Effective Action on Manifolds with Branes and Boundaries - PowerPoint PPT Presentation

About This Presentation
Title:

Effective Action on Manifolds with Branes and Boundaries

Description:

Effective Action on Manifolds with Branes and Boundaries. Lebedev ... local self-adjoint differential brane operator (generalized) Neumann Bulk propagator ... – PowerPoint PPT presentation

Number of Views:30
Avg rating:3.0/5.0
Slides: 15
Provided by: NDV5
Category:

less

Transcript and Presenter's Notes

Title: Effective Action on Manifolds with Branes and Boundaries


1
Effective Action on Manifolds with Branes and
Boundaries
Effective action in DGP brane models
Andrei Barvinsky Dmitry Nesterov
  • Lebedev Physics Institute, Moscow
  • Quarks-2008

2
References
  • A.O.Barvinsky and D.V.Nesterovin preparation
  • A.O.Barvinsky, A.Yu.Kamenshchik, C.Kiefer and
    D.V.Nesterov Effective action and heat kernel in
    a toy model of brane-induced gravity
  • Phys.Rev. D75 (2007) 044010
  • arXivhep-th/0611326
  • A.O.BarvinskyQuantum effective action in
    spacetimes with branes and boundaries
    diffeomorphism invariancePhys.Rev. D74 (2006)
    084033arXivhep-th/0608004
  • A.O.Barvinsky and D.V.NesterovQuantum effective
    action in spacetimes with branes and
    boundariesPhys.Rev. D73 (2006)
    066012arXivhep-th/0512291
  • A.O.Barvinsky and D.V.NesterovDuality of
    boundary value problems and braneworld action in
    curved brane modelsNucl.Phys. B654 (2003)
    225-247arXivhep-th/0210005

3
Map

Braneworld Field Theory
Braneworld effective action

Gauge aspects
weak field expansion
tree level
one-loop
higher loops


Neumann-to-Dirichlet reduction
Induced (brane) contribution
F.-P. ghostcontributions,
Dirichlet (Bulk) contribution


type of boundary (junction) conditions
DGP sector
Standard fields
Heat Kernelon manifolds with boundaries/singular
ities
Oblique fields
Heat Kernel Theory
4
Braneworld Setup(field theory framework)
Topological content
Field content
Next slide effective action approach
5
Effective action approach
  • starting point of braneworld field theory
  • local functional of brane and Bulk fields
  • functional of brane (induced) fields
  • essencially nonlocal functional
  • encorporates Bulk dynamics
  • functional of brane mean fields
  • essencially nonlocal functional
  • encorporates brane quantum effects

Next slide weak field (loop) expansion
6
Perturbative loop expansion
Tree
1-loop
Next slide Neumann-to-Dirichlet reduction
7
NeumanntoDirichlet Reduction
Systematic expression of Neumann quantities in
terms of Dirichlet quantities (based on
dualities between complementary boundary value
problems)
  • brane-to-brane inverse propagatortree-level
    duality relation(Dirichlet-to-Neumann map)
  • functional determinants1-loop duality
    relation(A.Barvinsky, D.N. 2005)

Next slide 1-loop effective action
8
1loop effective action
Next slide Brane contribution. DGP fields
9
DGP sector
1-loop brane contribution
-- purely brane functional --
essentially nonlocal
Key idea
  • well-known object
  • UV behavior Schwinger-DeWitt technique
  • IR behavior A.Barvinsky, D.N. (2003)
  • Nonperturbative curvature expansion
    A.Barvinsky, G.Vilkovisky (1987)
  • incorporates internal geometry of brane
  • incorporates the bundle geometry of induced
    brane field
  • canonical theory
  • pure Neumann junction (RS, )
  • Robin junction (generalized RS,)
  • DGP

Next slide generic braneworlds
10
General algorithm. Leading order.
Example UV expansion braneworld
generalization of Schwinger-DeWitt expansion.
Next slide subleading orders
11
General algorithm. Subleading orders.
Next slide Heat Kernel applications or
Conclusions
12
Heat Kernel Theory Applications
Schwinger-DeWitt expansion
  • Heat Kernel suitable tool for
  • one-loop divergences,
  • counterterms,
  • quantum anomalies,
  • Casimir effect,
  • UV asymptotics of 1-loop effective action and
    propagator

Heat Kernel on manifolds with boundaries
New ingredients boundary S-DW coefficients
  • Essentially depend on boundary conditions!
  • Can be regularly found for only Dirichlet
    and homogeneous Neumann cases using method of
    images, conformal properties (Branson, Gilkey,
    Dowker, Kirsten, Vassilevich, etc.)

13
Applying Neumann-to-Dirichlet Reduction
Generalized Neumann boundary conditions
Neumann boundary operator
large mass expansionof effective action
duality relation


reference coefficients (known)
1/M expansion (expansion method forintegrals
with weak peculiarity)
- are obtained!
for arbitrary generalized Neumann cases
14
Conclusion
  • Effective action approach is still effective for
    braneworlds!

15
Multibulk scenario
Bulks
braneworld configuration
three Bulks glued along single brane
determinant duality
one-loop brane effective action
brane
16
Duality Relations
tree-level
1-loop
where (case of codimension 1 brane in
(d1)-dimensional Bulk )
-- induced brane operator
-- brane-to-brane propagator
Path integral motivation
integration splitting
(generalized) Neumann propagator (Green function)
Dirichlet propagator (Green function)
Write a Comment
User Comments (0)
About PowerShow.com