1. 111 Indirect Search for New Dynamics –by Cunning CERN, Nov. 2011 Ikaros Bigi (Notre Dame du Lac) Ikaros Bigi: “ND by Cunning”

2. 222 Indirect Search for New Dynamics –by Cunning CERN, Nov. 2011 Ikaros Bigi (Notre Dame du Lac) Ikaros Bigi: “ND by Cunning” Motto for a Workshop: One should not give a lie!

3. 333 Indirect Search for New Dynamics –by Cunning CERN, Nov. 2011 Ikaros Bigi (Notre Dame du Lac) Ikaros Bigi: “ND by Cunning” Motto for a Workshop: One should not give a lie! No problem for an experimentalist -- they talk about empirical facts --

4. 444 Indirect Search for New Dynamics –by Cunning CERN, Nov. 2011 Ikaros Bigi (Notre Dame du Lac) Ikaros Bigi: “ND by Cunning” Motto for Workshop: One should not give a lie! No problem for an experimentalist -- they talk about empirical facts -- yet for a theorist?

5. 555 Indirect Search for New Dynamics –by Cunning CERN, Nov. 2011 Ikaros Bigi (Notre Dame du Lac) Ikaros Bigi: “ND by Cunning” Motto for Workshop: One should not give a lie! No problem for an experimentalist -- they talk about empirical facts -- yet for a theorist? Prof. Mannelli from Pisa once assured me that he does not entertain the illusion that theorists can speak the truth all the time -- speaking in good faith is all he expects from a theorist!

6. 666 Indirect Search for New Dynamics –by Cunning CERN, Nov. 2011 Ikaros Bigi (Notre Dame du Lac) Ikaros Bigi: “ND by Cunning” Motto Workshop: One should not give a lie! No problem for an experimentalist -- they talk about empirical facts -- yet for a theorist? Prof. Mannelli from Pisa once assured me that he does not entertain the illusion that theorists can speak the truth all the time -- speaking in good faith is all he expects from a theorist! I will do it.

7. 777 Indirect Search for New Dynamics –by Cunning CERN, Nov. 2011 Ikaros Bigi (Notre Dame du Lac) Ikaros Bigi: “ND by Cunning” Motto for Workshop: One should not give a lie! No problem for an experimentalist -- they talk about empirical facts -- yet for a theorist? Prof. Mannelli from Pisa once assured me that he does not entertain the illusion that theorists can speak the truth all the time -- speaking in good faith is all he expects from a theorist! I will do it. [Remember: prediction ≠ postdiction!]

8. 888 Ikaros Bigi: “ND by Cunning” Theorist enthralled by Beauty & Charm

9. 999 Ikaros Bigi: “ND by Cunning” Theorist enthralled by Beauty & Charm

10. 10 Ikaros Bigi: “ND by Cunning” Theorist enthralled by Beauty & Charm

11. 11 Ikaros Bigi: “ND by Cunning” Theorist enthralled by Beauty & Charm minor asymmetry enhances their beauty & charm

12. 12 Ikaros Bigi: “ND by Cunning” Theorist enthralled by Beauty & Charm minor asymmetry enhances their beauty & charm

13. 13 Ikaros Bigi: “ND by Cunning” Theorist enthralled by Beauty & Charm minor asymmetry enhances their beauty & charm

14. 14 Ikaros Bigi: “ND by Cunning” Theorist enthralled by Beauty & Charm CP asymmetry enhances Beauty & Charm decays!

15. 15 Ikaros Bigi: “ND by Cunning” CKM dynamics has been found at least as the leading source of the observed CPV in  S ≠ 0 ≠  B dynamics

16. 16 Ikaros Bigi: “ND by Cunning” CKM dynamics has been found at least as the leading source of the observed CPV in  S ≠ 0 ≠  B dynamics the goal is to find impact of New Dynamics (ND) on CP asymmetries in  B ≠ 0 ≠  C ( & in  t ≠ 0);

17. 17 Ikaros Bigi: “ND by Cunning” CKM dynamics has been found at least as the leading source of the observed CPV in  S ≠ 0 ≠  B dynamics the goal is to find impact of New Dynamics (ND) on CP asymmetries in  B ≠ 0 ≠  C ( & in  t ≠ 0); indirect CP: establish in 2 transitions & find in 3 rd back-up one

18. 18 Ikaros Bigi: “ND by Cunning” CKM dynamics has been found at least as the leading source of the observed CPV in  S ≠ 0 ≠  B dynamics the goal is to find impact of ND on CP asymmetries in  B ≠ 0 ≠  C ( & in  t ≠ 0); indirect CP: establish in 2 transitions & find in 3 rd back-up one direct CP: find & establish it in many channels as possible

