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Related papers: The Nonperturbative Broken Phase Sphaleron Rate

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For the periodic sphaleron potential in the electroweak theory, we find the one-dimensional time-independent Schr\"{o}dinger equation with the Chern-Simons number as the coordinate, construct the Bloch wave function and determine the…

High Energy Physics - Theory · Physics 2015-08-11 S. -H. Henry Tye , Sam S. C. Wong

An instructional laboratory experiment to measure the muon mass is described. Using coincidence-anticoincidence detection, the decay of a cosmic-ray muon into an electron (or positron) is observed in a multiplate spark chamber, and recorded…

Physics Education · Physics 2010-02-05 Benjamin Brau , Christopher May , Robert Ormond , John Essick

Two-body weak decays / and are examined under isospin analysis to study nonfactorizable contributions. After extracting the strong phases and obtaining the factorizable contributions from spectator-quark diagrams for Nc=3, we determine…

High Energy Physics - Phenomenology · Physics 2024-12-04 Maninder Kaur , Supreet Pal Singh , R. C. Verma

Nuclear resonant inelastic x-ray scattering is used to measure the projected partial phonon density of states of materials. A relationship is derived between the low-energy part of this frequency distribution function and the sound velocity…

A triple-product correlation in the radiative \beta-decay rate of neutrons or of nuclei, characterized by the kinematic variable \xi\equiv (\vec{l}_\nu\times\vec{l}_e)\cdot\vec{k}, where, e.g., n(p) \to p(p') + e^-(l_e) + \bar{\nu}_e(l_\nu)…

High Energy Physics - Phenomenology · Physics 2013-08-09 Susan Gardner , Daheng He

The $CP^N$ model in three euclidean dimensions is studied in the presence of a Chern-Simons term using the $1/N$ expansion. The $\beta$-function for the CS coefficient $\theta$ is found to be zero to order $1/N$ in the unbroken phase by an…

High Energy Physics - Theory · Physics 2015-06-26 G. Ferretti , S. G. Rajeev

Determining the phase in one arm of a quantum interferometer is discussed taking into account the three non-ideal aspects in real experiments: non-deterministic state preparation, non-unitary state evolution due to losses during state…

Quantum Physics · Physics 2015-05-20 Thomas B. Bahder

This paper presents the first neutrino cross-section measurement from the ICARUS detector at Fermilab, using NuMI (Neutrinos at the Main Injector) beam data collected from two beam operation periods corresponding to $2.5\times10^{20}$…

High Energy Physics - Experiment · Physics 2026-04-29 ICARUS Collaboration , F. Abd Alrahman , P. Abratenko , N. Abrego-Martinez , A. Aduszkiewicz , F. Akbar , L. Aliaga Soplin , M. Artero Pons , J. Asaadi , W. F. Badgett , B. Baibussinov , B. Behera , V. Bellini , R. Benocci , J. Berger , S. Bertolucci , M. Betancourt , A. Blanchet , F. Boffelli , M. Bonesini , T. Boone , B. Bottino , A. Braggiotti , D. Brailsford , S. J. Brice , V. Brio , C. Brizzolari , H. S. Budd , A. Campani , A. Campos , D. Carber , M. Carneiro , I. Caro Terrazas , H. Carranza , F. Castillo Fernandez , S. Centro , G. Cerati , A. Chatterjee , D. Cherdack , S. Cherubini , N. Chithirasreemadam , M. Cicerchia , T. E. Coan , A. Cocco , M. R. Convery , L. Cooper-Troendle , S. Copello , H. Da Motta , M. Dallolio , A. A. Dange , A. de Roeck , S. Di Domizio , L. Di Noto , D. Di Ferdinando , M. Diwan , S. Dolan , S. Donati , F. Drielsma , J. Dyer , A. Falcone , C. Farnese , A. Fava , N. Gallice , C. Gatto , D. Gibin , A. Gioiosa , W. Gu , A. Guglielmi , G. Gurung , K. Hassinin , H. Hausner , A. Heggestuen , B. Howard , R. Howell , Z. Hulcher , G. Ingratta , M. S. Ismail , C. James , W. Jang , K. Jung , Y. -J. Jwa , L. Kashur , W. Ketchum , J. S. Kim , D. -H. Koh , J. Larkin , Y. Li , C. Mariani , C. M. Marshall , S. Martynenko , N. Mauri , K. S. McFarland , D. P. Méndez , A. Menegolli , G. Meng , O. G. Miranda , A. Mogan , N. Moggi , E. Montagna , C. Montanari , A. Montanari , M. Mooney , M. Moore , G. Moreno-Granados , J. Mueller , M. Murphy , D. Naples , S. Palestini , M. Pallavicini , V. Paolone , L. Pasqualini , L. Patrizii , G. Petrillo , C. Petta , V. Pia , F. Pietropaolo , F. Poppi , M. Pozzato , M. L. Pumo , G. Putnam , X. Qian , A. Rappoldi , G. L. Raselli , S. Repetto , F. Resnati , A. M. Ricci , M. Rosenberg , M. Rossella , N. Rowe , P. Roy , C. Rubbia , A. Ruggeri , S. Saha , G. Salmoria , S. Samanta , A. Scaramelli , D. Schmitz , A. Schukraft , D. Senadheera , S-H. Seo , F. Sergiampietri , G. Sirri , J. S. Smedley , J. Smith , M. Sotgia , L. Stanco , J. Stewart , H. A. Tanaka , M. Tenti , K. Terao , F. Terranova , V. Togo , D. Torretta , M. Torti , R. Triozzi , Y. -T. Tsai , K. V. Tsang , T. Usher , F. Varanini , N. Vardy , S. Ventura , M. Vicenzi , C. Vignoli , F. A. Wieler , Z. Williams , R. J. Wilson , P. Wilson , J. Wolfs , T. Wongjirad , A. Wood , E. Worcester , M. Worcester , S. Yadav , H. Yu , J. Yu , A. Zani , J. Zennamo , J. Zettlemoyer , S. Zucchelli

