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D s production in B meson decay. by Douglas Michael Gingrich

Published .

Written in English

Subjects:

• Physics Theses

Edition Notes

Thesis (Ph.D.), Dept. of Physics, University of Toronto

Book details

The Physical Object ID Numbers Contributions Orr, R. S. (supervisor) Pagination 177 p. Number of Pages 177 Open Library OL19051762M

In particle physics, B mesons are mesons composed of a bottom antiquark and either an up (B +), down (B 0), strange (B 0 s) or charm quark (B + c).The combination of a bottom antiquark and a top quark is not thought to be possible because of the top quark's short lifetime.

The combination of a bottom antiquark and a bottom quark is not a B meson, but rather bottomonium which is something. If the recently-discovered charmonium-like state X() is a loosely-bound S-wave molecule of the charm mesons D^0 \bar D^{*0} or D^{*0} \bar D^0, it can be.

For the study of the time dependent decay rate of B-meson, an interesting approach 35) was proposed. If the Upsilon(4S) is produced with substantial momentum, the B-meson’s momentum, P lab, also becomes large and is approximately one half of P Upsilon.

Two B-mesons move in parallel along the direction of the motion of the Upsilon (4S) by: 1. Eisenstein's research works w citations and 2, reads, including: Model independent measurement of form factors in the decay D+-> K-pi(+)e(+)nu(e). Leptonic Decays of the Charged B Meson DISSERTATION Presented in Partial Fulﬁllment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of The Ohio State University By Luke A.

Corwin, B.S. ***** The Ohio State University Dissertation Committee: Professor Klaus Honscheid, Adviser Professor Eric Braaten Professor.

D + mesons produced inZ 0→bb events were separated from theZ 0→cc component using a lifetime tag. Using a sample of million hadronicZ decays collected with theAleph detector theB 0 andD s + yields have been measured: \begin{gathered} \hfill B(b \to \bar B_s^0)B(\bar B_s^0 \to D_s^ +) = \pm (stat.) \\ \hfill \pm (stat.) \\ \hfill B(c \to D_s^ +) = \pm $D_s ^+$ mesons produced in Z0 → bb̅ events were separated from the Z0 → cc̅ component using a lifetime tag.

Using a sample of million hadronic Z decays. I P Volobuev's 34 research works with citations and reads, including: Observation of D$_{1}$()$^{+}$ and D$_{2}^{*}$() $^{+}$. The Table of Contents for the full book PDF is as follows: * Preface * Radiative Corrections in the Electroweak Standard Model * Introduction * The Electroweak Standard Model and its Renormalization * Basic Properties of the Standard Model * Renormalization of the Standard Model * Calculation of Radiative Corrections * One-Loop Integrals * Corrected Matrix Elements and.

Download PDF The Production Of Excited Charm Mesons In Semileptonic B Decay book full free. The Production Of Excited Charm Mesons In Semileptonic B Decay available for d.

A detailed description is presented of the method used and the results obtained for measuring various decay widths of the B-mesons into baryon-antibaryon pairs: (i) into two light baryons: B → p p, Δ p,(ii) into one light and one charmed baryon: B → p Σ c, p Λ c,(iii) into two charmed baryons: B → Σ c, Ξ c, Λ c Ξ c,(iv) the decays induced by the b → s.

34 meson, has been published by CDF [8]. They reconstruct the semileptonic decay Bc!J= ‘X, and extract a Bc mass of GeV/ c2. First indications of b production have been presented by the LEP Collaborations [9{10].

Excited B-meson states have. E.W. Varnes, (representing the BaBar collaboration), in Proceedings of the 31st International Conference on High Energy Physics Ichep3 B Meson Reconstruction. B mesons are reconstructed by combining tracks or photons to form candidates for the intermediate mesons in the decay, constraining these mesons to their known masses, and then combining them to form B candidates.

Edited by D. Lichtenberg and S. Rosen. Evidence for top quark production in p ˉ p \bar{p}p p ˉ p collisions at s = \sqrt{s} = s = 1. 8 TeV CDF. We have presented a new method to measure the Unitarity Triangle angle ϕ 1 using amplitude analysis of the multibody decay of the neutral D meson produced in the processes B ¯ 0 → D h 0.