19. 19 Ikaros Bigi: “ND by Cunning” CKM dynamics has been found at least as the leading source of the observed CPV in  S ≠ 0 ≠  B dynamics the goal is to find impact of ND on CP asymmetries in  B ≠ 0 ≠  C ( & in  t ≠ 0); indirect CP: establish in 2 transitions & find in 3 rd back-up one direct CP: find & establish it in many channels as possible  existence of ND &

20. 20 Ikaros Bigi: “ND by Cunning” CKM dynamics has been found at least as the leading source of the observed CPV in  S ≠ 0 ≠  B dynamics the goal is to find impact of ND CP asymmetries in  B ≠ 0 ≠  C ( & in  t ≠ 0); indirect CP: establish in 2 transitions & find in 3 rd back-up one direct CP: find & establish it in many channels as possible  existence of ND &  find out its shape & nature

21. 21 Ikaros Bigi: “ND by Cunning” Status  indir. & direct CPV established in 2-body final states for B d ;

22. 22 Ikaros Bigi: “ND by Cunning” Status  indir. & direct CPV established in 2-body final states for B d ;  indir. & direct CPV unclear in 2-body final states for B s ;

23. 23 Ikaros Bigi: “ND by Cunning” Status  indir. & direct CPV established in 2-body final states for B d ;  indir. & direct CPV unclear in 2-body final states for B s ; for SL transitions D0 showed on June 30, 2011: a SL (B d )| D0 =(-0.12 ± 0.52)x10 -2, a SL (B s )| D0 =(-1.81 ± 1.06)x10 -2

24. 24 Ikaros Bigi: “ND by Cunning” Status  indir. & direct CPV established in 2-body final states for B d ;  indir. & direct CPV unclear in 2-body final states for B s ; for SL transitions D0 showed on June 30, 2011: a SL (B d )| D0 =(-0.12 ± 0.52)x10 -2, a SL (B s )| D0 =(-1.81 ± 1.06)x10 -2 with input from LHCb satisfies Bell-Steinberger-Berger- Sehgal bound just unitary bound monotonicity of oscillations = `time not running backward’ D0 old LHCb

25. 25 Ikaros Bigi: “ND by Cunning” Status  indir. & direct CPV established in 2-body final states for B d ;  precision!  indir. & direct CPV unclear in 2-body final states for B s ;  precision!

26. 26 Ikaros Bigi: “ND by Cunning” Status  indir. & direct CPV established in 2-body final states for B d ;  precision!  indir. & direct CPV unclear in 2-body final states for B s ;  precision!  no indir. & dir. CPV found in 2-body final states in D decays

27. 27 Ikaros Bigi: “ND by Cunning” Status  indir. & direct CPV established in 2-body final states for B d ;  precision!  indir. & direct CPV unclear in 2-body final states for B s ;  precision!  no indir. & dir. CPV found in 2-body final states in D decays  accuracy & complementarity!

28. 28 Ikaros Bigi: “ND by Cunning” the goal is to find ND –

29. 29 Ikaros Bigi: “ND by Cunning” the goal is to find ND --  its existence &

30. 30 Ikaros Bigi: “ND by Cunning” the goal is to find ND --  its existence &  its (their ?) nature(s) & shape(s)!

31. 31 Ikaros Bigi: “ND by Cunning” the goal is to find ND --  its existence &  its (their ?) nature(s) & shape(s)! When the presence of ND has established, you want to find its features – CPV ~ S x P or V x A etc.

32. 32 Ikaros Bigi: “ND by Cunning” the goal is to find ND --  its existence &  its (their ?) nature(s) & shape(s)! When the presence of ND has established, you want to find its features – CPV ~ S x P or V x A etc.  Dalitz analyses of CKM suppr. 3-body transitions D/B (s) vs. D/B (s)  KK  K  etc. will help greatly,

33. 33 Ikaros Bigi: “ND by Cunning” the goal is to find ND --  its existence &  its (their ?) nature(s) & shape(s)! When the presence of ND has established, you want to find its features – CPV ~ S x P or V x A etc.  Dalitz analyses of CKM suppr. 3-body transitions D/B (s) vs. D/B (s)  KK  K  etc. will help greatly,  probably importantly so!

