GRAVITATIONAL THEORY WITH A DYNAMICAL SPACETIME

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GRAVITATIONAL THEORY WITH A DYNAMICAL SPACETIME Eduardo Guendelman, arXiv:0911.0178 [gr-qc] Ben Gurion University, Israel, MIAMI 2009, December 19, 2009

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GRAVITATIONAL THEORY WITH A DYNAMICAL SPACETIME. Eduardo Guendelman, arXiv:0911.0178  [gr-qc] Ben Gurion University, Israel, MIAMI 2009, December 19, 2009. DYNAMICAL SPACE TIME?. IN Gen. Rel., THE SPACE- TIME IS REPRESENTED BY COORDINATES, THESE ARE PARAMETERS, NOT DYNAMICAL VARIABLES. - PowerPoint PPT Presentation

Transcript of GRAVITATIONAL THEORY WITH A DYNAMICAL SPACETIME

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GRAVITATIONAL THEORY WITH A DYNAMICAL

SPACETIMEEduardo Guendelman, arXiv:0911.0178 [gr-qc]

Ben Gurion University, Israel,MIAMI 2009, December 19, 2009

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DYNAMICAL SPACE TIME?

• IN Gen. Rel., THE SPACE- TIME IS REPRESENTED BY COORDINATES, THESE ARE PARAMETERS, NOT DYNAMICAL VARIABLES.

• In Quantum mechanics there is no “time” operator that would be conjugate to the energy. Is there a possibility to construct a variable of this type?

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We start with a simple example

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The Equacion obtained from variation of a is:

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The integration of this eq. w/r to t leads us to the conservation of

energy

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ordinary equations are reproduced

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4D theory with invariance under transformation of coordinates

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Symmetries of Killing vectors

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Then the following is a symmetry

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Models with point particles

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Symmetries of Killing tensors

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Equations of the Gravitational Field

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Variation w/r to the metric gives

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The gravitacional energy momentum tensor

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We could add a conventional term

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Solutions for flat space-time

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Solution for an arbitrary space time in a locally inertial frame

• The solution found before for flat space time is in fact (up to a constant) the solution for the vector field for ANY space time in a locally inertial frame (LIF).

• This shows a way to construct the solution for the vector field in general: it is proportional to the local Minkowski coordinate in the LIF, then transform back to the Lab. frame .

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Contribution to the mass: study small perturbations of Flat Space.

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The constant c only redefines G .We study the string gas cosmology

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Milne coordinates

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Other Cosmological solutions

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For strings the same relation for the Grav. E&M tensor is valid

• we can reformulate the particle so as to have invariance under world line reparametrizacion, the expression for the E&M gravitacional tensor is not changed.

• the solution for the vector that implements the conservacion of the original E&M tensor is another indicacion that its interpretacion is that of a dynamical space-time.

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Conclusions

• we have formulated a theory with a dyna-mical spacetime. In flat space time and in a locally

inertial frame the vector field is proportional to the Minkowski coordinates.

• Symmetries associated to vector and ten-sors killing are found, as shifts of that vector.• 2 E&M tensors: original and gravitacional• Cosmological solutions of string gas that do not

curve space time are found, the Milne universe with non trivial matter .

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Perspectives

• Extension to fields, no only particles and strings, relation with the problem of the cosmological constant, as it has been done in the special case of the TMT,

• Possibles supersymmetric extensions,• Exploration of more general cosmological

solutions.• Possible aplication to the problem of time

in quantum cosmology.