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We argue that the Lorentzian path integral is a better starting point for quantum cosmology than the Euclidean version. In particular, we revisit the mini-superspace calculation of the Feynman path integral for quantum gravity with a…

High Energy Physics - Theory · Physics 2017-05-24 Job Feldbrugge , Jean-Luc Lehners , Neil Turok

Quantum cosmology based on Lorentzian path integrals is a promising avenue. However, many previous works allow non-Lorentzian configurations by integrating the squared scale factor over the whole real line. Here we show that restricting the…

General Relativity and Quantum Cosmology · Physics 2023-12-01 Ding Jia

For various reasons, it seems necessary to include complex saddle points in the "Euclidean" path integral of General Relativity. But some sort of restriction on the allowed complex saddle points is needed to avoid various unphysical…

High Energy Physics - Theory · Physics 2022-02-14 Edward Witten

Spacetimes have conventionally been described by a global Lorentzian metric on a differentiable four-manifold. Herein we explore the possibility of spacetimes defined by a connection, which is locally but not globally Levi-Civita. The…

Mathematical Physics · Physics 2008-04-21 Richard Atkins

In the Hartle-Hawking ``no boundary'' approach to quantum cosmology, a real tunneling geometry is a configuration that represents a transition from a compact Riemannian spacetime to a Lorentzian universe. I complete an earlier proof that in…

General Relativity and Quantum Cosmology · Physics 2010-04-28 S. Carlip

In two space-time dimensions, there is a theory of Lorentzian quantum gravity which can be defined by a rigorous, non-perturbative path integral and is inequivalent to the well-known theory of (Euclidean) quantum Liouville gravity. It has a…

High Energy Physics - Theory · Physics 2009-10-31 R. Loll , J. Ambjorn , K. N. Anagnostopoulos

We consider spacetime to be a 4-dimensional differentiable manifold that can be split locally into time and space. No metric, no linear connection are assumed. Matter is described by classical fields/fluids. We distinguish electrically…

General Relativity and Quantum Cosmology · Physics 2008-11-26 Friedrich W. Hehl , Yuri N. Obukhov

By assuming gravity and matter to be subject to a joint statistical mechanical concept (JSMC) and interpreting Rindler horizon sections as open thermodynamic systems, one arrives at a specific new form of non-perturbative Lorentzian path…

General Physics · Physics 2025-04-04 Pierre A Mandrin

Starting from the equations of motion in a 1 + 1 static, diagonal, Lorentzian spacetime, such as the Schwarzschild radial line element, I find another metric, but with Euclidean signature, which produces the same geodesics x(t). This…

General Relativity and Quantum Cosmology · Physics 2008-11-26 Rickard Jonsson

In this paper I discuss whether superluminal particles exist in the general relativistic theory of gravity. It seems that the answer to this question is negative. In truth the result may only represent a difficulty to {\bf special} but not…

General Relativity and Quantum Cosmology · Physics 2013-06-18 Asher Yahalom

Trajectories of light rays in a static spacetime are described by unparametrised geodesics of the Riemannian optical metric associated with the Lorentzian spacetime metric. We investigate the uniqueness of this structure and demonstrate…

General Relativity and Quantum Cosmology · Physics 2011-05-12 Stephen Casey , Maciej Dunajski , Gary Gibbons , Claude Warnick

It is conjectured that the symplectic structure of space-time is superior to the metric one. Instead of the commonly adopted pseudo-orthogonal groups SO(1,d-1), d\ge4, the complex symplectic ones Sp(2l,C), l\ge1 are proposed as the local…

High Energy Physics - Phenomenology · Physics 2007-05-23 Yu. F. Pirogov

We investigate connections between pairs of (pseudo-)Riemannian metrics whose sum is a (tensor) product of a covector field with itself. A bijective mapping between the classes of Euclidean and Lorentzian metrics is constructed as a special…

General Relativity and Quantum Cosmology · Physics 2007-05-23 Bozhidar Z. Iliev

We review both the kinematics and dynamics of non-lorentzian theories and their associated geometries. First, we introduce non-lorentzian kinematical spacetimes and their symmetry algebras. Next, we construct actions describing the particle…

High Energy Physics - Theory · Physics 2023-05-31 Eric Bergshoeff , José Figueroa-O'Farrill , Joaquim Gomis

Studying transition amplitudes in (2+1)-dimensional causal dynamical triangulations, Cooperman and Miller discovered speculative evidence for Lorentzian quantum geometries emerging from its Euclidean path integral. On the basis of this…

General Relativity and Quantum Cosmology · Physics 2017-05-31 Joshua H. Cooperman , Kyle Lee , Jonah M. Miller

Under normal circumstances most members of the general relativity community focus almost exclusively on the local properties of spacetime, such as the locally Euclidean structure of the manifold and the Lorentzian signature of the metric…

General Relativity and Quantum Cosmology · Physics 2017-11-28 Deloshan Nawarajan , Matt Visser

We outline an alternative approach to the geometric notion of a saddle point for real-valued functions of two variables. It is argued that this is more natural compared to the usual treatment of this topic in standard texts on Calculus.

History and Overview · Mathematics 2009-09-15 Sudhir R. Ghorpade , Balmohan V. Limaye

We show that the two-point function \sigma(x,x')=\sqrt{<[\phi(x)-\phi(x')]^{2}>} of a scalar quantum field theory is a metric (i.e., a symmetric positive function satisfying the triangle inequality) on space-time (with imaginary time). It…

High Energy Physics - Theory · Physics 2013-09-18 Arnab Kar , S. G. Rajeev

Quantum mechanical transition amplitudes directly tells the probability of each transition and which one is more favourable. Path-integrals offers a systematic methodology to compute this quantum mechanical process in a consistent manner.…

General Relativity and Quantum Cosmology · Physics 2019-12-17 Gaurav Narain , Hai-Qing Zhang

Given a Lorentzian spacetime $(M, g)$ and a non-vanishing timelike vector field $u(\lambda)$ with level surfaces $\Sigma$, one can construct on $M$ a Euclidean metric $g_E^{ab} = g^{ab} + 2 u^a u^b$. Motivated by this, we consider a class…

General Relativity and Quantum Cosmology · Physics 2018-01-16 Dawood Kothawala
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