Savoy Hotel Mnchen I Amalienstrae 25 I 80333

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Savoy Hotel München I Amalienstraße 25 I 80333 München String Model Building Stuart Raby

Savoy Hotel München I Amalienstraße 25 I 80333 München String Model Building Stuart Raby String Pheno 09 Warsaw University June 19, 2009 Title of talk 1

String Model Building or Searching for the MSSM § § § Outline Random searches

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 Title of talk 2

Random Searches for the MSSM Type II intersecting D brane models Gmeiner, Blumenhagen, Honecker,

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 !! Title of talk 3

Virtues of SUSY GUTs § § § § § MZ << MGUT “Natural” Explains

Virtues of SUSY GUTs § § § § § MZ << 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 Title of talk 4

Standard Model = Where would you look ? ? In this landscape ? Or

Standard Model = Where would you look ? ? In this landscape ? Or in a golf course ! = GUT Title of talk 5

E 8 x E 8 Heterotic models Smooth CY 3 Free fermions Orbifold Title

E 8 x E 8 Heterotic models Smooth CY 3 Free fermions Orbifold Title of talk 6

E 8 x E 8 Heterotic models Smooth CY 3 Bouchard & Donagi (

E 8 x E 8 Heterotic models Smooth CY 3 Bouchard & Donagi ( & Cvetic) SU(5) GUT Wilson line breaking to SM gauge group Higgs doublet – triplet splitting Title of talk 7

E 8 x E 8 Heterotic models Smooth CY 3 SM gauge group 3

E 8 x E 8 Heterotic models Smooth CY 3 SM gauge group 3 families 1 or 2 pairs ( Hu + Hd ) R parity cons. Function of moduli Need non-pert. physics Title of talk 8

E 8 x E 8 Heterotic models Free fermionic SM gauge group 3 families

E 8 x E 8 Heterotic models Free fermionic SM gauge group 3 families 1 pair ( Hu + Hd ) Cleaver, Faraggi, Nanopoulos (& Walker) 1998 Vector-like exotics decouple Non trivial Yukawa matrices & Neutrino See-Saw Title of talk 9

E 8 x E 8 Heterotic models Orbifolds § § Dixon, Harvey, Vafa &

E 8 x E 8 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 § Title of talk 10

Mini-Landscape search LNRRRVW 223 Models with 3 families, Higgs & ONLY vector-like exotics Out

Mini-Landscape search LNRRRVW 223 Models with 3 families, Higgs & ONLY vector-like exotics Out of ~ 30, 000 models Fertile patch in Heterotic landscape Title of talk 11

E 8 x E 8 heterotic string in 10 D Compactify 6 D on

E 8 x E 8 heterotic string in 10 D Compactify 6 D on (T 2)3 Then mod by Z 6 -II = (Z 3 x Z 2) and Add Wilson lines Z 6 embedded in E 8 x E 8 gauge lattice as shift V 6 : consistent with mod. inv. ! Title of talk 12

Orbifold GUTs First consider (T 2)3/Z 3 + W 3 [Wilson line in SU

Orbifold GUTs First consider (T 2)3/Z 3 + W 3 [Wilson line in SU 3 torus] Massless modes From Untwisted sector + (G 2 , SU 3) twisted sector Title of talk SU(6) GUT in 5 or 6 D 13

Then add Z 2 orbifold + W 2 [in long direction] P ( V

Then add Z 2 orbifold + W 2 [in long direction] P ( V 2 ) SU(6) P’ ( V 2+ W 2 ) SU(5) SU(3)x. SU(2)x. U(1) Title of talk 14

Two 4 D fixed points are special !! Local SO(10) GUT Title of talk

Two 4 D fixed points are special !! Local SO(10) GUT Title of talk 2 light families 15

2 (16) on SO(10) brane Title of talk 16

2 (16) on SO(10) brane Title of talk 16

Third family & Higgs in BULK Title of talk 17

Third family & Higgs in BULK Title of talk 17

Discrete non-Abelian Family symmetry Title of talk 18

Discrete non-Abelian Family symmetry Title of talk 18

S 1/Z 2 161 Title of talk 19

S 1/Z 2 161 Title of talk 19

D 4 family symmetry geometry space group sel. rule doublet singlets Title of talk

D 4 family symmetry geometry space group sel. rule doublet singlets Title of talk 20

Fermion mass hierarchy Natural Froggatt-Nielsen mechanism ! Title of talk 21

Fermion mass hierarchy Natural Froggatt-Nielsen mechanism ! Title of talk 21

Benchmark model Title of talk 22

Benchmark model Title of talk 22

Exact R-parity !! U(1)B-L broken to Z 2 matter parity Forbids R-parity violating operators

