logging in or signing up 03Hou Elodie Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINTLite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: (To copy code, click on the text box) Embed: URL: Thumbnail: WordPress Embed Customize Embed The presentation is successfully added In Your Favorites. Views: 35 Category: Entertainment License: All Rights Reserved Like it (0) Dislike it (0) Added: January 05, 2008 This Presentation is Public Favorites: 0 Presentation Description No description available. Comments Posting comment... Premium member Presentation Transcript Slide1: July 19, 2003 HEP2003, Aachen Indications for Large Rescatterings in Rare B DecaysOutline: Motivation Ansatz: (PP) Multimode Fit (Generalized) Factorization ⊕ Rescattering Phases Two Scenarios ― Driven by & Conclusion/Discussion Outline SU(3) Formalism: 8 ⊗ 8 → 8 ⊗ 8 RescatteringI. Motivation: I. Motivation History Kp/pp Large: Need for Large g [He-WSH-Yang ’99] and Factorization Works!I. Motivation: I. Motivation History Kp/pp Large: Need for Large g [He-WSH-Yang ’99]I. Motivation: I. Motivation Final State Isospin Decomposition History Kp/pp Large: Need for Large g [He-WSH-Yang ’99] Speculation: Rate/aCP Pattern (late ’99 Data) Rescattering ? [WSH-Yang ’00] In Principle Present Slide6: Can Shift Rate/CP Pattern —— esp. CPV Slide7: D: Dispersive A: Absorptive CP asymmetry needs ➀ ∃ A ⇒ CP-Inv. Phase [Strong Int.] ➁ ∃ Phase Difference btwn D & A ⇒ CP-Viol. Phase [Weak Int.] Mechanism for CP Violating Rate Asymmetries e.g. for b → s Complex CKM Matrix Elements I. Motivation: I. Motivation History Kp/pp Large: Need for Large g [He-WSH-Yang ’99] Speculation: Rate/DCP Pattern (late ’99) Rescattering? [WSH-Yang ’00] Present (Impact of B Factories!) 2001: D⁰h⁰ Discovery ― Large (Rescatt.?) [Chua-WSH-Yang ’02] K¯p⁺/K¯p⁰ DCPV: Sign p⁰p⁰ Hint Enigma Belle/CLEO; BaBar 2003 Revisit RescatteringSlide9: II. Ansatz: Multimode Fit ⊕ FSI Phases Naïve Factorization ⊗ Final State Rescattering Quasi-Elastic Inelastic Phases “Cancel” Gerard-WSH; Suzuki-Wolfenstein Otherwise Double Counting SpecialSlide10: B → PP Only: VP Unsettled (VV More So) P : 8 of SU(3), ∴ PP → PP FSI Rescattering i.e., 8 ⊗ 8 = 1⊕8⊕8⊕10⊕27 Symmetric TWO Physical Phase Difference: [Extend from D⁰h⁰ 3 ⊗ 8 → 3 ⊗ 8 Formalism] Unable to Treat 1, i.e. 1 ⊗ 8 ~ ηʹK etc. (η₁), Will take η ≃ η₈Slide11: Heuristic Picture SU(3) Correspondence Π ≡ P Slide12: δSlide13: δ,σ N.B. 1. 2. σ Arise from Combo Only Slide14: Heuristic Picture SU(3) Correspondence Π ≡ P Fit: à la WSH-Smith-Würthwein: Fit: à la WSH-Smith-Würthwein Inputs: Fit Parameters Output: Fitted Rates Crosscheck Reasonableness hep-ex/9910014Slide16: Large FSI Phases ! What Drives Them? “World Average” Not Good Less Good > > > > > > > > > >Slide17: Settle δ between themselves N.B. Disfavors sinδ<0 Correct Sign w/ RescatteringSlide18: Settle δ between themselves N.B. Disfavors sinδ<0 Correct Sign w/ RescatteringSlide19: N.B. Treating limits as Gaussian is Wrong. K-K+ Mode Can Be Small Slide20: Determine σ between each other (& KK) δ= δ(Fit)Slide22: δ= δ(Fit) Not Used in Fit Weak σ dep. Fit 1 ~ 99˚ Fit 2 = 60˚ Strong ϕ₃ dep.Slide23: Not Used in Fit Fit 2 = 60˚ Fit 1 ~ 96˚ δ= δ(Fit) Weak σ dep. δ= δ(Fit) Strong g/ϕ₃ dep.Slide24: Varied Landscape ! Flat forδ-σin First Quadrant III. Two Scenarios ― Driven by : III. Two Scenarios ― Driven by Otherwise, Difference is marginal except, Scenario 1 Better Fit Scenario 2 gives - Too Small p¯p⁰ ! (3σ) - Utilize Smaller F.F. … But Maybe Belle’s Right ? Discussion: Discussion In Past Two Years K¯p⁺/K¯p⁰ aCP: Sign p⁰p⁰ Hint App, Spp Enigma Large Color Suppressed D⁰h⁰ Rescattering? Two (Sizable) FSI Phases Improve Understanding it feels real … Should be Clarified Soon by DataConclusion: Conclusion N.B. Treatment of FSI SU(3) Phases as “Parameters”. You do not have the permission to view this presentation. In order to view it, please contact the author of the presentation.