The method is directly sensitive to the value of 2 ϕ 1 and can thus be used to resolve the discrete ambiguity 2 ϕ 1 ↔ π − 2 ϕ 1. The expected. • Recent highlights of meson spectroscopy include: 1. The discovery of the X, Y, Z states. High-statistics studies of e+e− → light quark vectors.

Precision measurements in charmonium. New dialogues on light quark hybrid mesons. (Also: the η b, D SJ states, D and D S decay constants, the glueball picture) • This is a time of.

Review of Particle Physics. Please use this CITATION: J. Beringer et al. (Particle Data Group), Phys. Rev. D86, (). Cut-off date for this update was Janu You can write a book review and share your experiences.

Other readers will always be interested in your opinion of the books you've read. Whether you've loved the book or not, if you give your honest and detailed thoughts then people will find new books that are right for them.

The muon (/ ˈ m juː ɒ n /; from the Greek letter mu (μ) used to represent it) is an elementary particle similar to the electron, with an electric charge of −1 e and a spin of 1 / 2, but with a much greater is classified as a with other leptons, the muon is not known to have any sub-structure – that is, it is not thought to be composed of any simpler particles.

Revised: June Measurement of D-meson production versus multiplicity in p{Pb collisions at 0 s = 7 TeV as well as The measurement of prompt D-meson production as a function of multiplicity in p{Pb collisions at psNN = TeV with the ALICE detector at the LHC is reported.

production in D+ s → π 0 transition in semileptonic decay. We also estimate the branching fraction of D+ s → π 0τ+ν τ, which is the only kinematically allowed semi-tauonic decay mode of the charmed meson, since the mass value of D+ s meson is just slightly above the threshold of π 0τ+ generation in the semi-tauonic decay.

The combination of experimental leptonic decay-rate measurements and theoretical decay-constant calculations enables the determination of several elements of the CKM matrix within the standard model.

These determinations are competitive with those obtained from semileptonic decays, and also complementary because they are sensitive to different. We review the present status for the determinations of the light and heavy quark masses, the light quark chiral condensate and the decay constants of light and heavy-light (pseudo)scalar mesons from QCD spectral sum rules (QSSR).

Bounds on the light quark running masses at 2 GeV are found to be: 6 MeVd+m_u)(2)s(2)< MeV. Production and decay of the K©. meson [Parker, Sherwood.] on *FREE* shipping on qualifying offers. Production and decay of the K©. meson. @article{osti_, title = {Decay of B mesons into charged and neutral kaons}, author = {Brody, A and Chen, A and Goldberg, M and Horwitz, N and Kandaswamy, J and Kooy, H and Moneti, G C and Pistilli, P and Alam, M S and Csorna, S E and Fridman, A and Hicks, R G and Panvini, R S and Andrews, D and Avery, P and Berkelman, K and Cabenda, R and Cassel, D G and DeWire, J W and Ehrlich, R.

The f 1 () meson with mass ± MeV/c 2 and width ± MeV (full width at half maximum) was measured for the first time in photoproduction from a proton target using CLAS at Jefferson Lab. Differential cross sections were obtained via the ηπ + π - K + K 0 π - and K -K 0 π + decay channels from threshold up to a center-of-mass energy of GeV.

In the s, particle physicists began to realize that hadrons are not elementary particles but are made of particles called quarks.

(The name ‘quark’ was coined by the physicist Murray Gell-Mann, from a phrase in the James Joyce novel Finnegans Wake.)Initially, it was believed there were only three types of quarks, called up (u), down (d), and strange (s). The BABAR detector: Upgrades, operation and r Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment.

In an e + e − B factory, charmonium states can be produced through different mechanisms, e.g. direct production in e + e − annihilation, double charmonium production, and in B-meson production of J/ψ or ψ(2S) in association with a second charmonium states has been observed by both the B A B AR and the Belle experiments.

