John H. Malmberg

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John Holmes Malmberg
Born(1927-07-05)July 5, 1927
Gettysburg, Pennsylvania
DiedNovember 1, 1992(1992-11-01) (aged 65)
Del Mar, California
NationalityAmerican
EducationIllinois State University (B.S.)
University of Illinois at Urbana–Champaign (M.S., Ph.D.)
Known forSingle-component and non-neutral plasma research, Penning–Malmberg trap, collisionless damping of plasma waves, plasma wave echo
Awards
Scientific career
FieldsPlasma physics
InstitutionsGeneral Atomics, University of California, San Diego

John Holmes Malmberg (July 5, 1927 – November 1, 1992) was an American plasma physicist and a professor at the University of California, San Diego.[1] He was known for making the first experimental measurements of Landau damping of plasma waves in 1964,[2] as well as for his research on non-neutral plasmas and the development of the Penning–Malmberg trap.[3][4]

In 1985, Malmberg won the James Clerk Maxwell Prize for Plasma Physics for his experimental work on wave-particle interactions in neutral plasmas and his studies on pure electron plasmas.[5] He was later co-awarded the John Dawson Award for Excellence in Plasma Physics Research in 1991 for his contribution to research on non-neutral plasmas.[6]

Early life and career[edit]

Malmberg studied at Illinois State University (bachelor 1949) and the University of Illinois at Urbana–Champaign (master 1951), where he received his doctorate in 1957. From 1957 to 1969, he was a staff scientist working in the area of plasma physics at General Atomics in San Diego, California. From 1967 until his death, he was a professor of physics at the University of California, San Diego (UCSD) in La Jolla, California.[1][7]

In 1980, Malmberg was appointed to the first Plasma Sciences Committee of the National Research Council.[citation needed] In that capacity, he was a strong voice for the importance of basic plasma experiments in maintaining the health of plasma science. In an era when small-scale and basic plasma physics research was nearing an ebb, Malmberg emphasized the importance of being able to follow the internal logic of the science, which he believed to be of paramount importance in doing basic research.

Scientific contributions[edit]

Landau damping of plasma waves[edit]

Malmberg and Charles Wharton made the first experimental measurements of Landau damping of plasma waves in 1964,[2] two decades after its prediction by Lev Landau.[8] Since this damping is collisionless, the free energy and phase-space memory associated with the damped wave are not lost, but are subtly stored in the plasma. Malmberg and collaborators demonstrated explicitly the reversible nature of this process by observation of the plasma wave echo[9][10] in which a wave “spontaneously” appears in the plasma as an ‘echo’ of two previously launched waves that had been Landau damped.

Penning–Malmberg traps and non-neutral plasmas[edit]

See also: Penning–Malmberg trap

Neutral plasmas are notoriously difficult to confine. In contrast, Malmberg and collaborators predicted and demonstrated experimentally[3][4][11] that plasmas with a single sign of charge, such as pure electron or pure ion plasmas, can be confined for long periods (e.g., hours). This was accomplished using an arrangement of electric and magnetic fields similar to that of a Penning trap, but optimized to confine single-component plasmas. In recognition of Malmberg’s contributions to the development of these devices, they are now referred to as Penning–Malmberg traps.

Malmberg and collaborators, realized that non-neutral plasmas offer research opportunities not available with neutral plasmas. In contrast to neutral plasmas, plasmas with a single sign of charge can reach states of global thermal equilibria.[12][13] The possibility of using thermal equilibrium statistical mechanics to describe the plasma provides a large advantage to theory. [14] Furthermore, states near such thermal equilibria can be more easily controlled experimentally and departures from equilibrium studied with precision.

