MATRIX ELEMENTS OF AREA OPERATOR IN (2+1) EUCLIDEAN LOOP QUANTUM GRAVITY
One of the problems in theoretical physics is the attempt to make the theory of general relativity leads to the quantum properties, which is called quantum gravity theory. An approach used in quantizing the gravitational field is to use canonical formulations. The general relativity theory (GRT)...
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Format: | Theses |
Language: | Indonesia |
Subjects: | |
Online Access: | https://digilib.itb.ac.id/gdl/view/45710 |
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Institution: | Institut Teknologi Bandung |
Language: | Indonesia |
Summary: | One of the problems in theoretical physics is the attempt to make the theory of
general relativity leads to the quantum properties, which is called quantum gravity
theory. An approach used in quantizing the gravitational field is to use canonical
formulations. The general relativity theory (GRT) initially used metrics as dynamic
variables. However, GRT can also be expressed in other variables, which is named
the Ashtekar variable that leads to an existing particle theory. The steps are used
in particle theory can be used to quantify the gravitational field even if it is not
completely. Gravity as a manifestation of spacetime itself carries the same problems
as quantizing geometry. Of course geometrical quantities such as volume, area
and length are the main quantities in the quantization problem of the gravitational
field. Various calculations have been carried out in the object and obtained that the
geometry operator has a discrete spectrum. Geometry operator can be represented
in the matrix and carried out matrix elemen from the operator which is assigned
this thesis. Here, an analysis of the matrix elements of a area operator in dimension
(2+1) with Euclidean signatures has been carried out and the results can be stated
in 6j-Symbols. The Euclidean signature is chosen because it has the same gauge
group as the TRU in dimension (3+1) with the Lorentzian signature which is the
SU(2) group.. |
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