Finite Temperature phase transitions in non-abelian gauge theories (Record no. 48775)
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000 -LEADER | |
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fixed length control field | 02506nam a2200241Ia 4500 |
008 - FIXED-LENGTH DATA ELEMENTS--GENERAL INFORMATION | |
fixed length control field | 160627s1996||||xx |||||||||||||| ||und|| |
080 ## - UNIVERSAL DECIMAL CLASSIFICATION NUMBER | |
Universal Decimal Classification number | UNM Th-48 |
100 ## - MAIN ENTRY--AUTHOR NAME | |
Personal name | Cheluvaraja, Srinath |
Relator term | author |
245 ## - TITLE STATEMENT | |
Title | Finite Temperature phase transitions in non-abelian gauge theories |
260 ## - PUBLICATION, DISTRIBUTION, ETC. (IMPRINT) | |
Year of publication | 1996 |
300 ## - PHYSICAL DESCRIPTION | |
Number of Pages | viii; 71p. |
502 ## - DISSERTATION NOTE | |
Dissertation note | 1996 |
502 ## - DISSERTATION NOTE | |
Degree Type | Ph.D |
502 ## - DISSERTATION NOTE | |
Name of granting institution | University of Madras |
520 3# - SUMMARY, ETC. | |
Summary, etc | This thesis makes a systematic study of the SO(3) Lattice Gauge Theory at finite temperature. The study of the SO(3) Lattice Gauge Theory is important in understanding the implications of lattice gauge theories for the high temperature phase of the SU(2) Yang-Mills theory. The existence of a first order bulk transition at zero temperature that can influence its finite temperature behaviour, and the presence of a local symmetry which requires the usage of a different set of observables to study its property - are some of the complications present in the study of SO(3) theory. The Wilson-Polyakov line in the adjoint representation of SU(2) is mainly used to make the present study. The role of Z(2) monopoles in determining the various phases is considered. The adjoint Wilson line displays an unusual behaviour at low and high temperature is found, whereas the fundamental Wilson line is always zero in this model. The high temperature phase of the theory is analyzed by looking at single site histograms for the fundamental and adjoint Wilson lines, and interpreted for comparisons with the high temperature phase. It is shown that the high temperature phase of SO(3) LGT is like the deconfined phase of the SU(2) LGT theory, but unlike the breaking of any symmetry as in SU(2) theory. An interference of the bulk transition in the finite temperature theory is observed. The evidence for a new phase transition, within the relevance region with respect to continuum theory is presented; The conjectures phase diagram for the SO(3) LGT theory at finite temperature is presented, and contrasted with that of SU(2) LGT. The implications of the study results for the high temperature phase of the SU(2) Yang-Mills theory is discussed with the argument that it is in the Higgs Phase. |
650 14 - SUBJECT ADDED ENTRY--TOPICAL TERM | |
Topical Term | Physics |
653 10 - INDEX TERM--UNCONTROLLED | |
Uncontrolled term | Phase Transitions |
653 10 - INDEX TERM--UNCONTROLLED | |
Uncontrolled term | SO(3) Lattice Gauge Theory |
720 1# - ADDED ENTRY--UNCONTROLLED NAME | |
Thesis Advisor | Sharatchandra, H. S. |
Relator term | Thesis advisor [ths] |
856 ## - ELECTRONIC LOCATION AND ACCESS | |
Uniform Resource Identifier | http://www.imsc.res.in/xmlui/handle/123456789/72 |
942 ## - ADDED ENTRY ELEMENTS (KOHA) | |
Koha item type | THESIS & DISSERTATION |
Withdrawn status | Lost status | Damaged status | Not for loan | Current library | Full call number | Accession Number | Uniform Resource Identifier | Koha item type |
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IMSc Library | UNM Th-48 | 36816 | http://www.imsc.res.in/xmlui/handle/123456789/72 | THESIS & DISSERTATION |