Advanced Applications of Cosmic-Ray Muon Radiography." (2013)
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Properties of the Lowest-Lying Baryons in Chiral Perturbation Theory Jorge Mart´In Camalich
Properties of the lowest-lying baryons in chiral perturbation theory Jorge Mart´ın Camalich Departamento De F´ısica Te´orica Universidad de Valencia TESIS DOCTORAL VALENCIA 2010 ii iii D. Manuel Jos´eVicente Vacas, Profesor Titular de F´ısica Te´orica de la Uni- versidad de Valencia, CERTIFICA: Que la presente Memoria Properties of the lowest- lying baryons in chiral perturbation theory ha sido realizada bajo mi direcci´on en el Departamento de F´ısica Te´orica de la Universidad de Valencia por D. Jorge Mart´ın Camalich como Tesis para obtener el grado de Doctor en F´ısica. Y para que as´ıconste presenta la referida Memoria, firmando el presente certificado. Fdo: Manuel Jos´eVicente Vacas iv A mis padres y mi hermano vi Contents Preface ix 1 Introduction 1 1.1 ChiralsymmetryofQCD. 1 1.2 Foundations of χPT ........................ 4 1.2.1 Leading chiral Lagrangian for pseudoscalar mesons . 4 1.2.2 Loops, power counting and low-energy constants . 6 1.2.3 Matrix elements and couplings to gauge fields . 7 1.3 Baryon χPT............................. 9 1.3.1 Leading chiral Lagrangian with octet baryons . 9 1.3.2 Loops and power counting in BχPT............ 11 1.4 The decuplet resonances in BχPT................. 14 1.4.1 Spin-3/2 fields and the consistency problem . 15 1.4.2 Chiral Lagrangian containing decuplet fields . 18 1.4.3 Power-counting with decuplet fields . 18 2 Electromagnetic structure of the lowest-lying baryons 21 2.1 Magneticmomentsofthebaryonoctet . 21 2.1.1 Formalism.......................... 22 2.1.2 Results............................ 24 2.1.3 Summary ......................... -
Muon Tomography Sites for Colombian Volcanoes
Muon Tomography sites for Colombian volcanoes A. Vesga-Ramírez Centro Internacional para Estudios de la Tierra, Comisión Nacional de Energía Atómica Buenos Aires-Argentina. D. Sierra-Porta1 Escuela de Física, Universidad Industrial de Santander, Bucaramanga-Colombia and Centro de Modelado Científico, Universidad del Zulia, Maracaibo-Venezuela, J. Peña-Rodríguez, J.D. Sanabria-Gómez, M. Valencia-Otero Escuela de Física, Universidad Industrial de Santander, Bucaramanga-Colombia. C. Sarmiento-Cano Instituto de Tecnologías en Detección y Astropartículas, 1650, Buenos Aires-Argentina. , M. Suárez-Durán Departamento de Física y Geología, Universidad de Pamplona, Pamplona-Colombia H. Asorey Laboratorio Detección de Partículas y Radiación, Instituto Balseiro Centro Atómico Bariloche, Comisión Nacional de Energía Atómica, Bariloche-Argentina; Universidad Nacional de Río Negro, 8400, Bariloche-Argentina and Instituto de Tecnologías en Detección y Astropartículas, 1650, Buenos Aires-Argentina. L. A. Núñez Escuela de Física, Universidad Industrial de Santander, Bucaramanga-Colombia and Departamento de Física, Universidad de Los Andes, Mérida-Venezuela. December 30, 2019 arXiv:1705.09884v2 [physics.geo-ph] 27 Dec 2019 1Corresponding author Abstract By using a very detailed simulation scheme, we have calculated the cosmic ray background flux at 13 active Colombian volcanoes and developed a methodology to identify the most convenient places for a muon telescope to study their inner structure. Our simulation scheme considers three critical factors with different spatial and time scales: the geo- magnetic effects, the development of extensive air showers in the atmosphere, and the detector response at ground level. The muon energy dissipation along the path crossing the geological structure is mod- eled considering the losses due to ionization, and also contributions from radiative Bremßtrahlung, nuclear interactions, and pair production. -
Weak Production of Strangeness and the Electron Neutrino Mass
