Antiproton Flux and Properties of Elementary Particle Fluxes In
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The Five Common Particles
The Five Common Particles The world around you consists of only three particles: protons, neutrons, and electrons. Protons and neutrons form the nuclei of atoms, and electrons glue everything together and create chemicals and materials. Along with the photon and the neutrino, these particles are essentially the only ones that exist in our solar system, because all the other subatomic particles have half-lives of typically 10-9 second or less, and vanish almost the instant they are created by nuclear reactions in the Sun, etc. Particles interact via the four fundamental forces of nature. Some basic properties of these forces are summarized below. (Other aspects of the fundamental forces are also discussed in the Summary of Particle Physics document on this web site.) Force Range Common Particles It Affects Conserved Quantity gravity infinite neutron, proton, electron, neutrino, photon mass-energy electromagnetic infinite proton, electron, photon charge -14 strong nuclear force ≈ 10 m neutron, proton baryon number -15 weak nuclear force ≈ 10 m neutron, proton, electron, neutrino lepton number Every particle in nature has specific values of all four of the conserved quantities associated with each force. The values for the five common particles are: Particle Rest Mass1 Charge2 Baryon # Lepton # proton 938.3 MeV/c2 +1 e +1 0 neutron 939.6 MeV/c2 0 +1 0 electron 0.511 MeV/c2 -1 e 0 +1 neutrino ≈ 1 eV/c2 0 0 +1 photon 0 eV/c2 0 0 0 1) MeV = mega-electron-volt = 106 eV. It is customary in particle physics to measure the mass of a particle in terms of how much energy it would represent if it were converted via E = mc2. -
Interactions of Antiprotons with Atoms and Molecules
University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln US Department of Energy Publications U.S. Department of Energy 1988 INTERACTIONS OF ANTIPROTONS WITH ATOMS AND MOLECULES Mitio Inokuti Argonne National Laboratory Follow this and additional works at: https://digitalcommons.unl.edu/usdoepub Part of the Bioresource and Agricultural Engineering Commons Inokuti, Mitio, "INTERACTIONS OF ANTIPROTONS WITH ATOMS AND MOLECULES" (1988). US Department of Energy Publications. 89. https://digitalcommons.unl.edu/usdoepub/89 This Article is brought to you for free and open access by the U.S. Department of Energy at DigitalCommons@University of Nebraska - Lincoln. It has been accepted for inclusion in US Department of Energy Publications by an authorized administrator of DigitalCommons@University of Nebraska - Lincoln. /'Iud Tracks Radial. Meas., Vol. 16, No. 2/3, pp. 115-123, 1989 0735-245X/89 $3.00 + 0.00 Inl. J. Radial. Appl .. Ins/rum., Part D Pergamon Press pic printed in Great Bntam INTERACTIONS OF ANTIPROTONS WITH ATOMS AND MOLECULES* Mmo INOKUTI Argonne National Laboratory, Argonne, Illinois 60439, U.S.A. (Received 14 November 1988) Abstract-Antiproton beams of relatively low energies (below hundreds of MeV) have recently become available. The present article discusses the significance of those beams in the contexts of radiation physics and of atomic and molecular physics. Studies on individual collisions of antiprotons with atoms and molecules are valuable for a better understanding of collisions of protons or electrons, a subject with many applications. An antiproton is unique as' a stable, negative heavy particle without electronic structure, and it provides an excellent opportunity to study atomic collision theory. -
1.1. Introduction the Phenomenon of Positron Annihilation Spectroscopy
