Imperial College London

DrBrianAppelbe

Faculty of Natural SciencesDepartment of Physics

Research Fellow
 
 
 
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Contact

 

+44 (0)20 7594 7651b.appelbe07 Website

 
 
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Location

 

740Blackett LaboratorySouth Kensington Campus

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Summary

 

Publications

Publication Type
Year
to

50 results found

Patel D, Shah RC, Betti R, Knauer JP, Forrest CJ, Woo KM, Gopalaswamy V, Glebov VY, Appelbe BD, Regan SPet al., 2023, Measuring higher-order moments of neutron-time-of-flight data for cryogenic inertial confinement fusion implosions on OMEGA, PHYSICS OF PLASMAS, Vol: 30, ISSN: 1070-664X

Journal article

Sio H, Moody JD, Pollock BB, Strozzi DJ, Ho DDM, Walsh CA, Kemp GE, Lahmann B, Kucheyev SO, Kozioziemski B, Carroll EG, Kroll J, Yanagisawa DK, Angus J, Bachmann B, Baker AA, Bayu Aji LB, Bhandarkar SD, Bude JD, Divol L, Engwall AM, Ferguson B, Fry J, Hagler L, Hartouni E, Herrmann MC, Hsing W, Holunga DM, Javedani J, Johnson A, Khan S, Kalantar D, Kohut T, Logan BG, Masters N, Nikroo A, Izumi N, Orsi N, Piston K, Provencher C, Rowe A, Sater J, Shin SJ, Skulina K, Stygar WA, Tang V, Winters SE, Zimmerman G, Chittenden JP, Appelbe B, Boxall A, Crilly A, O'Neill S, Barnak D, Davies J, Peebles J, Bae JH, Clark K, Havre M, Mauldin M, Ratledge M, Vonhof S, Adrian P, Reichelt B, Fujioka S, Fraenkel Met al., 2023, Performance scaling with an applied magnetic field in indirect-drive inertial confinement fusion implosions, PHYSICS OF PLASMAS, Vol: 30, ISSN: 1070-664X

Journal article

Moore AS, Schlossberg DJ, Appelbe BD, Chandler GA, Crilly AJ, Eckart MJ, Forrest CJ, Glebov VY, Grim GP, Hartouni EP, Hatarik R, Kerr SM, Kilkenny J, Knauer JPet al., 2023, Neutron time of flight (nToF) detectors for inertial fusion experiments, REVIEW OF SCIENTIFIC INSTRUMENTS, Vol: 94, ISSN: 0034-6748

Journal article

Hartouni EP, Moore AS, Crilly AJ, Appelbe BD, Amendt PA, Baker KL, Casey DT, Clark DS, Doppner T, Eckart MJ, Field JE, Gatu-Johnson M, Grim GP, Hatarik R, Jeet J, Kerr SM, Kilkenny J, Kritcher AL, Meaney KD, Milovich JL, Munro DH, Nora RC, Pak AE, Ralph JE, Robey HF, Ross JS, Schlossberg DJ, Sepke SM, Spears BK, Young C, Zylstra ABet al., 2023, Evidence for suprathermal ion distribution in burning plasmas, NATURE PHYSICS, Vol: 19, Pages: 72-+, ISSN: 1745-2473

Journal article

Crilly AJ, Appelbe BD, Mannion OM, Taitano W, Hartouni EP, Moore AS, Gatu-Johnson M, Chittenden JPet al., 2022, Constraints on ion velocity distributions from fusion product spectroscopy, NUCLEAR FUSION, Vol: 62, ISSN: 0029-5515

Journal article

Moody JD, Pollock BB, Sio H, Strozzi DJ, Ho DD-M, Walsh CA, Kemp GE, Lahmann B, Kucheyev SO, Kozioziemski B, Carroll EG, Kroll J, Yanagisawa DK, Angus J, Bachmann B, Bhandarkar SD, Bude JD, Divol L, Ferguson B, Fry J, Hagler L, Hartouni E, Herrmann MC, Hsing W, Holunga DM, Izumi N, Javedani J, Johnson A, Khan S, Kalantar D, Kohut T, Logan BG, Masters N, Nikroo A, Orsi N, Piston K, Provencher C, Rowe A, Sater J, Skulina K, Stygar WA, Tang V, Winters SE, Zimmerman G, Adrian P, Chittenden JP, Appelbe B, Boxall A, Crilly A, O'Neill S, Davies J, Peebles J, Fujioka Set al., 2022, Increased ion temperature and neutron yield observed in magnetized indirectly driven D_{2}-filled capsule implosions on the national ignition facility, Physical Review Letters, Vol: 129, ISSN: 0031-9007

