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a new Quantum Gravity paper
Madhavan Varadarajan
The graviton vacuum as a distributional state in kinematic Loop Quantum Gravity
44 pages
http://arxiv.org/abs/gr-qc/0410120
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Abstract:
The quantum behaviour of weak gravitational fields admits an adequate, albeit approximate, description by those graviton states in which the expectation values and fluctuations of the linearised gravitational field are small. Such states must approximate corresponding states in full quantum gravity. We analyse the nature of this approximation for the graviton vacuum state in the context of kinematical Loop Quantum Gravity (LQG) wherein the constraints are ignored. We identify the graviton vacuum state with kinematically non-normalizable, distributional states in LQG by demanding that relations between linearised operator actions on the former are mirrored by those of their non-linear counterparts on the latter. We define a semi- norm on the space of kinematical distributions and show that the identification is approximate upto distributions which are small in this semi-norm. We argue that our candidate states are annihilated by the linearised constraints (expressed as operators in the full theory) to leading order in the parameter characterising the approximation. This suggests the possibility, in a scheme such as ours, of solving the full constraints order by order in this parameter. The main drawback of our considerations is that they depend on certain auxilliary constructions which, though mathematically well defined, do not arise from physical insight. Our work is an attempt to implement an earlier proposal of Iwasaki and Rovelli.
I. Introduction:
A Dirac constraint quantization of a Hamiltonian formulation of gravity is defined through the following steps. First, a “kinematical” representation of the Poisson bracket algebra of a large enough set of functions on the unconstrained phase space is constructed such that these functions act as linear operators on the representation space. Next, the constraints of the theory are represented as quantum operators in this representation and physical states are identified with their kernel. Finally, an inner product on the space of physical states is chosen which enforces hermiticity conditions on a complete set of operators corresponding to Dirac observables, thus converting the physical state space to a Hilbert space...
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Varadarajan's 19 archived papers go back to 1993. He has co-authored with Abhay Ashtekar, and also at various times both with Rafael Sorkin, and with Fernando Barbero.
Here are the two Iwasaki-Rovelli papers he says were his point of departure
J. Iwasaki and C. Rovelli, Int.J.Mod.Phys.D1, 533 (1993);
J. Iwasaki and C. Rovelli, Class.Quant.Grav.11, 1653 (1994).
Madhavan Varadarajan
The graviton vacuum as a distributional state in kinematic Loop Quantum Gravity
44 pages
http://arxiv.org/abs/gr-qc/0410120
---quote---
Abstract:
The quantum behaviour of weak gravitational fields admits an adequate, albeit approximate, description by those graviton states in which the expectation values and fluctuations of the linearised gravitational field are small. Such states must approximate corresponding states in full quantum gravity. We analyse the nature of this approximation for the graviton vacuum state in the context of kinematical Loop Quantum Gravity (LQG) wherein the constraints are ignored. We identify the graviton vacuum state with kinematically non-normalizable, distributional states in LQG by demanding that relations between linearised operator actions on the former are mirrored by those of their non-linear counterparts on the latter. We define a semi- norm on the space of kinematical distributions and show that the identification is approximate upto distributions which are small in this semi-norm. We argue that our candidate states are annihilated by the linearised constraints (expressed as operators in the full theory) to leading order in the parameter characterising the approximation. This suggests the possibility, in a scheme such as ours, of solving the full constraints order by order in this parameter. The main drawback of our considerations is that they depend on certain auxilliary constructions which, though mathematically well defined, do not arise from physical insight. Our work is an attempt to implement an earlier proposal of Iwasaki and Rovelli.
I. Introduction:
A Dirac constraint quantization of a Hamiltonian formulation of gravity is defined through the following steps. First, a “kinematical” representation of the Poisson bracket algebra of a large enough set of functions on the unconstrained phase space is constructed such that these functions act as linear operators on the representation space. Next, the constraints of the theory are represented as quantum operators in this representation and physical states are identified with their kernel. Finally, an inner product on the space of physical states is chosen which enforces hermiticity conditions on a complete set of operators corresponding to Dirac observables, thus converting the physical state space to a Hilbert space...
---end quote---
Varadarajan's 19 archived papers go back to 1993. He has co-authored with Abhay Ashtekar, and also at various times both with Rafael Sorkin, and with Fernando Barbero.
Here are the two Iwasaki-Rovelli papers he says were his point of departure
J. Iwasaki and C. Rovelli, Int.J.Mod.Phys.D1, 533 (1993);
J. Iwasaki and C. Rovelli, Class.Quant.Grav.11, 1653 (1994).
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