1 Weak Production of Strangeness as a Probe of the Electron-Neutrino Mass Proposal to the Jefferson Lab PAC Abstract It is shown that the helicity dependence of the weak strangeness production process v νv Λ p(e, e ) may be used to precisely determine the electron neutrino mass. The difference in the reaction rate for two incident electron beam helicities will provide bounds on the electron neutrino mass of roughly 0.5 eV, nearly three times as precise as the current bound from direct-measurement experiments. The experiment makes use of the HKS and Enge Split Pole spectrometers in Hall C in the same configuration that is employed for the hypernuclear spectroscopy studies; the momentum settings for this weak production experiment will be scaled appropriately from the hypernuclear experiment (E01-011). The decay products of the hyperon will be detected; the pion in the Enge spectrometer, and the proton in the HKS. It will use an incident, polarized electron beam of 194 MeV scattering from an unpolarized CH2 target. The ratio of positive and negative helicity events will be used to either determine or put a new limit on the electron neutrino mass. This electroweak production experiment has never been performed previously. 2 Table of Contents Physics Motivation …………………………………………………………………… 3 Experimental Procedure ………………………….………………………………….. 16 Backgrounds, Rates, and Beam Time Request ...…………….……………………… 26 References ………………………………………………………………………….... 31 Collaborators ………………………………………………………………………… 32 3 Physics Motivation Valuable insights into nucleon and nuclear structure are possible when use is made of flavor degrees of freedom such as strangeness. The study of the electromagnetic production of strangeness using both nucleon and nuclear targets has proven to be a powerful tool to constrain QHD and QCD-inspired models of meson and baryon structure, and elastic and transition form factors [1-5]. -
Muon Tomography Algorithms for Nuclear Threat Detection
Muon Tomography Algorithms for Nuclear Threat Detection Richard Hoch 1, Debasis Mitra 1, Kondo Gnanvo 2, and Marcus Hohlmann 2 1D epartment of Computer Science & 2D epartment of Physics and Space Sciences Florida Institute of Technology, Melbourne, Florida, USA [email protected], {rhoch, hohlmann, kgnanvo}@fit.edu Abstract. In this article on Muon Tomography we report our work on the development of an intelligent pattern detection system for materials with high atomic numbers (Z) for Homeland Security application. Muons are naturally produced in the upper atmosphere by primary cosmic rays and are used as passive probes of a cargo volume. By sensing the incoming and outgoing tracks and measuring the momentum of each muon for a probed volume one may derive the scattering parameters. A statistical algorithm is being used to estimate scattering densities of the material in each unit volume (voxel) of the probed volume. The article describes the algorithm and some results from our simulation experiments. 1. Introduction Nuclear materials that pose a homeland security threat typically have high atomic numbers (Z > 82). It is of vital importance to develop smart, efficient, and inexpensive systems to detect such highZ materials without opening a container. Muons are produced by primary cosmic rays at the upper atmosphere provide an excellent source as passive probes for discriminating materials with different Z, without extra radiation or incurring any extra cost for the probe generation. Highly penetrating muon tracks may suffer from multiple scatterings by Coulomb Fig. 1. Scattering of a particle interaction with nuclei of atoms on its path. The amount of scattering depends on the charge Z of the corresponding nucleus [3] (Fig. -
Arxiv:1106.4843V1
Martina Blank Properties of quarks and mesons in the Dyson-Schwinger/Bethe-Salpeter approach Dissertation zur Erlangung des akademischen Grades Doktorin der Naturwissenschaften (Dr.rer.nat.) Karl-Franzens Universit¨at Graz verfasst am Institut f¨ur Physik arXiv:1106.4843v1 [hep-ph] 23 Jun 2011 Betreuer: Priv.-Doz. Mag. Dr. Andreas Krassnigg Graz, 2011 Abstract In this thesis, the Dyson-Schwinger - Bethe-Salpeter formalism is investi- gated and used to study the meson spectrum at zero temperature, as well as the chiral phase transition in finite-temperature QCD. First, the application of sophisticated matrix algorithms to the numer- ical solution of both the homogeneous Bethe-Salpeter equation (BSE) and the inhomogeneous vertex BSE is discussed, and the advantages of these methods are described in detail. Turning to the finite temperature formalism, the rainbow-truncated quark Dyson-Schwinger equation is used to investigate the impact of different forms of the effective interaction on the chiral transition temperature. A strong model dependence and no overall correlation of the value of the transition temperature to the strength of the interaction is found. Within one model, however, such a correlation exists and follows an expected pattern. In the context of the BSE at zero temperature, a representation of the inhomogeneous vertex BSE and the quark-antiquark propagator in terms of eigenvalues and eigenvectors of the homogeneous BSE is given. Using the rainbow-ladder truncation, this allows to establish a connection between the bound-state poles in the quark-antiquark propagator and the behavior of eigenvalues of the homogeneous BSE, leading to a new extrapolation tech- nique for meson masses. -
