1. Super Flavour Factory Presentation of the Physics case Part Paris 9 May 2007 444 pages 320 signers ~80 institutions M. Ciuchini, T. Gershon, A. Stocchi

2. The way we build the SuperB Physics Case : Experimental reach. -Precision we could reach on different measurements. -New measurement possible ? - U(4S), U(5S) and charm at threshold. Phenomenological impact. - SM - NP search + no loose theorem exists ? + MFV (mainly high tan  ) + MSSM - charm physics - tau physics LFV People who contributed to the Physics Case chapter. D. Asner, R. Baldini-Ferroli, E. Baracchini, E. Ben Haim, A.Bevan, I.Bigi, M. Bona, M. Ciuchini, J. Dingfelder, P. Gambino, T. Gershon, K. George, T. Hurth, G. Isidori, V. Lubicz,, V. Lutz, P. Paradisi, M. Pierini, F. Renga, M. Roney, P. Roudeau, M.A. Sanchis-Lozano, L. Silvestrini, F. Simonetto, A. Stocchi, Presentation in plenary Session by Marco Ciuchini

3. B factories have shown that a variety of measurements can be performed in the clean environment. By doing the work of extrapolating the existing measurements and the ones which will be possible with more statistics we observe that : - Several measurements are statistically limited and so it is worthwhile to collect >50ab -1 - The systematic errors are very rarely irreducible and can almost on all cases be controlled with control samples. On top of it detector improvements can be crucial for some analyses. B D D prim. sec ter. B events continuum events Thanks to better vertex resolution we can distinguish on vertex requirements B vs continuum events ( ~factor 5 background rejection) Not yet included in the extrapolations

4. Experimental Reach

5. The angle  Based on the present “savoir faire”  t(ps) 535M Golden B 0  J/  K 0 sin2  gives the best constraint on  plane and the error can still be reduced Example other modes : B 0  D 0 h 0 Babar SuperB will be able to make complementary measurements (beyond J  K 0 ) that help to ensure that the theoretical uncertainties are under control and to control them on data Important points : - We know how to perform these analyses - Very significant improvement from now  2ab -1  Superb luminosity SuperB (talk of Catherine Goerge)

6. The angle  Isospin analyses performed at the B-factories  @ 10 0 Some very important measurements start to be possible only now with about 0.5ab -1  modes consistent with no CP violation  eff ~90 o (0/180) o Important measurement because it gives the contributions of Penguins diagram Each of  analysis will be allow to get  (  ~2 degrees It allow consistency checks and to control theoretical uncertainties on data  ~1 o possible SuperB (*) theoretical limited (talk of Adrian Bevan)

7. The angle  Many independent methods GLW, ADS, Dalitz, with many different decay channels  ~1 o possible New D 0 decays starting to be explored BaBar Error vs D CP statistics 750pb -1 ( 4-5) o 20fb -1 (< 1) o Bondar Poluektov hep-ph/0510246 SuperB The model error can be reduced by running at threshold Best measurements from Dalitz analysis with D 0  K s  (talk of Alex Bondar)

8. Many channels can be measured with  S~(0.01-0.04) sin2  from “s Penguins”… SuperB (*) theoretical limited dd s b WW B0dB0d t s s  K0K0 g s b b s ~ ~ ~ (talk of Catherine Goerge)

9. Exp. likelihood BABAR+BELLE BR(B → τ ν) = (1.31 ± 0.48)10 -4 leptonic decay B  l Br(B   up to 3-4% (below limited by systematics) Br(B   can be measured with the same precision not limited by syst. Milestone : First leptonic decay seen on B meson SuperB (+) systematically limited BR(B → τ ν) = (0.85 ± 0.13)10 -4 SM expectation First test can be done, not yet precise

10. Radiative B decays - many measurements on B  s  - measurements of Br on B   - measurement of A CP on exclusive and inclusive modes Significant improvement on b  d  A CP in inclusive decay at ~0.5% ! (SM~0.5%) -Measurements of Br done -We start to perform A FB measur. CP and FB asymetries in sll exclusive and inclusive decays at few per cent (+) systematically limited(*) theoretically limited SuperB

