Title: Tachyon condensation and Vacuum SuperString Field Theory
1Super
String Field Theory
and Vacuum Super
String Field Theory
II SUMMER SCHOOL INMODERN
MATHEMATICAL PHYSICS September 1-12,
2002Kopaonik, (SERBIA) YUGOSLAVIA
2String Field Theory?
main motivations gauge invariance
principle behind string interactions
non-perturbative phenomena
we can calculate in String Field Theory?
(analog of Higgs and Goldstone Phenomena)
Condensation of Tachyon
Brane tensions
Rolling Tachyon
we can do calculations in SFT?
String Field Theory and Noncommutative Geometry
String Field Theory and CFT
3String 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)
4INTERACTION ?
Associative Product of String Fields
Examples of associative multiplications
5Wittens String Product
Associative Product of String Fields --
Coordinate representation
6(No Transcript)
7SFT Action
E.Witten (1986)
Gauge transformations
8SFT Action is given
9Tachyon Condensation in SFT
Kostelecky,Samuel (1989)
10Sens conjecture (1999)
Brane Tension
Vacuum Energy
Strings
Branes
11Sens 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
I.A, A.Giryavets, A.Koshelev
13 Rolling Tachyon
Spatially homogeneous field configurations
E.O.M.
where
14Rolling Tachyon
Anharmonic oscillator approximation
E.O.M.
15Anharmonic oscillator
16Rolling Tachyon
Initial condition near the top
Initial condition near the bottom
17Rolling Tachyon (bosonic case)
Initial condition near the top
Initial condition near the bottom
18Alpha corrections (boson case)
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
23Solutions to SFT E.O.M.
Analog of Yang-Feldman eq.
Resonance
Sen
Problems!!!
24OUTLOOK
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
2-nd
- Tachyon Condensation in SSFT
3-d
- Vacuum SuperString Field Theory
i) New BRST charge ii) Special solutions -
sliver, lump, etc. algebraic surface
states Moyal representation