Moduli stabilization and supersymmetry breaking for string phenomenology

1. Moduli stabilization and supersymmetry breaking forstring phenomenology TetsutaroHigaki (DESY) Based on works with Hiroyuki Abe, Ryuichiro Kitano, Tatsuo Kobayashi, Yuji Omura and Osamu Seto

2. Why moduli? Superstring theory: Unified theory including quantum gravity. If the world we observe (4D) is described by superstring theory (10D), the theory will be compactifiedon A six dimensional compact space e.g. Calabi-Yau (CY) 3-fold, 6-dim. torus.

3. Closed string moduli =dynamical volumes and shapes. Theyalways exist in string vacua! F.Quevedo at string pheno.09 4-cycle size: τ (Kählermoduli) 3-cycle size: U (Complex structure moduli) + String Dilaton: S

4. Moduli coupling to our sector (gauge field) localized on the D(3+n)-brane wrapping on , • where is an n-cycle in SUSY The moduli vevs = physical parameters!

5. Moduli stabilization: global (bulk) issues • Scales, couplings: GUT scale, gauge/Yukawas , νR mass, μ… • Cosmology:Cosmological constant, inflation, CMP… • SUSY breaking: moduli mediation, i.e. m3/2 ≧1TeV, • for new physics(plus other mediations) • Without the stabilization, a fifth force would be found … Kaplunovsky et al; Conlon et al; Strominger; Font et al; Cremades et al… Kachru et al.; Conlon et al.; Cicoli et al. … Kaplunovsky et al; Brignole et al.; Choi et al.;Endo et al.; Falskowski et al; Conlon et al….

6. Moduli stabilization: global (bulk) issues • Scales, couplings: GUT scale, gauge/Yukawas , νR mass, μ… • Cosmology:Cosmological constant, inflation, CMP… • SUSY breaking: moduli mediation, i.e. m3/2 ≧1TeV, • for new physics(plus other mediations) • Without the stabilization, a fifth force would be found … • Stabilizing hierarchy problem • Gauge coupling unification (GUT) • Dark matter candidate with R-parity • Discovery at the LHC? Kaplunovsky et al; Conlon et al; Strominger; Font et al; Cremades et al… Kachru et al.; Conlon et al.; Cicoli et al. … Kaplunovsky et al; Brignole et al.; Choi et al.;Endo et al.; Falskowski et al; Conlon et al….

7. Issue of the stabilization? SUSY moduli posses perturbativePeccei-Quinn symmetries: ∵Axions {a} come from tensor fields with gauge sym.

8. Issue of the stabilization? SUSY moduli posses perturbativePeccei-Quinn symmetries: ∵Axions {a} come from tensor fields with gauge sym. Moduli multipets =axion ones. : moduli = saxion that determines its decay const. Universe with many light axions = string axiverse. Arvanitaki et al.

9. How are they stabilized? • Background closed string flux: • = • → Heavier moduli: . • Gaugino condensations (GCs), instantons: • SUSY is important for analyzing strong dynamics. • → Heavymoduli: • SUSY breaking; Typically ignored in low energy

10. Moduli stabilization before KKLT: • Relevant interactions of moduli: • (TeV or intermediate string without moduli stabilizations.) • Mass scales of moduli mass, soft SUSY mass: • (also general but highly model dependent issue) Potential Flux compactification? Are all moduli fixed?, De Sitter/Minkowski?; Realistic world? ??? Moduli 0

11. Kachru, Kallosh, Linde, Trivedi Conlon and Quevedo Potential Choi, Falkowski, Nilles, Olechowski Moduli stabilization after KKLT: • Stronger interaction than the gravitational force. • moduli mass much larger than , • and soft mass much smaller than . 0 Moduli SupersymmetricAdS vacuum with stabilized moduli viafluxor GC/instanton.

12. Kachru, Kallosh, Linde, Trivedi Conlon and Quevedo Potential Choi, Falkowski, Nilles, Olechowski Moduli stabilization after KKLT: • Stronger interaction than the gravitational force. • moduli mass much larger than , • and soft mass much smaller than . !!! 0 Moduli + SUSY breaking Uplifting by the SUSY breaking sector (Technically controllable fine-tuning) SupersymmetricAdS vacuum with stabilized moduli via flux or GC/instanton.

