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Journal articles on the topic 'Electron and muon capture'

Author: Grafiati

Published: 2 June 2025

Last updated: 31 July 2025

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1

Ahmad, S., O. Häusser, J. A. Macdonald, et al. "Muon-induced fission in 235U and 238U." Canadian Journal of Physics 64, no. 6 (1986): 665–70. http://dx.doi.org/10.1139/p86-123.

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Muon-induced prompt and delayed fission yields in 235U and 238U have been measured. A coincidence with the muonic uranium Kα X-rays was used to identify the muon stop in the target. The experimental absolute fission yields per muon stop were 0.142 ± 0.023 for 235U and 0.068 ± 0.013 for 238U. The disappearance rate of muons from the 1s state of muonic uranium has also been measured in the fission mode. Muon-induced fission lifetimes were 71.6 ± 0.6 ns for 235U and 77.2 ± 0.4 ns for 238U. No evidence for a short-lifetime fission – isomer component was found. Comparison of lifetime results with p

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2

Glushkov, A. V. "RELATIVISTIC THEORY OF THE NEGATIVE MUON CAPTURE BY AN ATOM." Photoelectronics, no. 25 (December 25, 2016): 12–19. http://dx.doi.org/10.18524/0235-2435.2016.25.157523.

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We reviewed a new effective consistent approach to determination of the cross-section for the negative muon capture by an atomic system. The approach is based on the relativistic many-body perturbation (PT) theory with using the Feynman diagram technique and a generalized relativistic energy approach in a gauge-invariant formulation. The corresponding capture cross-section is connected with an imaginary (scattering) part of the electron subsystem energy shift ImδE (till the QED perturbation theory order). The some calculation results for cross-section of the negative muon m-capture by He atom

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3

Zhao, X., M. W. Heiss, F. Garcia, et al. "Drift time calibration of the ultra-low material budget GEM-based TPC for MIXE." Journal of Instrumentation 20, no. 06 (2025): C06067. https://doi.org/10.1088/1748-0221/20/06/c06067.

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Abstract Muon-Induced X-ray Emission (MIXE) is a non-destructive analytical technique that leverages negative muons to probe elemental and isotopic compositions by detecting characteristic muonic X-rays emitted during atomic cascades and gamma rays from nuclear capture processes. By controlling the muon beam momentum, MIXE enables depth-resolved analysis, spanning microns to centimeters, making it ideal for studying compositional variations in fragile, valuable, or operando samples. To enhance its capabilities, we integrated a twin Time Projection Chamber (TPC) tracker with Gas Electron Multip

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4

Holmlid, Leif. "Charge Asymmetry of Muons Generated in a Muon Generator from Ultra-Dense Hydrogen D(0) and p(0)." Particles 6, no. 1 (2023): 188–97. http://dx.doi.org/10.3390/particles6010010.

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Laser-induced nuclear reactions in ultra-dense hydrogen H(0) (review in Physica Scripta 2019) create mesons (kaons and pions). These mesons decay mainly to muons. The muons created are useful (patented source) for the muon-induced fusion process. The sign of the muons from the source depends on the initial baryons used. With D(0) (ultra-dense deuterium) the source produces mainly positive muons and with p(0) (ultra-dense protium) the source produces mainly negative muons. Negative muons are required for muon-induced fusion. This charge asymmetry was reported earlier, and has now been confirmed

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5

Moritsu, Manabu. "Search for Muon-to-Electron Conversion with the COMET Experiment." Universe 8, no. 4 (2022): 196. http://dx.doi.org/10.3390/universe8040196.

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Charged Lepton Flavor Violation is expected to be one of the most powerful tools to reveal physics beyond the Standard Model. The COMET experiment aims to search for the neutrinoless coherent transition of a muon into an electron in the field of a nucleus. Muon-to-electron conversion has never been observed, and can be, and would be, clear evidence of new physics if discovered. The experimental sensitivity of this process, defined as the ratio of the muon-to-electron conversion rate to the total muon capture rate, is expected to be significantly improved by a factor of 100 to 10,000 in the com

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6

Gmitro, M., and A. A. Ovchinnikova. "Continuity-equation constraint for electron scattering and radiative muon capture." Czechoslovak Journal of Physics 36, no. 3 (1986): 390–94. http://dx.doi.org/10.1007/bf01597844.

