6 8 10 12 14 16 18 200
The maximum R during the burn can be inferredfrom the downshift of the tail of the primary proton spectrum for targets with a 25 atm D-He3 fill
5MeV 14.7MeVBirth energy
9.7MeV E -1.5MeV *broadening =8.2 MeV downshift
2burnmax 0.25g/cmρR
DHe3 Primary Proton spectrum
Fit ofspectrum
FSC
The areal density is measured during the burn.Protons from secondary D-3He reactions are slowed down by the shell areal density
FSC
C. Zhou, W. Theobald, R. Betti, P.B. Radha, V. Smalyuk, C.K.Li et al, Phys. Rev. Lett. 98: 025004 (2007)
FSC
C. Zhou, W. Theobald, R. Betti, P.B. Radha, V. Smalyuk, C.K.Li et al, PRL98: 025004 (2007)
DHe3 Secondary Proton spectrum
Reconstructedspectra
A complete set of hydro-scaling relations is derivedfor fast-ignition target design
C.D. Zhou and R. Betti, submitted to Phys. Plasmas
1.85
0.9 7
345( )
3 10iVP Gbar
Slow implosions lead to a low pressure, low temperature fuel assembly optimal for cone-in-shell targets
FSC1.25
0.15 7
3( )
3 10iVT keV
Next step: slow implosions of cone-in-shell targets