11. Could the SuperB be a Super Flavour Factory ? Which is the interest ?

12. Charm physics at threshold D decay form factor and decay constant @ 1% Dalitz structure useful for  measurement 0.2 ab -1 Rare decays FCNC down to 10 -8 Consider that running 1 month at threshold we will collect 500 times the stat. of CLEO-C  ~1%, exclusive V ub ~ few % syst. error on  from Dalitz Model <1 o D mixing CP Violation in mixing should be now better addressed String dynamics and CKM measurements Charm physics using the charm produced at  (4S) Charm Physics Better studied using the high statistics collected at  (4S) @threshold(4GeV) HFAG preliminary (talk of David Asner Ikaros Bigi )

13. * Integrated quantities A SL and A CH at less than 0.5% Even a run at 1ab -1 will give less 1% error. Run at the  (5S) Possible with the same luminosity BB from B*B produced in C=+1 after B  B  decay  some sensitivity to S term in time integrated CP asym. BdBdBdBd B d *B d B d *B d * BsBsBsBs B s *B s B s *B s * B d,B + produced with factor 6 less than at  (4S) Dominated contribution ~95% For more details see E. Baracchini et al. hep-ph/0703258 * B d (B + ) and B s are produced and can be separated (talk of Francesco Renga)

14. In summary.. 1)superb measurements related to tree level/ ~tree level (some depending upon LCQD calculations )  (DK), V ub /V cb  2) superb measurements very sensitive to NP Physics sin(2  ) (Peng.) A FB (X s l + l - ), A FB (K*  ), A CP (K*  ), A CP (s  ), A CP (s+d)  ) B  K (*), LFV    3) several quantities depending upon LCQD calculations If Lattice QCD Calculations improve as the related experimental quantities, these measurements will be extremely powerfull Br(B  ( ,  ) Br(B  l ), Br(B  D  ) 4) <1% UT Fits for New Physics search (all the measurements mentioned before + others..) 5) charm measurements 6) Specific run at the  (5S)

15. 2 – 3%4 - 5%5.5 - 6.5%11% 3 – 4%---- 13% 0.5% (5% on 1-  ) 1.2% (13% on 1-  ) 2% (21% on 1-  ) 4% (40% on 1-  )  B → D/D*lν 0.5 – 0.8 % (3-4% on ξ-1) 1.5 - 2 % (9-12% on ξ-1) 3% (18% on ξ-1) 5% (26% on ξ-1) ξ 1 – 1.5%3 - 4%4 - 5%13% 1 – 1.5%2.5 - 4.0%3.5 - 4.5%14%fBfB 1%3%5%11%  0.1% (2.4% on 1-f + ) 0.4% (10% on 1-f + ) 0.7% (17% on 1-f + ) 0.9% (22% on 1-f + ) 1-10 PFlop Year 60 TFlop Year 6 TFlop Year Current lattice error Hadronic matrix element Estimates of error for 2015

16. Phenomenological Impact

17.  = 0.163 ± 0.028  = 0.344± 0.016 about 10 times better (not all measurements yet included…)  = ± 0.0028  = ± 0.0024 SuperB+Lattice improvements In SM Today

18. The problem of particle physics today is : where is the NP scale  ~ 0.5, 1…10 16 TeV The quantum stabilization of the Electroweak Scale suggest that  ~ 1 TeV LHC will search on this range What happens if the NP scale is at 2-3..10 TeV …naturalness is not at loss yet… Flavour Physics explore also this range We want to perform flavour measurements such that : - if NP particles are discovered at LHC we are able flavour structure of the NP to study the flavour structure of the NP NP scale - we can explore NP scale beyond the LHC reach

19. Two crucial questions : Can NP be flavour blind ? Can we define a “worst case” scenario No : NP couples to SM which violates flavour Yes : the class of model with Minimal Flavour Violation (MFV), namely : no new sources of flavour and CP violation and so : NP contributions governed by SM Yukawa couplings. Today  (MFV) > 2.3  0 @95C.L. NP masses >200GeV SuperB  (MFV) >~6  0 @95C.L. NP masses >600GeV As soon as you move from the worst case scenario…

20. Higgs-mediated NP in MFV at large tan  Similar formula in MSSM. M H (TeV) tan  2ab -1 M H ~0.4-0.8 TeV for tan  ~30-60 SuperB M H ~1.2-2.5 TeV for tan  ~30-60 B  Dl Similar to B   B  l Excl. 2 