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7

Jacot-Guillarmod, R., F. Bienz, M. Boschung, et al. "Muon capture through bonding electrons in pure silicon." Physical Review A 38, no. 6 (1988): 3106–8. http://dx.doi.org/10.1103/physreva.38.3106.

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8

Milojevic, Nenad, Ivan Mancev, and Milos Milenkovic. "Single-electron capture in collisions of positively charged muons with hydrogen and helium atoms." Facta universitatis - series: Physics, Chemistry and Technology 21, no. 1 (2023): 47–55. http://dx.doi.org/10.2298/fupct2301047m.

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The prior form of the three-body boundary-corrected first Born (CB1-3B) method is used to calculate the state-selective total cross sections for single-electron capture into 1s, 2s and 2s final states of a fast muon projectiles from a ground-state hydrogen and helium targets at energies 10 keV to 1 MeV. For helium target, the frozencore approximation and the independent particles model were used. The state-summed total cross sections for electron capture into all final states of the muonium systems (?+,e) are obtained by applying the Oppenheimer (n?3) scaling law. Unfortunately, there are no a

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9

Beder, Douglas. "Estimates of eē production from nuclear muon capture." Canadian Journal of Physics 63, no. 2 (1985): 154–58. http://dx.doi.org/10.1139/p85-025.

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Motivated by the experimental search for μ−A → e−A, we calculate [Formula: see text], which provides a small background of high-energy electrons, limiting experimental sensitivity. A reasonable extrapolation to the nuclear case, for a Ti target, indicates an effective background for Ee > 95 MeV of approximately 2 × 10−12 (branching ratio to total capture rate).

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10

Kosmas, T. S., and E. Oset. "Inclusive neutrino-nucleus reaction cross sections at intermediate energies." HNPS Proceedings 5 (February 19, 2020): 29. http://dx.doi.org/10.12681/hnps.2892.

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Inclusive neutrino-nucleus reaction cross sections at intermediate energies (20 MeV < Ey < 500 MeV) are calculated throughout the periodic table for the most interesting nu clei from an experimental point of view. The method used had previously proved to be very accurate in calculating the induced reaction cross section for T=0 light nuclei (12C and 16O) and in the study of other similar processes like the ordinary muon capture. The electron-neutrino (ve) cross section weighted by the Michel distribution is also discussed in conjuction with the existing experimental results at LAMPF and

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11

Atanov, N., V. Baranov, L. Borrel, et al. "Towards the construction of the Mu2e electromagnetic calorimeter at Fermilab." Journal of Physics: Conference Series 2374, no. 1 (2022): 012021. http://dx.doi.org/10.1088/1742-6596/2374/1/012021.

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Mu2e will search for the Charge Lepton Flavor Violating (CLFV) conversion of a muon into an electron in the field of a nucleus. A clean discovery signature is provided by the mono-energetic conversion electron (Ee = 104.96 MeV). If no events are observed, Mu2e will set a limit on the ratio between the conversion and the nuclear capture rate below 3 × 10−17 (at 90% C.L.). In order to confirm that the observed candidate is an electron, the calorimeter resolution requirements are to provide Eres < 10%, Tres < 500 ps for 100 MeV electrons while working in vacuum and in a high radiation envir

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12

Panagiotides, N., and T. S. Kosmas. "A Study of $\tau^-$ and $\mu^-$ in the Field of Nuclei Using Neural Network Techniques." HNPS Advances in Nuclear Physics 12 (August 30, 2021): 130. http://dx.doi.org/10.12681/hnps.3352.

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The rate of a heavy lepton (muon or tau) capture by nuclei as well as the heavy lepton to electron conversion rate can be calculated when the heavy lepton wavefunction is known. Analytical calculation of the wavefunction of any of these leptons around any nucleus is not feasible owning to their small Bohr radii, on the one hand, and to the finite nuclear extend on the other. A new numerical calculation algorithm is proposed hereby, which makes use of the concept of neural networks. The main advantage of this new technique is that the wave function is produced analytically as a sum of sigmoid f

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13

Hou, Zhilong, Ye Yuan, Jingyu Tang, et al. "Conceptual Design of the Capture Superconducting Solenoid for Experimental Muon Source." IEEE Transactions on Applied Superconductivity 30, no. 5 (2020): 1–7. http://dx.doi.org/10.1109/tasc.2020.2970226.

