Title: Time evolution of fields outside imploding directdrive capsules
1Time evolution of fields outside imploding
direct-drive capsules
Drive laser
Fredrick Séguin et al., MIT APS
2007
2Summary
Time-gated radiography shows a rich and complex
evolution of field structures in and around
imploding ICF capsules
- Different field structures appear during
well-defined time intervals - The field structures may be connected with
previous observations - Shells of charge ? Ablator ion spectrum features
- Radial filaments ? Anisotropies in fluence of
charged fusion products
Fredrick Séguin et al., MIT APS
2007
3Collaborators
MIT
U of R LLE
General Atomics
Implosions were supplied by the NLUF program
Fredrick Séguin et al., MIT APS
2007
4Experiment setup
- Subject capsule
- Spherical
- 20-µm CH shell
- 15-atm H2 fill
- 840-µm OD
- Drive beams
- 40
- 1-ns square
- SSD
- 15 kJ
- Proton backlighter
- 15-MeV p
- 120 ps
- 40 µm FWHM
CR-39 Detector
0.9 cm
30 cm
5laser
6Image structures at early times show expanding
charge shells
0.35 ns 0.55 ns
? Fluence
? Energy
Fluence images Darker means more
protons. Energy images Darker means lower
energy, or more matter traversed.
7Monte Carlo simulations illustrate how the images
have the signature of CH shell charge shells
8The observed discrete shells of positive
charge may reflect the ablator protons we see in
spectrum peaks
0.35 ns 0.55 ns
9The observed discrete shells of positive
charge may reflect the ablator protons we see in
spectrum peaks
0.35 ns 0.55 ns
- Our images imply 1011 protons / shell
- Measured spectra typically contain
- 1011 to 1013 protons / peak
D. Hicks, PoP 2001
10The observed discrete shells of positive
charge may reflect the ablator protons we see in
spectrum peaks
0.35 ns 0.55 ns
D. Hicks, PoP 2001
11laser
12Image structures at later times show radial
filaments
0.8 ns 1.2 ns 1.6
ns 1.9 ns
13Azimuthal lineout
What are the radial filaments?
- Strands of dense matter?
- E fields around filaments of charge?
- B fields around filaments of current?
- Isolated bundles of B?
- More complicated, periodic B fields?
14Azimuthal lineout
Fluence
What are the radial filaments?
- Strands of dense matter?
- E fields around filaments of charge?
- B fields around filaments of current?
- Isolated bundles of B?
- More complicated, periodic B fields?
15Azimuthal lineout
Fluence
What are the radial filaments?
- Strands of dense matter?
- E fields around filaments of charge?
- B fields around filaments of current?
- Isolated bundles of B?
- More complicated, periodic B fields?
J
16Azimuthal lineout
Fluence
What are the radial filaments?
- Strands of dense matter?
- E fields around filaments of charge?
- B fields around filaments of current?
- Isolated bundles of B?
- More complicated, periodic B fields?
B
17Azimuthal lineout
Fluence
What are the radial filaments?
- Strands of dense matter?
- E fields around filaments of charge?
- B fields around filaments of current?
- Isolated bundles of B?
- More complicated, periodic B fields?
18Azimuthal lineout
Fluence
Here are the candidates
- Strands of dense matter?
- E fields around filaments of charge 1011
electrons / µm - B fields around filaments of current?
- Isolated bundles of B?
- More complicated, periodic B fields B 0.3
MG
19These fields are probably responsible for
long-wavelength fluence variations seen
previously in charged fusion product self emission
Large-area detectors sometimes see fluence
variations
Fluence
Angle wrt capsule 3.7
Energy
14.7-MeV protons
Séguin et al., PoP (2002)
20Summary
Time-gated radiography shows a rich and complex
evolution of field structures in and around
imploding ICF capsules
- Different field structures appear during
well-defined time intervals - The field structures may be connected with
previous observations - Shells of charge ? Ablator ion spectrum features
- Radial filaments ? Anisotropies in fluence of
charged fusion products
Fredrick Séguin et al., MIT APS
2007
21Time evolution of fields outside imploding
direct-drive capsules
Drive laser
Fredrick Séguin et al., MIT APS
2007