The application of an external 26 Tesla axial magnetic field to a D_{2} gas-filled capsule indirectly driven on the National Ignition Facility is observed to increase the ion temperature by 40% and the neutron yield by a factor of 3.2 in a hot spot with areal density and temperature approaching what is required for fusion ignition [1]. The improvements are determined from energy spectral measurements of the 2.45 MeV neutrons from the D(d,n)^{3}He reaction, and the compressed central core B field is estimated to be ∼4.9  kT using the 14.1 MeV secondary neutrons from the D(T,n)^{4}He reactions. The experiments use a 30 kV pulsed-power system to deliver a ∼3  μs current pulse to a solenoidal coil wrapped around a novel high-electrical-resistivity AuTa_{4} hohlraum. Radiation magnetohydrodynamic simulations are consistent with the experiment.

Journal article

Forrest CJ, Crilly A, Schwemmlein A, Gatu-Johnson M, Mannion OM, Appelbe B, Betti R, Glebov VY, Gopalaswamy V, Knauer JP, Mohamed ZL, Radha PB, Regan SP, Stoeckl C, Theobald Wet al., 2022, Measurements of low-mode asymmetries in the areal density of laser-direct-drive deuterium-tritium cryogenic implosions on OMEGA using neutron spectroscopy, Review of Scientific Instruments, Vol: 93, Pages: 1-9, ISSN: 0034-6748

Areal density is one of the key parameters that determines the confinement time in inertial confinement fusion experiments, and low-mode asymmetries in the compressed fuel are detrimental to the implosion performance. The energy spectra from the scattering of the primary deuterium–tritium (DT) neutrons off the compressed cold fuel assembly are used to investigate low-mode nonuniformities in direct-drive cryogenic DT implosions at the Omega Laser Facility. For spherically symmetric implosions, the shape of the energy spectrum is primarily determined by the elastic and inelastic scattering cross sections for both neutron-deuterium and neutron-tritium kinematic interactions. Two highly collimated lines of sight, which are positioned at nearly orthogonal locations around the OMEGA target chamber, record the neutron time-of-flight signal in the current mode. An evolutionary algorithm is being used to extract a model-independent energy spectrum of the scattered neutrons from the experimental neutron time-of-flight data and is used to infer the modal spatial variations (l = 1) in the areal density. Experimental observations of the low-mode variations of the cold-fuel assembly (ρL0 + ρL1) show good agreement with a recently developed model, indicating a departure from the spherical symmetry of the compressed DT fuel assembly. Another key signature that has been observed in the presence of a low-mode variation is the broadening of the kinematic end-point due to the anisotropy of the dense fuel conditions.

Journal article

Crilly A, Garin-Fernandez I, Appelbe B, Chittenden Jet al., 2022, Efficacy of ICF experiments in light ion fusion cross section measurement at nucleosynthesis relevant energies, Frontiers in Physics, Vol: 10, Pages: 1-11, ISSN: 2296-424X

Inertial confinement fusion (ICF) experiments create a unique laboratory environment in which thermonuclear fusion reactionsoccur within a plasma, with conditions comparable to stellar cores and the early universe. In contrast, accelerator-basedmeasurements must compete with bound electron screening effects and beam stopping when measuring fusion cross sections atnucleosynthesis-relevant energies. Therefore, ICF experiments are a natural place to study nuclear reactions relevant to nuclearastrophysics. However, analysis of ICF-based measurements must address its own set of complicating factors. These include: theinherent range of reaction energies, spatial and temporal thermal temperature variation, and kinetic effects such as speciesseparation. In this work we examine these phenomena and develop an analysis to quantify and, when possible, compensate fortheir effects on our inference. Error propagation in the analyses are studied using synthetic data combined with Markov ChainMonte Carlo (MCMC) machine learning. The novel inference techniques will aid in the extraction of valuable and accurate data fromICF-based nuclear astrophysics experiments.

Journal article

Meaney KD, Kim Y, Hoffman NM, Geppert-Kleinrath H, Jorgenson J, Hochanadel M, Appelbe B, Crilly A, Basu R, Saw EY, Moore A, Schlossberg Det al., 2022, Design of multi neutron-to-gamma converter array for measuring time resolved ion temperature of inertial confinement fusion implosions., Review of Scientific Instruments, Vol: 93, Pages: 1-5, ISSN: 0034-6748

The ion temperature varying during inertial confinement fusion implosions changes the amount of Doppler broadening of the fusion products, creating subtle changes in the fusion neutron pulse as it moves away from the implosion. A diagnostic design to try to measure these subtle effects is introduced-leveraging the fast time resolution of gas Cherenkov detectors along with a multi-puck array that converts a small amount of the neutron pulse into gamma-rays, one can measure multiple snapshots of the neutron pulse at intermediate distances. Precise measurements of the propagating neutron pulse, specifically the variation in the peak location and the skew, could be used to infer time-evolved ion temperature evolved during peak compression.

