kaons and long distance meson mixing from lattice qcd
play

Kaons and long-distance meson mixing from lattice QCD Stephen R. - PowerPoint PPT Presentation

Kaons and long-distance meson mixing from lattice QCD Stephen R. Sharpe University of Washington S. Sharpe, Kaons & long-distance meson mixing 3/7/14 @ Lattice meets Experiment 2014, FNAL 1 /34 Friday, March 7, 14 Based partly on


  1. Kaons and long-distance meson mixing from lattice QCD Stephen R. Sharpe University of Washington S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 1 /34 Friday, March 7, 14

  2. Based partly on 2013 white paper www.usqcd.org/documents/13flavor.pdf S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 2 /34 Friday, March 7, 14

  3. Based partly on 2013 white paper Very helpful input from experimentalists and phenomenologists! S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 3 /34 Friday, March 7, 14

  4. Master Formula Expt = (CKM)(pQCD)(non-pert QCD) + BSM(non-pert QCD) LQCD provides first-principles method to calculate (some) non-perturbative QCD matrix elements S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 4 /34 Friday, March 7, 14

  5. Outline Standard vs non-standard/novel/new lattice calculations Results for standard quantities Results & prospects for new quantities K →ππ decays Δ M K (long distance) K →πνν and other rare decays D →ππ , D → KK and D-Dbar mixing Summary & Outlook S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 5 /34 Friday, March 7, 14

  6. Standard vs non - standard quantities Standard means matrix elements involving single particles d ⇒ f K2 (similarly f π , f D , f B ) A μ A μ s d ⇒ K →π form factor A μ A μ s u (similarly B → D, etc) J μ S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 6 /34 Friday, March 7, 14

  7. Standard vs non - standard quantities Standard means matrix elements involving single particles d H W ⇒ B K (similarly B D , B B ) A μ A μ s Nearly 20 standard matrix elements are fully controlled with small errors Decay constants: f π , f K , f D , f Ds , f B , f Bs Form factors: K →π , D → K, D →π , B → D, B → D * , B s → D s & B →π Mixing matrix elements: B K , B B , B Bs S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 7 /34 Friday, March 7, 14

  8. Standard vs non - standard quantities Non-standard: matrix elements involving two or more particles A μ ⇒ K →ππ (I=2) u d A μ d s u H W A μ S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 8 /34 Friday, March 7, 14

  9. Standard vs non - standard quantities Non-standard: matrix elements involving two or more particles and/or quark-disconnected contributions A μ ⇒ K →ππ (I=0) u d H W d A μ s u A μ S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 9 /34 Friday, March 7, 14

  10. Standard vs non - standard quantities Non-standard: matrix elements involving two or more particles and/or quark-disconnected contributions A μ ⇒ K →ππ (I=0) d H W d A μ s u u A μ S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 10 /34 Friday, March 7, 14

  11. Standard vs non - standard quantities Non-standard: matrix elements involving two or more particles and/or quark-disconnected contributions and/or two insertions of H W u d H W d H W A μ A μ s ⇒ Long distance part of Δ M K S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 11 /34 Friday, March 7, 14

  12. Standard vs non - standard quantities Non-standard: matrix elements involving two or more particles and/or quark-disconnected contributions and/or two insertions of H W u u H W d H W A μ A μ s ⇒ Long distance part of Δ M K S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 12 /34 Friday, March 7, 14

  13. Outline Standard vs non-standard/novel/new lattice calculations Results for standard quantities Results & prospects for new quantities K →ππ decays Δ M K (long distance) K →πνν and other rare decays D →ππ , D → KK and D-Dbar mixing Summary & Outlook S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 13 /34 Friday, March 7, 14

  14. Status of f K /f π FLAG 2013 (arXiv:1310.8555) 0.4% error (really 2% on difference from 1) ⇒ | V us | = 0 . 2256(3) exp (2 − 4) EM (10) lat (1) V ud Further lattice improvement underway, but will eventually require inclusion of EM effects. This is not easy since axial current not EM gauge invariant. S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 14 /34 Friday, March 7, 14

