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Recent Results in Hadronic Charm Decays

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36 diapositives · 479 Views · Sep 20, 2014

This presentation at the CIPANP 2003 conference highlighted key results and advancements in the field of hadronic charm decays. Notable discussions included new decay observations from CLEO-III, BaBar, and Belle experiments, in addition to theoretical insights offered by Harry Lipkin. Important measurements such as the first observation of X0_c decays and branching ratios for various charm baryons were also presented. Further emphasis was placed on the significance of charm quarks in particle physics, showcasing ongoing research and future prospects in this area.

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  1. Recent Results in Hadronic Charm Decays Mats Selen, University of Illinois2003 CIPANP, May 19-24, New York, NY

  2. I will NOT talk about Dsp0 Stay tuned for detailed experimental presentations:BaBar (Ray Cowan)CLEO (Jon Urheim)Belle (Tom Browder)plus a theoretical perspective from Harry Lipkin

  3. E791 The usual suspects CDF CLEO Belle FOCUS BaBar BES

  4. Charmed Baryons

  5. Phys.Lett.B523:53-59,2001 Charm Baryon Lifetimes Phys.Rev.Lett.88:161801,2002 Phys.Lett.B541:211-218,2002 Phys.Lett.B561:41-48,2003 Thanks to Kevin Stenson for summary figure

  6. L+cgLp+p+p-p0(Steve Blusk) CLEO-III Phys. Rev.D67:012001,2003 First Observation

  7. X0cg pK-K-p+(Basit Athar) 0cpKK 148 ± 18 ** Preliminary ** CLEO-III First branching ratio measurement of this mode. (Made possible by CLEO-III RICH) pKKp Mass (GeV/c2) 0c  77 ± 13 ** Preliminary ** p Mass (GeV/c2)

  8.  -0K- ; 0pp- 4291±93events previous 456±23events c0  -+ ** Preliminary ** New cMass Measurement mass scale 80.5±10.8events ** Preliminary **

  9. c0  -+ Production cross-section & xp spectrum: ** Preliminary ** From fit to Petersonfragmentation function ** Preliminary **

  10. Charmed Mesons

  11. Charm Meson Lifetimes Phys.Lett.B537:192-200,2002 Thanks to Kevin Stenson for summary figure

  12. Reconstructed withonline SVT tracks CDF: Huge charm physics potential • Charm potential • Trigger important • Huge future potential • Enormous production cross-section • Secondary Vertex Trigger is working well! 450,000events 78,000events

  13. DS+ - D+ Mass Difference FERMILAB-PUB-03/048-E • Charm potential • Trigger important • Huge future potential CDF

  14. D0  K+K-, +- ** Preliminary ** • Charm potential • Trigger important • Huge future potential ** Preliminary **

  15. 3453 ± 111 D0  K+K-, +- p-p+ hep-ex/0212058 10830 ± 148 K-K+ 105030 ± 372 K-p+

  16. D+ +0 , K+0, K+Ks(Chul Gwon) ** Preliminary ** CLEO-II.V • Unbinned maximum likelihood fit using FELIX. • Fit variables: M(D+), xpD, cosqhelicity • PDF’s obtained from MC & data D+p+p0 D+K+KS D+K+p0 171±22 34±21 278±21 M(D+) GeV M(D+) GeV M(D+) GeV < 0.0046 @ 90% CL ** Preliminary **

  17. Isospin analyses using new D0pp, KK numbers CLEO-II.V hep-ex/0212058 ** Preliminary ** pp KK New FOCUS p+p- , K+K-+old FOCUS K+K0+ PDG New CLEO p+p0+ PDG

  18. D0 K-K-K++, K-K+-+, -+-+ ** Preliminary ** FOCUS Preliminary PDG2002

  19. D+, DS 5-body Decays(Branching Ratios) fp+p+p- hep-ex/0211056 1st obs. p-p+p+p+p- K+K-p+p+p- (inclusive ratios) K-p+p+p+p- K+K-p+p+p- FOCUS also has new resultson D  6-body decays !

  20. K+K-p+p+p- K-p+p+p+p- 5-body Decays(Substructure) (7 ± 5 ± 1)% (10 ± 6 ± 5)% NR NR hep-ex/0211056 (21 ± 4 ± 6)% (21 ± 5 ± 6)% Consistent with hypothesis that structure dominated by quasi 2-body decays: K*0p-p+p+ fp-p+p+ Lipkin: Phys. Let. B 515, 81 (2001) (30 ± 4 ± 1)% < 3% @ 90%CL K-p+r0p+ K-K+r0p+ Central value of a1 mass is outside phase-space, but it’s wide (~400 MeV). (40 ± 3 ± 6)% (75 ± 6 ± 4)% K*0r0p+ fr0p+ sum sum (corrected for unseen modes)

