Introduction to Plasma Accelerators: the Basics
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Slowing Down of a Particle Beam in the Dusty Plasmas with Kappa
arXiv:1708.04525 Slowing Down of Charged Particles in Dusty Plasmas with Power-law Kappa-distributions Jiulin Du 1*, Ran Guo 2, Zhipeng Liu3 and Songtao Du4 1 Department of Physics, School of Science, Tianjin University, Tianjin 300072, China 2 School of Science, Civil Aviation University of China, Tianjin 300300, China 3 School of Science, Tianjin Chengjian University, Tianjin 300384, China 4 College of Electronic Information and Automation, Civil Aviation University of China, Tianjin 300300, China Keywords: Slowing down, Kappa-distributions, Dusty plasma, Fokker-Planck collision theory Abstract We study slowing down of a particle beam passing through the dusty plasma with power-law κ-distributions. Three plasma components, electrons, ions and dust particles, can have a different κ-parameter. The deceleration factor and slowing down time are derived and expressed by a hyper-geometric κ-function. Numerically we study slowing down property of an electron beam in the κ-distributed dusty plasma. We show that the slowing down in the plasma depends strongly on the κ-parameters of plasma components, and dust particles play a dominant role in the deceleration effects. We also show dependence of the slowing down on mass and charge of a dust particle in the plasma. 1 Introduction Dusty plasmas are ubiquitous in astrophysical, space and terrestrial environments, such as the interstellar clouds, the circumstellar clouds, the interplanetary space, the comets, the planetary rings, the Earth’s atmosphere, and the lower ionosphere etc. They can also exist in laboratory plasma environments. Dusty plasma consists of three components: electrons, ions and dust particles of micron- or/and submicron-sized particulates. -
Upgrading the CMS Detector on the Large Hadron Collider
Upgrading the CMS Detector on the Large Hadron Collider Stefan Spanier Professor, Department of Physics CURRENT RESEARCH AFFILIATION Putting a diamond on the largest ring in the world The University of Tennessee, Knoxville July 4, 2012 is one of the most exciting dates to remember in modern science. On this day, EDUCATION scientists working with the Large Hadron Collider (LHC) at the European Organization for Nuclear Research (CERN) in Switzerland discovered a particle consistent with the Ph.D., Johannes Gutenberg University, Mainz, Germany characteristics of the Higgs boson particle. This particle is predicted by the Standard Model of particle physics. The model is very successful in linking measurements made with previous RESEARCH AREAS particle accelerators, but still leaves unanswered questions about how the universe works. The model does ignores dark matter and dark energy, and while it describes the behavior of Technology, Materials Science / Physics the Higgs particle it does not predict its own mass. These mysteries indicate there must be a larger picture that includes new forces and particles, and the Standard Model is only part of FUNDING REQUEST it. Spanier is seeking $70,000 annually to fund this project. This will cover a graduate student This is where the LHC, the world’s largest and most powerful particle accelerator comes in. for one year, travel expenses to the particle beam physics laboratory, acquisition and The LHC was first conceived in 1984, and brought online in 2008. It consists of a 27-kilometer preparation of a new detector substrate from a diamond growth process batch and one ring of superconducting magnets with accelerating structures that boost protons to neutron irradiation in a nuclear reactor. -
Foundations of Newtonian Dynamics: an Axiomatic Approach For
Foundations of Newtonian Dynamics: 1 An Axiomatic Approach for the Thinking Student C. J. Papachristou 2 Department of Physical Sciences, Hellenic Naval Academy, Piraeus 18539, Greece Abstract. Despite its apparent simplicity, Newtonian mechanics contains conceptual subtleties that may cause some confusion to the deep-thinking student. These subtle- ties concern fundamental issues such as, e.g., the number of independent laws needed to formulate the theory, or, the distinction between genuine physical laws and deriva- tive theorems. This article attempts to clarify these issues for the benefit of the stu- dent by revisiting the foundations of Newtonian dynamics and by proposing a rigor- ous axiomatic approach to the subject. This theoretical scheme is built upon two fun- damental postulates, namely, conservation of momentum and superposition property for interactions. Newton’s laws, as well as all familiar theorems of mechanics, are shown to follow from these basic principles. 1. Introduction Teaching introductory mechanics can be a major challenge, especially in a class of students that are not willing to take anything for granted! The problem is that, even some of the most prestigious textbooks on the subject may leave the student with some degree of confusion, which manifests itself in questions like the following: • Is the law of inertia (Newton’s first law) a law of motion (of free bodies) or is it a statement of existence (of inertial reference frames)? • Are the first two of Newton’s laws independent of each other? It appears that -
