English
Related papers

Related papers: Muon lifetime and muon capture

200 papers

Starting this summer, Fermilab will host a key experiment dedicated to the search for signals of new physics: The Fermilab Muon g-2 Experiment. Its aim is to precisely measure the anomalous magnetic moment of the muon. In full operation, in…

For purely leptonic decays of pseudoscalar mesons, the decay rates are related to the product of the relevant weak interaction-based CKM matrix element of the constituent quarks on the one hand, and the strong interaction parameter, the…

High Energy Physics - Phenomenology · Physics 2013-04-12 Swee Ping Chia

We have performed a global analysis of muon decay measurements to establish model-independent limits on the space-time structure of the muon decay matrix element. We find limits on the scalar, vector and tensor coupling of right- and…

High Energy Physics - Phenomenology · Physics 2009-11-11 C. A. Gagliardi , R. E. Tribble , N. J. Williams

We analyze the hard scattering amplitude of gravitational form factors (GFFs) of hadrons within QCD factorization at large momentum transfers, focusing on their conformal field theory (CFT) description. These form factors are key to…

High Energy Physics - Phenomenology · Physics 2024-10-03 Claudio Corianò , Stefano Lionetti , Dario Melle , Riccardo Tommasi

Recent studies have proposed using a geocentric muon spin force to account for the $(g-2)_\mu$ anomaly, with the long-range force mediator being a light axion-like particle. The mediator exhibits a CP-violating scalar coupling to nucleons…

High Energy Physics - Phenomenology · Physics 2024-12-18 Rundong Fang , Ji-Heng Guo , Jia Liu , Xiao-Ping Wang

Muons have a similar latency/energy correlation from pion decay as do the neutrinos, and hence in each time-slice in a stroboscopic analysis measurements of their momentum spectra can reduce systematic uncertainties due to flux. There are,…

High Energy Physics - Experiment · Physics 2022-12-20 Henry J. Frisch

We employ a mathematical framework based on rational approximants in order to calculate meson form factors. The method profits from unitary, is systematic and data based, and is able to ascribe a systematic uncertainty which provides for…

High Energy Physics - Phenomenology · Physics 2018-02-15 Sergi Gonzàlez-Solís , Pere Masjuan , Pablo Sanchez-Puertas

Normal muon decay, $\mu^{+} \to e^{+}\nu_{e}\bar{\nu_{\mu}}$, is studied as a tool to discriminate between the Dirac and Majorana types of neutrinos and to survey the structure of the weak interaction. It is assumed that massive neutrinos…

High Energy Physics - Phenomenology · Physics 2009-11-11 Masaru Doi , Tsuneyuki Kotani , Hiroyuki Nishiura

We review the physics of purely leptonic decays of $\pi^\pm$, $K^\pm$, $D^{\pm}$, $D_s^\pm$, and $B^\pm$ pseudoscalar mesons. The measured decay rates are related to the product of the relevant weak-interaction-based CKM matrix element of…

High Energy Physics - Phenomenology · Physics 2016-03-10 Jonathan L. Rosner , Sheldon Stone , Ruth S. Van de Water

Monte Carlo simulation of a 2+1 dimensional model of voltage-biased bilayer graphene, consisting of relativistic fermions with chemical potential mu coupled to charged excitations with opposite sign on each layer, has exposed non-canonical…

Strongly Correlated Electrons · Physics 2015-12-30 Wes Armour , Simon Hands , Costas Strouthos

Hadronic corrections to the muon lifetime are calculated in the Fermi theory in the presence of QED using dispersion relations. The result, after convolution of hadron data with the calculated perturbative kernel is Delta Gamma_had =…

High Energy Physics - Phenomenology · Physics 2009-10-31 Timo van Ritbergen , Robin G. Stuart

The muon anomalous magnetic moment, $a_\mu=\frac{g-2}{2}$, is a low-energy observable which can be both measured and computed to high precision, making it a sensitive test of the Standard Model and a probe for new physics. This anomaly was…

High Energy Physics - Experiment · Physics 2025-03-13 Matteo Sorbara

Ordinary muon capture provides a benchmark for the nuclear physics models of neutrinoless double beta decay under comparable momentum transfer conditions. The total capture strength defines the lifetime of the muonic atom. The muon lifetime…

The new experiment data of muon g-2 is reported by the workers at Fermilab National Accelerator Laboratory(FNAL). Combined with the previous Brookhaven National Laboratory(BNL) E821 result, the departure from the standard model prediction…

High Energy Physics - Phenomenology · Physics 2022-04-13 Shu-Min Zhao , Lu-Hao Su , Xing-Xing Dong , Tong-Tong Wang , Tai-Fu Feng

The next generation of lepton flavor violation experiments need high intensity and high quality muon beams. Production of such beams requires sending a short, high intensity proton pulse to the pion production target, capturing pions and…

A precision measurement of the muon anomalous magnetic moment, $a_{\mu} = (g-2)/2$, was previously performed at BNL with a result of 2.2 - 2.7 standard deviations above the Standard Model (SM) theoretical calculations. The same experimental…

Accelerator Physics · Physics 2013-01-30 C. Yoshikawa , A. Leveling , N. V. Mokhov , J. Morgan , D. Neuffer , S. Striganov

Motivated by the recent developments in the determination of the experimental values of the nucleon axial-vector coupling constant $g_A$ and the pion-nucleon coupling constant $g_{\pi NN}$, we carry out a heavy-baryon chiral perturbation…

Nuclear Theory · Physics 2015-06-17 S. Pastore , F. Myhrer , K. Kubodera

The SHiP experiment is designed to search for very weakly interacting particles beyond the Standard Model which are produced in a 400 GeV/c proton beam dump at the CERN SPS. An essential task for the experiment is to keep the Standard Model…