When a neutral plasma is cooled, it simply recombines; but a plasma with a single sign of charge can be cooled without recombination. Malmberg constructed a trap for a pure electron plasma with walls at 4.2 K. Cyclotron radiation from the electrons then cooled the plasma to a few Kelvin. Theory argued that electron-electron collisions in such a strongly magnetized and low temperature plasma would be qualitatively different than those in warmer plasmas. Malmberg measured the equipartition rate between electron velocity components parallel to and perpendicular to the magnetic field and confirmed the striking prediction that it decreases exponentially with decreasing temperature.[15]

Malmberg and Thomas Michael O'Neil predicted that a very cold, single-species plasma would undergo a phase transition to a body-centered cubic crystalline state.[16] Later, John Bollinger and collaborators created such a state by laser cooling a plasma of singly ionized beryllium ions to temperatures of a few millikelvin.[17] In other experiments, trapped pure electron plasmas are used to model the two-dimensional (2D) vortex dynamics expected for an ideal fluid.[18][19]

In the late 1980s, pure positron (i.e., antielectron) plasmas were created using the Penning–Malmberg trap technology.[20] This, and advances in confining low-energy antiprotons,[21] led to the creation of low-energy antihydrogen a decade later.[22][23] These and subsequent developments[24][25] have spawned a wealth of research with low-energy antimatter.[26] This includes ever more precise studies of antihydrogen and comparison with the properties of hydrogen[27] and formation of the di-positronium molecule (Ps, )[28] predicted by J. A. Wheeler in 1946.[29] The Penning–Malmberg trap technology is now being used to create a new generation of high-quality positroniumatom () beams for atomic physics studies.[30][31]

In the broader view, Malmberg’s seminal studies with trapped single-component and non-neutral plasmas have stimulated vibrant sub-fields of plasma physics with surprisingly broad impacts in the wider world of physics.

Honors and awards[edit]

In 1985, Malmberg received the James Clerk Maxwell Prize for Plasma Physics from the American Physical Society for "his outstanding experimental studies which expanded our understanding of wave-particle interactions in neutral plasmas and increased our confidence in plasma theory; and for his pioneering studies of the confinement and transport of pure electron plasmas".[5]

And in 1991, he was co-awarded the John Dawson Award for Excellence in Plasma Physics Research with Charles F. Driscoll and Thomas Michael O'Neil, for their studies of single-component electron plasmas.[6]

Legacy[edit]

In 1993, the UCSD physics department established the John Holmes Malmberg Prize in his honor. It is awarded annually to an outstanding undergraduate physics major with interests in experimental physics.[32]

References[edit]

