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Tachyon condensation and Vacuum SuperString Field Theory

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Title: Tachyon condensation and Vacuum SuperString Field Theory


1
Super
String Field Theory
and Vacuum Super
String Field Theory
II SUMMER SCHOOL INMODERN
MATHEMATICAL PHYSICS September 1-12,
2002Kopaonik, (SERBIA) YUGOSLAVIA
2
  • Why

String Field Theory?
main motivations gauge invariance
principle behind string interactions
non-perturbative phenomena
  • What

we can calculate in String Field Theory?
(analog of Higgs and Goldstone Phenomena)
Condensation of Tachyon
Brane tensions
Rolling Tachyon
  • How

we can do calculations in SFT?

String Field Theory and Noncommutative Geometry

String Field Theory and CFT
3
String Field Theory ?Second Quantized String
Theory
  • Infinite number of local fields
  • String Field AX(s) - functional, or state
    in Fock space

  • Ghosts AX(s), c(s), b (s)
  • Example


4
INTERACTION ?

Associative Product of String Fields
Examples of associative multiplications

5
Wittens String Product
Associative Product of String Fields --
Coordinate representation
6
(No Transcript)
7
SFT Action
E.Witten (1986)
Gauge transformations
8
SFT Action is given
9
Tachyon Condensation in SFT
  • Bosonic String - Tachyon

Kostelecky,Samuel (1989)
10
Sens conjecture (1999)
Brane Tension

Vacuum Energy
Strings
Branes
11
Sens conjectures (1999)
12
Rolling Tachyon
Motivationscosmology,...
  • Anharmonic oscillator
  • alpha corrections
  • p-adic strings

I.Volovich(1987) P.Frampton, Nishino(1988) Brekk
e,Freund,Witten(1988), I.A,B.Dragovic,I.Volovich(1
988)
Moeller, Zwiebach, hep-th/0207107
p-adic and NC space-time
I.A.,I.Volovich, 1990
Sen, Strings2002
  • SFT

I.A, A.Giryavets, A.Koshelev
13
Rolling Tachyon
Spatially homogeneous field configurations
E.O.M.
where
14
Rolling Tachyon
Anharmonic oscillator approximation
E.O.M.
15
Anharmonic oscillator
16
Rolling Tachyon
Initial condition near the top
Initial condition near the bottom
17
Rolling Tachyon (bosonic case)
Initial condition near the top
Initial condition near the bottom
18
Alpha corrections (boson case)
  • First order

Solutions
19
Rolling Tachyon
E.O.M.
20
Rolling Tachyon
E.O.M. X-dependence
21
Rolling Tachyon
E.O.M.
Two analogues
i) p-adic strings
ii) non-commutative solitons in strong coupling
regime
Gopakumar, Minwalla,Strominger
22
Rolling Tachyon
Time evolution in the sliver-tachyon and p-adic
strings
p2,3,5,..
()
There is no solution such that
with
BUT this contradiction does not take place for ()
decreasing monotonically in time
23
Solutions to SFT E.O.M.
Analog of Yang-Feldman eq.
Resonance

Sen
Problems!!!
24
OUTLOOK
String Field Theory
L.Bonora
Noncommutative Field Theories and (Super) String
Field Theories, hep-th/0111208, I.A., D. Belov,
A.Giryavets, A.Koshelev,P.Medvedev
SuperString Field Theory
  • Cubic SSFT action

2-nd
  • Tachyon Condensation in SSFT
  • Rolling Tachyon

3-d
  • Vacuum SuperString Field Theory

i) New BRST charge ii) Special solutions -
sliver, lump, etc. algebraic surface
states Moyal representation
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