03Hou Elodie Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINTLite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: (To copy code, click on the text box) Embed: URL: Thumbnail: WordPress Embed Customize Embed The presentation is successfully added In Your Favorites. Views: 35 Category: Entertainment License: All Rights Reserved Like it (0) Dislike it (0) Added: January 05, 2008 This Presentation is Public Favorites: 0 Presentation Description No description available. Comments Posting comment... Premium member Presentation Transcript Slide1: July 19, 2003 HEP2003, Aachen Indications for Large Rescatterings in Rare B DecaysOutline: Motivation Ansatz: (PP) Multimode Fit (Generalized) Factorization ⊕ Rescattering Phases Two Scenarios ― Driven by & Conclusion/Discussion Outline SU(3) Formalism: 8 ⊗ 8 → 8 ⊗ 8 RescatteringI. Motivation: I. Motivation History Kp/pp Large: Need for Large g [He-WSH-Yang ’99] and Factorization Works!I. Motivation: I. Motivation History Kp/pp Large: Need for Large g [He-WSH-Yang ’99]I. Motivation: I. Motivation Final State Isospin Decomposition History Kp/pp Large: Need for Large g [He-WSH-Yang ’99] Speculation: Rate/aCP Pattern (late ’99 Data) Rescattering ? [WSH-Yang ’00] In Principle Present Slide6: Can Shift Rate/CP Pattern —— esp. CPV Slide7: D: Dispersive A: Absorptive CP asymmetry needs ➀ ∃ A ⇒ CP-Inv. Phase [Strong Int.] ➁ ∃ Phase Difference btwn D & A ⇒ CP-Viol. Phase [Weak Int.] Mechanism for CP Violating Rate Asymmetries e.g. for b → s Complex CKM Matrix Elements I. Motivation: I. Motivation History Kp/pp Large: Need for Large g [He-WSH-Yang ’99] Speculation: Rate/DCP Pattern (late ’99) Rescattering? [WSH-Yang ’00] Present (Impact of B Factories!) 2001: D⁰h⁰ Discovery ― Large (Rescatt.?) [Chua-WSH-Yang ’02] K¯p⁺/K¯p⁰ DCPV: Sign p⁰p⁰ Hint Enigma Belle/CLEO; BaBar 2003 Revisit RescatteringSlide9: II. Ansatz: Multimode Fit ⊕ FSI Phases Naïve Factorization ⊗ Final State Rescattering Quasi-Elastic Inelastic Phases “Cancel” Gerard-WSH; Suzuki-Wolfenstein Otherwise Double Counting SpecialSlide10: B → PP Only: VP Unsettled (VV More So) P : 8 of SU(3), ∴ PP → PP FSI Rescattering i.e., 8 ⊗ 8 = 1⊕8⊕8⊕10⊕27 Symmetric TWO Physical Phase Difference: [Extend from D⁰h⁰ 3 ⊗ 8 → 3 ⊗ 8 Formalism] Unable to Treat 1, i.e. 1 ⊗ 8 ~ ηʹK etc. (η₁), Will take η ≃ η₈Slide11: Heuristic Picture SU(3) Correspondence Π ≡ P Slide12: δSlide13: δ,σ N.B. 1. 2. σ Arise from Combo Only Slide14: Heuristic Picture SU(3) Correspondence Π ≡ P Fit: à la WSH-Smith-Würthwein: Fit: à la WSH-Smith-Würthwein Inputs: Fit Parameters Output: Fitted Rates Crosscheck Reasonableness hep-ex/9910014Slide16: Large FSI Phases ! What Drives Them? “World Average” Not Good Less Good > > > > > > > > > >Slide17: Settle δ between themselves N.B. Disfavors sinδ<0 Correct Sign w/ RescatteringSlide18: Settle δ between themselves N.B. Disfavors sinδ<0 Correct Sign w/ RescatteringSlide19: N.B. Treating limits as Gaussian is Wrong. K-K+ Mode Can Be Small Slide20: Determine σ between each other (& KK) δ= δ(Fit)Slide22: δ= δ(Fit) Not Used in Fit Weak σ dep. Fit 1 ~ 99˚ Fit 2 = 60˚ Strong ϕ₃ dep.Slide23: Not Used in Fit Fit 2 = 60˚ Fit 1 ~ 96˚ δ= δ(Fit) Weak σ dep. δ= δ(Fit) Strong g/ϕ₃ dep.Slide24: Varied Landscape ! Flat forδ-σin First Quadrant III. Two Scenarios ― Driven by : III. Two Scenarios ― Driven by Otherwise, Difference is marginal except, Scenario 1 Better Fit Scenario 2 gives - Too Small p¯p⁰ ! (3σ) - Utilize Smaller F.F. … But Maybe Belle’s Right ? Discussion: Discussion In Past Two Years K¯p⁺/K¯p⁰ aCP: Sign p⁰p⁰ Hint App, Spp Enigma Large Color Suppressed D⁰h⁰ Rescattering? Two (Sizable) FSI Phases Improve Understanding it feels real … Should be Clarified Soon by DataConclusion: Conclusion N.B. Treatment of FSI SU(3) Phases as “Parameters”.