PRINCIPLES OF POSITRON ANNIHILATION Chapter-1 __________________________________________________________________________________________ 1.1. Introduction The phenomenon of positron annihilation spectroscopy (PAS) has been utilized as nuclear method to probe a variety of material properties as well as to research problems in solid state physics. The field of solid state investigation with positrons started in the early fifties, when it was recognized that information could be obtained about the properties of solids by studying the annihilation of a positron and an electron as given by Dumond et al. [1] and Bendetti and Roichings [2]. In particular, the discovery of the interaction of positrons with defects in crystal solids by Mckenize et al. [3] has given a strong impetus to a further elaboration of the PAS. Currently, PAS is amongst the best nuclear methods, and its most recent developments are documented in the proceedings of the latest positron annihilation conferences [4-8]. PAS is successfully applied for the investigation of electron characteristics and defect structures present in materials, magnetic structures of solids, plastic deformation at low and high temperature, and phase transformations in alloys, semiconductors, polymers, porous material, etc. Its applications extend from advanced problems of solid state physics and materials science to industrial use. It is also widely used in chemistry, biology, and medicine (e.g. locating tumors). As the process of measurement does not mostly influence the properties of the investigated sample, PAS is a non-destructive testing approach that allows the subsequent study of a sample by other methods. As experimental equipment for many applications, PAS is commercially produced and is relatively cheap, thus, increasingly more research laboratories are using PAS for basic research, diagnostics of machine parts working in hard conditions, and for characterization of high-tech materials. -
Chapter 3 the Fundamentals of Nuclear Physics Outline Natural
Outline Chapter 3 The Fundamentals of Nuclear • Terms: activity, half life, average life • Nuclear disintegration schemes Physics • Parent-daughter relationships Radiation Dosimetry I • Activation of isotopes Text: H.E Johns and J.R. Cunningham, The physics of radiology, 4th ed. http://www.utoledo.edu/med/depts/radther Natural radioactivity Activity • Activity – number of disintegrations per unit time; • Particles inside a nucleus are in constant motion; directly proportional to the number of atoms can escape if acquire enough energy present • Most lighter atoms with Z<82 (lead) have at least N Average one stable isotope t / ta A N N0e lifetime • All atoms with Z > 82 are radioactive and t disintegrate until a stable isotope is formed ta= 1.44 th • Artificial radioactivity: nucleus can be made A N e0.693t / th A 2t / th unstable upon bombardment with neutrons, high 0 0 Half-life energy protons, etc. • Units: Bq = 1/s, Ci=3.7x 1010 Bq Activity Activity Emitted radiation 1 Example 1 Example 1A • A prostate implant has a half-life of 17 days. • A prostate implant has a half-life of 17 days. If the What percent of the dose is delivered in the first initial dose rate is 10cGy/h, what is the total dose day? N N delivered? t /th t 2 or e Dtotal D0tavg N0 N0 A. 0.5 A. 9 0.693t 0.693t B. 2 t /th 1/17 t 2 2 0.96 B. 29 D D e th dt D h e th C. 4 total 0 0 0.693 0.693t /th 0.6931/17 C. -
ANTIPROTON and NEUTRINO PRODUCTION ACCELERATOR TIMELINE ISSUES Dave Mcginnis August 28, 2005
ANTIPROTON AND NEUTRINO PRODUCTION ACCELERATOR TIMELINE ISSUES Dave McGinnis August 28, 2005 INTRODUCTION Most of the accelerator operating period is devoted to making antiprotons for the Collider program and accelerating protons for the NUMI program. While stacking antiprotons, the same Main Injector 120 GeV acceleration cycle is used to accelerate protons bound for the antiproton production target and protons bound for the NUMI neutrino production target. This is designated as Mixed-Mode operations. The minimum cycle time is limited by the time it takes to fill the Main Injector with two Booster batches for antiproton production and five Booster batches for neutrino production (7 x 0.067 seconds) and the Main Injector ramp rate (~ 1.5 seconds). As the antiproton stack size grows, the Accumulator stochastic cooling systems slow down which requires the cycle time to be lengthened. The lengthening of the cycle time unfortunately reduces the NUMI neutrino flux. This paper will use a simple antiproton stacking model to explore some of the tradeoffs between antiproton stacking and neutrino production. ACCUMULATOR STACKTAIL SYSTEM After the target, antiprotons are injected into the Debuncher ring where they undergo a bunch rotation and are stochastically pre-cooled for injection into the Accumulator. A fresh beam pulse injected into the Accumulator from the Debuncher is merged with previous beam pulses with the Accumulator StackTail system. This system cools and decelerates the antiprotons until the antiprotons are captured by the core cooling systems as shown in Figure 1. The antiproton flux through the Stacktail system is described by the Fokker –Plank equation ∂ψ ∂φ = − (1) ∂t ∂E where φ the flux of particles passing through the energy E and ψ is the particle density of the beam at energy E. -