13. Semi-realistic models can be gained → Explicit computations are motivated!

14. Two comments…

15. Remark:Model dependent problems • CMP (moduli-dominated universe) • Gravitino overproduction • Overshooting or destabilization by Temp or inflation Low Hinf (< mmoduli), very heavy moduli, late time entropy production (nB/s), low cutt-off, change DM, high H for stabilization, low Hinf (< m3/2), moduli inflation, low or very high temperature, negative exponent, no SUSY… • Open string moduli stabilization Branes on the rigid cycle e.g. dP, flux, non-perturbative effect... Coughlan et al; Banks et al; Carlos et al. Endo et al; Nakamura et al; Kawasaki et al.; Asaka et al. Brustein et al; Buchmüller et al; Kallosh et al. Dine et al; Fan et al; Lyth et al; Kawasaki et al; Nagai et al; Choi et al; Conlon et al; Nakamura et al; Kaloper et al; Brustein et al; Conlon et al; Lalak et al; Abe, TH, Kobayashi+Seto… Camara et al; Baumann et al…

16. Local model building: local (brane) issue • Realization of the SM: • chiral mass spectra, gauge group, gauge/Yukawa couplings, flavor symmetries, stable proton, open moduli stabilization… • SUSY breaking: gauge mediation(smaller ) • Often moduli stabilization is • ignored since it will demand • hidden, e.g. strong coupling, • sectors. Our talk will be • another aspects (or limit • against) in local model building. Aldazabal et al.; Heckman et al.; Donagi et al.; Watari et al. Marsano et al. and many authors. String compactified on

17. Local model building: local (brane) issue • Realization of the SM: • chiral mass spectra, gauge group, gauge/Yukawa couplings, flavor symmetries, stable proton, open moduli stabilization… • SUSY breaking: gauge mediation(smaller ) • Often moduli stabilization is • ignored since it will demand • hidden, e.g. strong coupling, • sectors. Our talk will be • another aspects (or limit • against) in local model building. Aldazabal et al.; Heckman et al.; Donagi et al.; Watari et al. Marsano et al. and many authors. We must not forget moduli stabilization besides the tadpole condition (global issue). String compactified on

18. Plan of Talk Introduction Kachru-Kallosh-Linde-Trivedi model Almost SUSY stabilization SUSY breaking field and moduli Non-QCD axion mass

19. 2.Kachru-Kallosh-Linde-Trivedi (KKLT) model

20. KKLT vacuum Kachru, Kallosh, Linde, Trivedi The Standard Model sector

21. KKLT vacuum Kachru, Kallosh, Linde, Trivedi Flux: fixing manymoduli, e.g. shape moduli. NSNS, RR Flux Kachru et al; Giryavets et al;Conlon et al; Grana; Douglas et al and many authors The Standard Model sector

22. KKLT vacuum Kachru, Kallosh, Linde, Trivedi Flux: fixing manymoduli, e.g. shape moduli. D-branes: fixingthe remaining (volume) moduli. The visible sector NSNS, RR Flux Kachru et al; Giryavets et al;Conlon et al; Grana; Douglas et al and many authors The Standard Model sector

23. KKLT vacuum Kachru, Kallosh, Linde, Trivedi Flux: fixing manymoduli, e.g. shape moduli. D-branes: fixingthe remaining (volume) moduli. The visible sector and SUSY breaking effects. → <V> = 0 NSNS, RR Flux Kachru et al; Giryavets et al;Conlon et al; Grana; Douglas et al and many authors SUSY breaking? The Standard Model sector

24. KKLT vacuum Kachru, Kallosh, Linde, Trivedi Flux: fixing manymoduli, e.g. shape moduli. D-branes: fixingthe remaining (volume) moduli. The visible sector and SUSY breaking effects. → <V> = 0 NSNS, RR Flux Kachru et al; Giryavets et al;Conlon et al; Grana; Douglas et al and many authors Axion? SUSY breaking? The Standard Model sector

25. Effective 4d N=1 supergravity:

26. Effective 4d N=1 supergravity: Type IIB CY orientifold models with SUSY breaking Polonyi etc. Grimm, Louis

27. KKLT model with one modulus T (up to SUSY sector)

28. KKLT model with one modulus T (up to SUSY sector) n=2: sequestered SUSY breaking, n=3: non-sequestered SUSY breaking. for low scale SUSY breaking phenomenology.