21. In the red regions the  are measured with a significance >3  away from zero 1 10 g s b b s ~ ~ ~ New Physics contribution (2-3 families) With the today precision we do not have 3  exclusion 1 10 -1 10 -2 In this case the main constraints are b  s  ACP(b  s  ) Today we would have magenta contour covering all the space ACP magenta Br(sg) green Br(sll) cyan All constr. blue MSSM+generic soft SUSY breaking terms Flavour-changing NP effects in the squark propagator  NP scale SUSY mass  flavour-violating coupling

22. Re (  d 13 ) LL vs Im (  d 13 ) LL with present disagreement Constraint from  m d Constraint from sin2  cos2  Constraint from sin2  All constraints Re (  d 13 ) LL vs Im (  d 13 ) LL superB if disagreement disapper. SM Due to the actual disagreement between V ub and sin2  we see a slight hint of new physics NP at high significance ! NP scale at 350 GeV

23.  = 350 GeV

24. These evaluations do not agree with those given in SuperKEKB : discussion undergoing LVF and Littlest Higgs Model LFV from CKM 10 7 BR (    M 1/2 SuperB LFV from PMNS

25. SFF can perform many measurements at <1% level of precision Precision on CKM parameters will be improved by more than a factor 10 NP will be studied (measuring the couplings) if discovered at LHC if NP is not seen at the TeV by LHC, SFF is the way of exploring NP scales of the several TeV (in some scenario several (>10 )TeV..) Summary … and do not forget… SFF is also a Super-Super  -charm factory… Adjusting the central values so that they are all compatible Keeping the central values as measured today with errors at the SuperB

26. BACKUP MATERIAL

27. Br ~ |V ub | 2 in a limited space phase region… Using Babar E l, (X s  ElEl Progress on V ub.. Inclusive : improving analyses and improving the control of the theory vs cuts untagged analysis is the most precise Exclusive : we start to have quite precise analysis of Br vs q 2 Important that we measure at high q 2 where Lattice QCD calculates better. B   l B  X u l Confirming disagreement…

28. Precision measurements of |V cb | limiting factor F(1) Inclusive V cb still progress… BaBar/CLEO/CDF/DELPHI Kinetic scheme here we extract : B  D*l Essential point is to control /“measure” the effects of strong interaction Same for exclusive.. Study on charm sector help in the understanding of strong dynamics (Babar) Events/0.5

29. Rare decays : SuperB can cover all channels mentionned but B s   Unless we perform a long run at the U5S CP asymetries in radiative exclusive and inclusive decays at a fraction of 1% B   at 4% CP and FB asymetries in sll exclusive and inclusive decays at few per cent B   at 5% 13% 2fb1 Only bb back. Linear fit Transv amplit. ?? 18% for 50ab-1 in Jeff

30. 5 new free parameters C s,  s B s mixing C d,  d B d mixing C  K K mixing Today : fit possible with 10 contraints and 7 free parameters (   C d,  d,C s,  s, C  K ) Constraints Parametrizing NP physics in  F=2 processes  F=2 Fit in a NP model independent approach  CdCd dd C s ss CKCK  D  X V ub /V cb XX mdmd XX ACP  J  X X ASLXX  XX ACHXXXX  s  s XX msms X KK XX In future : ACP  J  ~XX ASL(Bs) XX  D s K) X Tree processes 1  3 family 2  3 family 1  2 familiy No new physics C=1  =0

31. Model Indep. Analysis in  B=2 C = 1.24 ± 0.43  = (-3.0 ± 2.0) o C = ± 0.031  = (± 0.5) o

32. Bit more on B s C(Bs) ~ 0.026  Bs) ~ 1.9 o Today at Superb

33.  m d magenta A SL green  cyan All constr. blue New Physics contribution (1-3 families) 1 10 1 10 -1 |  13 | LL Example on how NP parameters can be measured Today SuperB In the red regions the  are measured with a significance >3  away from zero With the today precision we do not have 3  exclusion

34. SuperB will probe up to >100 TeV for arbitrary flavour structure! Let’s be more quantitative How to read this table, two examples. At the SuperB we can set a limit on the coupling at The natural coupling would be 1 we can test scale up to All this number are a factor ~10 better than the present ones