anomaly cancellations on heterotic 5-branes ( 前編 ) 矢田 雅哉
TRANSCRIPT
contents
• Introduction• NS5-brane• Small instanton’s configuration• Type-I Heterotic duality• Summary
introductionHeterotic string naturally has internal gauge symmetry.
→This is preferable structure in phenomenology.
・ Anomaly free・ There are some S.M.like structure with compactification.
→5-brane couples to the dual,B6,of the 2-form B
Heterotic string has 2-form B in NS-NS sector
NS5-braneHeterotic string effective action for the bosonic field
SUSY transformation for the fermionic fields
※Dirac matrix ※indices
=0…9(curved) =0…9(flat)
=6…9(curved)=0…5(curved)
[A.Strominger, J.A.Harvey, C.G.Callan Jr.,Nucl.Phys.B359(1991)]
Connection is given by
and
We will consider instanton solutions.So, we set
For simplicity we consider only the self-dual case.
Gauge solution [A.Strominger, Nucl.Phys.B343(1990)]
where
→ ・ Self-dual・ SU(2) subgroup of SO(4)
is a YM-instanton of scale size
This solution is valid when
Neutral solutionThis solution corresponding to a size instanton
is an integer.Only solution is reached as a limit of Gause solution as
⇒ later, we will explain…Near NS5-brane,the solution become wormhole throat.
→we can embed the connection in the gauge group.
⇒
This is SU(2) matrix that belongs to subgroup of SO(4)
generalized spin connection is
Now we calculate the connection…
And we recall the gauge field in gauge solutions…
Symmetric solution this solution embed the spin connection in the gauge group
Since the generalized connection is an SU(2) connection,the gauge field must lie in an SU(2) subgroup of E8 or SO(32).
⇒gauge symmetries spontaneous break
Wormhole throatFour-dimensional part of the metric
where
when , 1st term is not dominant
⇒wormhole throat
…Using spherical coordinates
Under the coordinate transformation
Small instanton’s configurationHere we consider instanton size → 0 case.In this case , gauge group is enhanced.
[E.Witten, Nucl.Phys.B460(1996)]
・ The Heterotic string on R6×K3
Supermultiplets are
(i) Graviton multiplet:(ii) Maxwell multiplet:(iii)Antisymmetric tensor multiplet:(iv)Hypermultiplet:
[P.K.Townsent ,Phys.lett.139B,num.4(1984)]
→Bosonic part of the hypermultiplet corresponding to instantons.
・ Hypermultiplet is on quaternionicmanifold →
・ Hypermultiplet originally has SU(2)R symmetry.
→
※The hypermultiplets transform as (2k,2) of
And the Gauge group that remains by Higgs mechanism
We treat the bosonic part of the hypermultiplet as…
※Here, the gauge group G generators are
We define the D-fields
the scalar potential
!The classical moduli space of vacua is obtained by setting V=0 anddividing the gauge group G.
→
…The gauge group G is remaining moduli space.
This deg
ree of fr
eedom wa
s
eaten by
the massi
ve vecto
r.
The moduli space will be singular when The unbroken gauge symmetry G is enhanced.
If there are k hypermultiplets,the dimension of moduli space is
We define the dimension of G is d:
One instanton Moduli spaceWhen an instanton shrinks to zero size…→we can simply think about the one instanton problem on R4
⇒ symmetric solution
We consider vacua for which the instanton are embedded in an SO(N)Subgroup of SO(32).
※ instanton’s position and scale size are embedded in SU(N)
The subgroup of SO(32) left unbroken by the instantons is SO(32-N)
unbroken
In symmetric solution, the instanton really has structure group K=SU(2)
⇒
The moduli space of these instantons has the dimension
center of mass decouples from the singularities...
The moduli space of instantons
Commute with K
Instanton’s moduli space
!known fact ; instanton shrinks to zero ⇒Full SO(N) is restored
if there are k hypermultiplets and the gauge group G has dimension d...
the most obvious way to obey the condition …
[C.G.Callan,Jr.,J.A.Harvey,A.Strominger, Nucl.Phys.B367(1991)]
・ k=N hypermultiplets form a representation of SO(N)
・ d=3 ⇒ G=SU(2)
This choice of gauge group and massless hypermultiplets lead to the correct moduli space.
small instantons have gauge symmetry
Type-I Heterotic duality
Instanton size:
Strong coupling with Heterotic stringS-duality:
↓↑
Weak coupling with type-I string
Hyper multiplet
NS sector
We consider D5-D9 system
Using Fermion zero mode dm0(m=6 ~ 9) ⇒2 of SU(2)
→Scalar boson ; D=6 Lorentz group
R sector
Using Fermion zero mode dμ0(μ=2 ~ 5) ⇒2 of SU(2)
→Weyl spinor;D=6 Lorentz group
・ Gauge symmetry is introduced by Chan-Paton factor