Abstract:Abstract:We study the effective transfer matrix within the semiclassical and bifurcation phases of CDT quantum gravity. We find that for sufficiently large lattice volumes the kinetic term of the effective transfer matrix has a different sign in each of the two phases. We argue that this sign change can be viewed as a Wick rotation of the metric. We discuss the likely microscopic mechanism responsible for the bifurcation phase transition, and propose an order parameter that can potentially be used to determine… Show more
“…Furthermore, the maximal slice in the C b phase is typically observed to be of B-type, with a volume ranging in a narrow interval which is separated from the volumes of the other slices. This alternating distribution of spatial volumes has been indeed one of the first signals of the presence of the new phase [3,4].…”
Section: A the Low Lying Spectrum And The Emergence Of A Gapmentioning
confidence: 86%
“…Among the various results, we will show that the different phases can be characterized by the presence or absence of a gap in the spectrum of the LB operator, as it happens for the spectrum of the Dirac operator in strong interactions, and we will give an interpretation of this fact in terms of the geometrical properties of the slices. The presence/absence of a gap will also serve to better characterize the two different classes of spatial slices which are found in the recently discovered bifurcation phase [3][4][5][6]. Moreover, we will show how the spectrum can be used to derive an effective dimensionality of the triangulations at different length scales, and to investigate quantities useful to characterize the critical behavior expected around a possible secondorder transition point.…”
Section: Introductionmentioning
confidence: 94%
“…With this prescription, simplexes in the same class (according to the above definition) not only are equivalent topologically, but also geometrically, so that the expression of the discretized action greatly simplifies. Indeed, at the end of the day, 4 the standard fourdimensional action employed in CDT simulations with S 3 topology of the slices and periodic time conditions becomes a functional of the triangulation T , and takes the relatively simple form…”
Section: A Brief Review On Cdt and Numerical Setupmentioning
confidence: 99%
“…where N 0 counts the total number of vertices, N 4 counts the total number of pentachorons, and N 41 is the sum of the total numbers of type (4,1) and type (1,4) pentachorons, while k 4 , k 0 and Δ are free dimensionless parameters, related to the Cosmological constant, the Newton constant, and the freedom in the choice of the time/space asymmetry parameter α (see Ref. [1] for more details).…”
Section: A Brief Review On Cdt and Numerical Setupmentioning
We propose a new method to characterize the different phases observed in the nonperturbative numerical approach to quantum gravity known as causal dynamical triangulations. The method is based on the analysis of the eigenvalues and the eigenvectors of the Laplace-Beltrami operator computed on the triangulations: it generalizes previous works based on the analysis of diffusive processes and proves capable of providing more detailed information on the geometric properties of the triangulations. In particular, we apply the method to the analysis of spatial slices, showing that the different phases can be characterized by a new order parameter related to the presence or absence of a gap in the spectrum of the Laplace-Beltrami operator, and deriving an effective dimensionality of the slices at the different scales. We also propose quantities derived from the spectrum that could be used to monitor the running to the continuum limit around a suitable critical point in the phase diagram, if any is found.
“…Furthermore, the maximal slice in the C b phase is typically observed to be of B-type, with a volume ranging in a narrow interval which is separated from the volumes of the other slices. This alternating distribution of spatial volumes has been indeed one of the first signals of the presence of the new phase [3,4].…”
Section: A the Low Lying Spectrum And The Emergence Of A Gapmentioning
confidence: 86%
“…Among the various results, we will show that the different phases can be characterized by the presence or absence of a gap in the spectrum of the LB operator, as it happens for the spectrum of the Dirac operator in strong interactions, and we will give an interpretation of this fact in terms of the geometrical properties of the slices. The presence/absence of a gap will also serve to better characterize the two different classes of spatial slices which are found in the recently discovered bifurcation phase [3][4][5][6]. Moreover, we will show how the spectrum can be used to derive an effective dimensionality of the triangulations at different length scales, and to investigate quantities useful to characterize the critical behavior expected around a possible secondorder transition point.…”
Section: Introductionmentioning
confidence: 94%
“…With this prescription, simplexes in the same class (according to the above definition) not only are equivalent topologically, but also geometrically, so that the expression of the discretized action greatly simplifies. Indeed, at the end of the day, 4 the standard fourdimensional action employed in CDT simulations with S 3 topology of the slices and periodic time conditions becomes a functional of the triangulation T , and takes the relatively simple form…”
Section: A Brief Review On Cdt and Numerical Setupmentioning
confidence: 99%
“…where N 0 counts the total number of vertices, N 4 counts the total number of pentachorons, and N 41 is the sum of the total numbers of type (4,1) and type (1,4) pentachorons, while k 4 , k 0 and Δ are free dimensionless parameters, related to the Cosmological constant, the Newton constant, and the freedom in the choice of the time/space asymmetry parameter α (see Ref. [1] for more details).…”
Section: A Brief Review On Cdt and Numerical Setupmentioning
We propose a new method to characterize the different phases observed in the nonperturbative numerical approach to quantum gravity known as causal dynamical triangulations. The method is based on the analysis of the eigenvalues and the eigenvectors of the Laplace-Beltrami operator computed on the triangulations: it generalizes previous works based on the analysis of diffusive processes and proves capable of providing more detailed information on the geometric properties of the triangulations. In particular, we apply the method to the analysis of spatial slices, showing that the different phases can be characterized by a new order parameter related to the presence or absence of a gap in the spectrum of the Laplace-Beltrami operator, and deriving an effective dimensionality of the slices at the different scales. We also propose quantities derived from the spectrum that could be used to monitor the running to the continuum limit around a suitable critical point in the phase diagram, if any is found.
“…Signature change is known to be a possible feature of both classical and quantum gravity. [19]- [28] The region bounded by the singular latitudes has Lorentzian signature, and describes a closed two-dimensional space-time. The two singular latitudes behave as cosmological singularities, which get resolved at finite N .…”
Four-dimensional manifolds with changing signature are obtained by taking the large N limit of fuzzy CP 2 solutions to a Lorentzian matrix model. The regions of Lorentzian signature give toy models of closed universes which exhibit cosmological singularities. These singularities are resolved at finite N , as the underlying CP 2 solutions are expressed in terms of finite matrix elements.
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