Publications

Mattsson, Thomas M.; Lemke, Raymond W.; Dolan, Daniel H.; Dalton, Devon D.; Brown, Justin L.; Tomlinson, Kurt T.; Robertson, Grafton K.; Knudson, Marcus D.; Harding, Eric H.; Mattsson, Ann E.; Carpenter, John H.; Drake, Richard R.; Cochrane, Kyle C.; Blue, Brent B.; Robinson, Allen C.

Abstract not provided.

Jones, Brent M.; Hahn, Kelly D.; Ruiz, Carlos L.; Chandler, Gordon A.; Fehl, David L.; Lash, Joel S.; Knapp, Patrick K.; Gomez, Matthew R.; Hansen, Stephanie B.; Harding, Eric H.; McPherson, Leroy A.; Nelson, Alan J.; Rochau, G.A.; Schmit, Paul S.; Sefkow, Adam B.; Sinars, Daniel S.; Torres, Jose A.; Bur, James A.; Cooper, Gary W.; Bonura, Michael A.; Long, Joel L.; Styron, Jedediah D.; Buckles, Rob B.; Garza, Irene G.; Moy, Kenneth J.; Davis, Brent D.; Tinsley, Jim T.; Tiangco, Rod T.; Miller, Kirk M.; Mckenna, Ian M.

Abstract not provided.

High Energy Density Physics

Ao, Tommy A.; Harding, Eric H.; Bailey, James E.; Lemke, Raymond W.; Desjarlais, Michael P.; Hansen, Stephanie B.; Smith, Ian C.; Geissel, Matthias G.; Maurer, A.; Reneker, Joseph R.; Romero, D.; Sinars, Daniel S.; Rochau, G.A.; Benage, John F.

Experiments on the Sandia Z pulsed-power accelerator have demonstrated the ability to produce warm dense matter (WDM) states with unprecedented uniformity, duration, and size, which are ideal for investigations of fundamental WDM properties. For the first time, space-resolved x-ray Thomson scattering (XRTS) spectra from shocked carbon foams were recorded on Z. The large (>20 MA) electrical current produced by Z was used to launch Al flyer plates up to 25 km/s. The impact of the flyer plate on a CH2 foam target produced a shocked state with an estimated pressure of 0.75 Mbar, density of 0.52 g/cm3, and temperature of 4.3 eV. Both unshocked and shocked portions of the foam target were probed with 6.2 keV x-rays produced by focusing the Z-Beamlet laser onto a nearby Mn foil. The data are composed of three spatially distinct spectra that were simultaneously captured with a single spectrometer with high spectral (4.8 eV) and spatial (190 μm) resolutions. Detailed spectral information from three target locations is provided simultaneously: the incident x-ray source, the scattered signal from unshocked foam, and the scattered signal from shocked foam.

Jennings, Christopher A.; Harding, Eric H.; Gomez, Matthew R.; Hansen, Stephanie B.; Awe, T.J.A.; McBride, Ryan D.; Martin, M.R.M.; Peterson, Kyle J.; Knapp, Patrick K.; Chittenden, J.P.C.

Abstract not provided.

Journal of Applied Physics

Lemke, Raymond W.; Dolan, Daniel H.; Dalton, D.G.; Brown, Justin L.; Tomlinson, K.; Robertson, G.R.; Knudson, Marcus D.; Harding, Eric H.; Mattsson, A.E.; Carpenter, John H.; Drake, Richard R.; Cochrane, Kyle C.; Blue, B.E.; Robinson, Allen C.; Mattsson, Thomas M.

We report on a new technique for obtaining off-Hugoniot pressure vs. density data for solid metals compressed to extreme pressure by a magnetically driven liner implosion on the Z-machine (Z) at Sandia National Laboratories. In our experiments, the liner comprises inner and outer metal tubes. The inner tube is composed of a sample material (e.g., Ta and Cu) whose compressed state is to be inferred. The outer tube is composed of Al and serves as the current carrying cathode. Another aluminum liner at much larger radius serves as the anode. A shaped current pulse quasi-isentropically compresses the sample as it implodes. The iterative method used to infer pressure vs. density requires two velocity measurements. Photonic Doppler velocimetry probes measure the implosion velocity of the free (inner) surface of the sample material and the explosion velocity of the anode free (outer) surface. These two velocities are used in conjunction with magnetohydrodynamic simulation and mathematical optimization to obtain the current driving the liner implosion, and to infer pressure and density in the sample through maximum compression. This new equation of state calibration technique is illustrated using a simulated experiment with a Cu sample. Monte Carlo uncertainty quantification of synthetic data establishes convergence criteria for experiments. Results are presented from experiments with Al/Ta, Al/Cu, and Al liners. Symmetric liner implosion with quasi-isentropic compression to peak pressure ∼1000 GPa is achieved in all cases. These experiments exhibit unexpectedly softer behavior above 200 GPa, which we conjecture is related to differences in the actual and modeled properties of aluminum.

