Framed X-Ray Imaging of Cryogenic Target Implosion Cores on OMEGA KBFRAMED optic assembly KBFRAMED core image OMEGA cryogenic DT target implosion shot 77064 F. J. Marshall University of Rochester Laboratory for Laser Energetics 100 100-nm image regions Relative x-ray intensity 0 Max 57th Annual Meeting of the American Physical Society Division of Plasma Physics Savannah, GA 16 20 November 2015 1
Summary Time-resolved x-ray imaging of cryogenic target-core emission provides improved estimates of bang time, burnwidth, and peak core pressure Cryogenic DT target-implosion cores are imaged on OMEGA by a combination of a high-speed framing camera coupled to a pinhole array and a 16-image framed x-ray microscope (KBFRAMED) The time history of the core x-ray emission, determined by the high-speed framing-camera pinhole array, gives absolute values of the bang time and burnwidth (with ~5-ps accuracy) The core pressure is inferred from the measured core size, ion temperature, neutron yield, and burnwidth E23696a 2
Collaborators V. N. Goncharov,* V. Yu. Glebov, S. P. Regan,* T. C. Sangster, and C. Stoeckl University of Rochester Laboratory for Laser Energetics * Related talks: V. N. Goncharov et al., U04.00005, this conference; S. P. Regan, CI3.00005, this conference (invited). 3
KBFRAMED is a 16-channel Kirkpatrick Baez (KB) x-ray microscope that provides time-resolved images of the core around stagnation Gate width: ~30 ps Image to image: 15 to 60 ps Spatial resolution: ~6 nm Energy range: 2 to 8 kev OMEGA KB microscope chassis Framing camera Single mirror 1 cm 16 imaging pairs per assembly Optic assembly E22996e F. J. Marshall, J. A. Oertel, and P. J. Walsh, Rev. Sci. Instrum. 75, 4045 (2004). 4
KBFRAMED optic magnification and framed resolution have been measured using an x-ray backlit grid on OMEGA Image 10 KBFRAMED OMEGA shot 76806 4 3 2 1 500 nm 8 7 6 5 E23991e Intensity (arbitrary units) 0.08 0.06 0.04 Dx. 6 nm 0.02 0.00 0 20 40 60 80 100 Distance (nm) M = 12 with 6-nm resolution 12 16 15 11 M = 12.0 within 1% Resolution (FWHM* of the PSF**). 6 nm varies from image to image 10 14 9 13 * FWHM: full width at half maximum ** PSF: point spread function 5
KBFRAMED records an image (Dt = 30 ps) of the stagnating core every ~15 ps in the 4- to 8-keV photon-energy range OMEGA cryogenic DT target implosion, shot 76828 PSF t = 2.717 ns t = 2.729 ns t = 2.766 ns t = 2.774 ns t = 2.786 ns t = 2.792 ns t = 2.811 ns t = 2.825 ns t = 2.838 ns t = 2.855 ns E24014b 100 100-nm regions 0 Max Relative x-ray intensity 6
The detailed cryogenic core hot-spot evolution is seen every ~15 ps with KBFRAMED Image 3: 23 ps OMEGA shot 77064 KBFRAMED x-ray images Image 14: 3 ps Image 7: +2 ps Image 11: +22 ps PSF Relative x-ray intensity 100 100-nm image regions 0 Max Image-to-image timing is precisely determined from position and the use of measured cables (!2 ps). E24420a 7
The cryogenic target implosion s hot-spot size is determined from an elliptical super-gaussian fit OMEGA shot 77064 KBFRAMED core image near peak compression Image Super-Gaussian fit ^x xch ^y ych I = I0 # exp = G a2 b2 2 2 n/ 2 Difference E24509a ) =, ^ x, y h I I PSF R R 1 /e = 17 ab 1 n = ^177. h / # R1/e Fit is to super-gaussian convolved with PSF (I*) For KBFRAMED: PSF. 6 nm FWHM Gaussian Lineout indicated 100 100-nm regions by dotted line Image (black) and fit (red) Intensity (arbitrary units) 0.8 0.6 0.4 0.2 0.0 0.2 0 50 100 150 Position (nm) 8
The x-ray bang time is independently determined by measuring the time from the first picket peak to the stagnation peak UV power (TW) 30 25 20 15 10 5 OMEGA cryogenic target shot 77339 0 0 0 1 2 3 Time (ns) 200 150 100 50 Neutron temporal diagnostic (NTD) signal (arbitrary units) SFC3* with 46-pinhole array Dt = 0.393 ns X-ray bang Time First picket Dt = 2.5 ns Dt = 2.3 ns Dt = 2.1 ns Dt = 0 ns T bang = 2.3 ns + Dt = 2.393 ns E24761 *SFC3: Sydor framing camera 9
The pinhole-array framing-camera images determine the absolute x-ray bang time and burnwidth of the cryogenic target implosion Integrated x-ray flux (arbitrary units) E24421a 2000 1500 1000 500 0 2.25 Core x-ray emission, OMEGA shot 77339 2.30 2.35 2.40 2.45 2.50 2.55 Time (ns) SFC3 with 46-pinhole array Dt = 2.3 ns Dt = 2.5 ns Dt = 2.1 ns Dt = 2.3 ns Dt = 0 ns Dt = 2.1 ns Time Best fit: I 0 = 1710 t bang (exp) = 2.393!0.005 ns t bang (1-D) = 2.38 ns Dt burn (exp) = 64!5 ps Dt burn (1-D) = 64 ps Flat fielded by framing constant-emission x rays. Dt = 0 ns From first picket 10
The hot-spot pressure and volume are inferred from the neutron yield, burnwidth, ion temperature, and core size / 4r Phs * -; 8Y ln2 r Dtburn # dv vv T and Vhs. R V E 3 hs 2 12 3 17% OMEGA cryogenic target shot 77066 R 17 = 22.0!0.4 nm (KBFRAMED + framed pinholes) Y n = 4.0 10 13 Dt burn = 63!5 ps (x rays), 67!5 ps (neutrons), 66 ps (1-D) T i = 3.2!0.4 kev GP hs H exp = 56!7 Gbar GP hs H 1-D = 90 Gbar E23702b *C. Cerjan, P. T. Springer, and S. M. Sepke, Phys. Plasmas 20, 056319 (2013); R. Betti et al., Phys. Plasmas 17, 058102 (2010). 11
Summary/Conclusions Time-resolved x-ray imaging of cryogenic target-core emission provides improved estimates of bang time, burnwidth, and peak core pressure Cryogenic DT target-implosion cores are imaged on OMEGA by a combination of a high-speed framing camera coupled to a pinhole array and a 16-image framed x-ray microscope (KBFRAMED) The time history of the core x-ray emission, determined by the high-speed framing-camera pinhole array, gives absolute values of the bang time and burnwidth (with ~5-ps accuracy) The core pressure is inferred from the measured core size, ion temperature, neutron yield, and burnwidth E23696a 12