Antiproton–Proton Scattering Experiments with Polarization ( Collaboration) PAX Abstract
Technical Proposal for Antiproton–Proton Scattering Experiments with Polarization ( Collaboration) PAX arXiv:hep-ex/0505054v1 17 May 2005 J¨ulich, May 2005 2 Technical Proposal for PAX Frontmatter 3 Technical Proposal for Antiproton–Proton Scattering Experiments with Polarization ( Collaboration) PAX Abstract Polarized antiprotons, produced by spin filtering with an internal polarized gas target, provide access to a wealth of single– and double–spin observables, thereby opening a new window to physics uniquely accessible at the HESR. This includes a first measurement of the transversity distribution of the valence quarks in the proton, a test of the predicted opposite sign of the Sivers–function, related to the quark dis- tribution inside a transversely polarized nucleon, in Drell–Yan (DY) as compared to semi–inclusive DIS, and a first measurement of the moduli and the relative phase of the time–like electric and magnetic form factors GE,M of the proton. In polarized and unpolarized pp¯ elastic scattering, open questions like the contribution from the odd charge–symmetry Landshoff–mechanism at large t and spin–effects in the extraction | | of the forward scattering amplitude at low t can be addressed. The proposed de- | | tector consists of a large–angle apparatus optimized for the detection of DY electron pairs and a forward dipole spectrometer with excellent particle identification. The design and performance of the new components, required for the polarized antiproton program, are outlined. A low–energy Antiproton Polarizer Ring (APR) yields an antiproton beam polarization of Pp¯ = 0.3 to 0.4 after about two beam life times, which is of the order of 5–10 h. -
The W and Z at LEP
50YEARSOFCERN The W and Z at LEP 1954-2004 The Large Electron Positron collider made significant contributions to the process of establishing the Standard Model as the basis for matter and 5 forces, and also built a platform for physics scenarios beyond the model. The Standard Model of particle physics is arguably one of the greatest achievements in physics in the 20th century. Within this framework the electroweak interactions, as introduced by Sheldon Glashow, Abdus Salam and Steven Weinberg, are formulated as an SU(2)xll(l) gauge field theory with the masses of the fundamental particles generated by the Higgs mechanism. Both of the first two crucial steps in establishing experimentally the electroweak part of the Standard Model occurred at CERN. These were the discovery of neutral currents in neutrino scattering by the Gargamelle collab oration in 1973, and only a decade later the discovery by the UA1 and UA2 collaborations of the W and Z gauge bosons in proton- antiproton collisions at the converted Super Proton Synchrotron (CERN Courier May 2003 p26 and April 2004 pl3). Establishing the theory at the quantum level was the next logical step, following the pioneering theoretical work of Gerard 't Hooft Fig. 1. The cover page and Martinus Veltman. Such experimental proof is a necessary (left) of the seminal requirement for a theory describing phenomena in the microscopic CERN yellow report world. At the same time, performing experimental analyses with high 76-18 on the physics precision also opens windows to new physics phenomena at much potential of a 200 GeV higher energy scales, which can be accessed indirectly through e+e~ collider, and the virtual effects. -
A Relativistic One Pion Exchange Model of Proton-Neutron Electron-Positron Pair Production