Exact R-parity !! U(1)B-L broken to Z 2 matter parity Forbids R-parity violating operators Title of talk 23

m term m = 0 in flat space SUSY limit Yukawa couplings Not realistic

m term m = 0 in flat space SUSY limit Yukawa couplings Not realistic - yet Neutrino masses via See-Saw Title of talk 24

Note: Yukawa couplings, gauge couplings and Vector-like exotic masses are functions of moduli (along

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 !! Title of talk 25

F theory / Type IIB models § § § Beasley, Heckman & Vafa Donagi

F theory / Type IIB models § § § Beasley, Heckman & Vafa Donagi & Wijnholt Blumenhagen, Braun, Grimm & Weigand Chen & Chung Marsano, Saulina & Schaefer-Nameki • SU(5) GUT on D 7 brane / • Chiral matter in 6 D / • Yukawa couplings at triple intersect’n of matter branes – • Fermion flavor hierarchy natural Title of talk 26

Gauge 7 -brane / Matter 7 -brane / Title of talk 27

Gauge 7 -brane / Matter 7 -brane / Title of talk 27

F theory / Type IIB models • SU(5) breaks to SM gauge group with

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

F theory / Type IIB models § § Heckman & Vafa Randall & Simmons-Duffin

F theory / Type IIB models § § Heckman & Vafa Randall & Simmons-Duffin Due to flux in 2 -3 surface breaking geometric flavor symmetry Title of talk 29

Gravity decouples w/ non-compact z 1 direction Local construction ! Blumenhagen, Braun, Grimm &

Gravity decouples w/ non-compact z 1 direction Local construction ! Blumenhagen, Braun, Grimm & Weigand global constructions Marsano, Saulina & Schaefer-Nameki Title of talk 30

E 8 x E 8 heterotic - F theory duality Title of talk 31

E 8 x E 8 heterotic - F theory duality Title of talk 31

Work in progress We are now attempting to construct the F theory dual to

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 ? § Title of talk 32

Step 1: E 8 x E 8 heterotic orbifold on ‘smooth’ CY 3 manifold

Step 1: E 8 x E 8 heterotic orbifold on ‘smooth’ CY 3 manifold ? After first Z 3 orbifold + Wilson line W 3 we find 6 D SU(6) orbifold GUT compactified on (T 2) 2 / Z 3 x T 2 Title of talk 33

Complete spectrum of 6 D orbifold GUT Dundee, Raby & Wingerter Satisfies Gravity anomaly

Complete spectrum of 6 D orbifold GUT Dundee, Raby & Wingerter Satisfies Gravity anomaly constraint Title of talk 34

Bershadsky, Intriligator, Kachru, Morrison, Sadov & Vafa hep-th/9605200 E 8 x E 8 heterotic

Bershadsky, Intriligator, Kachru, Morrison, Sadov & Vafa hep-th/9605200 E 8 x E 8 heterotic on K 3 x T 2 w/instantons E 8 [12 instantons in SU(3)x. SU(2)] SU(6) + (20 + cc) + 18 (6 + c. c. ) E 8 [12 instantons in E(6) + higgsing] SO(8) + 4 (8 v+ 8 s+ 8 c + c. c. ) K 3 + instantons dual to T 4 / Z 3 orbifold + Wilson line !! Title of talk 35

Bershadsky, Intriligator, Kachru, Morrison, Sadov & Vafa hep-th/9605200 F-theory CY 3 [T 2 fibration

Bershadsky, Intriligator, Kachru, Morrison, Sadov & Vafa hep-th/9605200 F-theory CY 3 [T 2 fibration over Fn] x. T 2 dual to E 8 x E 8 heterotic K 3 x T 2 w/instantons visible SU(6) 20 + 18 (6) Title of talk 36

Bulk gauge fields live in 8 D & matter fields live in 6 D

Bulk gauge fields live in 8 D & matter fields live in 6 D added fiber & Z 2 orb… breaks N=2 to N=1 U 1 flux breaks SU(6) to SU(5) Title of talk 37

Possible obstruction to finding F theory dual of Heterotic orbifold model Need to keep

Possible obstruction to finding F theory dual of Heterotic orbifold model Need to keep two orbifold fixed points 1. Otherwise hypercharge gets mass 2. 3. Groot Nibbelink, Ha & Trapletti Wilson line shrinks to point blow up modes on heterotic side leave 2 orbifold fixed points Title of talk 38

Orbifold takes torus to sphere Wilson line in z 3 breaks GUT to SM

Orbifold takes torus to sphere Wilson line in z 3 breaks GUT to SM Need orbifold fixed points !! Two light families on D 3 branes at fixed points ? ? Title of talk 39

Other model building considerations • Gauge coupling unification • Proton decay from dimension 5

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 Title of talk 40

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

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 ! Title of talk 41