Fotini Markopoulou- Quantum Gravity and Emergent Locality
Transcript of Fotini Markopoulou- Quantum Gravity and Emergent Locality
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QUANTUM GRAVITYAND EMERGENT LOCALITY
Fotini MarkopoulouPerimeter Institute
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QUANTUM GRAVITYAND EMERGENT LOCALITY
QUANTUM GRAPHITY:a background independent condensedmatter model of emergent space
Fotini MarkopoulouPerimeter Institute
T. Konopka, FM & L.Smolin, hep-th/0611197
also with: O. Dreyer, S. Severini
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Preview
geometrogenesis
phase transition
Permutation symmetry No locality (no space) Relational
High-Translations Local Relational
Low- ground state
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Outline.
1. Motivation
2. Quantum Graphity: A Model of emergent space (time)
3. Could we observe this? Early universe application
4. Discussion
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1. Emergence of near-flat geometry in low-energy limit of background
independent quantum gravity: long-standing challenge.
Motivation for the model.
cf. Ambjorn talk
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2. Locality: underutilized.
combinatorial quantum geometry classical geometry
: quantum geometry
spin foam vertex properties
1. Emergence of near-flat geometry in low-energy limit of background
independent quantum gravity: long-standing challenge.
Motivation for the model.
cf. Ambjorn talk
i j
k
l
local statements
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1. Emergence of near-flat geometry in low-energy limit of background
independent quantum gravity: long-standing challenge.
Motivation for the model.
cf. Ambjorn talk
FM&L.Smolin, gr-qc/0702044
2. Locality: underutilized.
combinatorial quantum geometry classical geometry
: quantum geometry
spin foam vertex properties
nodes one-edge perturbations locality is unstable
locality?
i j
k
l
local statements
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Phase transition + background independence
micro-locality macro-locality
background independence means dynamics determines locality.
phase transition
O.Dreyer, hep-th/0409048
FM&D.Kribs, gr-qc/0510052
FM, gr-qc/0703097
Motivation for the model.
2. Locality, cont.
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Phase transition + background independence
micro-locality macro-locality
background independence means dynamics determines locality.
phase transition
O.Dreyer, hep-th/0409048
FM&D.Kribs, gr-qc/0510052
FM, gr-qc/0703097
Motivation for the model.
2. Locality, cont.
Lots of other hints: AdS/CFT, black holes, causets,...
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Motivation for the model.
3. Background independence vs emergent gravity
Geometry and gravity are only
classical, emergent concepts.
- condensed matter approaches(e.g. Volovik)
- string theory
Background independence:dynamical nature of
spacetime geometry
What is the role of the lattice/geometry
and the symmetries of the lattice?
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Motivation for the model.
3. Background independence vs emergent gravity
Geometry and gravity are only
classical, emergent concepts.
- condensed matter approaches(e.g. Volovik)
- string theory
Background independence:dynamical nature of
spacetime geometry
What is the role of the lattice/geometry
and the symmetries of the lattice?
Reconcile:
Background independence: no fundamental geometric degrees of freedom
Today: background independent condensed matter models.Dreyer 04, 06, Lloyd 05,FM&Kribs 05, FM07.
Background independence is normally implemented by a superposition
of quantum geometries: - loop quantum gravity- dynamical triangulations- causal sets
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4. Matter vs Geometry.
New results on emergent matter are suitable for a background independent
treatment:
5. No fundamental locality large-scale observational consequences of
quantum gravity.
Motivation for the model.
gauge theory -like
excitations
and fermions
M.Levin & X-G.Wen, hep-th/0507118
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The model: kinematics.
Complete graph : vertices, edges.
one-edge state space:
edge on
edge off
total state space:
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The model: dynamics.
Complete graph : vertices, edges.
want ground state
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The model: dynamics.
Complete graph : vertices, edges.
want ground state
turns off edges and has minimum when all edges have degree .
E.g., for ,
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The model: dynamics.
Complete graph : vertices, edges.
want ground state
values:
strings
turns off edges and has minimum when all edges have degree .
E.g., for ,
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The model: dynamics.
Complete graph : vertices, edges.
want ground state
does not likeopen strings tension
wants all
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The model: dynamics.
Complete graph : vertices, edges.
want ground state
length of loop
cf. kinetic energy
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The model: dynamics.
Complete graph : vertices, edges.
want ground state
length of loop
cf. kinetic energy
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The model: dynamics.
Complete graph : vertices, edges.
want ground state
length of loop
cf. kinetic energy
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The model: dynamics.
Complete graph : vertices, edges.
want ground state
length of loop
Let . There is a preferred loop length :
cf. kinetic energy
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erases edges to give lattice with extension
The model: dynamics.
Complete graph : vertices, edges.
makes lattice regular and gives macro-matter
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Matter.
and are generalizations of the rotor model ofstring-net
condensation of Levin and Wen to a dynamical lattice.
tension K.E. : ground state has almost no strings
tension K.E. : ground state is a superposition of many closed strings,
i.e., string-net condensed:
high-energy charged excitations: open strings
emergent gauge theory.
M.Levin & X-G.Wen, hep-th/0507118
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Ground state geometry plus matter.
Local lattice: large average distance .
Small vertex degree
Loops of average size .
Possibly also regular?
For number of minimal loops
is maximized by the honeycomb lattice:
In our model: the balance between tension and K.E. controls both the
loop size when the lattice is dynamical and gives the matter.
T.Konopka, FM& S.Severini
Plus string condensation on the ground state
lattice, as in string nets.
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Summary of quantum graphity.
geometrogenesis
phase transition
Permutation symmetry No locality
Relational -dimensional no subsystems external time
micro-matter
Translations Local
Relational large low-dimensional subsystems external and internal time
macro-matter and dynamicalgeometry
Model has 4 couplings ( ) and 3 parameters ( ).
Some obey generic conditions:
Some have to be adjusted:
High- Low-
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Cosmology of emergent space.
Horizon problem
This is an extrapolation
of our causal and localstructure to the initial time
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Cosmology of emergent space.
Horizon problem
This is an extrapolation
of our causal and localstructure to the initial time
inflation
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In our model:
Cosmology of emergent space.
Horizon problem
This is an extrapolation
of our causal and localstructure to the initial time
inflation
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In our model:
Cosmology of emergent space.
Horizon problem
This is an extrapolation
of our causal and localstructure to the initial time
inflation
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In our model:
Cosmology of emergent space.
Horizon problem
This is an extrapolation
of our causal and localstructure to the initial time
inflation
Are the CMB correlations a consequence of pre-geometry?
Compare, e.g., to the phenomenology of discretization.
A geometrogenesis scenario has the potential of large-scale effects.
C
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Comments.
1. Time, temperature?
Emergent space or emergent spacetime?
Time-reparametrization invariance as the noiseless sector of atheory with time: T. Konopka and FM, gr-qc/0601028.
Does the temperature imply a bath?
Internal vs external time and geometry.Internal: subsystems observing subsystems. Our emergent space
gives emergent spacecetime internally.
2. The terms that give rise to matter are also responsible for the geometry
of the lattice: we dont just erase edges, we also order them.
This is a new use for unification.
T d
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To do.
Understand the ground state
Graph theory analysis of the terms in the Hamiltonian
Cosmology: perturbations
Effective disordered locality description
Understand the role of the temperature
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