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String Model Building

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Virtues of SUSY GUTs. MZ MGUT 'Natural' Explains charge quantization ... we find 6D SU(6) orbifold GUT compactified on (T2) 2 / Z3 x T2 ... – PowerPoint PPT presentation

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Title: String Model Building


1
Savoy Hotel München I Amalienstraße 25 I 80333
München
String Model Building
Stuart Raby
String Pheno 09 Warsaw University June 19, 2009
2
String Model Building or Searching for the MSSM
  • Outline
  • Random searches for the MSSM
  • Virtues of SUSY GUTs
  • Heterotic model building
  • Smooth manifolds Free fermions
  • Orbifolds
  • F theory / Type IIB
  • Heterotic - F theory duals
  • Conclusion

3
Random Searches for the MSSM
Type II intersecting D brane models


Gmeiner, Blumenhagen, Honecker, Lust Weigand
Gepner orientifolds
Anastasopoulos, Dijkstra, Kiritsis Schellekens
Heterotic free fermion landscape analysis
Dienes, Lennek, Senechal Wasnik
MSSM is quite rare !!
4
Virtues of SUSY GUTs
  • MZ ltlt MGUT Natural
  • Explains charge quantization
  • Predicts gauge coupling unification !!
  • Predicts SUSY particles at LHC !
  • Predicts proton decay
  • Predicts Yukawa coupling unification
  • w/Family symmetry Fermion mass
    hierarchy
  • Neutrino masses and mixing via See-Saw
  • LSP - Dark Matter candidate
  • Baryogenesis via leptogenesis

5
Standard Model
Where would you look ??
In this landscape ?
Or in a golf course ! GUT
6
E8 x E8 Heterotic models
Smooth CY3 Free fermions Orbifold
7
E8 x E8 Heterotic models Smooth CY3
Bouchard Donagi ( Cvetic)

SU(5) GUT
Wilson line breaking to SM gauge group
Higgs doublet triplet splitting
8
E8 x E8 Heterotic models Smooth CY3

SM gauge group 3 families 1 or 2 pairs ( Hu
Hd )
R parity cons.
Function of moduli Need non-pert. physics
9
E8 x E8 Heterotic models Free fermionic
Cleaver, Faraggi, Nanopoulos ( Walker) 1998

SM gauge group 3 families 1 pair ( Hu Hd )
Vector-like exotics decouple Non trivial Yukawa
matrices Neutrino See-Saw
10
E8 x E8 Heterotic models Orbifolds
  • Dixon, Harvey, Vafa Witten
  • Font, Ibanez, kim, Nilles, Quevedo

  • Kobayashi, Raby Zhang
  • Buchmuller, Hamaguchi, Lebedev Ratz
  • Lebedev, Nilles, Raby, Ramos-Sanchez, Ratz,
  • Vaudrevange Wingerter
  • Kim, Kim Kyae

11
Mini-Landscape search LNRRRVW
  • Models with 3 families, Higgs
  • ONLY vector-like exotics
  • Out of 30,000 models

Fertile patch in Heterotic landscape
12
E8 x E8 heterotic string in 10D
Compactify 6D on (T2)3
Then mod by Z6-II (Z3 x Z2) and Add
Wilson lines
Z6 embedded in E8 x E8 gauge lattice as shift
V6 consistent with mod. inv. !
13
Orbifold GUTs
First consider (T2)3/Z3 W3
Wilson line in
SU3 torus
Massless modes From Untwisted sector
(G2 , SU3) twisted sector
SU(6) GUT in 5 or 6D
14
Then add Z2 orbifold W2
in long direction
P
( V2 )
P
( V2 W2 )
SU(6)
SU(5)
SU(3)xSU(2)xU(1)
15
Two 4D fixed points are special !!
2 light families
Local SO(10) GUT
16
2 (16) on SO(10) brane
17
Third family Higgs in BULK
18
Discrete non-Abelian Family symmetry
19
S1/Z2

162
161
20
D4 family symmetry

geometry
space group sel. rule
doublet
singlets
21
Fermion mass hierarchy

Natural Froggatt-Nielsen mechanism !
22
Benchmark model

23
Exact R-parity !!
U(1)B-L broken to Z2 matter parity

Forbids R-parity violating operators
24
m term
m 0 in flat space SUSY limit

Yukawa couplings
Not realistic - yet
Neutrino masses via See-Saw
25
Note Yukawa couplings, gauge couplings and
Vector-like exotic masses are functions of
moduli (along SUSY flat directions). Some of
these moduli are blow up modes for some, BUT NOT
ALL, of the orbifold fixed points.