Journal article

Abu-Shawareb H, Acree R, Adams P, Adams J, Addis B, Aden R, Adrian P, Afeyan BB, Aggleton M, Aghaian L, Aguirre A, Aikens D, Akre J, Albert F, Albrecht M, Albright BJ, Albritton J, Alcala J, Alday C, Alessi DA, Alexander N, Alfonso J, Alfonso N, Alger E, Ali SJ, Ali ZA, Alley WE, Amala P, Amendt PA, Amick P, Ammula S, Amorin C, Ampleford DJ, Anderson RW, Anklam T, Antipa N, Appelbe B, Aracne-Ruddle C, Araya E, Arend M, Arnold P, Arnold T, Asay J, Atherton LJ, Atkinson D, Atkinson R, Auerbach JM, Austin B, Auyang L, Awwal AS, Ayers J, Ayers S, Ayers T, Azevedo S, Bachmann B, Back CA, Bae J, Bailey DS, Bailey J, Baisden T, Baker KL, Baldis H, Barber D, Barberis M, Barker D, Barnes A, Barnes CW, Barrios MA, Barty C, Bass I, Batha SH, Baxamusa SH, Bazan G, Beagle JK, Beale R, Beck BR, Beck JB, Bedzyk M, Beeler RG, Beeler RG, Behrendt W, Belk L, Bell P, Belyaev M, Benage JF, Bennett G, Benedetti LR, Benedict LX, Berger R, Bernat T, Bernstein LA, Berry B, Bertolini L, Besenbruch G, Betcher J, Bettenhausen R, Betti R, Bezzerides B, Bhandarkar SD, Bickel R, Biener J, Biesiada T, Bigelow K, Bigelow-Granillo J, Bigman V, Bionta RM, Birge NW, Bitter M, Black AC, Bleile R, Bleuel DL, Bliss E, Bliss E, Blue B, Boehly T, Boehm K, Boley CD, Bonanno R, Bond EJ, Bond T, Bonino MJ, Borden M, Bourgade J-L, Bousquet J, Bowers J, Bowers M, Boyd R, Bozek A, Bradley DK, Bradley KS, Bradley PA, Bradley L, Brannon L, Brantley PS, Braun D, Braun T, Brienza-Larsen K, Briggs TM, Britten J, Brooks ED, Browning D, Bruhn MW, Brunner TA, Bruns H, Brunton G, Bryant B, Buczek T, Bude J, Buitano L, Burkhart S, Burmark J, Burnham A, Burr R, Busby LE, Butlin B, Cabeltis R, Cable M, Cabot WH, Cagadas B, Caggiano J, Cahayag R, Caldwell SE, Calkins S, Callahan DA, Calleja-Aguirre J, Camara L, Camp D, Campbell EM, Campbell JH, Carey B, Carey R, Carlisle K, Carlson L, Carman L, Carmichael J, Carpenter A, Carr C, Carrera JA, Casavant D, Casey A, Casey DT, Castillo A, Castillo E, Castor JI, Castro C, Caugheyet al., 2022, Lawson criterion for ignition exceeded in an inertial fusion experiment, Physical Review Letters, Vol: 129, ISSN: 0031-9007

For more than half a century, researchers around the world have been engaged in attempts to achieve fusion ignition as a proof of principle of various fusion concepts. Following the Lawson criterion, an ignited plasma is one where the fusion heating power is high enough to overcome all the physical processes that cool the fusion plasma, creating a positive thermodynamic feedback loop with rapidly increasing temperature. In inertially confined fusion, ignition is a state where the fusion plasma can begin "burn propagation" into surrounding cold fuel, enabling the possibility of high energy gain. While "scientific breakeven" (i.e., unity target gain) has not yet been achieved (here target gain is 0.72, 1.37 MJ of fusion for 1.92 MJ of laser energy), this Letter reports the first controlled fusion experiment, using laser indirect drive, on the National Ignition Facility to produce capsule gain (here 5.8) and reach ignition by nine different formulations of the Lawson criterion.