Muon Tomography for Imaging and Verification of Spent Fuel
IAEA-CN-184/9 Muon Tomography for Imaging and Verification of Spent Fuel G. Jonkmans1, V. N. P. Anghel1, C. Jewett, M. Thompson1 1 Atomic Energy of Canada Limited, Chalk River Labs, Chalk River, Canada [email protected] Abstract This paper explores the use of cosmic ray muons to image the content of, and to detect high-Z Special Fissionable Material inside, shielded containers. Cosmic ray muons are a naturally occurring form of radiation, are highly penetrating and exhibit large scattering angles on high-Z materials. Specifically, we investigated how radiographic and tomographic techniques can be effective for non-invasive nuclear material accountancy of spent fuel inside dry storage containers. We show that the tracking of individual muons, as they enter and exit a structure, can potentially improve the accuracy and availability of data on Dry Storage Containers (DSC) used for spent fuel storage at CANDU plants. This could be achieved in near real time, with the potential for unattended and remotely monitored operations. We show that the expected sensitivity to perform material accountancy, in the case of the DSC, exceeds the IAEA detection target for nuclear material accountancy. 1. Introduction Because of their unique ability to penetrate matter, cosmic ray muons can be used to image the interior of structures. Recently, a number of groups have extended the concept of muon radiography to the tracking of individual muons as they enter and exit a structure. Most current efforts have been toward demonstrating the potential for muon tomography to detect the smuggling of Special Nuclear Material (SFM) in cargo. This paper explores the application of muon tomography for nuclear material accountancy of spent fuel inside Dry Storage Containers (DSC) used to store spent CANDU® fuel. -
Imaging the Core of Fukushima Reactor with Muons
MUON TOMOGRAPHY IMAGING THE CORE OF FUKUSHIMA REACTOR WITH MUONS The 9.0-magnitude earthquake, followed by the vast tsunami on March 11, 2011, caused a nuclear crisis at the Fukushima Daiichi reactors. Damage of the reactor cores attracted worldwide attention to the issue of the fundamental safety of nuclear energy. The Japanese government announced a cold shutdown in December 2011, and began a new phase of cleanup and decommissioning. However, it is difficult to plan the dismantling of the reactors without a used experiments and modeling to show how muon imaging with de- realistic estimate of the extent of the damage to the cores and knowl- tectors external to the reactors can enable damage assessment inside edge of the location of the melted fuel. Access to the reactor buildings Fukushima. Physical Review Letters, AIP Advances, and the Journal of is very limited due to high radiation fields. Los Alamos researchers have Applied Physics have published different aspects of this work. Image from “Los Alamos, Toshiba probing Fukushima with cosmic rays,” Los Alamos National Laboratory YouTube video. Muon imaging offers the potential to image the nuclear reactor cores with- out access to the cores. The method utilizes naturally occurring cosmic-ray muons to image dense objects. There are two types of muon imaging: transmission and scattering. In practical applications, muon transmission imaging often suffers from poor position resolution due to the continuous scattering along the muon path, and from poor signal-to-noise ratio due to the small detection area (typically on the order of 2 m2). In addition, calcu- lating transmission requires precise knowledge the incident muon flux that can be difficult to estimate. -
Muon Geotomography: Selected Case Studies Rsta.Royalsocietypublishing.Org Doug Schouten
