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Scherk-Schwarz SUSY brea Scherk-Schwarz SUSY brea king king from the viewpoint of from the viewpoint of 5D conformal supergravit 5D conformal supergravit y y Yutaka Sakamura (Osaka Uni v.) in collaboration with Hiroyuki Abe (YITP) JHEP0602 (2006) 014 (hep-th/051 326 ) 8/29/2006@SI06

Scherk-Schwarz SUSY breaking from the viewpoint of 5D conformal supergravity

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Scherk-Schwarz SUSY breaking from the viewpoint of 5D conformal supergravity. Yutaka Sakamura (Osaka Univ.) in collaboration with Hiroyuki Abe (YITP) JHEP0602 (2006) 014 (hep-th/051 2326 ) 8/29/2006@SI06. Introduction. SUSY : a solution of hierarchy problem SUSY breaking is necessary - PowerPoint PPT Presentation

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Page 1: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

Scherk-Schwarz SUSY breaking Scherk-Schwarz SUSY breaking frfrom the viewpoint ofom the viewpoint of 5D conformal supergravity5D conformal supergravity

Yutaka Sakamura   (Osaka Univ.) in collaboration with Hiroyuki Abe (YITP)

JHEP0602 (2006) 014 (hep-th/051 2326 )

8/29/2006@SI06

Page 2: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

Introduction

SUSY: a solution of hierarchy problem SUSY breaking is necessary Scherk-Schwarz SUSY breaking:

the simplest case is 5D theory on or different b.c. on bosons and fermions

Page 3: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

Conformal SUGRA (off-shell formulation of SUGRA)useful and powerful to describe the SUGRA action with boundaries

In conformal SUGRA, various properties of SS mechanism can be easily understood.

Page 4: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

SS twist in 5D SUGRA

5D SUGRA on with the radiusIt has symmetry. Orbifold b.c. : We choose as Twisting b.c. for

Page 5: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

Consistency condition:

This requires           .

Page 6: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

5D conformal supergravity Symmetries:

Field content: Weyl multiplet: Hypermultiplet:

Vector multiplet:

( Kugo & Ohashi )

compensatorPhysical fields

Page 7: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

Superconformal gauge fixing Extra symmetries: Ordinary gauge fixing conditions

Page 8: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

Combining and gauge fixings,

We will modify this as

while the physical fields remain periodic.

Page 9: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

gauge field on-shell is given by

is shifted and

This corresponds to the nonvanishing F-term of

the radion superfield in the superfield formalism. (G.v. Gersdorff, M.Quiros, …)

Page 10: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

SUSY breaking terms:

All SUSY terms are proportional to .

gravitino gaugino

hyperscalar

Page 11: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

Singular gauge fixingWe take a gauge fixing parameter as

Page 12: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

Namely,

Thus becomes boundary terms.

SS twist

⇔ Boundary Constant superpotential

provided that .

SS SUSY breaking is spontaneous.

Page 13: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

SS twist and warped geometry

SS twist yields an inconsistency on the warped geometry. (Hall,Nomura,Okui,Oliver (2004))

Gauging of by graviphoton is necessary to realize geometry.

From , a graviphoton mass term appears, which is proportional to .

Page 14: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

Consistency condition:

Models of (Gherghetta,Pomarol;Falkowski,Lalak,Pokorski) gauging with odd couplingi.e.,

Model of (Altendorfer,Bagger,Nemeschansky) gauging with even coupling i.e., SS twisting seems possible. But this model is not derived from known off-shell SUGRA.

Page 15: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

-even case:Boundary tension terms come from

Then,

SUSY condition:

Randall-Sundrum condition:

Page 16: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

Summary

From the viewpoint of 5D conformal SUGRA, SS twisting for is understood as

twisted gauge fixing.

SS twist ⇔ Boundary constant superpotential

SS twist in leads to massive graviphoton.

Page 17: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

Future works The case that both SS twist and bounda

ry constant superpotentials exist (model of Altendorfer,Bagger,Nemeschansky?)

Extension to two-compensator case(e.g. effective theory of heterotic M theory)

Page 18: Scherk-Schwarz SUSY breaking  from the viewpoint of 5D conformal supergravity

In the flat case, SS twist ⇔ b.d. constant superpotential

Is it possible to restore SUSY by tuning ?

The answer is NO. SS twist does not lead to the b.d. tensions.

Relation to the ABN model is still an open question.