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14

ZIMMERMANN, FRANK. "R&D FOR FUTURE ACCELERATORS." International Journal of Modern Physics A 21, no. 08n09 (2006): 1987–99. http://dx.doi.org/10.1142/s0217751x06032927.

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Research & development for future accelerators are reviewed. First, I discuss colliding hadron beams, in particular upgrades to the Large Hadron Collider (LHC). This is followed by an overview of new concepts and technologies for lepton ring colliders, with examples taken from VEPP-2000, DAFNE-2, and Super-KEKB. I then turn to recent progress and studies for the multi-TeV Compact Linear Collider (CLIC). Some generic linear-collider research, centered at the KEK Accelerator Test Facility, is described next. Subsequently, I survey the neutrino factory R&D performed in the framework of th

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15

Kanishka, R., Supratik Mukhopadhyay, Nayana Majumdar, and Sandip Sarkar. "Primary Ionization Simulation for Different Gas Mixtures." Journal of Physics: Conference Series 2349, no. 1 (2022): 012019. http://dx.doi.org/10.1088/1742-6596/2349/1/012019.

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The primary ionization in a gas mixture is crucial in nuclear and particle physics experiments. In many particle physics experiments, the primary ionization is utilized in understanding the charge density and discharge formation studies. We present the simulation of primary ionization in argon based gas mixtures to get the number of primaries, energy and spatial information with geant4 and heed++ toolkits that have been used to simulate the passage of particles through the matter. The geant4 toolkit has an advantage of obtaining the particle information like energy deposition and position co-o

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16

Garcia, Luis Guillermo, Romina Soledad Molina, Maria Liz Crespo, et al. "Muon–Electron Pulse Shape Discrimination for Water Cherenkov Detectors Based on FPGA/SoC." Electronics 10, no. 3 (2021): 224. http://dx.doi.org/10.3390/electronics10030224.

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The distinction of secondary particles in extensive air showers, specifically muons and electrons, is one of the requirements to perform a good measurement of the composition of primary cosmic rays. We describe two methods for pulse shape detection and discrimination of muons and electrons implemented on FPGA. One uses an artificial neural network (ANN) algorithm; the other exploits a correlation approach based on finite impulse response (FIR) filters. The novel hls4ml package is used to build the ANN inference model. Both methods were implemented and tested on Xilinx FPGA System on Chip (SoC)

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17

Kusakabe, Motohiko, Grant J. Mathews, Toshitaka Kajino, and Myung-Ki Cheoun. "Review on effects of long-lived negatively charged massive particles on Big Bang Nucleosynthesis." International Journal of Modern Physics E 26, no. 08 (2017): 1741004. http://dx.doi.org/10.1142/s021830131741004x.

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We review important reactions in the Big Bang Nucleosynthesis (BBN) model involving a long-lived negatively charged massive particle, [Formula: see text], which is much heavier than nucleons. This model can explain the observed 7Li abundances of metal-poor stars, and predicts a primordial 9Be abundance that is larger than the standard BBN prediction. In the BBN epoch, nuclei recombine with the [Formula: see text] particle. Because of the heavy [Formula: see text] mass, the atomic size of bound states [Formula: see text] is as small as the nuclear size. The nonresonant recombination rates are t

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18

Kiyotani, Tamiko, Masayoshi Kobayashi, Ichiro Tanaka, and Nobuo Niimura. "Observation of electron transfer associated with enzymatic process by muSR." Acta Crystallographica Section A Foundations and Advances 70, a1 (2014): C1463. http://dx.doi.org/10.1107/s2053273314085362.

