Hagen Kleinert

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Hagen Kleinert
Hagmich.jpg
Photo taken in 2006
Born (1941-06-15) June 15, 1941 (age 72)
Festenberg, Germany
(now Twardogóra, Poland)
Fields Theoretical Physics
Institutions Free University of Berlin
Alma mater University of Hanover,
University of Colorado, Boulder
Influenced George Gamow,
Richard Feynman
Notable awards Max Born Prize (2008)
Majorana Prize (2008)

Hagen Kleinert (born 15 June 1941) is Professor of Theoretical Physics at the Free University of Berlin, Germany (since 1968), Honorary Doctor at the West University of Timişoara, and at the Kyrgyz-Russian Slavic University in Bishkek. He is also Honorary Member of the Russian Academy of Creative Endeavors. For his contributions to particle and solid state physics he was awarded the Max Born Prize 2008 with Medal. His contribution[1] to the memorial volume celebrating the 100th birthday of Lev Davidovich Landau earned him the Majorana Prize 2008 with Medal.

Publications[edit]

Kleinert has written ~400 papers on mathematical physics and the physics of elementary particles, nuclei, solid state systems, liquid crystals, biomembranes, microemulsions, polymers, and the theory of financial markets.[2] He has written several books on theoretical physics,[3] the most notable of which, Path Integrals in Quantum Mechanics, Statistics, Polymer Physics, and Financial Markets, has been published in five editions since 1990 and has received enthusiastic reviews.[4]

Education[edit]

He studied physics at the University of Hanover between 1960 and 1963, and at several American universities including Georgia Institute of Technology, where he learned general relativity as a graduate student from George Gamov, one of the fathers of the Big Bang theory. Kleinert earned his doctorate in 1967 at the University of Colorado, Boulder.

Career[edit]

As a young professor in 1972, Kleinert visited Caltech and was impressed by noted US physicist Richard Feynman. Later, Kleinert was to collaborate with Feynman[5] in some of the latter's last work.[6] This collaboration led to a mathematical method for converting divergent weak-coupling power series into convergent strong-coupling ones. This so-called variational perturbation theory yields at present the most accurate theory of critical exponents[7] observable close to second-order phase transitions, as confirmed for superfluid helium in satellite experiments.[8] He also discovered an alternative to Feynman's time-sliced path integral construction which can be used to solve the path integral formulations of the hydrogen atom and the centrifugal barrier, i.e. to calculate their energy levels and eigenstates, as special cases of a general strategy for treating systems with singular potentials using path integrals.[9][10]

Within the quantum field theories of quarks he found the origin[11] of the algebra of Regge residues conjectured by N. Cabibbo, L. Horwitz, and Y. Ne'eman (see p. 232 in reference [12]).

Discoveries[edit]

For superconductors he predicted in 1982 a tricritical point in the phase diagram between type-I and type-II superconductors where the order of the transition changes from second to first.[13] The predictions were confirmed in 2002 by Monte Carlo computer simulations.[14]

The theory is based on a disorder field theory dual to the order field theory of L.D. Landau for phase transitions which Kleinert developed in the books on Gauge Fields in Condensed Matter. In this theory, the statistical properties of fluctuating vortex or defect lines are described as elementary excitations with the help of fields, whose Feynman diagrams are the pictures of the lines.

At the 1978 summer school in Erice he proposed the existence of broken supersymmetry in atomic nuclei,[15] which has since been observed experimentally.[16]

His theory of collective quantum fields[17] and the Hadronization of Quark Theories[18] are prototypes for numerous developments in the theory of condensed matter, nuclear and elementary particle physics.

Together with K. Maki he proposed and clarified in 1981 a possible icosahedral phase of quasicrystals.[19] This structure was discovered three years later in aluminum transition metal alloys by Dan Shechtman, which earned him the Nobel Prize 2011. See historical notes.

String theory contributions[edit]

In 1986 he introduced[20] stiffness into the theory of strings, which had formerly been characterized by tension alone. This greatly improved the description of the physical properties of strings. The Russian physicist A. Polyakov simultaneously proposed a similar extension, and so the model is now known as the Polyakov-Kleinert string.

Theory of distributions[edit]

Together with A. Chervyakov, Kleinert developed an extension of the theory of distributions from linear spaces to semigroups by defining their products uniquely (in the mathematical theory, only linear combinations are defined). The extension is motivated by the physical requirement that the corresponding path integrals must be invariant under coordinate transformations,[21] which is necessary for the equivalence of the path integral formulation to Schrödinger theory.

String theory alternative[edit]

As an alternative to string theory, Kleinert used the complete analogy between non-Euclidean geometry and the geometry of crystals with defects to construct a model of the universe called the World Crystal or Planck-Kleinert crystal. In this model, matter creates defects in spacetime which generate curvature. This curvature reproduces all the effects of general relativity, but leads to different physics than string theory at the scale of the Planck length. This theory inspired Italian artist Laura Pesce to create glass sculptures entitled "world crystal" (see also lower left on this page).

Current[edit]

Kleinert is a senior member of the faculty for the International Relativistic Astrophysics Ph.D. (IRAP) Project, which forms part of the international network for astrophysics (ICRANet). He was also involved in the European Science Foundation's project Cosmology in the Laboratory.