Geissel, Matthias G.; Awe, Thomas J.; Campbell, E.M.C.; Gomez, Matthew R.; Harding, Eric H.; Harvey-Thompson, Adam J.; Hansen, Stephanie B.; Jennings, Christopher A.; Kimmel, Mark W.; Knapp, Patrick K.; Lewis, Sean M.; McBride, Ryan D.; Peterson, Kyle J.; Schollmeier, Marius; Sefkow, Adam B.; Shores, Jonathon S.; Sinars, Daniel S.; Slutz, Stephen A.; Smith, Ian C.; Speas, Christopher S.; Vesey, Roger A.; Porter, John L.

Abstract not provided.

Proceedings of SPIE - The International Society for Optical Engineering

Geissel, Matthias G.; Awe, T.J.; Bliss, David E.; Campbell, Edward M.; Gomez, Matthew R.; Harding, Eric H.; Harvey-Thompson, Adam J.; Hansen, Stephanie B.; Jennings, C.; Kimmel, Mark W.; Knapp, Patrick K.; Lewis, Sean M.; McBride, Ryan D.; Peterson, Kyle J.; Schollmeier, Marius; Scoglietti, Daniel S.; Sefkow, Adam B.; Shores, J.E.; Sinars, Daniel S.; Slutz, S.A.; Smith, Ian C.; Speas, C.S.; Vesey, Roger A.; Porter, John L.

Sandia National Laboratories is pursuing a variation of Magneto-Inertial Fusion called Magnetized Liner Inertial Fusion, or MagLIF. The MagLIF approach requires magnetization of the deuterium fuel, which is accomplished by an initial external B-Field and laser-driven pre-heat. While magnetization is crucial to the concept, it is challenging to couple sufficient energy to the fuel, since laser-plasma instabilities exist, and a compromise between laser spot size, laser entrance window thickness, and fuel density must be found. Nonlinear processes in laser plasma interaction, or laser-plasma instabilities (LPI), complicate the deposition of laser energy by enhanced absorption, backscatter, filamentation and beam-spray. Key LPI processes are determined, and mitigation methods are discussed. Results with and without improvement measures are presented.

Hansen, Stephanie B.; Gomez, Matthew R.; Knapp, Patrick K.; Harding, Eric H.

Abstract not provided.

Harding, Eric H.; Gomez, Matthew R.; Knapp, Patrick K.; Hansen, Stephanie B.; Jennings, Christopher A.; Slutz, Stephen A.; Sefkow, Adam B.; Awe, Thomas J.; Peterson, Kyle J.; Hahn, Kelly D.; McBride, Ryan D.; Rochau, G.A.; Sinars, Daniel S.; Golovkin, Igor G.

Abstract not provided.

Geissel, Matthias G.; Harvey-Thompson, Adam J.; Awe, Thomas J.; Campbell, Edward M.; Gomez, Matthew R.; Harding, Eric H.; Hansen, Stephanie B.; Jennings, Christopher A.; Kimmel, Mark W.; Knapp, Patrick K.; Lewis, Sean M.; McBride, Ryan D.; Peterson, Kyle J.; Schollmeier, Marius; Sefkow, Adam B.; Shores, Jonathon S.; Sinars, Daniel S.; Slutz, Stephen A.; Smith, Ian C.; Speas, Christopher S.; Vesey, Roger A.; Porter, John L.

Abstract not provided.