2 fixed points are not blown up !!
26
F theory / Type IIB models
  • Beasley, Heckman Vafa
  • Donagi Wijnholt
  • Blumenhagen, Braun, Grimm Weigand
  • Chen Chung
  • Marsano, Saulina Schaefer-Nameki

  • SU(5) GUT on D7 brane /
  • Chiral matter in 6D /
  • Yukawa couplings at triple intersectn
  • of matter branes
  • Fermion flavor hierarchy natural

27
Gauge 7-brane /

Matter 7-brane /
28
F theory / Type IIB models
  • SU(5) breaks to SM gauge group
  • with ltFYgt hypercharge flux
  • Not possible in Heterotic string !
  • ltFYgt on Higgs brane
  • doublet-triplet splitting
  • Spinor reps of SO(10) possible !
  • Not possible in perturbative IIB


29
F theory / Type IIB models
  • Heckman Vafa
  • Randall Simmons-Duffin


Due to flux in 2-3 surface breaking geometric
flavor symmetry
30
Gravity decouples w/ non-compact z1
direction Local construction !

Blumenhagen, Braun, Grimm Weigand Marsano,
Saulina Schaefer-Nameki
global constructions
31
E8 x E8 heterotic - F theory duality

32
Work in progress
  • We are now attempting to construct the F theory
    dual to our MSSM-like models.
  • w/ Bobkov, Weigand Westphal
  • Find more general description i.e. all
    models in the same universality class
  • Provide a general understanding of moduli
    space
  • Help understand moduli stabilization
    SUSY breaking ?


33
Step 1 E8 x E8 heterotic orbifold on
smooth CY3 manifold ?
After first Z3 orbifold Wilson line W3 we
find 6D SU(6) orbifold GUT compactified on
(T2) 2 / Z3 x T2

34
Complete spectrum of 6D orbifold GUT
Dundee, Raby Wingerter
Satisfies Gravity anomaly constraint
35
Bershadsky, Intriligator, Kachru,
Morrison, Sadov Vafa hep-th/9605200
E8 x E8 heterotic on K3 x T2 w/instantons

E8 12 instantons in SU(3)xSU(2) ? SU(6)
(20 cc) 18 (6 c.c.) E8
12 instantons in E(6) higgsing?SO(8)
4 (8v 8s 8c
c.c.)
K3 instantons dual to T4 / Z3 orbifold
Wilson line !!
36
Bershadsky, Intriligator, Kachru,
Morrison, Sadov Vafa hep-th/9605200
F-theory CY3 T2 fibration over Fn xT2 dual
to E8 x E8 heterotic K3 x T2 w/instantons

visible SU(6) 20 18 (6)
37
Bulk gauge fields live in 8D matter fields
live in 6D
added fiber Z2 orb breaks N2 to N1

U1 flux breaks SU(6) to SU(5)
38
Possible obstruction to finding F theory dual of
Heterotic orbifold model
  • Need to keep two orbifold fixed points -
  • Otherwise hypercharge gets mass
  • Groot
    Nibbelink, Ha Trapletti
  • Wilson line shrinks to point
  • blow up modes on heterotic side leave
  • 2 orbifold fixed points

39
Wilson line in z3 breaks GUT to SM
Orbifold takes torus to sphere

Need orbifold fixed points !! Two light
families on D3 branes at fixed points ??
40
Other model building considerations
  • Gauge coupling unification
  • Proton decay from dimension 5 6 ops.
  • Supersymmetry breaking sparticle masses
  • Heckman Vafa Aparicio, Cerdeno
    Ibanez
  • Moduli stabilization
  • Cosmological constant
  • 10500 vacua ??
  • Cosmology


41
Conclusions
Important to test string theory
Several new ideas in string model building

Orbifold Local GUT MSSM
Global F theory constructions may open window
to general MSSM landscape
Final test at the LHC !
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