These processes provide an. For the study of the time dependent decay rate of B-meson, an interesting approach (35) was proposed. If the Upsilon(4S) is produced with substantial momentum, the B-meson's momentum, Plab, also becomes large and is approximately one half of [n].

Along with the running of Large Hadron Collider (LHC) located at CERN in Novembera large number of data samples of B c meson have been collected and some hadronic B c decay modes have been measured by the LHC experiments. In view of the special and important roles of Bc meson decays playing in the heavy flavor.

The book focuses on the reactions, properties, characteristics, and transformations of heavy flavors. The publication first offers information on flavor factories and monochromatization as the way to maximum luminosity B-factories, as well as design strategies and parameters, requirements, luminosity limitations, and B-factory with.

() Event generation with SHERPA - Gleisberg, T. et al. JHEP () arXiv [hep-ph] FERMILAB-PUBT, SLAC-PUB, ZU-TH, DCPT, IPPP, EDINBURGH, MCNET () Herwig++ Physics and Manual - Bahr, M. et al. C58 () arXiv [hep-ph] CERN-PH-TH, CAVENDISH-HEP, KA. −, D− s → K ∗0K−, D− s → π +π−π−, • φ → K+K−, • K∗0 → K+π−, • J/ψ→ µ+µ−.

Charge-conjugated states are implicitly assumed throughout the text. The full list of decay chains is shown explicitly in Table The B meson decays studied fall into two categories: fully reconstructed and partially.

Measurement of branching fractions for exclusive B meson decays to charmonium final states, B. Aubert et al., Phys. Rev. D 65 () Measurement of D+s and D*+s production in B meson decays and from continuum e+e– annihilation at Ec.m.

= GeV, B. Aubert et al., Phys. Rev. D 65 () (R) [a] ^ Strong definite lifetime (see kaon notes below) [b] ^ Weak is missing small CP–violating term (see notes on neutral kaons below). [c] ^ The mass of the K 0 L and K 0 S are given as that of the K 0However, it is known that a difference between the masses of the K 0 L and K 0 S on the order of × 10 −12 MeV/c 2 exists.

Although the. We present the results on the mid-rapidity φ meson production in the K+K− decay channel in Au + Au collisions at √ s NN = GeV measured by the PHENIX experiment at RHIC. The spectral shape of the φ resonance, studied at diﬀerent collision centralities, is consistent with the particle data book.

The transverse mass spectra are. An illustration of an open book. Books. An illustration of two cells of a film strip. Video. An illustration of an audio speaker. Audio. An illustration of a " floppy disk. ()\$ and the production in heavy meson decays Item Preview There Is No Preview Available For This Item.

The T region / G.R. Kalbfleisch --The U-meson region / Gerald A. Smith --Charged non-strange bosons with masses higher than GeV / R. Baud [and others] --Comparison of the CERN boson spectrometer results with a [pi]p experiment at 13 GeV/c in a bubble chamber / David H.

Miller --Photoproduction of high mass dipion pairs at 15 BeV / F. Bulos. Get this from a library. Meson 7th International Workshop on Production, Properties and Interaction of Mesons, Cracow, Poland, May [Lucjan Jarczyk;] -- This volume deals with both the experimental and theoretical aspects of meson physics; in particular, it presents new results.

The main topics are: hadronic and electromagnetic meson production in. A similar decay, ρ0 → π+ + π–, has a mean lifetime of 4 × 10–24 s. What difference in the decay mechanism might explain the huge difference in lifetime? (Hint: the ρ0 is a meson with.New physics in b→ss¯s decay Cosmogenic production as a background in searching for rare physics processes Search for New Physics in rare decays at LHCb New Rare Decay Results from KTeV Signature of new physics in B→ϕπ decay Rare Decays as a Probe for New Physics.The upper two rows (first three columns in purple) contain six quarks.

These quarks are arranged into two particle families: up, charm, and top (u, c, t), and down, strange, and bottom (d, s, b). Members of the same particle family share the same properties but differ in mass (given in).

For example, the mass of the top quark is much greater.

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