Geissel, Matthias G.; Harvey-Thompson, Adam J.; Awe, Thomas J.; Campbell, Michael E.; Gomez, Matthew R.; Harding, Eric H.; Jennings, Christopher A.; Kimmel, Mark W.; Knapp, Patrick K.; Lewis, Sean M.; McBride, Ryan D.; Peterson, Kyle J.; Schollmeier, Marius; Schmit, Paul S.; Sefkow, Adam B.; Shores, Jonathon S.; Sinars, Daniel S.; Slutz, Stephen A.; Smith, Ian C.; Speas, Christopher S.; Vesey, Roger A.; Porter, John L.

Abstract not provided.

Hahn, Kelly D.; Chandler, Gordon A.; Ruiz, Carlos L.; Cooper, Gary W.; Gomez, Matthew R.; Slutz, Stephen A.; Sefkow, Adam B.; Sinars, Daniel S.; Hansen, Stephanie B.; Knapp, Patrick K.; Schmit, Paul S.; Harding, Eric H.; Jennings, Christopher A.; Awe, Thomas J.; Geissel, Matthias G.; Rovang, Dean C.; Torres, Jose A.; Bur, James A.; Cuneo, M.E.; Glebov, V.Yu.; Harvey-Thompson, Adam J.; Herrmann, M.C.H.; Hess, Mark H.; Johns, Owen J.; Jones, Brent M.; Lamppa, Derek C.; Martin, Matthew; McBride, Ryan D.; Peterson, Kyle J.; Porter, John L.; Reneker, Joseph R.; Robertson, Grafton K.; Rochau, G.A.; Savage, Mark E.; Smith, Ian C.; Styron, Jedediah D.; Vesey, Roger A.

Abstract not provided.

Schollmeier, Marius; Loisel, Guillaume P.; Geissel, Matthias G.; Harding, Eric H.; Rambo, Patrick K.; Schwarz, Jens S.; Shores, Jonathon S.; Smith, Ian C.; Speas, Christopher S.; Porter, John L.; vargas, mark v.

Abstract not provided.

Harding, Eric H.; Gomez, Matthew R.; Slutz, Stephen A.; Sefkow, Adam B.; Geissel, Matthias G.; Harvey-Thompson, Adam J.; Schollmeier, Marius; Peterson, Kyle J.; Awe, Thomas J.; Hansen, Stephanie B.; Hahn, Kelly D.; Knapp, Patrick K.; Schmit, Paul S.; Ruiz, Carlos L.; Sinars, Daniel S.; Jennings, Christopher A.; Smith, Ian C.; Rovang, Dean C.; Chandler, Gordon A.; Martin, Matthew; McBride, Ryan D.; Porter, John L.; Rochau, G.A.; Harding, Eric H.

Abstract not provided.

Harding, Eric H.; Gomez, Matthew R.; Slutz, Stephen A.; Geissel, Matthias G.; Harvey-Thompson, Adam J.; Schollmeier, Marius; Peterson, Kyle J.; Awe, Thomas J.; Hansen, Stephanie B.; Schmit, Paul S.; Ruiz, Carlos L.; Sinars, Daniel S.; Jennings, Christopher A.; Smith, Ian C.; Rovang, Dean C.; Chandler, Gordon A.; Martin, Matthew; McBride, Ryan D.; Porter, John L.; Rochau, G.A.

Abstract not provided.

Harding, Eric H.; Gomez, Matthew R.; Jennings, Christopher A.; Knapp, Patrick K.; Slutz, Stephen A.; Sefkow, Adam B.; Awe, Thomas J.; Hansen, Stephanie B.; Peterson, Kyle J.; Hahn, Kelly D.; McBride, Ryan D.; Rochau, G.A.; Sinars, Daniel S.

Abstract not provided.

Geissel, Matthias G.; Harvey-Thompson, Adam J.; Awe, Thomas J.; Campbell, Edward M.; Gomez, Matthew R.; Harding, Eric H.; Jennings, Christopher A.; Kimmel, Mark W.; Knapp, Patrick K.; Lewis, Sean M.; McBride, Ryan D.; Peterson, Kyle J.; Schollmeier, Marius; Schmit, Paul S.; Sefkow, Adam B.; Shores, Jonathon S.; Sinars, Daniel S.; Slutz, Stephen A.; Smith, Ian C.; Speas, Christopher S.; Stahoviak, J.W.S.; Vesey, Roger A.; Porter, John L.

Abstract not provided.

