56,916 research outputs found

    Source of CP Violation for the Baryon Asymmetry of the Universe

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    We give a description of why the existence of a fourth generation is likely to provide enough CP violation for baryogenesis, and trace how this observation came about. We survey the current experimental and theoretical pursuits and outline a research agenda, touching upon unitarity violation and very heavy chiral quarks, and comment on how the electroweak phase transition picture might be altered.Comment: Invited talk presented at 2nd International Workshop on Dark Matter, Dark Energy and Matter-antimatter Asymmetry, Hsinchu, Taiwan, November 5-6, 201

    Heavy QQ(bar) "Fireball" Annihilation to Multiple Vector Bosons

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    Drawing analogy of replacing the nucleon by heavy chiral quark QQ, the pion by Goldstone boson GG, and Ο€NN\pi NN coupling by GQQGQQ coupling, we construct a statistical model for QQΛ‰β†’nGQ\bar Q \to nG annihilation, i.e. into nn longitudinal weak bosons. This analogy is becoming prescient since the LHC direct bound mQ>611m_Q > 611 GeV implies strong Yukawa coupling. Taking mQ∈(1,2)m_Q \in (1, 2) TeV, the mean number ranges from 6 to over 10, with negligible two or three boson production. With individual tβ€²t' or bβ€²b' decays suppressed either by phase space or quark mixing, and given the strong Yukawa coupling, QQΛ‰β†’nVLQ\bar Q\to nV_L is the likely outcome for very heavy QQΛ‰Q\bar Q production at the LHC.Comment: 4 pages, 1 figur

    Indications for Large Rescattering in Rare B Decays

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    The sign of ACP(Kβˆ’Ο€+)<0A_{\rm CP}(K^-\pi^+) < 0, the evidence for BΛ‰0β†’Ο€0Ο€0\bar B^0 \to \pi^0\pi^0, and the possibly sizable AππA_{\pi\pi} and SππS_{\pi\pi} in BΛ‰0β†’Ο€+Ο€βˆ’\bar B^0 \to \pi^+\pi^- all suggest that final state rescattering may be needed in BΛ‰β†’PP\bar B\to PP decay, which is echoed by large color suppressed BΛ‰0β†’D0h0\bar B^0\to D^0h^0 modes. An SU(3) formalism of 8βŠ—8β†’8βŠ—8{\bf 8}\otimes {\bf 8} \to {\bf 8}\otimes {\bf 8} rescattering in PPPP final states leads to interesting predictions, in particular allowing for small BΛ‰0β†’Kβˆ’K+\bar B^0 \to K^-K^+.Comment: 3 pages, 3 figures. Talk presented at EPS2003 Conference, Aachen, Germany, July 200

    A brief (p)review on a possible fourth generation world to come

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    We pick up the thread of Bβ†’KΟ€B\to K\pi direct CPV (DCPV) difference, linking to the 4th generation prediction (and current quest) of tt-dependent CPV (TCPV) in Bsβ†’J/Οˆβ€‰Ο•B_s \to J/\psi\,\phi. We then soar up to the heavens with possible source of CPV for the Universe (CPV-4-U); for the "cauldron" that stirs strong phase transitions, we raise the possible link between electroweak symmetry breaking and large Yukawa couplings (4-EWSB). With the prognosis for 2011, 2012 and beyond, we stress these as preview for the possible 4th generation to come: CPV-4-U and the \emph{raison d'\^etre} for our Universe (and ourselves); 4-EWSB and the \emph{raison d'\^etre} for the LHC itself.Comment: Talk given at 35th International Conference on High Energy Physics (ICHEP2010), Paris, France, July 22-28, 201

    Fourth Generation -- Towards Effect of Large Yukawa Coupling

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    In this talk we cover two threads regarding the 4th generation: on CP violation, from Earth up to the Heavens, i.e. from accelerator-based experimental studies, towards baryon asymmetry of the Universe; and on direct search bounds on mtβ€²m_{t'} and mbβ€²m_{b'}, towards the possibility of electroweak symmetry breaking through large Yukawa couplings. Prospects and discussions are presented.Comment: Plenary talk presented at TOP2010, May 31 - June 4, 2010, Bruges, Belgiu
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