Abstract

We address the reasons why the “Wick-rotated”, positive-definite, space-time metric obeys the Pythagorean theorem. An answer is proposed based on the convexity and smoothness properties of the functional spaces purporting to provide the kinematic framework of approaches to quantum gravity. We employ moduli of convexity and smoothness which are eventually extremized by Hilbert spaces. We point out the potential physical significance that functional analytical dualities play in this framework. Following the spirit of the variational principles employed in classical and quantum Physics, such Hilbert spaces dominate in a generalized functional integral approach. The metric of space-time is induced by the inner product of such Hilbert spaces.

Highlights

  • When one looks at the equations describing the four fundamental interactions of nature, s/he immediately notices that the kinematic equations in the Lagrangian formalism involve second order derivatives with respect to space-time variables

  • In all of the above, and in the Lagrangian approach which we employ throughout this work, the Euler-Lagrange equations that describe the underlying dynamics can be seen to emerge from variational principles; such equations could use derivatives of arbitrarily high order and a formalism for accommodating this fact has already been developed

  • One may be able to demand a stronger property along the lines of reflexivity, from physically relevant Banach spaces, for the purposes of determining the space-time metric, First a definition: a Banach space X is finitely representable in a Banach space Z if for every e > 0 and for every finite-dimensional subspace X0 ⊂ X there is a subspace Z0 ⊂ Z such that d BM (X0, Z0 ) < 1 + e

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Summary

Introduction

When one looks at the equations describing the four fundamental interactions of nature, s/he immediately notices that the kinematic equations in the Lagrangian formalism involve second order derivatives with respect to space-time variables. The statements on the number of derivatives in the equations of dynamics can be seen to be essentially equivalent, upon partial integration, to the fact that the kinetic terms as well as relevant potential energy terms are at most quadratic with respect to first order derivatives of the fundamental variables/fields/order parameters This in turn, allows one to use Euclidean/Riemannian concepts to model the evolution of such systems; for particle systems one uses the more familiar aspects of finite-dimensional Riemannian spaces [1], and for field theories one may have to resort to using aspects of infinite dimensional manifolds [2] which involve further subtleties. Even though considerable progress has been made toward such an understanding, it is probably fair to state that many important issues still remain unresolved [7] It is not clear, for instance, why space-time is 4-dimensional, to what extent it is smooth and how such a smoothness arises, why its Wick-rotated metric obeys the Pythagorean theorem etc.

Background and Physical Interpretation of Some Concepts
Norms on Linear Spaces
Norm Equivalence
The Operator Norm and the Banach-Mazur Distance
Reflexive and Super-Reflexive Spaces
Convexity and Smoothness
Why Convexity and Smoothness?
A Modulus of Convexity
A Modulus of Smoothness and a Duality
The Space-Time Metric from Variational Principles
Discussion and Outlook

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