34. 34 Ikaros Bigi: “ND by Cunning” the goal is to find ND –

35. 35 Ikaros Bigi: “ND by Cunning” the goal is to find ND – like a criminal case where you did not see two witnesses at the crime:

36. 36 Ikaros Bigi: “ND by Cunning” the goal is to find ND – like a criminal case where you did not see two witnesses at the crime: No golden test of flavour dynamics -- you have to rely on a series of several arguments with correlations!

37. 37  A Catholic Scenario for B/D  PPP: single path to heaven - asymmetries in the Dalitz plot Ikaros Bigi: “ND by Cunning”

38. 38  A Catholic Scenario for B/D  PPP: single path to heaven - asymmetries in the Dalitz plot  can rely on relative rather than absolute CP asym much less dependent on production asym. Ikaros Bigi: “ND by Cunning”

39. 39  A Catholic Scenario for B/D  PPP: single path to heaven - asymmetries in the Dalitz plot  can rely on relative rather than absolute CP asym much less dependent on production asym. need  lots of statistics Ikaros Bigi: “ND by Cunning”

40. 40  A Catholic Scenario for B/D  PPP: single path to heaven - asymmetries in the Dalitz plot  can rely on relative rather than absolute CP asym much less dependent on production asym. need  lots of statistics robust pattern recognition Ikaros Bigi: “ND by Cunning”

41. 41  A Catholic Scenario for B/D  PPP: single path to heaven - asymmetries in the Dalitz plot  can rely on relative rather than absolute CP asym much less dependent on production asym. need  lots of statistics robust pattern recognition `Miranda’ procedure pattern recognition learnt from astronomers Bediaga et al.:`significance’ [N(i)–N(i)]/[N(i)+N(i)] 1/2 Ikaros Bigi: “ND by Cunning”

42. 42 Ikaros Bigi: “ND by Cunning” 42 Formalism of Dalitz plots

43. 43 Ikaros Bigi: “ND by Cunning” 43 Formalism of Dalitz plots DP depend on |T(3P)| 2 vs. |T(3P)| 2, weak & strong phases Analyze the topologies of Dalitz plots

44. 44 Ikaros Bigi: “ND by Cunning” 44 Formalism of Dalitz plots DP depend on |T(3P)| 2 vs. |T(3P)| 2, weak & strong phases Analyze the topologies of Dalitz plots  like an analysis without theoretical input for an immediate process: significance s(i) =[N(i)–N(i)]/[N(i)+N(i)] 1/2

45. 45 Ikaros Bigi: “ND by Cunning” 45 Formalism of Dalitz plots DP depend on |T(3P)| 2 vs. |T(3P)| 2, weak & strong phases Analyze the topologies of Dalitz plots  like an analysis without theoretical input for an immediate process: significance s(i) =[N(i)–N(i)]/[N(i)+N(i)] 1/2  most CP asymmetries in the DP are independent of production asymmetries!

46. 46 theoretical guidance: B/D  PPP Ikaros Bigi: “ND by Cunning”

47. 47 theoretical guidance: B/D  PPP  chiral dynamics & FSI are not strengths of LQCD Ikaros Bigi: “ND by Cunning”

48. 48 theoretical guidance: B/D  PPP  chiral dynamics & FSI are not strengths of LQCD  from Hadron Physics/MEP often unused great experience for chiral dynam. & FSI – use for profit! Ikaros Bigi: “ND by Cunning”

49. 49 theoretical guidance: B/D  PPP  chiral dynamics & FSI are not strengths of LQCD  from Hadron Physics/MEP often unused great experience for chiral dynam. & FSI – use for profit!  working group of theorists & experimentalists founded by Hanhart,Mannel,Meissner,ibi to deal with CPV in Dalitz studies Name: `Les Nabis’ = `The Prophets’ ! Ikaros Bigi: “ND by Cunning”

50. 50 theoretical guidance: B/D  PPP  chiral dynamics & FSI are not strengths of LQCD  from Hadron Physics/MEP often unused great experience for chiral dynam. & FSI – use for profit!  working group of theorists & experimentalists founded by Hanhart,Mannel,Meissner,ibi to deal with CPV in Dalitz studies Name: `Les Nabis’ = `The Prophets’ ! CP Ikaros Bigi: “ND by Cunning”

51. 51 theoretical guidance: B/D  PPP  chiral dynamics & FSI are not strengths of LQCD  from Hadron Physics/MEP often unused great experience for chiral dynam. & FSI – use for profit!  working group of theorists & experimentalists founded by Hanhart,Mannel,Meissner,ibi to deal with CPV in Dalitz studies Name: `Les Nabis’ = `The Prophets’ ! CP: 3 sources  with quasi-2-body final states (resonances) Ikaros Bigi: “ND by Cunning”

