Harald J. W. Mueller-Kirsten

Last updated
Harald J.W. Mueller-Kirsten
Harald J.W. Muller-Kirsten.jpg
H.J.W. Müller-Kirsten
Born (1935-05-19) May 19, 1935 (age 88)
Nationality German Flag of Germany.svg
Alma mater University of Western Australia
Known for Asymptotic expansions of Functions of mathematical physics and their eigenvalues, Quantum field theory, Periodic instantons, Supersymmetry
Scientific career
Fields Theoretical Physics
Doctoral advisor Robert Balson Dingle

Harald J.W. Mueller-Kirsten (born 1935) is a German theoretical physicist specializing in Theoretical particle physics and Mathematical physics.

Contents

Education and career

Müller-Kirsten obtained the B.Sc. (First Class Honours) in 1957 and the Ph.D. in 1960 from the University of Western Australia in Perth, where his doctoral advisor was Robert Balson Dingle. [1] Thereafter he was postdoc at the Ludwig Maximilians University in Munich (Institute of F. Bopp) and obtained the habilitation there in 1971. Müller-Kirsten was an assistant professor at the American University of Beirut in 1967, NATO-Fellow at the Lawrence Radiation Laboratory in Berkeley in 1970, and Max-Kade-Foundation Fellow at SLAC, Stanford in 1974–75. In 1972 he was appointed Wissenschaftlicher Rat and Professor (H2) at the University of Kaiserslautern, then there in 1976 University Professor (C2) and in 1995 University Professor (C3).

Research achievements

  1. Asymptotic expansions of Mathieu functions, spheroidal wave functions, Lamé functions and ellipsoidal wave functions and their eigenvalues. [2]
  2. Asymptotic expansions of Regge poles for Yukawa potentials (in agreement with Langer-corrected WKB calculations). [3]
  3. Eigenvalue and level-splitting formula for double-well potentials. [4]
  4. Path integral method applied to quartic and cosine potentials. [5]
  5. Discovery that for quartic and cosine potentials the equation of small fluctuations around the classical solution is a Lamé equation. [6]
  6. Derivation of S-matrix and absorptivity for the singular potential (cf. modified Mathieu equation) and application to string theory. [7]
  7. Construction and quantization of gauge theory models, [8] Faddeev–Jackiw quantization of systems with constraints, [9]

Books

Outside of physics

Related Research Articles

<span class="mw-page-title-main">Mathematical physics</span> Application of mathematical methods to problems in physics

Mathematical physics refers to the development of mathematical methods for application to problems in physics. The Journal of Mathematical Physics defines the field as "the application of mathematics to problems in physics and the development of mathematical methods suitable for such applications and for the formulation of physical theories". An alternative definition would also include those mathematics that are inspired by physics, known as physical mathematics.

<span class="mw-page-title-main">Instanton</span> Solitons in Euclidean spacetime

An instanton is a notion appearing in theoretical and mathematical physics. An instanton is a classical solution to equations of motion with a finite, non-zero action, either in quantum mechanics or in quantum field theory. More precisely, it is a solution to the equations of motion of the classical field theory on a Euclidean spacetime.

The Chern–Simons theory is a 3-dimensional topological quantum field theory of Schwarz type developed by Edward Witten. It was discovered first by mathematical physicist Albert Schwarz. It is named after mathematicians Shiing-Shen Chern and James Harris Simons, who introduced the Chern–Simons 3-form. In the Chern–Simons theory, the action is proportional to the integral of the Chern–Simons 3-form.

In particle physics, the hypothetical dilaton particle is a particle of a scalar field that appears in theories with extra dimensions when the volume of the compactified dimensions varies. It appears as a radion in Kaluza–Klein theory's compactifications of extra dimensions. In Brans–Dicke theory of gravity, Newton's constant is not presumed to be constant but instead 1/G is replaced by a scalar field and the associated particle is the dilaton.

In mathematics, the isometry group of a metric space is the set of all bijective isometries from the metric space onto itself, with the function composition as group operation. Its identity element is the identity function. The elements of the isometry group are sometimes called motions of the space.