Instrumentation and Detectors · Physics 2017-05-19 SHiP collaboration , A. Akmete , A. Alexandrov , A. Anokhina , S. Aoki , E. Atkin , N. Azorskiy , J. J. Back , A. Bagulya , A. Baranov , G. J. Barker , A. Bay , V. Bayliss , G. Bencivenni , A. Y. Berdnikov , Y. A. Berdnikov , M. Bertani , C. Betancourt , I. Bezshyiko , O. Bezshyyko , D. Bick , S. Bieschke , A. Blanco , J. Boehm , M. Bogomilov , K. Bondarenko , W. M. Bonivento , A. Boyarsky , R. Brenner , D. Breton , R. Brundler , M. Bruschi , V. Büscher , A. Buonaura , S. Buontempo , S. Cadeddu , A. Calcaterra , M. Campanelli , J. Chauveau , A. Chepurnov , M. Chernyavsky , K. -Y. Choi , A. Chumakov , P. Ciambrone , G. M. Dallavalle , N. D'Ambrosio , G. D'Appollonio , G. De Lellis , A. De Roeck , M. De Serio , L. Dedenko , A. Di Crescenzo , N. Di Marco , C. Dib , H. Dijkstra , V. Dmitrenko , D. Domenici , S. Donskov , A. Dubreuil , J. Ebert , T. Enik , A. Etenko , F. Fabbri , L. Fabbri , O. Fedin , G. Fedorova , G. Felici , M. Ferro-Luzzi , R. A. Fini , P. Fonte , C. Franco , T. Fukuda , G. Galati , G. Gavrilov , S. Gerlach , L. Golinka-Bezshyyko , D. Golubkov , A. Golutvin , D. Gorbunov , S. Gorbunov , V. Gorkavenko , Y. Gornushkin , M. Gorshenkov , V. Grachev , E. Graverini , V. Grichine , A. M. Guler , Yu. Guz , C. Hagner , H. Hakobyan , E. van Herwijnen , A. Hollnagel , B. Hosseini , M. Hushchyn , G. Iaselli , A. Iuliano , R. Jacobsson , M. Jonker , I. Kadenko , C. Kamiscioglu , M. Kamiscioglu , M. Khabibullin , G. Khaustov , A. Khotyantsev , S. H. Kim , V. Kim , Y. G. Kim , N. Kitagawa , J. -W. Ko , K. Kodama , A. Kolesnikov , D. I. Kolev , V. Kolosov , M. Komatsu , N. Konovalova , M. A. Korkmaz , I. Korol , I. Korol'ko , A. Korzenev , S. Kovalenko , I. Krasilnikova , K. Krivova , Y. Kudenko , V. Kurochka , E. Kuznetsova , H. M. Lacker , A. Lai , G. Lanfranchi , O. Lantwin , A. Lauria , H. Lebbolo , K. Y. Lee , J. -M. Lévy , V. Likacheva , L. Lopes , V. Lyubovitskij , J. Maalmi , A. Magnan , V. Maleev , A. Malinin , A. Mefodev , P. Mermod , S. Mikado , Yu. Mikhaylov , D. A. Milstead , O. Mineev , A. Montanari , M. C. Montesi , K. Morishima , S. Movchan , N. Naganawa , M. Nakamura , T. Nakano , A. Novikov , B. Obinyakov , S. Ogawa , N. Okateva , P. H. Owen , A. Paoloni , B. D. Park , L. Paparella , A. Pastore , M. Patel , D. Pereyma , D. Petrenko , K. Petridis , D. Podgrudkov , V. Poliakov , N. Polukhina , M. Prokudin , A. Prota , A. Rademakers , F. Ratnikov , T. Rawlings , M. Razeti , F. Redi , S. Ricciardi , T. Roganova , A. Rogozhnikov , H. Rokujo , G. Rosa , T. Rovelli , O. Ruchayskiy , T. Ruf , V. Samoylenko , A. Saputi , O. Sato , E. S. Savchenko , W. Schmidt-Parzefall , N. Serra , A. Shakin , M. Shaposhnikov , P. Shatalov , T. Shchedrina , L. Shchutska , V. Shevchenko , H. Shibuya , A. Shustov , S. B. Silverstein , S. Simone , M. Skorokhvatov , S. Smirnov , J. Y. Sohn , A. Sokolenko , N. Starkov , B. Storaci , P. Strolin , S. Takahashi , I. Timiryasov , V. Tioukov , N. Tosi , D. Treille , R. Tsenov , S. Ulin , A. Ustyuzhanin , Z. Uteshev , G. Vankova-Kirilova , F. Vannucci , P. Venkova , S. Vilchinski , M. Villa , K. Vlasik , A. Volkov , R. Voronkov , R. Wanke , J. -K. Woo , M. Wurm , S. Xella , D. Yilmaz , A. U. Yilmazer , C. S. Yoon , Yu. Zaytsev

In an explicitly covariant light-front formalism, we analyze transition form factors between pseudoscalar and scalar mesons. Application is performed in case of the $B \to f_0(980)$ transition in the full available transfer momentum range…

High Energy Physics - Phenomenology · Physics 2007-05-23 O. M. A Leitner , B. El-Bennich , B. Loiseau , J. P. Dedonder

The Mu2e experiment measures the conversion rate of muons into electrons and the Muon g-2 experiment measures the muon magnetic moment. Both experiments require 53 MHz batches of 8 GeV protons to be re-bunched into 150 ns, 2.5 MHz pulses…

Accelerator Physics · Physics 2018-03-28 P. Varghese , B. Chase