52. 52 theoretical guidance: B/D  PPP  chiral dynamics & FSI are not strengths of LQCD  from Hadron Physics/MEP often unused great experience for chiral dynam. & FSI – use for profit!  working group of theorists & experimentalists founded by Hanhart,Mannel,Meissner,ibi to deal with CPV in Dalitz studies Name: `Les Nabis’ = `The Prophets’ ! CP: 3 sources  with quasi-2-body final states (resonances)  with interference between quasi-2-body final states Ikaros Bigi: “ND by Cunning”

53. 53 theoretical guidance: B/D  PPP  chiral dynamics & FSI are not strengths of LQCD  from Hadron Physics/MEP often unused great experience for chiral dynam. & FSI – use for profit!  working group of theorists & experimentalists founded by Hanhart,Mannel,Meissner,ibi to deal with CPV in Dalitz studies Name: `Les Nabis’ = `The Prophets’ ! CP: 3 sources  with quasi-2-body final states (resonances)  with interference between quasi-2-body final states  contributions from true 3-body FS or broad resonances like . Ikaros Bigi: “ND by Cunning”

54. 54 Ikaros Bigi: “ND by Cunning” One example: D/B d   +  -  0 D/B d  0  0,  +/-  -/+, f 0 (980)  0,  0 V+P, V+P, S+P, S+P BW, BW, ~ BW, not BW! BW = Breit-Wigner experience of HP/MEP very useful! 

55. 55  Need detailed analyses of 3- & 4-body final states, including CPV – despite the large start-up work! Ikaros Bigi: “ND by Cunning”

56. 56  Need detailed analyses of 3- & 4-body final states, including CPV – despite the large start-up work! Remember – finding the Devil on a fresco in the Basilica San Francesco in Assisi in Italy painted in the 14 th century took till now! Ikaros Bigi: “ND by Cunning”

57. 57  Need detailed analyses of 3- & 4-body final states, including CPV – despite the large start-up work!  Dalitz plots, T odd correlations Ikaros Bigi: “ND by Cunning”

58. 58  Need detailed analyses of 3- & 4-body final states, including CPV – despite the large start-up work!  Dalitz plots, T odd correlations  include progresses in hadron analyses  chiral dynamics etc., not only LQCD Ikaros Bigi: “ND by Cunning”

59. 59  Need detailed analyses of 3- & 4-body final states, including CPV – despite the large start-up work!  Dalitz plots, T odd correlations  include progresses in hadron analyses  chiral dynamics etc., not only LQCD Ikaros Bigi: “ND by Cunning” Observables Lagrangian

60. 60  Need detailed analyses of 3- & 4-body final states, including CPV – despite the large start-up work!  Dalitz plots, T odd correlations  include progresses in hadron analyses  chiral dynamics etc., not only LQCD Ikaros Bigi: “ND by Cunning” Observables Lagrangian

61. 61  Need detailed analyses of 3- & 4-body final states, including CPV – despite the large start-up work!  Dalitz plots, T odd correlations  include progresses in hadron analyses  chiral dynamics etc., not only LQCD Ikaros Bigi: “ND by Cunning” Observables Lagrangian theoretical technology ! “plumbers” (like me)

62. 62 Ikaros Bigi: “ND by Cunning” AchillesAias

63. 63 Ikaros Bigi: “ND by Cunning” Achilles = ATLAS Aias

64. 64 Ikaros Bigi: “ND by Cunning” Achilles = ATLAS Aias = CMS

65. 65 Ikaros Bigi: “ND by Cunning” Achilles = ATLAS Aias = CMS Odysseus = need force & lots of cunning of exp. & th.

66. 66 Ikaros Bigi: “ND by Cunning” Achilles = ATLAS Aias = CMS Odysseus = need force & lots of cunning of exp. & th. LHCb!

67. 67 Ikaros Bigi: “ND by Cunning”

68. 68 Ikaros Bigi: “ND by Cunning”

69. 69 Ikaros Bigi: “Odysseus conquering Troy” 69 theor. pre[post]dictions WA data  (  b )/  (B d ) `us’ 0.9 - 1.0 ’93 0.77 ± 0.05 ‘96 `us’ 0.94±0.03, >0.88 ’96,’98 0.79 ± 0.05 ‘99 `not us’ 0.86±0.05 ’03 0.806 ± 0.05 ’03 0.939 ± 0.022 ‘11 difference between prediction & postdiction!