We present a measurement of the inclusive electron spectrum in charmless semileptonic B decays near the kinematic limit for B->X_c e\nu transitions, using a sample of 88 million Upsilon(4S) decays recorded by the BABAR detector. Partial…

High Energy Physics - Experiment · Physics 2010-03-19 BABAR Collaboration , B. Aubert

Oscillations of the neutron into a hidden sector particle are processes predicted in various Standard Model extensions. This extra channel for neutron disappearance has not been tested experimentally in large portions of the oscillation…

The recent realization of a "Levy glass" (a three-dimensional optical material with a Levy distribution of scattering lengths) has motivated us to analyze its one-dimensional analogue: A linear chain of barriers with independent spacings s…

Disordered Systems and Neural Networks · Physics 2009-01-29 C. W. J. Beenakker , C. W. Groth , A. R. Akhmerov

Non-leptonic charm decays provide insights into both electro-weak and strong dynamics. This includes the study of long-distance hadronic effects, the approximate symmetries of strong interactions, and precision tests of the Standard Model.…

High Energy Physics - Experiment · Physics 2010-02-16 Jonas Rademacker

We study a nonlinear interferometer consisting of two consecutive parametric amplifiers, where all three optical fields (pump, signal and idler) are treated quantum mechanically, allowing for pump depletion and other quantum phenomena. The…

Quantum Physics · Physics 2018-12-27 Jefferson Flórez , Enno Giese , Davor Curic , Lambert Giner , Robert W. Boyd , Jeff S. Lundeen

We determine the $SU(3)$-breaking effects in the $\bar{B}/D \rar Kl\bar \nu$ decays from the ratio of the $\bar{B}/D\rar Kl\bar \nu$ over the $\bar{B}/D \rar \pi l\bar \nu$ semileptonic form factors using a {\it semi-analytic} expression…

High Energy Physics - Phenomenology · Physics 2010-11-01 S. Narison

In this paper, a new cooperation structure for spectrum sensing in cognitive radio networks is proposed which outperforms the existing commonly-used ones in terms of energy efficiency. The efficiency is achieved in the proposed design by…

Information Theory · Computer Science 2015-09-11 Younes Abdi , Tapani Ristaniemi

We report measured and calculated values of radiative decay rates and vibrational branching fractions for the A$^2\Pi$ state of MgF. The decay rate measurements use time-correlated single photon counting with roughly 1% total uncertainty.…

The rate of $B$-violation in the standard model at finite temperature is closely related to the diffusion rate $\Gamma$ of Chern-Simons number. We compute this rate for $m_H \approx m_W$ in the classical approximation in an effective…

High Energy Physics - Lattice · Physics 2007-05-23 Jan Smit , Wai Hung Tang

We measure the absolute branching fractions of $\Ds$ semileptonic decays where the hadron in the final state is one of $\phi$, $\eta$, $\etap$, $\Ks$, $\Kstar$, and $f_0$, using $2.8 \times 10^5$ $\epm \to \Ds\Dsstar$ decays collected in…

High Energy Physics - Experiment · Physics 2010-04-08 The CLEO Collaboration , J. Yelton

We propose a new nonparametric procedure for the detection and estimation of multiple structural breaks in the autocovariance function of a multivariate (second- order) piecewise stationary process, which also identifies the components of…

Statistics Theory · Mathematics 2013-09-06 Philip Preuß , Ruprecht Puchstein , Holger Dette

Reading out the state of superconducting artificial atoms typically relies on dispersive coupling to a readout resonator. For a given system noise temperature, increasing the circulating photon number $\bar{n}$ in the resonator enables a…