Utah State University DigitalCommons@USU All Graduate Theses and Dissertations Graduate Studies 5-1973 A Relativistic One Pion Exchange Model of Proton-Neutron Electron-Positron Pair Production William A. Peterson Utah State University Follow this and additional works at: https://digitalcommons.usu.edu/etd Part of the Physics Commons Recommended Citation Peterson, William A., "A Relativistic One Pion Exchange Model of Proton-Neutron Electron-Positron Pair Production" (1973). All Graduate Theses and Dissertations. 3674. https://digitalcommons.usu.edu/etd/3674 This Dissertation is brought to you for free and open access by the Graduate Studies at DigitalCommons@USU. It has been accepted for inclusion in All Graduate Theses and Dissertations by an authorized administrator of DigitalCommons@USU. For more information, please contact [email protected]. ii ACKNOWLEDGMENTS The author sincerely appreciates the advice and encouragement of Dr. Jack E. Chatelain who suggested this problem and guided its progress. The author would also like to extend his deepest gratitude to Dr. V. G. Lind and Dr. Ackele y Miller for their support during the years of graduate school. William A. Pete r son iii TABLE OF CONTENTS Page ACKNOWLEDGMENTS • ii LIST OF TABLES • v LIST OF FIGURES. vi ABSTRACT. ix Chapter I. INTRODUCTION. • . • • II. FORMULATION OF THE PROBLEM. 7 Green's Function Treatment of the Dirac Equation. • • • . • . • • • 7 Application of Feynman Graph Rules to Pair Production in Neutron- Proton Collisions 11 III. DIFFERENTIAL CROSS SECTION. 29 Symmetric Coplanar Case 29 Frequency Distributions 44 BIBLIOGRAPHY. 72 APPENDIXES •• 75 Appendix A. Notation and Definitions 76 Appendix B. Expressi on for Cross Section. 79 Appendix C. -
Neutrino Masses-How to Add Them to the Standard Model
he Oscillating Neutrino The Oscillating Neutrino of spatial coordinates) has the property of interchanging the two states eR and eL. Neutrino Masses What about the neutrino? The right-handed neutrino has never been observed, How to add them to the Standard Model and it is not known whether that particle state and the left-handed antineutrino c exist. In the Standard Model, the field ne , which would create those states, is not Stuart Raby and Richard Slansky included. Instead, the neutrino is associated with only two types of ripples (particle states) and is defined by a single field ne: n annihilates a left-handed electron neutrino n or creates a right-handed he Standard Model includes a set of particles—the quarks and leptons e eL electron antineutrino n . —and their interactions. The quarks and leptons are spin-1/2 particles, or weR fermions. They fall into three families that differ only in the masses of the T The left-handed electron neutrino has fermion number N = +1, and the right- member particles. The origin of those masses is one of the greatest unsolved handed electron antineutrino has fermion number N = 21. This description of the mysteries of particle physics. The greatest success of the Standard Model is the neutrino is not invariant under the parity operation. Parity interchanges left-handed description of the forces of nature in terms of local symmetries. The three families and right-handed particles, but we just said that, in the Standard Model, the right- of quarks and leptons transform identically under these local symmetries, and thus handed neutrino does not exist. -
Can Any Anti-Particle Make a Probe?
NEWS AND VIEWS Can any anti-particle make a probe? Positron probes (of the solid state) are already a booming business and may soon be applied to the study of liquids. Can anti-proton probes be far away? EACH new particle of matter discovered from zero to some maximum. So what is new? Two things, both in the may most immediately be of interest to The trick of making a mono-energetic same issue of Physical Review Letters (2 those with theories to check (or invent, as beam of reasonable but still low energy September). First, E. Gramsch, KG.Lynn, the case may be), but one thing is certain: usually entails some interaction with a J. Throwe and I Kanazawa, from the somebody will eventually use the particle solid within which the energy of incident Brookhaven National Laboratory, have as a probe for some purpose or another. positrons is first reduced to the average extended the use of positrons as probes And that is likely to be true even if the thermal energy, whereupon some propor from solids to liquids, and with surprising newly discovered particle is inherently tion of the incident particles is afterwards results (67, 1,282; 1991). The incentive unstable, or if it interacts with and is de- re-emitted by scattering, but with an en has been to see whether positron probes stroyed by some component of the envi- ergy that is a measure of the work function can throw light on the structure of liquids, ronment in which it finds itself. What - the potential difference between the for which purpose they have studied matters is merely that the particle should interior and the exteriorofthe solid. -
