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Emergence of space, general relativity and gauge theory from tensor models

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Title: Emergence of space, general relativity and gauge theory from tensor models


1
Emergence of space, general relativity and gauge
theoryfrom tensor models
  • Naoki Sasakura
  • Yukawa Institute for Theoretical Physics

2
Kawamoto-sans education
  • A class guided by Kawamoto-san
  • Text the original BPZ paper on CFT
  • Not allow superficial understanding
  • Everything must be understood certainly
  • Full of discussions
  • No care about time
  • Unusual members
  • Students and staff members from other
    universities
  • Russian style

3
Kawamoto-san loves discussions
  • 1330 Class starts
  • 1500 Continue (Official end)
  • 1700 Continue (End for most classes)
  • 1900 End of the class
  • 1900 Go to drink at Izakaya
  • Various discussions on physics and
    non-physics
  • 2200 Go to Kawamoto-sans home
  • Discussions continue
  • 600 Back home

4
Spacetime is lattice (literally)
--- Kawamoto-sans philosophy ---
Not new but has potential to solve problems in
the frontiers.
  • Reduce degrees of freedom
  • Free from infinities
  • Incorporate minimal length
  • May prevent physically unwanted fields
  • (e.g. scalar massless moduli fields in
    string theory)
  • Unified theory on lattice
  • Matter contents are related to lattice
    structures
  • Kawamoto-sans talk at 13th Nishinomiya Yukawa
    Memorial Symposium (1998)
  • Non-String Pursuit towards Unified Model on the
    Lattice
  • Reconnection ?Dynamical spacetime
  • Possible route to quantum gravity
  • Intrinsically background independent

5
Random surface
Numerical Simulation
Matrix model
2D quantum gravity
Kawamoto, Kazakov, Watabiki,
6
Tensor models
  • Generalization of matrix models

Random surface
Random volume
Matrix model
Tensor model
Master thesis under Kawamoto-san (1990)
Sasakura, Mod.Phys.Lett.A6,2613,1991
7
Tensor models were not successful
  • Continuum limit ? Large volume ?

  • Large Feynman diagram
  • But no analytical methods known for
    non-perturbative computations in tensor models.
  • Topological expansions not known.
  • Difficulty in physical interpretation of the
    partition function.

8
A different interpretation of tensor models
--- My proposal ---
  • Tensor models may be regarded as dynamical
    theory of fuzzy spaces.
  • The structure constant defining a
    fuzzy space may be identified with the dynamical
    variable of tensor models.

Sasakura, Mod.Phys.Lett.A211017-1028,2006
9
Fuzzy space
  • Defines algebraically a space. No coordinates.
  • Points replaced with operators
  • Includes noncommutative spaces
  • Connect distinct topologies and dimensions

10
Fuzzy space
Lattice
11
  • Symmetry of continuous relabeling of points

Total number of points
12
The symmetry contains local transformations.
A background fuzzy space causes symmetry breaking
Non-linearly realized local symmetry ?
Gauge symmetry ( Gen.Coord.Trans.Sym.)
Ferrari, Picasso 1971 Borisov, Ogievetsky 1974
Relabeling symmetry ? Origin of local gauge
symmetries
13
Contents of the following talk
  • Gaussian fuzzy space (Flat D-dimensional fuzzy
    space)
  • Construction of an action having Gaussian sol.
  • Fluctuation mode analysis around the sol.
  • --- Emergence of general relativity
  • Kaluza-Klein set up
  • --- Emergence of gauge theory
  • --- Emergent scalar field is supermassive
    (Planck order)
  • Summary and future problems

14
Gaussian fuzzy space
  • Ordinary continuum space
  • Gaussian fuzzy space
  • ß parameter of fuzziness

Sasai,Sasakura, JHEP 0609046,2006.
15
  • Gaussian fuzzy space
  • Simplest fuzzy space
  • Poincare symmetry ? Flat D-dimensional fuzzy
    space
  • Can naturally generalize to curved space

16
This metric-tensor correspondence derives DeWitt
supermetric from the configuration measure of
tensor models.
Tensor models
DeWitt supermetric in general relativity
Used in the comparison of modes
Sasakura, Int.J.Mod.Phys.A233863-3890,2008.
17
Construction of an action
  • Demand has Gaussian fuzzy spaces as classical
    solutions
  • Infinitely many such actions
  • Generally very complicated and unnatural

--- Future problems
  • The action in this talk ---- Convenient but
    singular
  • (There exists also non-singular but
    inconvenient one.)
  • Least number of terms.
  • The singular property will not harm the
    fluctuation analysis.
  • The low-frequency property independent of the
    actions.

18
(Symmetric, positive definite)
19
  • This action does not depend explicitly on D
  • All the dimensional Gaussian fuzzy spaces are the
    classical solutions of this single action.
  • --- An aspect of background independence

A cartoon for the action
20
Analysis of the small fluctuations around
Gaussian solutions
Eigenvalue and eigenmode analysis
21
List of numerical analysis performed
Classical sol. (Gaussian) fuzzy flat
D-dimensional torus
  • Emergence of general relativity
  • D2 Results shown
  • D1,3,4 Similar good results
  • Kaluza-Klein mechanism
  • D21 Results shown
  • D11 Similar good results

22
Emergence of general relativity
D2 , L10
  • 3 states at P0
  • 1 state at each P?0
  • Zero eigenmodes

Sasakura, Prog.Theor.Phys.1191029-1040,2008.
23
The three modes at P0
Tensor model
General Relativity
24
The mode at P?0
One mode remains.
General relativity
Tensor model
25
Kaluza-Klein mechanism
  • In continuum theory

MS1 S1 with small radius
26
Fuzzy Kaluza-Klein mechanism in tensor models
Classical solution
21 dimensional flat torus


27
Numerical analysis of fluctuation modes
L3
L6
  • Scalar mass does not scale
  • Slopes of lines scale

Scalar
Vector
L ? Large
Supermassive scalar field (Planck order)
Gravity
28
Summary and future problems
  • Tensor models are physically interesting

Tensor models seem physically interesting.
Emergence of
  • Space
  • General relativity
  • Gauge theory
  • Gauge symmetry (Gen.Cood.Trans.Sym.)

from one single dynamical variable Cabc.
Background independent
Supermassive scalar field in Kaluza-Klein
mechanism. Possible resolution to moduli
stabilization.
  • Natural action ?
  • Fermion ?

29
Thank you very much for many suggestions ! And
Happy Birthday !
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