  15. Status of K → π form factor FLAG 2014 (preliminary) f + (0) = 0 . 9661(32) ( N f = 2 + 1) 0.3% error [really 10% on f + (0) − 1] ⇒ | V us | = 0 . 2239(5) exp (2) EM (7) lat Lattice errors will be reduced using physical light-quark masses (underway) “EM wall” not far away S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 15 /34 Friday, March 7, 14

  16. Status of B K FLAG 2013 (arXiv:1310.8555) 1.3% error Can be further improved, but already other errors dominate when using B K in unitarity triangle analysis (V cb , long distance in ε K , PT errors) S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 16 /34 Friday, March 7, 14

  17. Reasons for future improvement Steadily improve calculations of standard matrix elements, in particular using: Physical light-quark masses Isospin breaking & EM effects Charmed sea Finer lattice spacings & improved actions (heavy quarks) Improved statistical errors Improved methods of normalizing operators (e.g. SMOM) Already in use for some quantities, will soon become widespread S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 17 /34 Friday, March 7, 14

  18. Expanding portfolio of standard quantities Contributions of BSM physics to K (and D & B) mixing B → K l + l - , Λ b →Λ l + l - and related form factors Tensor form factors for K →π ; needed to constrain BSM theories Others? Can achieve few-10% accuracy on few year timescale, which is commensurate with experimental program, and significantly enhances search for BSM physics S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 18 /34 Friday, March 7, 14

  19. Outline Standard vs non-standard/novel/new lattice calculations Results for standard quantities Results & prospects for new quantities K →ππ decays Δ M K (long distance) K →πνν and other rare decays D →ππ , D → KK and D-Dbar mixing Summary & Outlook S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 19 /34 Friday, March 7, 14

  20. K → ππ (I =2 ) decay amplitudes [RBC/UKQCD arXiv:1111.1699, 1206.5142, 1311.3844(Lattice 2013) ] First controlled result for an amplitude involving two particles Isospin 2 ⇒ no quark-disconnected contributions Uses physical kinematics (physical quark masses, moving pions so M K =2E π ) which requires box with L ≈ 5.5 fm Original result at a ≈ 0.14 fm; two new (prelim.) results at a ≈ 0.12 & 0.9 fm, allowing continuum extrapolation Systematic error now ≈ 11% (down from 19%); statistical errors 1-2% A μ u d A μ d s u H W A μ S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 20 /34 Friday, March 7, 14

  21. ππ (I =2 ) phase shi fu [RBC/UKQCD arXiv:1111.1699, 1206.5142] Auxiliary calculation needed to make finite volume correction (few % effect) First calculation of phase shift with physical quark masses u Lattice I=2 Experiment phase shift S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 21 /34 Friday, March 7, 14

  22. Comparison with experiment Lattice Results (2012) [RBC/UKQCD arXiv:1111.1699, 1206.5142] expt. 1.479(4) 10 − 8 [K + ] Re A 2 =1.38 (5) stat (26) syst 10 − 8 GeV 1.57(6) 10 − 8 [K S ] New information! Im A 2 = − 6.5 (5) stat (12) syst 10 − 13 GeV Can use with expt result for ε ’ to determine Im A 0 Present lattice errors about half this size [arXiv:1311.3844; RBC/UKQCD article in progress] S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 22 /34 Friday, March 7, 14

  23. K → ππ (I =0 ) amplitude & Δ I =1 / 2 rule I=0 involves disconnected contractions ⇒ numerics much more challenging Several other technical challenges too. Fermions with chiral symmetry essential. Pilot calculation in 2012: decay at threshold for M K ~660, 880MeV [RBC/UKQCD arXiv:1212.1474] Demonstrates that technology (& related theory) exists. Statistical errors ~ 15%. u A μ A μ d d H W H W d d A μ A μ s s u u u A μ A μ S. Sharpe, “Kaons & long-distance meson mixing” 3/7/14 @ Lattice meets Experiment 2014, FNAL 23 /34 Friday, March 7, 14

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend