Spelling suggestions: "subject:"kaon"" "subject:"raons""
21 |
Hyperon production by K⁻ interactions in deuteriumDahl, Orin Iver. January 1962 (has links)
Thesis (Ph.D.)--University of California, Berkeley, 1962. / "UC-34 Physics Distribution" -t.p. "TID-4500 (17th Ed.)" -t.p. Includes bibliographical references (p. 62-63).
|
22 |
Total cross section of K⁻ mesons on nucleons in the momentum region 630 Mev/c to 1100 Mev/cMaung, Maung Tin, January 1962 (has links)
Thesis (Ph.D.)--University of California, Berkeley, 1962. / "UC-34 Physics" -t.p. "TID-4500 (17th Ed.)" -t.p. Includes bibliographical references (p. 80-82).
|
23 |
Measurements of direct CP-violation and CPT-invariance in the neutral kaon system /Prasad, Valmiki. January 2002 (has links)
Thesis (Ph. D.)--University of Chicago, Dept. of Physics, June 2002. / Includes bibliographical references. Also available on the Internet.
|
24 |
The measurement of polarization effects in the elastic scattering of K⁻₋mesons by protonsCox, C. R. January 1968 (has links)
No description available.
|
25 |
Kaon to two-pion decay and pion-pion scattering from lattice QCDWang, Tianle January 2021 (has links)
In this work, we present a lattice QCD calculation of two closely related quantities: 1). The 𝜋𝜋 scattering phase shift for both 𝑰=0 and 𝑰=2 channels at seven energies in total, and 2). The 𝜟𝑰=1/2, 𝛫 → 𝜋𝜋 decay amplitude 𝐴₀ and 𝜖′, the measure of direct CP violation. These two results improve our earlier calculation presented in 2015 [1]. The calculation is performed on an ensemble of 32³ × 64 lattice with 𝛼⁻¹=1.3784(68)GeV. This is a physical calculation, where the chiral symmetry breaking is controlled by the 2+1 flavor Möbius Domain Wall Fermion, and we take the physical value for both kaon and pion. The G-parity boundary condition is used and carefully tuned so that the ground state energy of the 𝜋𝜋₁₌₀ state matches the kaon mass. Three sets of 𝜋𝜋 interpolating operators are used, including a scalar bilinear ``σ" operator and paired single-pion bilinear operators with the constituent pions carrying various relative momenta. Several techniques, including correlated fits and a bootstrap determination of the 𝑝-value have been used, and a detailed analysis of all major systematic error is performed. The 𝜋𝜋 scattering phase shift results are presented in Fig. 5.10 and Tab. 5.12. For the Kaon decay amplitude, we finally get Re(𝐴₀) = 2.99(0.32)(0.59) × 10⁻⁷GeV, which is consistent with the experimental value of Re(𝐴₀) = 3.3201(18) × 10⁻⁷GeV, and Im(𝐴₀) = -6.98(0.62)(1.44) × 10⁻¹¹GeV. Combined with our earlier lattice calculation of 𝐴₂ [2], we obtained Re(𝜖′/𝜖) = 21.7(2.6)(6.2)(5.0) × 10⁻⁴, which agrees well with the experimental value of Re(𝜖′/𝜖) = 16.6(2.3) × 10⁻⁴, and Re(𝐴₀)/Re(𝐴₂) = 19.9(2.3)(4.4), consistent with the experimental value of Re(𝐴₀)/Re(𝐴₂) = 22.45(6), known as the 𝜟𝑰=1/2 rule.
|
26 |
A search for the rare decay of a charged B meson into a charged K meson, a neutrino and an anti-neutrino /Harnois-Déraps, Joachim. January 2006 (has links)
No description available.
|
27 |
A cloudy Quark Bag Model of S, P, and D wave interactions for the coupled channel antikaon-nucleon systemHe, Guangliang 15 May 1992 (has links)
Graduation date: 1993
|
28 |
A measurement of the branching fraction of the Ds meson decay into a tau and a neutrino /He, Lian Harry. January 2000 (has links)
Thesis (Ph. D.)--University of Washington, 2000. / Vita. Includes bibliographical references (p. 120-123).
|
29 |
A search for the rare decay of a charged B meson into a charged K meson, a neutrino and an anti-neutrino /Harnois-Déraps, Joachim. January 2006 (has links)
The document describes a search for the rare decay B¯ → K¯vv̄ in a data set of about 230 millions of BB̄ pairs recorded by the BABAR detector at the PEP-II B Factory, via the process e⁺e⁻ → ϒ(4S) → BB̄. The method used selects events in which the B+ meson is fully reconstructed, and looks for a K¯ in the rest of the event. This is accomplished by applying kinematical and topological restrictions that select B¯ → K¯vv̄ events with the largest possible efficiency, while rejecting a maximum amount of background events. The number of background events is estimated from data and from simulated events, while the value of the selection efficiency relies solely on the simulation of B¯ → K¯vv̄ decays in the BABAR detector. These two numbers are required in order to set an upper limit on the branching ratio. We analyze a subset of the data sample and provide an interpretation of the result.
|
30 |
A preliminary cross section measurement for K⁰*[Sigma]⁺ electroproductionWeisberg, Adam. January 2001 (has links)
Thesis (M.S.)--Ohio University, November, 2001. / Title from PDF t.p.
|
Page generated in 0.0535 seconds