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We propose muSR experiments on trypsin-BPTI complex to visualize the electron and proton transfer processes occurring in the catalytic reaction of the trypsin. The mechanism of an inhibitory effect of the BPTI is interpreted that the reaction products of BPTI remain at a part of the structure and the reverse reaction reforms the stable trypsin–BPTI complex, which has been confirmed by neutron diffraction experiment of the trypsin-BPTI complex [1]. However, it never sees the real image of the proton and electron transfer processes directly. According to the model provided by the results of neut

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19

Shoukavy, D. V., D. N. Grigoriev, and D. S. Vasileuskaya. "The method of events separation with overlapping signals." Proceedings of the National Academy of Sciences of Belarus. Physics and Mathematics Series 57, no. 4 (2021): 470–78. http://dx.doi.org/10.29235/1561-2430-2021-57-4-470-478.

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In this paper, we propose a method for the rejection of the background from the superposition of signals from different, almost simultaneously occurring events in the calorimeter for the COMET experiment. The basic idea is to use the chi-squared distribution obtained from fitting the recorded shape of the signal with an average waveform. The elaborated method is applied for the reconstruction of events with overlapping signals from the electron and radiative capture of neutrons by the 175Lu nucleus, as well as overlapping signals from two electrons born as a result of the decay of muons in the

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20

Zacharias, M., A. Reimer, C. Boisson, and A. Zech. "ExHaLe-jet: an extended hadro-leptonic jet model for blazars – I. Code description and initial results." Monthly Notices of the Royal Astronomical Society 512, no. 3 (2022): 3948–71. http://dx.doi.org/10.1093/mnras/stac754.

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ABSTRACT The processes operating in blazar jets are still an open question. Modelling the radiation emanating from an extended part of the jet allows one to capture these processes on all scales. Kinetic codes solving the Fokker–Planck equation along the jet flow are well suited to this task, as they can efficiently derive the radiation and particle spectra without the need for computationally demanding plasma physical simulations. Here, we present a new extended hadro-leptonic jet code – ExHaLe-jet– which considers simultaneously the processes of relativistic protons and electrons. Within a p

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21

Ferroni, Fernando. "LUCIFER: A new technique for Double Beta Decay." Il Nuovo cimento della Societa italiana di fisica. C 33, no. 5 (2011): 27–34. https://doi.org/10.1393/ncc/i2011-10696-1.

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LUCIFER (Low-background Underground Cryogenic Installation For Elusive Rates) is a new project aiming to study the neutrinoless Double Beta Decay. It will be based on the technology of the scintillating bolometers. These devices shall have a great power in distinguishing signals from α’s and β/γ’s promising a background-free experiment, provided that the Q value of the candidate isotope is higher than the 208Tl line. The baseline candidate for LUCIFER is 82Se. Here the LUCIFER concept will be introduced and the prospects related to this project will be discussed.

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22

Asres, Mulugeta Weldezgina, Christian Walter Omlin, Long Wang, et al. "Spatio-Temporal Anomaly Detection with Graph Networks for Data Quality Monitoring of the Hadron Calorimeter." Sensors 23, no. 24 (2023): 9679. http://dx.doi.org/10.3390/s23249679.

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The Compact Muon Solenoid (CMS) experiment is a general-purpose detector for high-energy collision at the Large Hadron Collider (LHC) at CERN. It employs an online data quality monitoring (DQM) system to promptly spot and diagnose particle data acquisition problems to avoid data quality loss. In this study, we present a semi-supervised spatio-temporal anomaly detection (AD) monitoring system for the physics particle reading channels of the Hadron Calorimeter (HCAL) of the CMS using three-dimensional digi-occupancy map data of the DQM. We propose the GraphSTAD system, which employs convolutiona

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23

Kammel, Peter, and Kuniharu Kubodera. "Precision Muon Capture." Annual Review of Nuclear and Particle Science 60, no. 1 (2010): 327–53. http://dx.doi.org/10.1146/annurev-nucl-100809-131946.

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24

Chiang, H. C., E. Oset, and P. Fernández De Córdoba. "Muon capture revisited." Nuclear Physics A 510, no. 4 (1990): 591–608. http://dx.doi.org/10.1016/0375-9474(90)90350-u.

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25

Soln, Josip. "Limiting Velocities of Primary, Obscure and Normal Particles: Self-Annihilating Obscure Particle as an Example of Dark Matter Particle." Applied Physics Research 8, no. 5 (2016): 1. http://dx.doi.org/10.5539/apr.v8n5p1.