In mathematical physics, geometric quantization is a mathematical approach to defining a quantum theory corresponding to a given classical theory. It attempts to carry out quantization, for which there is in general no exact recipe, in such a way that certain analogies between the classical theory and the quantum theory remain manifest. For example, the similarity between the Heisenberg equation in the Heisenberg picture of quantum mechanics and the Hamilton equation in classical physics should be built in.

In quantum physics, Regge theory is the study of the analytic properties of scattering as a function of angular momentum, where the angular momentum is not restricted to be an integer multiple of ħ but is allowed to take any complex value. The nonrelativistic theory was developed by Tullio Regge in 1959.

In theoretical physics, there are many theories with supersymmetry (SUSY) which also have internal gauge symmetries. Supersymmetric gauge theory generalizes this notion.

<span class="mw-page-title-main">Ludvig Faddeev</span> Russian mathematician and physicist (1934–2017)

Ludvig Dmitrievich Faddeev was a Soviet and Russian mathematical physicist. He is known for the discovery of the Faddeev equations in the theory of the quantum mechanical three-body problem and for the development of path integral methods in the quantization of non-abelian gauge field theories, including the introduction of Faddeev–Popov ghosts. He led the Leningrad School, in which he along with many of his students developed the quantum inverse scattering method for studying quantum integrable systems in one space and one time dimension. This work led to the invention of quantum groups by Drinfeld and Jimbo.

In mathematics, a Lamé function, or ellipsoidal harmonic function, is a solution of Lamé's equation, a second-order ordinary differential equation. It was introduced in the paper. Lamé's equation appears in the method of separation of variables applied to the Laplace equation in elliptic coordinates. In some special cases solutions can be expressed in terms of polynomials called Lamé polynomials.

In physics, relativistic quantum mechanics (RQM) is any Poincaré covariant formulation of quantum mechanics (QM). This theory is applicable to massive particles propagating at all velocities up to those comparable to the speed of light c, and can accommodate massless particles. The theory has application in high energy physics, particle physics and accelerator physics, as well as atomic physics, chemistry and condensed matter physics. Non-relativistic quantum mechanics refers to the mathematical formulation of quantum mechanics applied in the context of Galilean relativity, more specifically quantizing the equations of classical mechanics by replacing dynamical variables by operators. Relativistic quantum mechanics (RQM) is quantum mechanics applied with special relativity. Although the earlier formulations, like the Schrödinger picture and Heisenberg picture were originally formulated in a non-relativistic background, a few of them also work with special relativity.

Combinatorial physics or physical combinatorics is the area of interaction between physics and combinatorics.

Gennadi Sardanashvily was a theoretical physicist, a principal research scientist of Moscow State University.

In mathematics, any Lagrangian system generally admits gauge symmetries, though it may happen that they are trivial. In theoretical physics, the notion of gauge symmetries depending on parameter functions is a cornerstone of contemporary field theory.

In quantum physics, the quantum inverse scattering method (QISM) or the algebraic Bethe ansatz is a method for solving integrable models in 1+1 dimensions, introduced by Leon Takhtajan and L. D. Faddeev in 1979.

The so-called double-well potential is one of a number of quartic potentials of considerable interest in quantum mechanics, in quantum field theory and elsewhere for the exploration of various physical phenomena or mathematical properties since it permits in many cases explicit calculation without over-simplification.

<span class="mw-page-title-main">Daya Shankar Kulshreshtha</span> Indian theoretical physicist

Daya Shankar Kulshreshtha is an Indian theoretical physicist, specializing in formal aspects of quantum field theory, string theory, supersymmetry, supergravity and superstring theory, Dirac's instant-form and light-front quantization of field theories and D-brane actions. His work on the models of gravity focuses on the studies of charged compact boson stars and boson shells.

