Finite Temperature phase transitions in non-abelian gauge theories (Record no. 48775)

000 -LEADER
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
Holdings
Withdrawn status Lost status Damaged status Not for loan Current library Full call number Accession Number Uniform Resource Identifier Koha item type
        IMSc Library UNM Th-48 36816 http://www.imsc.res.in/xmlui/handle/123456789/72 THESIS & DISSERTATION
The Institute of Mathematical Sciences, Chennai, India

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