✦ LIBER ✦

Guided random walks for solving Hamiltonian lattice gauge theories: S. A. Chin, Department of Physics, University of California, Los Angeles, California 90024; J. W. Negele, Center for Theoretical Physics, Laboratory for Nuclear Science and Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139; and S. E. Koonin, Kellogg Radiation Laboratory, California Institute of Technology, Pasadena, California 91125

Publisher: Elsevier Science
Year: 1984
Tongue: English
Weight: 75 KB
Volume: 155
Category: Article
ISSN: 0003-4916
DOI: 10.1016/0003-4916(84)90015-0

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📜 SIMILAR VOLUMES

Functional integral representation of th

Functional integral representation of the nuclear many-body grand partition function: A. K. Kerman, Center for Theoretical Physics, Laboratory for Nuclear Science and Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, and T. Troudet, Institute for Theoretical Physics, University of California at Santa Barbara, Santa Barbara, California 93106, and W. K. Kellogg Radiation Laboratory, California Institute of Technology, Pasadena, California 91125

📂 Article 📅 1984 🏛 Elsevier Science 🌐 English ⚖ 50 KB

The statistical theory of multi-step com

The statistical theory of multi-step compound and direct reactions: Herman Feshbach, Arthur Kerman, and Steven Koonin, Center for Theoretical Physics, Laboratory for Nuclear Science and Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139; and California Institute of Technology, Pasadena, California 91109

📂 Article 📅 1980 🏛 Elsevier Science 🌐 English ⚖ 87 KB

The theory of nuclear reactions is extended so as to include a statistical treatment of multi-step processes. Two types are distinguished, the multi-step compound and the multi-step direct. The wave functions for the system are grouped according to their complexity. The multi-step direct process inv

Topologically massive gauge theories: S.

Topologically massive gauge theories: S. Deser, Department of Physics, Brandeis University, Waltham, Massachusetts 02254; and R. Jackiw and S. Templeton, Center for Theoretical Physics, Laboratory for Nuclear Science and Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139

📂 Article 📅 1982 🏛 Elsevier Science 🌐 English ⚖ 69 KB

Mesonic processes in deep-inelastic elec

Mesonic processes in deep-inelastic electron scattering from nuclei: J. W. Van Orden, Institute of Theoretical Physics, Department of Physics, Stanford University, Stanford, California 94305, and Department of Physics and Astronomy, University of Maryland, College Park, Maryland 20742; and T. W. Donnelly, Institute of Theoretical Physics, Department of Physics, Stanford University, Stanford, California 94305, and Center for Theoretical Physics, Laboratory for Nuclear Science and Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139

📂 Article 📅 1981 🏛 Elsevier Science 🌐 English ⚖ 84 KB

A generally covariant formulation of cla

A generally covariant formulation of classical electrodynamics for changes of finite extension: Ronald J. Crowley, W. K. Kellogg Radiation Laboratory, California Institute of Technology, Pasadena, California 91125, and California State University, Fullerton, California 92634; and John S. Nodvik, Department of Physics, University of Southern California, Los Angeles, California 90007

📂 Article 📅 1978 🏛 Elsevier Science 🌐 English ⚖ 90 KB

Supersymmetry in anti-de Sitter space: C

Supersymmetry in anti-de Sitter space: Christopher J. C. Burges and Daniel Z. Freedman, Department of Mathematics and Center for Theoretical Physics, Laboratory for Nuclear Science, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139; and S. Davis and G. W. Gibbons, Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Silver Street, Cambridge, CB3 9EW, United Kingdom

📂 Article 📅 1986 🏛 Elsevier Science 🌐 English ⚖ 77 KB