Journal article

Crilly AJ, Appelbe BD, Mannion OM, Forrest CJ, Knauer JP, Schlossberg DJ, Hartouni EP, Moore AS, Chittenden JPet al., 2022, Neutron backscatter edges as a diagnostic of burn propagation, PHYSICS OF PLASMAS, Vol: 29, ISSN: 1070-664X

Journal article

Moody JD, Pollock BB, Sio H, Strozzi DJ, Ho DD-M, Walsh C, Kemp GE, Kucheyev SO, Kozioziemski B, Carroll EG, Kroll J, Yanagisawa DK, Angus J, Bhandarkar SD, Bude JD, Divol L, Ferguson B, Fry J, Hagler L, Hartouni E, Herrmann MC, Hsing W, Holunga DM, Javedani J, Johnson A, Kalantar D, Kohut T, Logan BG, Masters N, Nikroo A, Orsi N, Piston K, Provencher C, Rowe A, Sater J, Skulina K, Stygar WA, Tang V, Winters SE, Chittenden JP, Appelbe B, Boxall A, Crilly A, O'Neill S, Davies J, Peebles J, Fujioka Set al., 2022, The Magnetized Indirect Drive Project on the National Ignition Facility, JOURNAL OF FUSION ENERGY, Vol: 41, ISSN: 0164-0313

Journal article

Mannion OM, Crilly AJ, Forrest CJ, Appelbe BD, Betti R, Glebov VY, Gopalaswamy V, Knauer JP, Mohamed ZL, Stoeckl C, Chittenden JP, Regan SPet al., 2022, Measurements of the temperature and velocity of the dense fuel layer in inertial confinement fusion experiments, PHYSICAL REVIEW E, Vol: 105, ISSN: 2470-0045

Journal article

Bose A, Peebles J, Walsh CA, Frenje JA, V Kabadi N, Adrian PJ, Sutcliffe GD, Johnson MG, Frank CA, Davies JR, Betti R, Glebov VY, Marshall FJ, Regan SP, Stoeckl C, Campbell EM, Sio H, Moody J, Crilly A, Appelbe BD, Chittenden JP, Atzeni S, Barbato F, Forte A, Li CK, Seguin FH, Petrasso RDet al., 2022, Effect of strongly magnetized electrons and Ions on heat flow and symmetry of inertial fusion implosions, Physical Review Letters, Vol: 128, ISSN: 0031-9007

This Letter presents the first observation on how a strong, 500 kG, externally applied B field increases the mode-two asymmetry in shock-heated inertial fusion implosions. Using a direct-drive implosion with polar illumination and imposed field, we observed that magnetization produces a significant increase in the implosion oblateness (a 2.5× larger P2 amplitude in x-ray self-emission images) compared with reference experiments with identical drive but with no field applied. The implosions produce strongly magnetized electrons (ωeτe≫1) and ions (ωiτi>1) that, as shown using simulations, restrict the cross field heat flow necessary for lateral distribution of the laser and shock heating from the implosion pole to the waist, causing the enhanced mode-two shape.

Journal article

Walsh CA, O'Neill S, Chittenden JP, Crilly AJ, Appelbe B, Strozzi DJ, Ho D, Sio H, Pollock B, Divol L, Hartouni E, Rosen M, Logan BG, Moody JDet al., 2022, Magnetized ICF implosions: Scaling of temperature and yield enhancement, PHYSICS OF PLASMAS, Vol: 29, ISSN: 1070-664X

Journal article

Sio H, Moody JD, Ho DD, Pollock BB, Walsh CA, Lahmann B, Strozzi DJ, Kemp GE, Hsing WW, Crilly A, Chittenden JP, Appelbe Bet al., 2021, Diagnosing plasma magnetization in inertial confinement fusion implosions using secondary deuterium-tritium reactions, Review of Scientific Instruments, Vol: 92, Pages: 1-5, ISSN: 0034-6748

Diagnosing plasma magnetization in inertial confinement fusion implosions is important for understanding how magnetic fields affect implosion dynamics and to assess plasma conditions in magnetized implosion experiments. Secondary deuterium–tritium (DT) reactions provide two diagnostic signatures to infer neutron-averaged magnetization. Magnetically confining fusion tritons from deuterium–deuterium (DD) reactions in the hot spot increases their path lengths and energy loss, leading to an increase in the secondary DT reaction yield. In addition, the distribution of magnetically confined DD-triton is anisotropic, and this drives anisotropy in the secondary DT neutron spectra along different lines of sight. Implosion parameter space as well as sensitivity to the applied B-field, fuel ρR, temperature, and hot-spot shape will be examined using Monte Carlo and 2D radiation-magnetohydrodynamic simulations.

Journal article

Appelbe B, Velikovich AL, Sherlock M, Walsh C, Crilly A, O' Neill S, Chittenden Jet al., 2021, Magnetic field transport in propagating thermonuclear burn, Physics of Plasmas, Vol: 28, Pages: 1-9, ISSN: 1070-664X

High energy gain in inertial fusion schemes requires the propagation of a thermonuclear burn wave from hot to cold fuel. We consider the problem of burn propagation when a magnetic field is orthogonal to the burn wave. Using an extended-MHD model with a magnetized α energy transport equation, we find that the magnetic field can reduce the rate of burn propagation by suppressing electron thermal conduction and α particle flux. Magnetic field transport during burn propagation is subject to competing effects: the field can be advected from cold to hot regions by ablation of cold fuel, while the Nernst and α particle flux effects transport the field from hot to cold fuel. These effects, combined with the temperature increase due to burn, can cause the electron Hall parameter to grow rapidly at the burn front. This results in the formation of a self-insulating layer between hot and cold fuel, which reduces electron thermal conductivity and α transport, increases the temperature gradient, and reduces the rate of burn propagation.

