11 research outputs found

    The general relation between the weak inclusive decays of bound and free heavy quarks

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    We derive a new parton formula for the inclusive B decays and briefly discuss its applications to semileptonic and weak radiative decays of the B-meson.Comment: espcrc2.sty (included), 3 pages, Presented at the Third International Conference on Hyperons, Charm and Beauty Hadrons, Genova, June 30 --July 3, 1998, to appear in proceeding

    Lifetimes of the b-flavored baryons in the light-front quark model

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    The calculation of lifetimes of heavy-flavored baryons in the light-front quark model approach is briefly reviewed.Comment: 4 pages, proceedings of the IV International Conference on Hyperons, Charm and Beauty Hadrons, Valencia, June 27--30, 200

    Quark-binding effects in inclusive decays of heavy mesons

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    We present a new approach to the analysis of quark-binding effects in inclusive decays of heavy mesons within the relativistic dispersion quark model. Various differential distributions, such as electron energy spectrum, q2q^2- and MXM_X-distributions, are calculated in terms of the BB meson soft wave function which also determines long-distance effects in exclusive transition form factors. Using the quark-model parameters and the BB meson wave function previously determined from the description of the exclusive b→ub \to u transitions within the same dispersion approach, we provide numerical results on various distributions in the inclusive B→XclνB \to X_c l\nu decays.Comment: revtex, 18 pages, preprint HD-THEP-99-50 (Heidelberg) and RM3-TH/99-13 (Roma

    The Kalman-Tran-D'Souza Model and the Semileptonic Decay Rates of Heavy Baryons

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    We present an investigation of the inclusive semileptonic decay widths of the heavy baryons Lambda_Q and Xi_Q, (Q=b,c) performed within a relativistic constituent quark model, formulated on the light-front. In a way conceptually similar to the deep-inelastic scattering case, the H_Q baryon inclusive width is expressed as the integral of the free Q-quark partial width multiplied by a bound-state factor related to the Q-quark distribution function in the H_Q. The non-perturbative meson structure is described through the quark-model wave functions, constructed via the Hamiltonian light-front formalism using as input the Kalman-Tran-D'Souza equal time wave functions. A link between spectroscopic quark models and the H_Q decay physics is obtained in this way. It is shown that the bound-state effects and the Fermi motion of the b-quark remarkably reduce the decay rate with respect to the free-quark result. Our predictions for the BR(Lambda_c ->X_s e nu_e) and BR(Lambda_b->X_c e nu_e) decays are in good agreement with existing data.Comment: 6 pages, latex, espcrc2.sty (included), 3 figures. The invited talk presented by C.S.K. at the 4-th International Conference on Hyperons, Charm and Beauty Hadrons, Valencia, June 27-30, 200

    A connection between inclusive semileptonic decays of bound and free heavy quarks

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    A relativistic constituent quark model, formulated on the light-front, is used to derive a new parton approximation for the inclusive semileptonic decay width of the B-meson. A simple connection between the decay rate of a free heavy-quark and the one of a heavy-quark bound in a meson or in a baryon is established. The main features of the new approach are the treatment of the b-quark as an on-mass-shell particle and the inclusion of the effects arising from the b-quark transverse motion in the B-meson. In a way conceptually similar to the deep-inelastic scattering case, the B-meson inclusive width is expressed as the integral of the free b-quark partial width multiplied by a bound-state factor related to the b-quark distribution function in the B-meson. The non-perturbative meson structure is described through various quark-model wave functions, constructed via the Hamiltonian light-front formalism using as input both relativized and non-relativistic potential models. A link between spectroscopic quark models and the B-meson decay physics is obtained in this way. Our predictions for the B -> X_c l nu_l and B -> X_u l nu_l decays are used to extract the CKM parameters |V_cb| and |V_ub| from available inclusive data. After averaging over the various quark models adopted and including leading-order perturbative QCD corrections, we obtain |V_cb| = (43.0 +/- 0.7_exp +/- 1.8_th) 10^-3 and |V_ub| = (3.83 +/- 0.48_exp +/- 0.14_th) 10^-3, implying |V_ub / V_cb| = 0.089 +/- 0.011_exp +/- 0.005_th, in nice agreement with existing predictions.Comment: revised version with pQCD corrections included, to appear in Physical Review