Muon geotomography: selected case studies rsta.royalsocietypublishing.org Doug Schouten CRM Geotomography Technologies, Inc., 4004 Wesbrook Mall, Review Vancouver, Canada DS, 0000-0002-0452-6320 Cite this article: Schouten D. 2018 Muon geotomography: selected case studies. Phil. Muon attenuation in matter can be used to infer the average material density along the path length Trans. R. Soc. A 377: 20180061. of muons underground. By mapping the intensity http://dx.doi.org/10.1098/rsta.2018.0061 of cosmic ray muons with an underground sensor, a radiographic image of the overburden above the Accepted: 12 October 2018 sensor can be derived. Multiple such images can be combined to reconstruct a three-dimensional density model of the subsurface. This article One contribution of 22 to a Theo Murphy summarizes selected case studies in applying muon meeting issue ‘Cosmic-ray muography’. tomography to mineral exploration, which we call muon geotomography. Subject Areas: This article is part of the Theo Murphy meeting geophysics, high energy physics, issue ‘Cosmic-ray muography’. particle physics Keywords: 1. Introduction muon tomography, muon geotomography, geophysics Muon radiography is a means of inferring average material density by measuring the attenuation of muons along a path length through matter. Muon tomography Author for correspondence: uses tomographic methods to derive three-dimensional Doug Schouten density maps from multiple muon radiographic images. e-mail: [email protected] Measurements of the muon intensity attenuation were first used by George [1] to measure the overburden of a railway tunnel, and by Alvarez et al. [2]insearches for hidden chambers within pyramids. More recently, muon radiography has been used in volcanology [3–7], in mineral exploration [8,9] and in various other industrial and security applications as summarized in [10]. -
Measuring Particle Collisions Fundamental
From Last Time… Something unexpected • Particles are quanta of a quantum field • Raise the momentum and the electrons and see – Represent excitations of the associated field what we can make. – Particles can appear and disappear • Might expect that we make a quark and an • Particles interact by exchanging other particles antiquark. The particles that make of the proton. – Electrons interact by exchanging photons – Guess that they are 1/3 the mass of the proton 333MeV • This is the Coulomb interaction µ, Muon mass: 100MeV/c2, • Electrons are excitations of the electron field electron mass 0.5 MeV/c2 • Photons are excitations of the photon field • Today e- µ- Instead we get a More particles! muon, acts like a heavy version of Essay due Friday µ + the electron e+ Phy107 Fall 2006 1 Phy107 Fall 2006 2 Accelerators CERN (Switzerland) • What else can we make with more energy? •CERN, Geneva Switzerland • Electrostatic accelerator: Potential difference V accelerate electrons to 1 MeV • LHC Cyclic accelerator • Linear Accelerator: Cavities that make EM waves • 27km, 14TeV particle surf the waves - SLAC 50 GeV electrons 27 km 7+7=14 • Cyclic Accelerator: Circular design allows particles to be accelerated by cavities again and again – LEP 115 GeV electrons – Tevatron 1 TeV protons – LHC 7 TeV protons(starts next year) Phy107 Fall 2006 3 Phy107 Fall 2006 4 Measuring particle collisions Fundamental Particles Detectors are required to determine the results of In the Standard Model the basic building blocks are the collisions. said to be ‘fundamental’ or not more up of constituent parts. Which particle isn’t ‘fundamental’: A. -
An Abstract of the Dissertation Of
AN ABSTRACT OF THE DISSERTATION OF Can Liao for the degree of Doctor of Philosophy in Nuclear Engineering presented on May 31, 2018. Title: A Cosmic-ray Muon Tomography System for Safeguarding Dry Storage Casks. Abstract approved: ______________________________________________________ Haori Yang Because of the growth of the nuclear power industry in the United States and the policy to ban reprocessing of commercial spent nuclear fuel, the spent fuel inventory at commercial reactor sites has been increasing. With the Yucca Mountain project on hold, more spent fuel is expected to be stored in dry storage casks (DSC) at the independent spent fuel storage installation (ISFSI) for extended periods of time. These fuel assemblies are practically inaccessible for inspection purposes, as reopening a DSC would require special facilities and be tremendously expensive. There is currently no practical method to