Adaptive Perturbation Theory [electronic resource] : Quantum Mechanics and Field Theory.
Theory-hep,hepth, Math, Phys.
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Online Access: |
Online Access |
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Corporate Author: | |
Format: | Government Document Electronic eBook |
Language: | English |
Published: |
Washington, D.C : Oak Ridge, Tenn. :
United States. Dept. of Energy ; distributed by the Office of Scientific and Technical Information, U.S. Dept. of Energy,
2005.
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Subjects: |
MARC
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245 | 0 | 0 | |a Adaptive Perturbation Theory |h [electronic resource] : |b Quantum Mechanics and Field Theory. |
260 | |a Washington, D.C : |b United States. Dept. of Energy ; |a Oak Ridge, Tenn. : |b distributed by the Office of Scientific and Technical Information, U.S. Dept. of Energy, |c 2005. | ||
300 | |a 10 pages : |b digital, PDF file. | ||
336 | |a text |b txt |2 rdacontent. | ||
337 | |a computer |b c |2 rdamedia. | ||
338 | |a online resource |b cr |2 rdacarrier. | ||
500 | |a Published through the Information Bridge: DOE Scientific and Technical Information. | ||
500 | |a 10/19/2005. | ||
500 | |a "slac-pub-11532" | ||
500 | |a "hep-th/0510160" | ||
500 | |a Invited talk at Workshop on Light-Cone QCD and Nonperturbative Hadron Physics 2005 (LC 2005), Cairns, Queensland, Australia, 7-15 Jul 2005. | ||
500 | |a Weinstein, Marvin. | ||
520 | 3 | |a Adaptive perturbation is a new method for perturbatively computing the eigenvalues and eigenstates of quantum mechanical Hamiltonians that are widely believed not to be solvable by such methods. The novel feature of adaptive perturbation theory is that it decomposes a given Hamiltonian, H, into an unperturbed part and a perturbation in a way which extracts the leading non-perturbative behavior of the problem exactly. In this talk I will introduce the method in the context of the pure anharmonic oscillator and then apply it to the case of tunneling between symmetric minima. After that, I will show how this method can be applied to field theory. In that discussion I will show how one can non-perturbatively extract the structure of mass, wavefunction and coupling constant renormalization. | |
520 | 0 | |a Theory-hep,hepth, Math, Phys. | |
536 | |b AC02-76SF00515. | ||
650 | 7 | |a Eigenvalues. |2 local. | |
650 | 7 | |a Renormalization. |2 local. | |
650 | 7 | |a Tunneling. |2 local. | |
650 | 7 | |a Hamiltonians. |2 local. | |
650 | 7 | |a Hadrons. |2 local. | |
650 | 7 | |a Quantum Chromodynamics. |2 local. | |
650 | 7 | |a Eigenstates. |2 local. | |
650 | 7 | |a Light Cone. |2 local. | |
650 | 7 | |a Quantum Mechanics. |2 local. | |
650 | 7 | |a Physics. |2 local. | |
650 | 7 | |a Coupling Constants. |2 local. | |
650 | 7 | |a Anharmonic Oscillators. |2 local. | |
650 | 7 | |a Perturbation Theory. |2 local. | |
650 | 7 | |a Classical And Quantum Mechanics, General Physics. |2 edbsc. | |
650 | 7 | |a Physics Of Elementary Particles And Fields. |2 edbsc. | |
710 | 2 | |a Stanford Linear Accelerator Center. |4 res. | |
710 | 1 | |a United States. |b Department of Energy. |4 spn. | |
710 | 1 | |a United States. |b Department of Energy. |b Office of Scientific and Technical Information. |4 dst. | |
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