zero-norm states and high-energy scattering amplitudes of superstring theory
DESCRIPTION
Zero-norm States and High-energy Scattering Amplitudes of Superstring Theory. Jen-Chi Lee Dept. of Electrophysics, National Chiao-Tung Univ. Hsin-Chu, Taiwan. Outline. Introduction & Overview A simple example Three calculations of string symmetry (a) High-energy zero-norm states (HZNS) - PowerPoint PPT PresentationTRANSCRIPT
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Zero-norm States and High-energy Scattering Amplitudes of
Superstring Theory
Jen-Chi Lee
Dept. of Electrophysics, National Chiao-Tung Univ. Hsin-Chu, Taiwan
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Outline
1. Introduction & Overview
2. A simple example
3. Three calculations of string symmetry
(a) High-energy zero-norm states (HZNS)
(b) Virasoro constraints
(c) Saddle-point Method
4. Compares with Gross’s
5. (a) 2D string (b) Superstring
(c) Closed string
6. Conclusion
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1. Introduction & Overview
• Q.F.T : “Symmetry dictates interaction”
e.g : Y. M. , G. R.
• String: Interaction Symmetry ?
Prescribed by self-consistent conditions of quantum string
e.g : 1-loop modular invariance of 10D Heterotic string.
massless Y.M.2E8 SO(32), aθ
...,(ab)θ(ab)θ [μν]μ
e.g :
Massive symmetries
……………?
How to identify string symmetry?
Lee, (1994)
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1st Key
• Q.F.T :
• String:
hidden at low-energy
evident at high-energy!!
suggested by
• UV finiteness of quantum string!
• states with No free parameter.
: ' or E
fixedCM. ( Gross 1988)
PRL
•R. G., Asymptotic freedom, O.P.E. etc.•Spontaneous broken Symmetries
• High-energy limit. Saddle-point Approx.
• Infinite symmetry are
Huge symmetry Group!?
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Conjectures
1. Existence of linear relations among High-energy Scattering Amplitudes (HSA) of different string states.
2. All HSA can be expressed in terms of that of tachyons.
However
1. Origin of symmetry charges were not understood.
2. Proportionality constants among HSA of different string states were Not calculated.
~4321 VVVV
( Gross 1988 P.R.L.)
4321 TTTT...
Tachyon
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2nd Key
Zero-norm states (ZNS) in the old covariant first quantized (OCFR) spectrum
(Lee 1990)
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There are two types of ZNS:
0x|L 0,x|Lx|L , x|L 0211-
0,x|Lx|L , x|)L23
(L~
2
~
1
~21-2-
where
where
D=26 only
Type I:
Type II:
0x|1)(L~
0
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2. A simple example (Chan & Lee 2003)
Combine 1st key and 2nd key
)'( (ZNS)
2nd key : Decoupling of ZNS
Ward Identity, 0VVVZNSV
(Lee 1994)M2=4
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1st key : Taking high energy limit
fixed
E
CM
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4M 2
CM2Te
3Te
1Te
2k 3k-
1k4k-
4Te
Index of the 2nd vertex
Can be measured!?
For Tachyon, tensor
(-1):(-1):1:8[LT] TTTT ::: (LT)LLTTTT
(3)TT CM39
TTT θsin-8E(tree)
1,2,3v 2v
E as ee LP
,0)2k,(EM1
e 22
P
(0,0,1)eT
,0)E, 22k (M1
e2
L
Sample calculation
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(1)
!1)!-(2m21
M1
-VVVV i
qm4
1i
q2m
4321
iiii
......T...T...TTnnnn
4321
4321T
(valids to all loops order!)
,k0,|)(α)(α)(αqn,2m,|V qL2-
2mL1-
2q-2m-nT1-
(2)
Algebraically!!