Periodic instantons are finite energy solutions of Euclidean-time field equations which communicate between two turning points in the barrier of a potential and are therefore also known as bounces. Vacuum instantons, normally simply called instantons, are the corresponding zero energy configurations in the limit of infinite Euclidean time. For completeness we add that ``sphalerons´´ are the field configurations at the very top of a potential barrier. Vacuum instantons carry a winding number, the other configurations do not. Periodic instantons were discovered with the explicit solution of Euclidean-time field equations for double-well potentials and the cosine potential with non-vanishing energy and are explicitly expressible in terms of Jacobian elliptic functions. Periodic instantons describe the oscillations between two endpoints of a potential barrier between two potential wells. The frequency of these oscillations or the tunneling between the two wells is related to the bifurcation or level splitting of the energies of states or wave functions related to the wells on either side of the barrier, i.e. . One can also interpret this energy change as the energy contribution to the well energy on either side originating from the integral describing the overlap of the wave functions on either side in the domain of the barrier.

<span class="mw-page-title-main">Usha Kulshreshtha</span> Indian theoretical physicist

Usha Kulshreshtha is an Indian theoretical physicist, specializing in the Dirac's instant-form and light-front quantization of quantum field theory models, string theory models and D-brane actions using the Hamiltonian, path integral and BRST quantization methods, constrained dynamics, construction of gauge theories and their quantizaton under gauge-fixing as well as study of boson stars, and wormholes in general relativity and gravity theory.

References

  1. "Archived copy" (PDF). Archived from the original (PDF) on 2017-12-22. Retrieved 2020-07-01.{{cite web}}: CS1 maint: archived copy as title (link)
  2. R.B. Dingle and H.J.W. Müller, J. reine angew. Math. 211 (1962) 11–32, 216 (1964) 123–133; H.J.W. Müller, J. reine angew. Math. 211 (1962) 33.47, 211 (1962) 179–190, 212 (1963) 26–48; H.J.W. Müller, Math. Nachr. 31 (1966) 89–101, 32 (1966) 49–62, 32 (1966) 157–374.
  3. H.J.W. Müller, Ann. d. Phys. (Leipzig) 15 (1965) 395–411.; H.J.W. Müller and K. Schilcher, J. Math. Phys. 9 (1968) 255–259.
  4. H.J.W. Müller-Kirsten, Introduction to Quantum Mechanics: Schrödinger Equation and Path Integral, World Scientific Singapore, 2nd ed., 2012, ISBN   978-981-4397-73-5, pp. 524–527; J.-Q. Liang and H.J.W. Müller-Kirsten, Anharmonic Oscillator Equations: Treatment Parallel to Mathieu Equation, quant-ph/0407235; P. Achuthan, H.J.W. Müller-Kirsten and A. Wiedemann, Fortschr. Physik 38 (1990) 77.
  5. J.-Q. Liang and H.J.W. Müller-Kirsten, Phys. Rev. D46 (1992) 4685, D50 (1994) 6519, D51 (1995) 718.
  6. J.-Q. Liang, H.J.W. Müller-Kirsten and D.H. Tchrakian, Phys. Lett. B282 (1992) 105.
  7. H.H. Aly, H.J.W. Müller-Kirsten and N. Vahedi-Faridi, J. Math. Phys. 16 (1975) 961; R. Manvelyan, H.J.W. Müller-Kirsten, J.-Q. Liang and Yunbo Zhang, Nucl. Phys. B579 (2000) 177, hep-th/0001179; D.K. Park, S.N. Tamaryan, H.J.W. Müller-Kirsten and Jian-Zu Zhang, Nucl. Phys. B594 (2001) 243, hep-th/0005165.
  8. Usha Kulshreshtha, Daya Shankar Kulshreshtha, Harald J.W. Mueller-Kirsten, ``A Gauge invariant theory of chiral bosons: Wess–Zumino term, Hamiltonian and BRST formulations``, Zeit. Phys. C 60 (1993) 427–431.
  9. Daya Shankar Kulshreshtha, Harald J.W. Mueller-Kirsten, ``Quantization of systems with constraints: The Faddeev–Jackiw method versus Dirac's method applied to superfields``, Phys. Rev. D43 (1991) 3376–3383; ``Faddeev-Jackiw quantization of selfdual fields``, Phys. Rev. D 45 (1992) 393–397.
  10. H.J.W. Müller-Kirsten, Rätsel Wahrheit, Verlag Haag+Herchen GmbH, 2017, ISBN   978-3-89846-783-4.