Ao, Tommy A.; Harding, Eric H.; Bailey, James E.; Lemke, Raymond W.; Desjarlais, Michael P.; Hansen, Stephanie B.; Smith, Ian C.; Reneker, Joseph R.; Romero, Dustin H.; Sinars, Daniel S.; Rochau, G.A.; Benage, John F.

Abstract not provided.

Gomez, Matthew R.; Slutz, Stephen A.; Sefkow, Adam B.; Geissel, Matthias G.; Harvey-Thompson, Adam J.; Peterson, Kyle J.; Hansen, Stephanie B.; Hahn, Kelly D.; Knapp, Patrick K.; Schmit, Paul S.; Ruiz, Carlos L.; Sinars, Daniel S.; Awe, Thomas J.; Harding, Eric H.; Jennings, Christopher A.; Smith, Ian C.; Rovang, Dean C.; Chandler, Gordon A.; Cuneo, M.E.; Lamppa, Derek C.; Martin, Matthew; McBride, Ryan D.; Porter, John L.; Rochau, G.A.

Abstract not provided.

Gomez, Matthew R.; Slutz, Stephen A.; Sefkow, Adam B.; Geissel, Matthias G.; Harvey-Thompson, Adam J.; Peterson, Kyle J.; Awe, Thomas J.; Hansen, Stephanie B.; Harding, Eric H.; Hahn, Kelly D.; Knapp, Patrick K.; Schmit, Paul S.; Ruiz, Carlos L.; Sinars, Daniel S.; Jennings, Christopher A.; Smith, Ian C.; Rovang, Dean C.; Chandler, Gordon A.; Martin, Matthew; McBride, Ryan D.; Porter, John L.; Rochau, G.A.

Abstract not provided.

McBride, Ryan D.; Sinars, Daniel S.; Slutz, Stephen A.; Gomez, Matthew R.; Sefkow, Adam B.; Hansen, Stephanie B.; Awe, Thomas J.; Peterson, Kyle J.; Knapp, Patrick K.; Schmit, Paul S.; Rovang, Dean C.; Geissel, Matthias G.; Vesey, Roger A.; Harvey-Thompson, Adam J.; Jennings, Christopher A.; Martin, Matthew; Lemke, Raymond W.; Hahn, Kelly D.; Harding, Eric H.; Cuneo, M.E.; Porter, John L.; Rochau, G.A.; Stygar, William A.

Abstract not provided.

Shulenburger, Luke N.; Seagle, Christopher T.; Haill, Thomas A.; Harding, Eric H.

Abstract not provided.

Physics of Plasmas

Knapp, P.F.; Schmit, Paul S.; Hansen, Stephanie B.; Gomez, Matthew R.; Hahn, K.D.; Sinars, Daniel S.; Peterson, Kyle J.; Slutz, S.A.; Sefkow, Adam B.; Awe, T.J.; Harding, Eric H.; Jennings, C.A.; Desjarlais, M.P.; Chandler, Gordon A.; Cooper, Gary W.; Cuneo, M.E.; Geissel, Matthias G.; Harvey-Thompson, Adam J.; Porter, John L.; Rochau, G.A.; Rovang, Dean C.; Ruiz, Carlos L.; Savage, Mark E.; Smith, Ian C.; Stygar, William A.; Herrmann, M.C.

By magnetizing the fusion fuel in inertial confinement fusion (ICF) systems, the required stagnation pressure and density can be relaxed dramatically. This happens because the magnetic field insulates the hot fuel from the cold pusher and traps the charged fusion burn products. This trapping allows the burn products to deposit their energy in the fuel, facilitating plasma self-heating. Here, we report on a comprehensive theory of this trapping in a cylindrical DD plasma magnetized with a purely axial magnetic field. Using this theory, we are able to show that the secondary fusion reactions can be used to infer the magnetic field-radius product, BR, during fusion burn. This parameter, not ρR, is the primary confinement parameter in magnetized ICF. Using this method, we analyze data from recent Magnetized Liner Inertial Fusion experiments conducted on the Z machine at Sandia National Laboratories. We show that in these experiments BR ≈ 0.34(+0.14/-0.06) MG cm, a ∼ 14x increase in BR from the initial value, and confirming that the DD-fusion tritons are magnetized at stagnation. This is the first experimental verification of charged burn product magnetization facilitated by compression of an initial seed magnetic flux.