Journal article

Meaney KD, Hoffman NM, Kim Y, Geppert-Kleinrath H, Herrmann HW, Cerjan C, Landen OL, Appelbe Bet al., 2021, Time resolved ablator areal density during peak fusion burn on inertial confinement fusion implosions, PHYSICS OF PLASMAS, Vol: 28, ISSN: 1070-664X

Journal article

Crilly AJ, Appelbe BD, Mannion OM, Forrest CJ, Chittenden JPet al., 2021, The effect of areal density asymmetries on scattered neutron spectra in ICF implosions, Physics of Plasmas, Vol: 28, Pages: 1-9, ISSN: 1070-664X

Scattered neutron spectroscopy is a diagnostic technique commonly used to measure areal density in inertial confinement fusion experiments. Deleterious areal density asymmetries modify the shape of the scattered neutron spectrum. In this work, a novel analysis is developed, which can be used to fit the shape change. This will allow experimental scattered neutron spectroscopy to directly infer the amplitude and mode of the areal density asymmetries, with little sensitivity to confounding factors that affect other diagnostics for areal density. The model is tested on spectra produced by a neutron transport calculation with both isotropic and anisotropic primary fusion neutron sources. Multiple lines of sight are required to infer the areal density distribution over the whole sphere—we investigate the error propagation and optimal detector arrangement associated with the inference of mode 1 asymmetries.

Journal article

Gatu Johnson M, Adrian PJ, Anderson KS, Appelbe BD, Chittenden JP, Crilly AJ, Edgell D, Forrest CJ, Frenje JA, Glebov VY, Haines BM, Igumenshchev I, Jacobs-Perkins D, Janezic R, Kabadi NV, Knauer JP, Lahmann B, Mannion OM, Marshall FJ, Michel T, Seguin FH, Shah R, Stoeckl C, Walsh CA, Petrasso RDet al., 2020, Impact of stalk on directly driven inertial confinement fusion implosions, Physics of Plasmas, Vol: 27, Pages: 1-18, ISSN: 1070-664X

Low-mode asymmetries have emerged as one of the primary challenges to achieving high-performing inertial confinement fusion (ICF) implosions. In direct-drive ICF, an important potential seed of such asymmetries is the capsule stalk mount, the impact of which has remained a contentious question. In this paper, we describe the results from an experiment on the OMEGA laser with intentional offsets at varying angles to the capsule stalk mount, which clearly demonstrates the impact of the stalk mount on implosion dynamics. The angle between stalk and offset is found to significantly impact observables. Specifically, a larger directional flow is observed in neutron spectrum measurements when the offset is toward rather than away from the stalk, while an offset at 42° to the stalk gives minimal directional flow but still generates a large flow field in the implosion. No significant directional flow is seen due to stalk only. Time-integrated x-ray images support these flow observations. A trend is also seen in implosion yield, with lower yield obtained for offsets with a smaller angle than with a larger angle toward the stalk. Radiation hydrodynamic simulations using 2D DRACO and 2D/3D Chimera not including the stalk mount and using 2D xRAGE including the stalk mount are brought to bear on the data. The yield trend, the minimal directional flow with stalk only, and the larger flow enhancement observed with the offset toward the stalk are all reproduced in the xRAGE simulations. The results strongly indicate that the stalk impact must be considered and mitigated to achieve high-performing implosions.

Journal article

Volegov PL, Batha SH, Geppert-Kleinrath V, Danly CR, Merrill FE, Wilde CH, Wilson DC, Casey DT, Fittinghoff D, Appelbe B, Chittenden JP, Crilly AJ, McGlinchey Ket al., 2020, Density determination of the thermonuclear fuel region in inertial confinement fusion implosions, Journal of Applied Physics, Vol: 127, Pages: 1-10, ISSN: 0021-8979

Understanding of the thermonuclear burn in an inertial confinement fusion implosion requires knowledge of the local deuterium–tritium (DT) fuel density. Neutron imaging of the core now provides this previously unavailable information. Two types of neutron images are required. The first is an image of the primary 14-MeV neutrons produced by the D + T fusion reaction. The second is an image of the 14-MeV neutrons that leave the implosion hot spot and are downscattered to lower energy by elastic and inelastic collisions in the fuel. These neutrons are measured by gating the detector to record the 6–12 MeV neutrons. Using the reconstructed primary image as a nonuniform source, a set of linear equations is derived that describes the contribution of each voxel of the DT fuel region to a pixel in the downscattered image. Using the measured intensity of the 14-MeV neutrons and downscattered images, the set of equations is solved for the density distribution in the fuel region. The method is validated against test problems and simulations of high-yield implosions. The calculated DT density distribution from one experiment is presented.

