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Master Constraint Operator in Loop Quantum Gravity
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6
Master Constraint Operators in Loop Quantum
Gravity
Muxin Han
1,2?
and Yongge Ma
1?
1. Department of Physics, Beijing Normal University,
Beijing 100875, CHINA
2. Horace Hearne Jr. Institute for Theoretical Physics,
Louisiana State University,
Baton Rouge, LA 70803, USA
February 5, 2008
Abstract
We introduce a master constraint operator M? densely defined in the diffeomor-
phism invariant Hilbert space in loop quantum gravity, which corresponds classi-
cally to the master constraint in the programme. It is shown that M? is positive and
symmetric, and hence has its Friedrichs self-adjoint extension. The same conclu-
sion is tenable for an alternative master operator M?
′
, whose quadratic form coin-
cides with the one proposed by Thiemann. So the master constraint programme
for loop quantum gravity can be carried out in principle by employing either of the
two operators.
Keywords: loop quantum gravity, master constraint, quantum dynamics.
PACS number(s): 04.60.Pp, 04.60.Ds
1 Introduction
It is well known that the quantization programme of loop quantum gravity is based on
the connection dynamics of general relativity [1][2][3]. The basic conjugate pairs in the
phase space are su(2)-valued connections A
i
a
and densitized triads P?
a
i
on a 3-manifold
Σ. In the case where Σ is a compact set without boundary, the Hamiltonian is a linear
combination of constraints as follows:
Htot = G(Λ) +V(~N) +H(N). (1)
?
Email address: mhan1@lsu.edu
?
Email address: mayg@bnu.edu.cn
1
As an infinite dimensional Poisson algebra, the constraints algebra is not a Lie algebra
unfortunately, because the Poisson bracket between the two scalar (Hamiltonian) con-
straints H(N) and H(M) has structure function depending on dynamical variables [1].
This character causes much trouble in solving the constraints quantum mechanically.
On the other hand, the algebra generated by the Gaussian constraints G(Λ) forms not
only a subalgebra but
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