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From recently established bicubic equation, three particle limiting velocities are derived, primary, c1,obscure, c2 and normal, c3,that in principle may belong to a single particle. The values of limiting velocities are governed by the congruent particle parameter, z = 3\sqrt3mv2=2E, with m; v and E being, respectively, particle mass, velocity and energy, generally satisfying 1 &lt;= z &lt;= 1, and here just 0 &lt;= z &lt;= 1.<br />While c3 is practically the same in value as v, c1 and c2 can depart from v as z changes from 1 to 0, since c1, c2 and c3; are, in forms, expl

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26

HWANG, W. Y. P., and B. J. LIN. "MUON CAPTURE IN DEUTERIUM." International Journal of Modern Physics E 08, no. 02 (1999): 101–6. http://dx.doi.org/10.1142/s0218301399000070.

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Muon capture in deuterium, μ-+ D →νμ+n+n, is a weak process of fundamental importance. The capture rate depends critically on the spin configuration of the initial (μ D ) state, which is in turn related closely to the availability of having two nearby deuteron nuclei. In this paper, we calculate the capture rates from the doublet [Formula: see text] and quartet [Formula: see text] hyperfine states. In addition to using the gaseous or liquid deuterium target, we wish also to propose to employ the deuterated target such as PdD or TiD to carry out the muon capture measurement, since it is known t

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27

Winter, Peter. "Muon capture at PSI." Physics Procedia 17 (2011): 239–44. http://dx.doi.org/10.1016/j.phpro.2011.06.042.

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28

Ricci, P., E. Truhlík, B. Mosconi, and J. Smejkal. "Muon capture in deuterium." Nuclear Physics A 837, no. 1-2 (2010): 110–44. http://dx.doi.org/10.1016/j.nuclphysa.2010.02.009.

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29

Kammel, Peter. "Muon capture in hydrogen." Nuclear Physics A 844, no. 1-4 (2010): 181c—184c. http://dx.doi.org/10.1016/j.nuclphysa.2010.05.032.

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30

Christillin, P., and M. Gmitro. "Radiative muon capture on." Physics Letters B 150, no. 1-3 (1985): 50–52. http://dx.doi.org/10.1016/0370-2693(85)90135-2.

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31

Deutsch, Jules. "The future of muon physics: Nuclear muon capture." Zeitschrift für Physik C Particles and Fields 56, S1 (1992): S143—S145. http://dx.doi.org/10.1007/bf02426788.

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32

Wang, Ling, and Mu-ming Poo. "Yifang Wang: high energy physics in China." National Science Review 3, no. 2 (2016): 252–56. http://dx.doi.org/10.1093/nsr/nww033.

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Abstract On 8 March 2012, Yifang Wang, co-spokesperson of the Daya Bay Experiment and Director of Institute of High Energy Physics, Chinese Academy of Sciences, announced the discovery of a new type of neutrino oscillation with a surprisingly large mixing angle (θ13), signifying ‘a milestone in neutrino research’. Now his team is heading for a new goal—to determine the neutrino mass hierarchy and to precisely measure oscillation parameters using the Jiangmen Underground Neutrino Observatory, which is due for completion in 2020. Neutrinos are fundamental particles that play important roles in b

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33

Filchenkov, V. V. "Physical applications of muon catalysis: Muon capture in hydrogen." Physics of Particles and Nuclei 47, no. 4 (2016): 591–626. http://dx.doi.org/10.1134/s1063779616040055.

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34

Kardaras, I. S., V. N. Stavrou, I. G. Tsoulos, and T. S. Kosmas. "Nuclear muon capture rates by using relativistic muon wavefunctions." HNPS Proceedings 18 (November 23, 2019): 55. http://dx.doi.org/10.12681/hnps.2538.

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35

Zinatulina, D. R., Ch Briançon, V. B. Brudanin, et al. "Negative-muon capture in 150Sm." Bulletin of the Russian Academy of Sciences: Physics 74, no. 6 (2010): 825–28. http://dx.doi.org/10.3103/s1062873810060201.

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36

Marcucci, Laura Elisa. "Muon capture on light nuclei." Journal of Physics: Conference Series 336 (December 28, 2011): 012026. http://dx.doi.org/10.1088/1742-6596/336/1/012026.

