Obstacles to the quantization of general relativity using symplectic - - PowerPoint PPT Presentation

obstacles to the quantization of general relativity using
SMART_READER_LITE
LIVE PREVIEW

Obstacles to the quantization of general relativity using symplectic - - PowerPoint PPT Presentation

Obstacles to the quantization of general relativity using symplectic structures Tom McClain Department of Physics and Engineering, Washington and Lee University Overview The problem Classical field theory with symplectic structures


slide-1
SLIDE 1

Obstacles to the quantization of general relativity using symplectic structures

Tom McClain Department of Physics and Engineering, Washington and Lee University

slide-2
SLIDE 2

Overview

The problem Classical field theory with symplectic structures Quantization with symplectic structures Obstacles for general relativity

slide-3
SLIDE 3

Statement of the problem

General relativity is not perturbatively renormalizable Normal quantum field theory methods fail Other quantum field theory methods might succeed

slide-4
SLIDE 4

Wish list for polysymplectic Hamiltonian field theory for quantum field theory

Right equations of motion for real physical systems Fully differential geometric Use only polysymplectic structures with direct analogs in

Hamiltonian particle theory

slide-5
SLIDE 5

Configuration, (extended) phase, and “symplectic” spaces

slide-6
SLIDE 6

Polysymplectic structures

slide-7
SLIDE 7

Hamilton’s equations

slide-8
SLIDE 8

A simple quantization map

slide-9
SLIDE 9

Space of states?

slide-10
SLIDE 10

A complicated quantization map

slide-11
SLIDE 11

Issues with quantization of fields

Integrated commutation relation! Right operators? Right states? Where does the vector field in our quantization map come

from?

slide-12
SLIDE 12

Quantizing general relativity

slide-13
SLIDE 13

Issues with quantizing general relativity

What vector field should we use to define Q? Hamiltonian not well-defined (Legendre transformation) Cannot take the quantization process seriously if the classical

theory isn’t well defined!

Purely classical problems!

slide-14
SLIDE 14

Solutions?

Different starting geometries? Extended Legendre transformations? Different Lagrangians? Eliminate the Lagrangian and Legendre transform? Other approaches?

slide-15
SLIDE 15

Questions?

For closely related work, please see…

Günther, Christian. "The polysymplectic Hamiltonian formalism in

field theory and calculus of variations. I. The local case." Journal of differential geometry 25.1 (1987): 23-53.

Struckmeier, Jürgen, and Andreas Redelbach. "Covariant Hamiltonian

field theory." International Journal of Modern Physics E 17.03 (2008): 435-491.

Kanatchikov, Igor V. "Toward the Born-Weyl quantization of fields."

International journal of theoretical physics 37.1 (1998): 333-342.

Magnano, Guido, Marco Ferraris, and Mauro Francaviglia. "Legendre

transformation and dynamical structure of higher-derivative gravity." Classical and Quantum Gravity 7.4 (1990): 557.Different Lagrangians?

slide-16
SLIDE 16

Appendix

More words on symplectic structures

slide-17
SLIDE 17

The tautological tensor

Intrinsic definition In local canonical coordinates:

slide-18
SLIDE 18

The polysymplectic structure (Part I)

Intrinsic definition (first try): In canonical coordinates: (depends on β!)

slide-19
SLIDE 19

The polysymplectic structure (Part II)

Solution: restrict to vertical vector fields:

Now

slide-20
SLIDE 20

Hamilton’s field equations (Part I)

Vertical differential of a section: In coordinates:

slide-21
SLIDE 21

Hamilton’s field equations (Part II)

Solution sections must satisfy: for all vertical vector fields u Gives Hamilton’s equations

slide-22
SLIDE 22

Poisson brackets (Part I)

For each function f on P, there exists a family of sections Sf such that: In canonical coordinates: (the last components must be trace-free)

slide-23
SLIDE 23

Poisson brackets (Part II)

Define a new tensor via: for all functions on the phase space Imposing anti-symmetry gives: (no contribution from the trace-free components!)

slide-24
SLIDE 24

Poisson brackets (Part III)

Define the Poisson bracket via: for all functions on the phase space In canonical coordinates: