2006
DOI: 10.1103/physrevd.73.104009
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Wave functions for the Schwarzschild black hole interior

Abstract: Using the Hamiltonian constraint derived by Ashtekar and Bojowald, we look for pre-classical wave functions in the Schwarzschild interior. In particular, when solving this difference equation by separation of variables, an inequality is obtained relating the Immirzi parameter γ to the quantum ambiguity δ appearing in the model. This bound is violated when we use a natural value for δ based on loop quantum gravity together with a recent proposal for γ. We also present numerical solutions of the constraint.

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Cited by 34 publications
(46 citation statements)
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“…The numerical results are based on using the triad component p c as an internal clock, however, our results suggest that p c bounces and hence would not play the role of a good clock. Thus to reconcile our results with those of [21,22], the numerical evolutions would probably require different initial conditions to incorporate both the expanding and contracting parts of the wave-packets at the initial instance in "time". This issue is solved in the isotropic case by including a scalar field that plays the role of a global internal clock.…”
Section: Discussionmentioning
confidence: 75%
See 1 more Smart Citation
“…The numerical results are based on using the triad component p c as an internal clock, however, our results suggest that p c bounces and hence would not play the role of a good clock. Thus to reconcile our results with those of [21,22], the numerical evolutions would probably require different initial conditions to incorporate both the expanding and contracting parts of the wave-packets at the initial instance in "time". This issue is solved in the isotropic case by including a scalar field that plays the role of a global internal clock.…”
Section: Discussionmentioning
confidence: 75%
“…In the works cited, numerical instabilities of the difference equation are found which bring into question whether any effective picture is valid near the singularity. In [21] it is argued that no proper semi-classical states exist unless the Immirzi parameter γ is less the the accepted value in the LQG literature raising a further question. In this article, our aim has been to probe the improved, non-constant δ quantization and thus we do not see a direct contradiction.…”
Section: Discussionmentioning
confidence: 99%
“…In such models, limitations similar to that of a cosmological constant have been observed as possible instabilities of solutions in classical regions or the lack of a sufficient number of semiclassical states [27,28,29]. For the partial difference equations of anisotropic models in loop quantum cosmology, stability issues can be much more severe than in isotropic models and thus lead to further consistency tests which might help to restrict possible quantization freedom (see, e.g., [30]). In this paper we therefore introduce the general setting of anisotropic models taking into account lattice refinements of Hamiltonian constraint operators, focusing mainly on the anisotropic model which corresponds to the Schwarzschild interior.…”
Section: Introductionmentioning
confidence: 99%
“…At odd integer multiples of µ 2 = 2δ 2 , we obtain a recurrence relation which requires s 2δ1,2(2n+1)δ2 = s −2δ1,2(2n+1)δ2 for all integer n. There are thus reflection symmetry conditions which directly follow from the dynamical law even in the presence of parity-violating terms. (This symmetry has been observed first in the vacuum case [46].) However, evolution away from µ 1 = ±1 depends on whether µ 1 is positive or negative if parity is not preserved.…”
Section: Cosmological Implicationsmentioning
confidence: 94%