    The lifetime of B_c-meson and some relevant problems

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    The lifetime of the B_c-meson is estimated with consistent considerations on all of the heavy mesons (B0,BΒ±,Bs,D0,DΒ±DsB^0, B^\pm, B_s, D^0, D^\pm D_s) and the double heavy meson B_c. In the estimate, the framework, where the non-spectator effects for nonleptonic decays are taken into account properly, is adopted, and the parameters needed to be fixed are treated carefully and determined by fitting the available data. The bound-state effects in it are also considered. We find that in decays of the meson B_c, the QCD correction terms of the penguin diagrams and the main component terms c_1O_1, c_2O_2 of the effective interaction Lagrangian have direct interference that causes an enhancement about 3 ~ 4% in the total width of the B_c meson.Comment: 27 pages, 0 figur

    НСттінг β€” Π±Π°Π½ΠΊΡ–Π²ΡΡŒΠΊΠ° новація Ρƒ Ρ€ΠΎΠ·Ρ€Π°Ρ…ΡƒΠ½ΠΊΠ°Ρ…

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    Розглянуто поняття Π½Π΅Ρ‚Ρ‚Ρ–Π½Π³Ρƒ, ΠΉΠΎΠ³ΠΎ основні риси, ΠΊΠ»Π°ΡΠΈΡ„Ρ–ΠΊΠ°Ρ†Ρ–ΡŽ різновидностСй Π½Π΅Ρ‚Ρ‚Ρ–Π½Π³Ρƒ ΠΉ особливості ΠΉΠΎΠ³ΠΎ застосування, Π²ΠΈΠ·Π½Π°Ρ‡Π΅Π½Ρ– Π²Ρ–Π΄ΠΌΡ–Π½Π½Ρ– риси Π½Π΅Ρ‚Ρ‚Ρ–Π½Π³Ρƒ Ρ– Π·Π°Π»Ρ–ΠΊΡƒ Π²Π·Π°Ρ”ΠΌΠ½ΠΈΡ… Π²ΠΈΠΌΠΎΠ³, Ρ€ΠΎΠ·ΠΊΡ€ΠΈΡ‚ΠΎ використання Π»Ρ–ΠΊΠ²Ρ–Π΄Π°Ρ†Ρ–ΠΉΠ½ΠΎΠ³ΠΎ Π½Π΅Ρ‚Ρ‚Ρ–Π½Π³Ρƒ для ΠΊΡ€Π΅Π΄ΠΈΡ‚ΠΎΡ€Π°-Π±ΠΎΡ€ΠΆΠ½ΠΈΠΊΠ° Π² ΡƒΠΌΠΎΠ²Π°Ρ… фінансової ΠΊΡ€ΠΈΠ·ΠΈ.РассмотрСно понятиС Π½Π΅Ρ‚Ρ‚ΠΈΠ½Π³Π°, Π΅Π³ΠΎ основныС Ρ‡Π΅Ρ€Ρ‚Ρ‹, классификация разновидностСй Π½Π΅Ρ‚Ρ‚ΠΈΠ½Π³Π° ΠΈ особСнности Π΅Π³ΠΎ примСнСния, ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Ρ‹ ΠΎΡ‚Π»ΠΈΡ‡ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Π΅ Ρ‡Π΅Ρ€Ρ‚Ρ‹ Π½Π΅Ρ‚Ρ‚ΠΈΠ½Π³Π° ΠΈ Π·Π°Ρ‡Π΅Ρ‚Π° Π²Π·Π°ΠΈΠΌΠ½Ρ‹Ρ… Ρ‚Ρ€Π΅Π±ΠΎΠ²Π°Π½ΠΈΠΉ, раскрыто использованиС Π»ΠΈΠΊΠ²ΠΈΠ΄Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Π½Π΅Ρ‚Ρ‚ΠΈΠ½Π³Π° для ΠΊΡ€Π΅Π΄ΠΈΡ‚ΠΎΡ€Π°-Π΄ΠΎΠ»ΠΆΠ½ΠΈΠΊΠ° Π² условиях финансового кризиса.The article deals with the concept of netting, its main features, the classification of varieties of netting and features of its application, the distinctive features of netting and set-off of mutual claims are identified, the use of close-out netting for the creditor-debtor in the context of the financial crisis is presented in the paper
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