Kleinert's 60. birthday was honored by a Festschrift and a Festcolloquium with 65 contributions by international colleagues (for instance Y. Ne'eman, R. Jackiw, H. Fritzsch, R. Ruffini, C. DeWitt, L. Kauffman, J. Devreese, and K. Maki).

References[edit]

  1. ^ Kleinert H. (2009). "From Landau's Order Parameter to Modern Disorder Fields". In "Lev Davidovich Landau and his Impact on Contemporary Theoretical Physics", publ. in "Horizons in World Physics") 264: 103. Bibcode:2010AIPC.1205..103K. doi:10.1063/1.3382313. 
  2. ^ His Papers.
  3. ^ His books.
  4. ^ Henry B.I. (2007). "Book Reviews". Australian Physics 44 (3): 110. 
  5. ^ Kleinert H. (2004). "Travailler avec Feynman". Science (French edition) 19: 89–95. 
  6. ^ Feynman R.P., Kleinert H. (1986). "Effective classical partition functions". Physical Review A 34 (6): 5080–5084. Bibcode:1986PhRvA..34.5080F. doi:10.1103/PhysRevA.34.5080. PMID 9897894. 
  7. ^ Kleinert, H., "Critical exponents from seven-loop strong-coupling φ4 theory in three dimensions". Physical Review D 60, 085001 (1999)
  8. ^ Lipa J.A.; Nissen, J.; Stricker, D.; Swanson, D.; Chui, T. (2003). "Specific heat of liquid helium in zero gravity very near the lambda point". Physical Review B 68 (17): 174518. arXiv:cond-mat/0310163. Bibcode:2003PhRvB..68q4518L. doi:10.1103/PhysRevB.68.174518. 
  9. ^ Duru I.H., Kleinert H. (1979). "Solution of the path integral for the H-atom". Physics Letters B 84 (2): 185–188. Bibcode:1979PhLB...84..185D. doi:10.1016/0370-2693(79)90280-6. 
  10. ^ Duru I.H., Kleinert H. (1982). "Quantum Mechanics of H-Atom from Path Integrals". Fortschr. Phys 30 (2): 401–435. Bibcode:1982ForPh..30..401D. doi:10.1002/prop.19820300802. 
  11. ^ Kleinert H. (1973). "Bilocal Form Factors and Regge Couplings". Nucl. Physics B65: 77–111. Bibcode:1973NuPhB..65...77K. doi:10.1016/0550-3213(73)90276-9. 
  12. ^ Ne'eman Y, Reddy V.T.N. (1981). "Universality in the Algebra of Vertex Strengths as Generated by Bilocal Currents". Nucl. Phys. B 84: 221–233. Bibcode:1975NuPhB..84..221N. doi:10.1016/0550-3213(75)90547-7. 
  13. ^ Kleinert H. (1982). "Disorder Version of the Abelian Higgs Model and the Order of the Superconductive Phase Transition". Lett. Nuovo Cimento 35 (13): 405–412. doi:10.1007/BF02754760. 
  14. ^ Hove J., Mo S., Sudbo A. (2002). "Vortex interactions and thermally induced crossover from type-I to type-II superconductivity". Phys. Rev. B 66 (6): 064524. arXiv:cond-mat/0202215. Bibcode:2002PhRvB..66f4524H. doi:10.1103/PhysRevB.66.064524. 
  15. ^ Ferrara S., Discussion Section of 1978 Erice Lecture publ. in (1980). "The New Aspects of Subnuclear Physics". Plenum Press, N.Y., Zichichi A. Ed.: 40. 
  16. ^ Metz A., Jolie J., Graw G., Hertenberger R., Gröger J., Günther C., Warr N., Eisermann Y. (1999). "Evidence for the Existence of Supersymmetry in Atomic Nuclei". Physical Review Letters 83 (8): 1542. Bibcode:1999PhRvL..83.1542M. doi:10.1103/PhysRevLett.83.1542. 
  17. ^ Kleinert H. (1978). "Collective Quantum Fields". Fortschritte der Physik 36 (11-12): 565–671. Bibcode:1978ForPh..26..565K. doi:10.1002/prop.19780261102. 
  18. ^ Kleinert H., Lectures presented at the Erice Summer Institute 1976 (1978). "On the Hadronization of Quark Theories". Understanding the Fundamental Constituents of Matter, Plenum Press, New York, 1978 (A. Zichichi ed.) 62 (4): pp. 289–390. Bibcode:1976PhLB...62..429K. doi:10.1016/0370-2693(76)90676-6. 
  19. ^ Kleinert H., Maki K. (1981). "Lattice Textures in Cholesteric Liquid Crystals". Fortschritte der Physik 29 (5): 219–259. Bibcode:1981ForPh..29..219K. doi:10.1002/prop.19810290503. 
  20. ^ Kleinert H. (1989). "The Membrane Properties of Condensing Strings". Phys. Lett. B 174 (3): 335. Bibcode:1986PhLB..174..335K. doi:10.1016/0370-2693(86)91111-1. 
  21. ^ Kleinert H., Chervyakov A. (2001). "Rules for integrals over products of distributions from coordinate independence of path integrals". Europ. Phys. J. C 19 (4): 743–747. arXiv:quant-ph/0002067. Bibcode:2001EPJC...19..743K. doi:10.1007/s100520100600. 

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