Journal article

Crilly AJ, Appelbe BD, Mannion OM, Forrest CJ, Gopalaswamy V, Walsh CA, Chittenden JPet al., 2020, Neutron backscatter edge: A measure of the hydrodynamic properties of the dense DT fuel at stagnation in ICF experiments, Physics of Plasmas, Vol: 27, Pages: 012701-1-012701-11, ISSN: 1070-664X

The kinematic lower bound for the single scattering of neutrons produced in deuterium-tritium (DT) fusion reactions produces a backscatter edge in the measured neutron spectrum. The energy spectrum of backscattered neutrons is dependent on the scattering ion velocity distribution. As the neutrons preferentially scatter in the densest regions of the capsule, the neutron backscatter edge presents a unique measurement of the hydrodynamic conditions in the dense DT fuel. It is shown that the spectral shape of the edge is determined by the scattering rate weighted fluid velocity and temperature of the dense DT fuel layer during neutron production. In order to fit the neutron spectrum, a model for the various backgrounds around the backscatter edge is developed and tested on synthetic data produced from hydrodynamic simulations of OMEGA implosions. It is determined that the analysis could be utilized on current inertial confinement fusion experiments in order to measure the dense fuel properties.

Journal article

Appelbe B, Sherlock M, El-Amiri O, Walsh C, Chittenden Jet al., 2019, Modification of classical electron transport due to collisions between electrons and fast ions, Physics of Plasmas, Vol: 26, Pages: 102704-1-102704-12, ISSN: 1070-664X

A Fokker-Planck model for the interaction of fast ions with the thermal electrons in a quasineutral plasma is developed. When the fast ion population has a net flux (i.e., the distribution of fast ions is anisotropic in velocity space), the electron distribution function is perturbed from Maxwellian by collisions with the fast ions, even if the fast ion density is orders of magnitude smaller than the electron density. The Fokker-Planck model is used to derive classical electron transport equations (a generalized Ohm's law and a heat flow equation) that include the effects of the electron-fast ion collisions. It is found that these collisions result in a collisionally induced current term in the transport equations which can be significant. The new transport equations are analyzed in the context of a number of scenarios including α particle heating in inertial confinement fusion and magnetoinertial fusion plasmas as well as ion beam heating of dense plasmas.

Journal article

Tong JK, McGlinchey K, Appelbe BD, Walsh CA, Crilly AJ, Chittenden JPet al., 2019, Burn regimes in the hydrodynamic scaling of perturbed inertial confinement fusion hotspots, Nuclear Fusion, Vol: 59, Pages: 1-16, ISSN: 0029-5515

We present simulations of ignition and burn based on the Highfoot and high-density carbon indirect drive designs of the National Ignition Facility for three regimes of alpha-heating—self-heating, robust ignition and propagating burn—exploring hotspot power balance, perturbations and hydrodynamic scaling. A Monte-Carlo particle-in-cell charged particle transport package for the radiation-magnetohydrodynamics code Chimera was developed for this purpose, using a linked-list type data structure.The hotspot power balance between alpha-heating, electron thermal conduction and radiation was investigated in 1D for the three burn regimes. Stronger alpha-heating levels alter the hydrodynamics: sharper temperature and density gradients at hotspot edge; and increased hotspot pressures which further compress the shell, increase hotspot size and induce faster re-expansion. The impact of perturbations on this power balance is explored in 3D using a single Rayleigh–Taylor spike. Heat flow into the perturbation from thermal conduction and alpha-heating increases by factors of , due to sharper temperature gradients and increased proximity of the cold, dense material to the main fusion regions respectively. The radiative contribution remains largely unaffected in magnitude.Hydrodynamic scaling with capsule size and laser energy of different perturbation scenarios (a short-wavelength multi-mode and a long-wavelength radiation asymmetry) is explored in 3D, demonstrating the differing hydrodynamic evolution of the three alpha-heating regimes. The multi-mode yield increases faster with scale factor due to more synchronous compression producing higher temperatures and densities, and therefore stronger bootstrapping of alpha-heating. The perturbed implosions exhibit differences in hydrodynamic evolution due to alpha-heating in addition to the 1D effects, including: reduced perturbation growth due to ablation from both fire-polishing and stronger thermal conduction; and fa