  1. ^ a b "Plasma Physics Pioneer at UCSD Dies". Los Angeles Times. 1992-11-24. Retrieved 2020-02-23.
  2. ^ a b Malmberg, J. H.; Wharton, C. B. (1964). "Collisionless Damping of Electrostatic Plasma Waves". Physical Review Letters. 13 (6): 184–186. Bibcode:1964PhRvL..13..184M. doi:10.1103/PhysRevLett.13.184.
  3. ^ a b Malmberg, J. H.; Degrassie, J. S. (1975). "Properties of Nonneutral Plasma". Physical Review Letters. 35 (9): 577–580. Bibcode:1975PhRvL..35..577M. doi:10.1103/PhysRevLett.35.577.
  4. ^ a b Malmberg, J. H.; Driscoll, C. F. (1980). "Long-Time Containment of a Pure Electron Plasma". Physical Review Letters. 44 (10): 654–657. Bibcode:1980PhRvL..44..654M. doi:10.1103/PhysRevLett.44.654.
  5. ^ a b "1985 James Clerk Maxwell Prize for Plasma Physics Recipient". American Physical Society. Retrieved 2020-02-23.
  6. ^ a b "John Dawson Award for Excellence in Plasma Physics Research". www.aps.org. Retrieved 2020-02-23.
  7. ^ "Malmberg, J. H." history.aip.org. Retrieved 2020-02-23.
  8. ^ Landau, L. D. "On the vibrations of the electronic plasma". Zh. Eksp. Teor. Fiz. 16: 574–86 (reprinted 1965 Collected Papers of Landau ed D ter Haar (Oxford: Pergamon) pp 445–60).
  9. ^ Gould, R. W.; O'Neil, T. M.; Malmberg, J. H. (1967). "Plasma Wave Echo". Physical Review Letters. 19 (5): 219–222. Bibcode:1967PhRvL..19..219G. doi:10.1103/PhysRevLett.19.219.
  10. ^ Malmberg, J. H.; Wharton, C. B.; Gould, R. W.; O’Neil, T. M. (1968). "Observation of Plasma Wave Echoes" (PDF). Physics of Fluids. 11 (6): 1147. Bibcode:1968PhFl...11.1147M. doi:10.1063/1.1692075.
  11. ^ o'Neil, T. M. (1980). "A confinement theorem for nonneutral plasmas". Physics of Fluids. 23 (11): 2216. Bibcode:1980PhFl...23.2216O. doi:10.1063/1.862904.
  12. ^ Prasad, S. A.; o'Neil, T. M. (1979). "Finite length thermal equilibria of a pure electron plasma column". Physics of Fluids. 22 (2): 278. Bibcode:1979PhFl...22..278P. doi:10.1063/1.862578.
  13. ^ Driscoll, C. F.; Malmberg, J. H.; Fine, K. S. (1988). "Observation of transport to thermal equilibrium in pure electron plasmas". Physical Review Letters. 60 (13): 1290–1293. Bibcode:1988PhRvL..60.1290D. doi:10.1103/PhysRevLett.60.1290. PMID 10037997.
  14. ^ Dubin, Daniel H. E.; o'Neil, T. M. (1999). "Trapped nonneutral plasmas, liquids, and crystals (The thermal equilibrium states)". Reviews of Modern Physics. 71 (1): 87–172. Bibcode:1999RvMP...71...87D. doi:10.1103/RevModPhys.71.87.
  15. ^ Beck, B. R.; Fajans, J.; Malmberg, J. H. (1992). "Measurement of collisional anisotropic temperature relaxation in a strongly magnetized pure electron plasma". Physical Review Letters. 68 (3): 317–320. Bibcode:1992PhRvL..68..317B. doi:10.1103/PhysRevLett.68.317. PMID 10045861.
  16. ^ Malmberg, J. H.; O'Neil, T. M. (1977). "Pure Electron Plasma, Liquid, and Crystal". Physical Review Letters. 39 (21): 1333–1336. Bibcode:1977PhRvL..39.1333M. doi:10.1103/PhysRevLett.39.1333.
  17. ^ Bollinger, J. J.; Mitchell, T. B.; Huang, X.-P.; Itano, W. M.; Tan, J. N.; Jelenković, B. M.; Wineland, D. J. (2000). "Crystalline order in laser-cooled, non-neutral ion plasmas". Physics of Plasmas. 7 (1): 7–13. Bibcode:2000PhPl....7....7B. doi:10.1063/1.873818.
  18. ^ Fine, K. S.; Driscoll, C. F.; Malmberg, J. H.; Mitchell, T. B. (1991). "Measurements of symmetric vortex merger". Physical Review Letters. 67 (5): 588–591. Bibcode:1991PhRvL..67..588F. doi:10.1103/PhysRevLett.67.588. PMID 10044936.
  19. ^ Fine, K. S.; Cass, A. C.; Flynn, W. G.; Driscoll, C. F. (1995). "Relaxation of 2D Turbulence to Vortex Crystals". Physical Review Letters. 75 (18): 3277–3280. Bibcode:1995PhRvL..75.3277F. doi:10.1103/PhysRevLett.75.3277. PMID 10059543.
  20. ^ Surko, C. M.; Leventhal, M.; Passner, A. (1989). "Positron Plasma in the Laboratory". Physical Review Letters. 62 (8): 901–904. Bibcode:1989PhRvL..62..901S. doi:10.1103/PhysRevLett.62.901. PMID 10040367.