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37

Moftah, B. A., E. Gete, D. F. Measday, et al. "Muon capture in 28Si and." Physics Letters B 395, no. 3-4 (1997): 157–62. http://dx.doi.org/10.1016/s0370-2693(97)00081-6.

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38

Bertl, W., S. Ahmad, D. S. Armstrong, et al. "Radiative muon capture on hydrogen." Zeitschrift für Physik C Particles and Fields 56, S1 (1992): S150—S155. http://dx.doi.org/10.1007/bf02426790.

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39

Döbeli, M., M. Doser, L. van Elmbt, et al. "Radiative muon capture in nuclei." Physical Review C 37, no. 4 (1988): 1633–46. http://dx.doi.org/10.1103/physrevc.37.1633.

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40

Marcucci, L. E., and M. Piarulli. "Muon Capture on Light Nuclei." Few-Body Systems 49, no. 1-4 (2010): 35–39. http://dx.doi.org/10.1007/s00601-010-0157-x.

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41

Huan Ching, Chiang, and Eulogio Oset. "Neutron densities from muon capture." Nuclear Physics A 532, no. 3-4 (1991): 647–56. http://dx.doi.org/10.1016/0375-9474(91)90602-3.

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42

Ahmad, S., G. Azuelos, M. Blecher, et al. "Search for muon-electron and muon-positron conversion." Physical Review D 38, no. 7 (1988): 2102–20. http://dx.doi.org/10.1103/physrevd.38.2102.

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43

Jändel, Magnus. "Density dependence of convoy-muon capture after muon-catalyzed fusion." Physical Review A 43, no. 1 (1991): 598–600. http://dx.doi.org/10.1103/physreva.43.598.

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44

Lu, Meng, Andrew Michael Levin, Congqiao Li, et al. "The Physics Case for an Electron-Muon Collider." Advances in High Energy Physics 2021 (February 25, 2021): 1–6. http://dx.doi.org/10.1155/2021/6693618.

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An electron-muon collider with an asymmetric collision profile targeting multi-ab-1 integrated luminosity is proposed. This novel collider, operating at collision energies of, e.g., 20–200 GeV, 50–1000 GeV, and 100–3000 GeV, would be able to probe charged lepton flavor violation and measure Higgs boson properties precisely. The collision of an electron and muon beam leads to less physics background compared with either an electron-electron or a muon-muon collider, since electron-muon interactions proceed mostly through higher-order vector boson fusion and vector boson scattering processes. The

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45

Kurup, A. "Muon to electron conversion: how to find an electron in a muon haystack." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 368, no. 1924 (2010): 3645–55. http://dx.doi.org/10.1098/rsta.2010.0058.

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The standard model (SM) of particle physics describes how the Universe works at a fundamental level. Even though this theory has proven to be very successful over the past 50 years, we know it is incomplete. Many theories that go beyond the SM predict the occurrence of certain processes that are forbidden by the SM, such as muon to electron conversion. This paper will briefly review the history of muon to electron conversion and focus on the high-precision experiments currently being proposed, COMET (Coherent Muon to Electron Transition) and Mu2e, and a next-generation experiment, PRISM. The P

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46

Adams, D., A. Alekou, M. Apollonio, et al. "Electron-muon ranger: performance in the MICE muon beam." Journal of Instrumentation 10, no. 12 (2015): P12012. http://dx.doi.org/10.1088/1748-0221/10/12/p12012.

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47

Elmeshneb, A. E. "Muon capture on the deuteron and3He." EPJ Web of Conferences 81 (2014): 06004. http://dx.doi.org/10.1051/epjconf/20148106004.

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48

Luo, Xiao. "MuSun: muon capture on the deuteron." EPJ Web of Conferences 95 (2015): 04037. http://dx.doi.org/10.1051/epjconf/20159504037.

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49

Congleton, J. G. "Hyperfine populations prior to muon capture." Physical Review A 48, no. 1 (1993): R12—R14. http://dx.doi.org/10.1103/physreva.48.r12.

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50

Gmitro, M., O. Richter, H. R. Kissener, and A. A. Ovchinnikova. "Ordinary and radiative muon capture onN14." Physical Review C 43, no. 3 (1991): 1448–53. http://dx.doi.org/10.1103/physrevc.43.1448.

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