Journal article

Walsh CA, McGlinchey K, Tong JK, Appelbe BD, Crilly A, Zhang MF, Chittenden JPet al., 2019, Perturbation modifications by pre-magnetisation of inertial confinement fusion implosions, Physics of Plasmas, Vol: 26, ISSN: 1070-664X

Pre-magnetisation of inertial confinement fusion implosions on the National Ignition Facility has the potential to raise current high-performing targets into the ignition regime [Perkins et al. "The potential of imposed magnetic fields for enhancing ignition probability and fusion energy yield in indirect-drive inertial confinement fusion," Phys. Plasmas 24, 062708 (2017)]. A key concern with this method is that the application of a magnetic field inherently increases asymmetry. This paper uses 3-D extended-magnetohydrodynamics Gorgon simulations to investigate how thermal conduction suppression, the Lorentz force, and α-particle magnetisation affect three hot-spot perturbation scenarios: a cold fuel spike, a time-dependent radiation drive asymmetry, and a multi-mode perturbation. For moderate magnetisations (B0 = 5 T), the single spike penetrates deeper into the hot-spot, as thermal ablative stabilisation is reduced. However, at higher magnetisations (B0 = 50 T), magnetic tension acts to stabilise the spike. While magnetisation of α-particle orbits increases the peak hot-spot temperature, no impact on the perturbation penetration depth is observed. The P4-dominated radiation drive asymmetry demonstrates the anisotropic nature of the thermal ablative stabilisation modifications, with perturbations perpendicular to the magnetic field penetrating deeper and perturbations parallel to the field being preferentially stabilised by increased heat-flows. Moderate magnetisations also increase the prevalence of high modes, while magnetic tension reduces vorticity at the hot-spot edge for larger magnetisations. For a simulated high-foot experiment, the yield doubles through the application of a 50 T magnetic field-an amplification which is expected to be larger for higher-performing configurations.

Journal article

Johnson MG, Appelbe BD, Chittenden JP, Crilly A, Delettrez J, Forrest C, Frenje JA, Glebov VY, Grimble W, Haines BM, Igumenshchev IV, Janezic R, Knauer JP, Lahmann B, Marshall FJ, Michel T, Seguin FH, Stoeckl C, Walsh C, Zylstra AB, Petrasso RDet al., 2019, Impact of imposed mode 2 laser drive asymmetry on inertial confinement fusion implosions, Physics of Plasmas, Vol: 26, ISSN: 1070-664X

Low-mode asymmetries have emerged as one of the primary challenges to achieving high-performing inertial confinement fusion implosions. These asymmetries seed flows in the implosions, which will manifest as modifications to the measured ion temperature (Tion) as inferred from the broadening of primary neutron spectra. The effects are important to understand (i) to learn to control and mitigate low-mode asymmetries and (ii) to experimentally more closely capture thermal Tion used as input in implosion performance metric calculations. In this paper, results from and simulations of a set of experiments with a seeded mode 2 in the laser drive are described. The goal of this intentionally asymmetrically driven experiment was to test our capability to predict and measure the signatures of flows seeded by the low-mode asymmetry. The results from these experiments [first discussed in M. Gatu Johnson et al., Phys. Rev. E 98, 051201(R) (2018)] demonstrate the importance of interplay of flows seeded by various asymmetry seeds. In particular, measured Tion and self-emission x-ray asymmetries are expected to be well captured by interplay between flows seeded by the imposed mode 2 and the capsule stalk mount. Measurements of areal density asymmetry also indicate the importance of the stalk mount as an asymmetry seed in these implosions. The simulations brought to bear on the problem (1D LILAC, 2D xRAGE, 3D ASTER, and 3D Chimera) show how thermal Tion is expected to be significantly lower than Tion as inferred from the broadening of measured neutron spectra. They also show that the electron temperature is not expected to be the same as Tion for these implosions.

Journal article

McGlinchey K, Appelbe BD, Crilly AJ, Tong JK, Walsh CA, Chittenden JPet al., 2018, Diagnostic signatures of performance degrading perturbations in inertial confinement fusion implosions, Physics of Plasmas, Vol: 25, ISSN: 1070-664X