verify the content of a DSC once continuity of knowledge is lost, but cosmic ray muon imaging is under development as a method that could meet this need. Imaging with these muons has been demonstrated to be a viable non-destructive assay method for high-Z materials, such as those inside used nuclear fuel assemblies. Most often a gas-based detector system has been used. In this work, we report on a proof-of-concept muon tomography system made out of plastic scintillator and wavelength shifting (WLS) fibers. The prototype muon tomography system was designed, built, assembled and tested for the purpose of monitoring used nuclear fuel content inside dry storage casks. First, the simulation study suggested muon was a promising tool to image dense objects and benchmarked the idea of utilizing the muon image for cask inspection. -
Imaging a Dry Storage Cask with Cosmic Ray Muons
Project No. 14-6656 Imaging a Dry Storage Cask with Cosmic Ray Muons Fuel Cycle Research and Development Haori Yang Oregon State University Collaborators University of Tennessee, Knoxville Dan Vega, Federal POC Mike Miller, Technical POC Final Technical Report Project Title: Imaging a Dry Storage Cask with Cosmic Ray Muons Covering Period: October 2014 through December 2017 Date of Report: Mar. 31, 2018 Recipient: Oregon State University B308 Kerr Administration Corvallis, OR 97331 Identification Number: DE-NE0008292 Principal Investigator: Haori Yang, 541-737-7057, [email protected] Co-PI: Jason Hayward, University of Tennessee, Knoxville (UTK); David Chichester, Idaho National Laboratory (INL) Graduate Students: Can Liao, [email protected] Zhengzhi Liu, [email protected] Project Objective: The goal of this project is to build a scaled prototype system for monitoring used nuclear fuel (UNF) dry storage casks (DSCs) through cosmic ray muon imaging. Such a system will have the capability of verifying the content inside a DSC without opening it. Because of the growth of the nuclear power industry in the U.S. and the policy decision to ban reprocessing of commercial UNF, the used fuel inventory at commercial reactor sites has been increasing. Currently, UNF needs to be moved to independent spent fuel storage installations (ISFSIs), as its inventory approaches the limit on capacity of on-site wet storage. Thereafter, the fuel will be placed in shipping containers to be transferred to a final disposal site. The ISFSIs were initially licensed as temporary facilities for ~20-yr periods. Given the cancellation of the Yucca mountain project and no clear path forward, extended dry-cask storage (~100 yr.) at ISFSIs is very likely. -
Creation of a Geant4 Muon Tomography Package for Imaging of Nuclear Fuel in Dry Cask Storage
Project No. 13-5376 Creation of a Geant4 Muon Tomography Package for Imaging of Nuclear Fuel in Dry Cask Storage Fuel Cycle Research and Development Leeri Tsoukalas Purdue University Dan Vegas, Federal POC Mike Miller, Technical POC PURDUE UNIVERSITY School of Nuclear Engineering 400 Central Drive West Lafayette, IN 47907 FINAL REPORT Project Title: Creation of a Geant4 Muon Tomography Package for Imaging of Nuclear Fuel in Dry Cask Storage (13-5376) Institution: School of Nuclear Engineering, Purdue University Workscope: FC-3 PICSNE Workpackage: NU-13-IN-PU__0301-03 Project Period: December 1, 2013 to November 30, 2015 Principal Investigator: Prof. Lefteri H. Tsoukalas, 765-496-9696, [email protected] West Lafayette, IN March 2016 ii PURDUE UNIVERSITY Document No: School of Nuclear Engineering Document Title: Final Report DOCUMENT REVISION SHEET Revision Description of Date Initials Notes Revision Prepared Reviewed 1 Original Version March 2016 SC LHT For submission to NEUP File Name: NEUP_Project_13-5376_FY2013_Final Report Revision: 1 iii Executive Summary This is the final report of the NEUP project “Creation of a Geant4 Muon Tomography Package for Imaging of Nuclear Fuel in Dry Cask Storage”, DE-NE0000695. The project started on December 1, 2013 and this report covers the period December 1, 2013 through November 30, 2015. The project was successfully completed and this report provides an overview of the main achievements, results and findings throughout the duration of the project. Additional details can be found in the main body of this report and on the individual Quarterly Reports and associated Deliverables of the project, uploaded in PICS-NE.