Valentine Bargmann
Born(1908-04-06)6 April 1908
Died20 July 1989(1989-07-20) (aged 81)
Alma materUniversity of Berlin
Known forBargmann algebra
Bargmann kernel
Bargmann's limit
Bargmann's theorem
Bargmann–Wigner equations
Bargmann–Michel–Telegdi equation
Segal–Bargmann space
Representation theory of SL2(R)
AwardsMax Planck Medal (1988)
Wigner Medal (1978)
Scientific career
FieldsPhysics
InstitutionsPrinceton University
ThesisÜber die durch Elektronenstrahlen in Kristallen angeregte Lichtemission (1937)
Doctoral advisorGregor Wentzel

Valentine "Valya" Bargmann (April 6, 1908 – July 20, 1989)[1] was a German-American mathematician and theoretical physicist.

Biography

Born in Berlin, Germany, to a German Jewish family, Bargmann studied there from 1925 to 1933. After the National Socialist Machtergreifung, he moved to Switzerland to the University of Zürich where he received his Ph.D. under Gregor Wentzel.

He emigrated to the U.S., barely managing immigration acceptance as his German passport was to be revoked—with only two days of validity left.

At the Institute for Advanced Study in Princeton (1937–46) he worked as an assistant to Albert Einstein,[2] publishing with him and Peter Bergmann on classical five-dimensional Kaluza–Klein theory (1941). He taught at Princeton University since 1946, to the rest of his career.

He pioneered understanding of the irreducible unitary representations of SL2(R) and the Lorentz group (1947). He further formulated the Bargmann–Wigner equations with Eugene Wigner (1948), for particles of arbitrary spin, building up on work of several theorists who pioneered quantum mechanics.[3][4]

Bargmann's theorem (1954) on projective unitary representations of Lie groups gives a condition for when a projective unitary representation of a Lie group comes from an ordinary unitary representation of its universal cover.

Bargmann further discovered the Bargmann–Michel–Telegdi equation (1959) describing relativistic precession; Bargmann's limit of the maximum number of QM bound states of a potential (1952); the notion of Bargmann potentials[5] for the radial Schrödinger equations with bound states but no non-trivial scattering, which play a basic rôle in the theory of Solitons, and the holomorphic representation in the Segal–Bargmann space (1961), including the Bargmann kernel.

Bargmann was elected a Fellow of the American Academy of Arts and Sciences in 1968.[6] In 1978, he received the Wigner Medal, together with Wigner himself, in the founding year of the prize. In 1979, Bargmann was elected to the US National Academy of Sciences.[7] In 1988, he received the Max Planck Medal of the German Physical Society.

He was also a talented pianist.

He died in Princeton in 1989.

References

  1. ^ "Valentine Bargmann". Biographical Memoirs, Vol. 76. National Academy Press. 1999. pp. 37–50. ISBN 0-309-06434-1.
  2. ^ Witten, E. (2014). "A Note On Einstein, Bergmann, and the Fifth Dimension", arXiv:1401.8048
  3. ^ V. Bargmann Irreducible Unitary Representations of the Lorentz Group The Annals of Mathematics 2nd Ser., Vol. 48, No. 3 (Jul., 1947), pp. 568-640
  4. ^ Bargmann, V.; Wigner, E. P. (1948). "Group theoretical discussion of relativistic wave equations". Proc. Natl. Acad. Sci. USA. 34 (5): 211–23. Bibcode:1948PNAS...34..211B. doi:10.1073/pnas.34.5.211. PMC 1079095. PMID 16578292.
  5. ^ V. Bargmann (1949). "On the Connection between Phase Shifts and Scattering Potential", Reviews of Modern Physics, 21(3), 488–493. doi:10.1103/revmodphys.21.488
  6. ^ "Book of Members, 1780-2010: Chapter B" (PDF). American Academy of Arts and Sciences. Retrieved May 17, 2011.
  7. ^ "NAS Membership Directory". National Academy of Sciences. Retrieved March 22, 2020.

Selected bibliography