Physics of Plasmas

Hansen, Stephanie B.; Gomez, Matthew R.; Sefkow, Adam B.; Slutz, S.A.; Sinars, Daniel S.; Hahn, K.D.; Harding, Eric H.; Knapp, P.F.; Schmit, Paul S.; Awe, T.J.; McBride, Ryan D.; Jennings, C.A.; Geissel, Matthias G.; Harvey-Thompson, Adam J.; Peterson, K.J.; Rovang, Dean C.; Chandler, Gordon A.; Cooper, Gary W.; Cuneo, M.E.; Herrmann, M.C.; Hess, Mark H.; Johns, Owen J.; Lamppa, Derek C.; Martin, M.R.; Porter, J.L.; Robertson, G.K.; Rochau, G.A.; Ruiz, C.L.; Savage, M.E.; Smith, I.C.; Stygar, W.A.; Vesey, R.A.; Blue, B.E.; Ryutov, D.; Schroen, D.G.; Tomlinson, K.

Magnetized Liner Inertial Fusion experiments performed at Sandia's Z facility have demonstrated significant thermonuclear fusion neutron yields (∼10¹² DD neutrons) from multi-keV deuterium plasmas inertially confined by slow (∼10 cm/μs), stable, cylindrical implosions. Effective magnetic confinement of charged fusion reactants and products is signaled by high secondary DT neutron yields above 10¹⁰. Analysis of extensive power, imaging, and spectroscopic x-ray measurements provides a detailed picture of ∼3 keV temperatures, 0.3 g/cm³ densities, gradients, and mix in the fuel and liner over the 1-2 ns stagnation duration.

Physics of Plasmas

Gomez, Matthew R.; Slutz, S.A.; Sefkow, Adam B.; Hahn, K.D.; Hansen, Stephanie B.; Knapp, P.F.; Schmit, Paul S.; Ruiz, Carlos L.; Sinars, Daniel S.; Harding, Eric H.; Jennings, C.A.; Awe, T.J.; Geissel, Matthias G.; Rovang, Dean C.; Smith, Ian C.; Chandler, Gordon A.; Cooper, Gary W.; Cuneo, M.E.; Harvey-Thompson, Adam J.; Herrmann, M.C.; Hess, Mark H.; Lamppa, Derek C.; Martin, M.R.; McBride, Ryan D.; Peterson, Kyle J.; Porter, John L.; Rochau, G.A.; Savage, Mark E.; Schroen, D.G.; Stygar, William A.; Vesey, Roger A.

The magnetized liner inertial fusion concept [S. A. Slutz et al., Phys. Plasmas 17, 056303 (2010)] utilizes a magnetic field and laser heating to relax the pressure requirements of inertial confinement fusion. The first experiments to test the concept [M. R. Gomez et al., Phys. Rev. Lett. 113, 155003 (2014)] were conducted utilizing the 19 MA, 100-ns Z machine, the 2.5-kJ, 1 TW Z Beamlet laser, and the 10-T Applied B-field on Z system. Despite an estimated implosion velocity of only 70-km/s in these experiments, electron and ion temperatures at stagnation were as high as 3-keV, and thermonuclear deuterium-deuterium neutron yields up to 2-×-10¹² have been produced. X-ray emission from the fuel at stagnation had widths ranging from 50 to 110 μm over a roughly 80% of the axial extent of the target (6-8-mm) and lasted approximately 2-ns. X-ray yields from these experiments are consistent with a stagnation density of the hot fuel equal to 0.2-0.4-g/cm³. In these experiments, up to 5-×-10¹⁰ secondary deuterium-tritium neutrons were produced. Given that the areal density of the plasma was approximately 1-2-mg/cm², this indicates the stagnation plasma was significantly magnetized, which is consistent with the anisotropy observed in the deuterium-tritium neutron spectra. Control experiments where the laser and/or magnetic field were not utilized failed to produce stagnation temperatures greater than 1-keV and primary deuterium-deuterium yields greater than 10¹⁰. An additional control experiment where the fuel contained a sufficient dopant fraction to substantially increase radiative losses also failed to produce a relevant stagnation temperature. The results of these experiments are consistent with a thermonuclear neutron source.