  21. BaBar D0 K0K-+,K0K+-and K0K+K- hep-ex/0207089 Normalizing mode 11659 ± 40 15279 ± 129 805 ± 35 2109 ± 48 Errors are ~ 3-5 times smallerthan previous measurements A Dalitz analysis was also done for each mode…

  22. BaBar D0 K0K-+Dalitz Analysis hep-ex/0207089

  23. BaBar D0 K0K+-Dalitz Analysis hep-ex/0207089

  24. BaBar D0 K0K+K- Dalitz Analysis hep-ex/0207089

  25. D0Ks (Mikhail Dubrovin) ** Preliminary ** CLEO-II.V • Motivated by interest in KSp-p+ and KSK-K+ analyses. • KSa0(980) seen in KSK-K+ • but a0(980) is dominant • First measurement of this BR ** Preliminary **

  26. D0Ks (Mikhail Dubrovin) ** Preliminary ** CLEO-II.V KSa0(980) is dominant K*(892)h is seen Something else needed for good CL(but exactly what hard to sort out): NR, KSa2(1320), KSa0(1450)kh, K0(1430)h, K1(1410)h … Under investigation: stay tuned !

  27. 2 0 1 2 3 0 1 2 3 0 1 2 3 m2(KSp-) (GeV2) m2(KSp+) (GeV2) m2(p-p+) (GeV2) D0 Ks-+(David Asner) S/(S+B) ~ 98% S ~ 5300 Phys. Rev. Lett.89:251802,2002 CLEO-II.V m2(p-p+) (GeV2) 1 0 0 3 2 1 m2(KSp)RS (GeV2)

  28. BaBar D0 KSp-p+ From Brian Meadows, Moriond/03 • BaBar has incredible statistics! • Unprecedented sensitivity ! • Will the standard approach work ? • There are hint of “problems” in many lower statistics Dalitz analyses. • Will have to confront these!

  29. 0 1 2 3 m2pp(GeV2) D+ p+p-+ Dalitz E791 Phys.Rev.Lett.86:770-774,2001 Phase motion consistent with s:(Method discussed inPLB 550:135-139,2002) 0 1 2 3 m2pp(GeV2)

  30. 0 1 2 3 m2(p+p0) (GeV2) D0-+0(Charles Plager) S/(S+B) ~ 80% S ~ 1100 ** Preliminary ** CLEO-II.V m2(p+p0) (GeV2) No contribution from s(500) at ~1% level m2(p+p-) (GeV2) 0 1 2 3 0 1 2 3 m2(p+p-) (GeV2) m2(p-p0) (GeV2)

  31. 0 1 2 3 0 1 2 3 m2Kp(GeV2) m2Kp(GeV2) D+ K-p++Dalitz Phys.Rev.Lett.89:121801,2002 E791 CLEO Dalitz analysisof D0 K-p+0 seesno evidence for k.Phys. Rev.D63:092001,2001

  32. D+ K+K-+, +-+Dalitz Stay TunedNew results expected later this year

  33. BES s & k from J/ decays Preliminary BES results indicate significant contributionfrom s and k in J/ and J/K*Krespectively Ning Wu (IHEP, Beijing) from talk given at “Hadron Spectroscopy….” Tokyo, Feb/03

  34. K*(890) + K0(1430) + f0 + NR K*(890) + K0(1430) + f0 + NR + s 0 1 2 0 1 2 m2(p0p0) (GeV2) m2(p0p0) (GeV2) D0 Ks00(Scott Davis)(Just a peek…stay tuned) S/(S+B) ~ 70% S ~ 700 CLEO-II.V+III m2(p0p0) (GeV2) • Complement KSp-p+ analyses • Good place to search for low mass pp • No r00 to get in the way! • Fit seems to prefer presence of a broad scalar pp resonance (?) • No unique solution using BW’s. • Also trying K-matrix approach. m2(KSp0)RS (GeV2) Not the only way to get a good fit…more work needed

  35. D0K-K+0(Paras Naik)(Just a peek…stay tuned) S/(S+B) ~ 55% S ~ 400 CLEO-III • Made possible by CLEO-III RICH • Motivated by method for measuring “g” using B±→ D0K; D0→K*K[Grossman, Ligeti, Sopher & others] • Ingredient: Strong phase between D0→K*+K-and D0→K*+K- •  Exactly what this analysis measures • Stay Tuned 0 1 2 3 0 1 2 3 0 1 2 3 m2(K-p0) (GeV2) m2(K+p0) (GeV2) m2(K-K+) (GeV2)

  36. CLEO-c Summing Up Too many new charm results to do them all justice in 30 minutes !! c etc. D** • There are many more on the way. • The next few years should be very exciting for those of us interested in charm physics!