  21. ^ Gabrielse, G.; Fei, X.; Helmerson, K.; Rolston, S. L.; Tjoelker, R.; Trainor, T. A.; Kalinowsky, H.; Haas, J.; Kells, W. (1986). "First Capture of Antiprotons in a Penning Trap: A Kiloelectronvolt Source". Physical Review Letters. 57 (20): 2504–2507. Bibcode:1986PhRvL..57.2504G. doi:10.1103/PhysRevLett.57.2504. PMID 10033784.
  22. ^ Amoretti, M.; Amsler, C.; Bonomi, G.; Bouchta, A.; Bowe, P.; Carraro, C.; Cesar, C. L.; Charlton, M.; Collier, M. J. T.; Doser, M.; Filippini, V.; Fine, K. S.; Fontana, A.; Fujiwara, M. C.; Funakoshi, R.; Genova, P.; Hangst, J. S.; Hayano, R. S.; Holzscheiter, M. H.; Jørgensen, L. V.; Lagomarsino, V.; Landua, R.; Lindelöf, D.; Rizzini, E. Lodi; MacRì, M.; Madsen, N.; Manuzio, G.; Marchesotti, M.; Montagna, P.; et al. (2002). "Production and detection of cold antihydrogen atoms". Nature. 419 (6906): 456–459. Bibcode:2002Natur.419..456A. doi:10.1038/nature01096. PMID 12368849. S2CID 4315273.
  23. ^ Gabrielse, G.; Bowden, N. S.; Oxley, P.; Speck, A.; Storry, C. H.; Tan, J. N.; Wessels, M.; Grzonka, D.; Oelert, W.; Schepers, G.; Sefzick, T.; Walz, J.; Pittner, H.; Hänsch, T. W.; Hessels, E. A.; ATRAP Collaboration (2002). "Driven Production of Cold Antihydrogen and the First Measured Distribution of Antihydrogen States". Physical Review Letters. 89 (23): 233401. Bibcode:2002PhRvL..89w3401G. doi:10.1103/PhysRevLett.89.233401. PMID 12485006.
  24. ^ Danielson, J. R.; Dubin, D. H. E.; Greaves, R. G.; Surko, C. M. (2015). "Plasma and trap-based techniques for science with positrons". Reviews of Modern Physics. 87 (1): 247–306. Bibcode:2015RvMP...87..247D. doi:10.1103/RevModPhys.87.247.
  25. ^ Fajans, J.; Surko, C. M. (2020). "Plasma and trap-based techniques for science with antimatter". Physics of Plasmas. 27 (3): 030601. Bibcode:2020PhPl...27c0601F. doi:10.1063/1.5131273.
  26. ^ Surko, C. M.; Gribakin, G. F.; Buckman, S. J. (2005). "Low-energy positron interactions with atoms and molecules". Journal of Physics B: Atomic, Molecular and Optical Physics. 38 (6): R57–R126. doi:10.1088/0953-4075/38/6/R01. S2CID 15031194.
  27. ^ Ahmadi, M.; Alves, B. X. R.; Baker, C. J.; Bertsche, W.; Capra, A.; Carruth, C.; Cesar, C. L.; Charlton, M.; Cohen, S.; Collister, R.; Eriksson, S.; Evans, A.; Evetts, N.; Fajans, J.; Friesen, T.; Fujiwara, M. C.; Gill, D. R.; Hangst, J. S.; Hardy, W. N.; Hayden, M. E.; Isaac, C. A.; Johnson, M. A.; Jones, J. M.; Jones, S. A.; Jonsell, S.; Khramov, A.; Knapp, P.; Kurchaninov, L.; Madsen, N.; et al. (2018). "Characterization of the 1S–2S transition in antihydrogen". Nature. 557 (7703): 71–75. Bibcode:2018Natur.557...71A. doi:10.1038/s41586-018-0017-2. PMC 6784861. PMID 29618820.
  28. ^ Cassidy, D. B.; Mills, A. P. (2007). "The production of molecular positronium". Nature. 449 (7159): 195–197. Bibcode:2007Natur.449..195C. doi:10.1038/nature06094. PMID 17851519. S2CID 11269624.
  29. ^ Wheeler, John Archibald (1946). "Polyelectrons". Annals of the New York Academy of Sciences. 48 (3): 219–238. doi:10.1111/j.1749-6632.1946.tb31764.x. S2CID 222088254.
  30. ^ Cassidy, David B. (2018). "Experimental progress in positronium laser physics". The European Physical Journal D. 72 (3): 53. Bibcode:2018EPJD...72...53C. doi:10.1140/epjd/e2018-80721-y.
  31. ^ Michishio, K.; Chiari, L.; Tanaka, F.; Oshima, N.; Nagashima, Y. (2019). "A high-quality and energy-tunable positronium beam system employing a trap-based positron beam". Review of Scientific Instruments. 90 (2): 023305. Bibcode:2019RScI...90b3305M. doi:10.1063/1.5060619. PMID 30831693. S2CID 73497181.
  32. ^ "UC San Diego | Fellowships and Awards in Physics". www-physics.ucsd.edu. Retrieved 2020-02-23.
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