HIGH ENERGY ASTROPHYSICS - Lecture 10
HIGH ENERGY ASTROPHYSICS - Lecture 10 PD Frank Rieger ITA & MPIK Heidelberg Wednesday 1 Pair Plasmas in Astrophysics 1 Overview • Pair Production γ + γ ! e+ + e− (threshold) • Compactness parameter • Example I: "internal" γγ-absorption in AGN (Mkn 421) • Example II: EBL & limited transparency of the Universe to TeV photons • Pair Annihilation e+ + e− ! γ + γ (no threshold) • Example: Annihilation-in-flight (energetics) 2 2 Two-Photon Pair Production Generation of e+e−-pairs in environments with very high radiation energy density: γ + γ ! e+ + e− • Reaction threshold for pair production (see lecture 9): 2 2 e1e2 − p1p2 cos θ = m1m2c + δm c (m1 + m2 + 0:5 δm) With mi = 0; ei := i=c = pi (photons) and δm = 2me: 2 4 2 4 12(1 − cos θ) = 0:5 (δm) c = 2mec 2 4 ) 12 = mec for producing e+e− at rest in head-on collision (lab frame angle cos θ = −1). 12 • Example: for TeV photon 1 = 10 eV, interaction possible with soft photons 2 2 ≥ (0:511) eV = 0:26 eV (infrared photons). 3 • Cross-section for pair-production: πr2 1 + β∗ σ (β∗) = 0 (1 − β∗2) 2β∗(β∗2 − 2) + (3 − β∗4) ln γγ 2 1 − β∗ with β∗ = v∗=c velocity of electron (positron) in centre of momentum frame, 2 and πr0 = 3σT =8. In terms of photon energies and collision angle θ (cf. above): ∗2 ∗ ∗ 2 2 ∗2 −1=2 12(1 − cos θ) = 2Ee and Ee = γ mec = mec (1 − β ) ∗ where Ee =total energy of electron (positron) in CoM frame, so 1 (1 − cos θ) = 2γ∗2m2c4 = 2m2c4 1 2 e e (1 − β∗2) s 2m2c4 ) β∗ = 1 − e 12(1 − cos θ) 4 1 + - "+" --> e + e T ! / 0.1 "" ! 0.01 1 10 100 #1 #2 (1-cos$) Figure 1: Cross-section for γγ-pair production in units of the Thomson cross-section σT as a function of 2 2 interacting photon energies (1=mec )(2=mec ) (1−cos θ). -
New Trends in the Investigation of Antiproton-Nucleus Annihilation
сообщения объединенного института ядерных исследований дубна E15-90-t50 A.M. Rozhdestvenskyк$Г/ ММ..< С.Sapozhnikov NEW TRENDS IN THE INVESTIGATION OF ANTIPROTON-NUCLEUS ANNIHILATION 1990 © Объединенный институт ядерных исследований Дубна, 1990 1. INTRODUCTION Experiments at LEAR have provided valuable information on the antiproton-nucleus interaction at low energies, T < 200 MeV (see, reviews [1,2]). Such gross features of the pA interaction as the energy dependence of cross sections, multiplicity distributions of annihilation mesons, angular and momentum spectra of outgoing particles etc. are known nov. This information provides a reference frame for future tasks to be carried out at high intensity hadron facilities such as the KAON factory or SUPERLEAR-type machines. In high energy antiproton-nucleus physics one can single out at least two types of j.rc|blems . The first involves investigation of the mechanisms of antiproton interaction with nuclei. In a certain sense it represents a repetition of the program performed with protons and pions. Such experiments are needed for a better understanding of which phenomena are to be regarded as conventional. Problems of the second type include the investigation of specific antiproton-nucleus annihilation phenomena. How does a nucleus react to a near 2 GeV energy release occurring in a small volume on the surface or inside the nucleus? How strong is the final state interaction of annihilation mesons? Is annihilation on few-nucleon clusters possible? Does the annihilation probability on a bound nucleon differ from the annihilation probability on a free nucleon? All these problems represent examples of "pure" antiproton physics. We believe it is these aspects of antiproton-nucleus physics that will become more and more important in the future.