We present 3D radiation-hydrodynamics simulations of indirect-drive inertial confinement fusion experiments performed at the National Ignition Facility (NIF). The simulations are carried out on two shots from different NIF experimental campaigns: N130927 from the high foot series and N161023 from the ongoing high density carbon series. Applying representative perturbation sources from each implosion, synthetic nuclear diagnostics are used to post-process the simulations to infer the stagnation parameters. The underlying physical mechanisms that produce the observed signatures are then explored. We find that the radiation asymmetry and tent scar perturbations extend the nuclear burn width; this is due to an asymmetric stagnation of the shell that causes the delivery of mechanical PdV work to be extended compared to an idealised implosion. Radiation asymmetries seed directed flow patterns that can result in a difference in the inferred ion temperature ranging from 80 eV to 230 eV depending on the magnitude and orientation of the asymmetry considered in the simulation; the tent scar shows no such temperature difference. For N130927, radiation asymmetries dominate the yield and inferred ion temperature and the tent scar has the largest influence on the neutron burnwidth. For N161023, the fill tube decreases the burn width by injecting mix into the hot spot, leading to a smaller hot spot and increased energy losses. Both the radiation asymmetry and the fill tube generate directed flows that lead to an anisotropic inferred temperature distribution. Through existing and novel synthetic neutron imaging techniques, we can observe the hot spot and shell shape to a degree that accurately captures the perturbations present.

Journal article

Crilly AJ, Appelbe BD, McGlinchey K, Walsh CA, Tong JK, Boxall AB, Chittenden JPet al., 2018, Synthetic nuclear diagnostics for inferring plasma properties of inertial confinement fusion implosions, Physics of Plasmas, Vol: 25, ISSN: 1070-664X

A suite of synthetic nuclear diagnostics has been developed to post-process radiation hydrodynamics simulations performed with the code Chimera. These provide experimental observables based on simulated capsule properties and are used to assess alternative experimental and data analysis techniques. These diagnostics include neutron spectroscopy, primary and scattered neutron imaging, neutron activation, γ-ray time histories and carbon γ-ray imaging. Novel features of the neutron spectrum have been analysed to infer plasma parameters. The nT and nD backscatter edges have been shown to provide a shell velocity measurement. Areal density asymmetries created by low mode perturbations have been inferred from the slope of the downscatter spectrum down to 10 MeV. Neutron activation diagnostics showed significant aliasing of high mode areal density asymmetries when observing a capsule implosion with 3D multimode perturbations applied. Carbon γ-ray imaging could be used to image the ablator at a high convergence ratio. Time histories of both the fusion and carbon γ signals showed a greater time difference between peak intensities for the perturbed case when compared to a symmetric simulation.

Journal article

Gatu Johnson M, Appelbe BD, Chittenden JP, Delettrez J, Forrest C, Frenje JA, Glebov VY, Grimble W, Haines BM, Igumenshchev I, Janezic R, Knauer JP, Lahmann B, Marshall FJ, Michel T, Séguin FH, Stoeckl C, Walsh C, Zylstra AB, Petrasso RDet al., 2018, Impact of asymmetries on fuel performance in inertial confinement fusion, Physical Review E, Vol: 98, ISSN: 2470-0045

Low-mode asymmetries prevent effective compression, confinement, and heating of the fuel in inertial confinement fusion (ICF) implosions, and their control is essential to achieving ignition. Ion temperatures (Tion) in ICF experiments are inferred from the broadening of primary neutron spectra. Directional motion (flow) of the fuel at burn also impacts broadening and will lead to artificially inflated "Tion" values. Flow due to low-mode asymmetries is expected to give rise to line-of-sight variations in measured Tion. We report on intentionally asymmetrically driven experiments at the OMEGA laser facility designed to test the ability to accurately predict and measure line-of-sight differences in apparent Tion due to low-mode asymmetry-seeded flows. Contrasted to chimera and xrage simulations, the measurements demonstrate how all asymmetry seeds have to be considered to fully capture the flow field in an implosion. In particular, flow induced by the stalk that holds the target is found to interfere with the seeded asymmetry. A substantial stalk-seeded asymmetry in the areal density of the implosion is also observed.

Journal article

Walsh C, Chittenden JP, McGlinchey K, Niasse NPL, Appelbe BDet al., 2017, Self-Generated magnetic fields in the stagnation phase of indirect-drive implosions on the national ignition facility, Physical Review Letters, Vol: 118, ISSN: 1079-7114

Three-dimensional extended-magnetohydrodynamic simulations of the stagnation phase of inertial confinement fusion implosion experiments at the National Ignition Facility are presented, showing self-generated magnetic fields over 10^4 T. Angular high mode-number perturbations develop large magnetic fields, but are localized to the cold, dense hot-spot surface, which is hard to magnetize. When low-mode perturbations are also present, the magnetic fields are injected into the hot core, reaching significant magnetizations, with peak local thermal conductivity reductions greater than 90%. However, Righi-Leduc heat transport effectively cools the hot spot and lowers the neutron spectra-inferred ion temperatures compared to the unmagnetized case. The Nernst effect qualitatively changes the results by demagnetizing the hot-spot core, while increasing magnetizations at the edge and near regions of large heat loss.

Journal article

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