29. Properties of KKLT vacuum • Supersymmetric stabilization of moduli • . • Mass hierarchy between , and • . • i.e. = 1TeV, = 30TeV, =1000TeV. • Note that anomaly mediated SUSY breaking • contributes to ;we could obtain degenerate masses. • LSP = bino (+ higgsino). Choi, Falkowski, Nilles, Olechowski Choi, Jeong, Okumura; Endo, Yoshioka, Yasmaguchi

30. Why is (was) KKLT viable?

31. Standard procedure of modern moduli stabilization • IIB moduli stabilization on CY (KKLT, KL on SUSY vac.) All moduli can be fixed via 3-form flux + GCs/instantons on 4-cycles (+ D-term stabilization via <Fij> or SUSY breaking) Uplifting (SUSY breaking) is necessary in many cases. But… <Wflux>=O(1) + α’ corrections -> de Sitter vacuum without uplifting? Westphal et al.

32. Standard procedure of modern moduli stabilization • IIA moduli stabilization on (non-)CY All moduli can be fixed via flux compactifications. (There are both even and odd-form fluxes.CY; ∃axions, AdS as KKLT) Uplifting will not be necessary. • Gaugino condensation would be viable in addition to D-term stabilization and SUSY breaking.

33. Standard procedure of modern moduli stabilization • Heteroticmoduli stabilization on (non-)CY? Extra dimension is mathematically complicated with 3-form fluxcompactifications. Instead, 2-from flux and GCs/world sheet instanton on CY space viable? (+ D-term stabilization and SUSY breaking) Strominger; Becker et al.; Yau et al… Anderson, Gray, Lukas, Ovrut

34. 3. Other variant models based on supersymmetricstabilization

35. Recent SUSY pheno. models via moduli stabilization • KKLT + string theoretic axion • Minimal LARGE volume scenario • G2 MSSM + string theoretic axions (no flux) Mass hierarchy: e.g.

36. KKLT model + axion Conlon; Choi, Jeong T1-T2 is absent from W; the direction becomes light axion.

37. KKLT model + axion Conlon; Choi, Jeong T1-T2 is absent from W; the direction becomes light axion. This model can be rewritten as

38. KKLT model + axion Conlon; Choi, Jeong T1-T2 is absent from W; the direction becomes light axion. This model can be rewritten as Sequestered anti D3-brane:

39. Balasubramanian, Berglund, Conlon, Quevedo ; Conlon, Quevedo, Suruliz • Minimal LARGE volume scenario (LVS)

40. Balasubramanian, Berglund, Conlon, Quevedo ; Conlon, Quevedo, Suruliz • Minimal LARGE volume scenario (LVS) LSP = bino

41. Balasubramanian, Berglund, Conlon, Quevedo ; Conlon, Quevedo, Suruliz • Minimal LARGE volume scenario (LVS) GeV O(10) TeV LSP = bino

42. G2 MSSM (M-theory on G2 space without flux) , , , : integer, . ADS superpotential with one meson

43. G2 MSSM (M-theory on G2 space without flux) , , , : integer, . ADS superpotential with one meson : racetrack sol., , + many axions LSP = Wino. Axions Non-sequestered

44. 3. Almost SUSY moduli stabilization: Generic result

45. Main points of recent models: • No-scalemoduli Kähler potential • at the tree level (common property); • Calabi-Yau, torus, • (would-be) T-dual of Calabi-Yau or torus with flux. For instance, Grimm et al. {Φ}: heavy moduli, {u}: saxion-axionmultiplets

46. Almost relevant moduli are stabilized near the supersymmetric locationvia instantons or gaugino condensations (GCs) in the Minkowski vacuum. E.g. KKLT proposal. W = W(Φ) {X}: SUSY breaking and uplifting to the de Sitter/Minkowski vacuum.

47. One finds … (up to factors) Choi, Jeong • SUSY breaking F-term vevs (up to 1/2Re[Φ]): • Vev shifts from SUSY solution: . ; If moduli masses are degenerate, universal F-terms are obtained.

48. Saxion masses (degenerate): “<V>=0” is important. For Vlift∝ Exp[K] or Vlift∝ Exp[2K/3]. No decay into gravitino pair from these saxions. • Axino masses (degenerate):

49. SUSY breaking axionmultiplet: Let us consider a simple case of small mixing We will parameterize the metric as gs, α’-correction or choice of linear comb. etc.

50. One finds in the Minkowski vacuum… • SUSY breaking F-term vevs except for {Φ,u}: • Saxion (r) mass: • Axino mass for n≠3 (for n=3 goldstino):