1).-2(nM 2
Generalized to higher mass level
(tree only)(3)
)n]sinθ[-2E in
CM3......T...T...TT
nnnni
4321
4321T(T
with
2t)t)ln(s(s-tlntslns
-exp
2θ
cos2
θsinE2(-)π(n)
2n-5
CM
-3
CM2n-1-n-1-nT
is the only HSA at level )n ,n ,n ,(n4321
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3. Three calculations of string symmetry
a. High-energy zero-norm state
(1),
1q2,-n,2m|1)-(2mqn,2m,|Mq1,-1,2m-n|L1-
(2)
(1)
(2)
m)q(n,0,q)(n,2m,
M1
-M3
-...M
1-2m-
TT
1qn,0,|Mqn,0,|21
q2,0,-n|L 2-
(n,0,0)TTq
q)(n,0,
2M1
-
(n,0,0)TT !1)!-(2m21
M1
-qmq2m
q)(n,2m,
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(b) Virasoro constraints
“dual”0ψ|L1
Virasoro constraints are
Normalization factor & symmetry factors
Type I
'
E
Type II
By Type I
0ψ|L2
0x|L1-
0x|) (L~
2- 1-2L
2
3
0Ex. 4M 2
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(c) Saddle-point Method
ee LP (s-t channel)
Saddle point
!1)!-(2m21
M1
-qmq2m
...T
n,0,00,
2
Tn
2q-2m-n3
T0
2q2mn-0
q2m
210
(2m) )k)(-e''(f(2m)!x-1Mkk
)(xu
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Gross conjectures (1988)
are explicitly proved !
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4. Compares with Gross’sEx.
Ex.
Note!
(1) s are missing (=0) in Gross & Manes (N.B.1989)
inconsistent with the decoupling of ZNS
(or Ward identities)
Violates unitarity!!
(2) A corrected saddle-point calculation was given in Chan, Ho & Lee (N.B.2005)
4M 2
6M 2
32
:96
-:964
-:3
62-:
31
:34
:16
(LL)(LLL)(TTL)LTT,(LLLL)(TTLL)(TTTT) ::::: TTTTTTT :
(-1):(-1):1:8[LT] TTTT ::: (LT)LLTTTT
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One can construct a set of ZNS with discrete Polyakov momenta such that
• 2D discrete ZNS carry symmetry charges.
Space time symmetry algebra of 2D string was known to be
J,mG
a algebra!
}{Q mJ,
..(0))ψmJ-m(Jz2
..(0)(2)ψψ21212211 mm 1,-JJ1221mJmJ
( Chung & Lee 1994)
( Klebanov & Polyakov 1991)
( Witten 1992)
( Chung & Lee 1994)
(0))GmJ-m(J(0)(z)GG2πidz
21212211 mm 1,-JJ2112,mJ,mJ
“Ground ring”
21212211 m,mJJ,mJ,mJ QQQ
.
.
.
5 (a) 2D string
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• NS-sector, GSO even, polarization on the scattering plane
• GSO odd
5 (b) Superstring
L3/2-
T1/2- b,b|qn,2m,|
All are proportional to each other at each fixed mass level.
L3/2-
L1/2- b,b|q1,n,2m|
(Chan, Lee & Yang 2005)
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• Polarizations orthogonal to the scattering plane.
• New high-energy scattering amplitudes due to the fermion exchange in the correction functions.
• Needs to consider high-energy massive fermion scattering amplitudes in the R-sector.
T1/2-b
E.g.
iT1/2-b Same answer ( up to a sign)
i i
-
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Closed String
KLT formula :
High energy 4-tachyons :
‧Can be generalized to arbitrary mass levels.
5 (C)
(Chan, Lee & Yang 2005)
Veneziano (1968)
Gross & Mende (1987)
+ Are inconsistent with KLT formula !
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symmetry in 2D string
6. Conclusion The importance of zero-norm state (ZNS) in string theory has been largely underestimated for decades!
(Kao& Lee 2002, Chan, Lee& Yang 2005)
High-energy symmetry
(Gross)
Gauge symmetry In WSFT
Zero-norm state (ZNS)
Discrete duality symmetries
T-duality (Lee 2000)…
(Chung & Lee 1994)
(CHLTY 2005)