Particle Beam Diagnostics and Control
Particle beam diagnostics and control G. Kube Deutsches Elektronen-Synchrotron DESY Notkestraße 85, 22607 Hamburg, Germany Summary. | Beam diagnostics and instrumentation are an essential part of any kind of accelerator. There is a large variety of parameters to be measured for obser- vation of particle beams with the precision required to tune, operate and improve the machine. Depending on the type of accelerator, for the same parameter the working principle of a monitor may strongly differ, and related to it also the requirements for accuracy. This report will mainly focus on electron beam diagnostic monitors presently in use at 4th generation light sources (single-pass Free Electron Lasers), and present the state-of-the-art diagnostic systems and concepts. 1. { Introduction Nowadays particle accelerators play an important role in a wide number of fields where a primary or secondary beam from an accelerator can be used for industrial or medical applications or for basic and applied research. The interaction of such beam with matter is exploited in order to analyze physical, chemical or biological samples, for a modification of physical, chemical or biological sample properties, or for fundamental research in basic subatomic physics. In order to cover such a wide range of applications different accelerator types are required. Cyclotrons are often used to produce medical isotopes for positron emission to- ⃝c Societ`aItaliana di Fisica 1 2 G. Kube mography (PET) and single photon emission computed tomography (SPECT). For elec- tron radiotherapy mainly linear accelerators (linacs) are in operation, while cyclotrons or synchrotrons are additionally used for proton therapy. Third generation synchrotron light sources are electron synchrotrons, while the new fourth generation light sources (free electron lasers) operating at short wavelengths are electron linac based accelera- tors. -
4. Particle Generators/Accelerators
Joint innovative training and teaching/ learning program in enhancing development and transfer knowledge of application of ionizing radiation in materials processing 4. Particle Generators/Accelerators Diana Adlienė Department of Physics Kaunas University of Technolog y Joint innovative training and teaching/ learning program in enhancing development and transfer knowledge of application of ionizing radiation in materials processing This project has been funded with support from the European Commission. This publication reflects the views only of the author. Polish National Agency and the Commission cannot be held responsible for any use which may be made of the information contained therein. Date: Oct. 2017 DISCLAIMER This presentation contains some information addapted from open access education and training materials provided by IAEA TABLE OF CONTENTS 1. Introduction 2. X-ray machines 3. Particle generators/accelerators 4. Types of industrial irradiators The best accelerator in the universe… INTRODUCTION • Naturally occurring radioactive sources: – Up to 5 MeV Alpha’s (helium nuclei) – Up to 3 MeV Beta particles (electrons) • Natural sources are difficult to maintain, their applications are limited: – Chemical processing: purity, messy, and expensive; – Low intensity; – Poor geometry; – Uncontrolled energies, usually very broad Artificial sources (beams) are requested! INTRODUCTION • Beams of accelerated particles can be used to produce beams of secondary particles: Photons (x-rays, gamma-rays, visible light) are generated from beams -
Overview of the CALET Mission to the ISS 1 Introduction
32ND INTERNATIONAL COSMIC RAY CONFERENCE,BEIJING 2011 Overview of the CALET Mission to the ISS SHOJI TORII1,2 FOR THE CALET COLLABORATION 1Research Institute for Scinece and Engineering, Waseda University 2Space Environment Utilization Center, JAXA [email protected] DOI: 10.7529/ICRC2011/V06/0615 Abstract: The CALorimetric Electron Telescope (CALET) mission is being developed as a standard payload for the Exposure Facility of the Japanese Experiment Module (JEM/EF) on the International Space Station (ISS). The instrument consists of a segmented plastic scintillator charge measuring module, an imaging calorimeter consisting of 8 scintillating fiber planes with a total of 3 radiation lengths of tungsten plates interleaved with the fiber planes, and a total absorption calorimeter consisting of crossed PWO logs with a total depth of 27 radiation lengths. The major scientific objectives for CALET are to search for nearby cosmic ray sources and dark matter by carrying out a precise measurement of the electron spectrum (1 GeV - 20 TeV) and observing gamma rays (10 GeV - 10 TeV). CALET has a unique capability to observe electrons and gamma rays in the TeV region since the hadron rejection power is larger than 105 and the energy resolution better than 2 % above 100 GeV. CALET has also the capability to measure cosmic ray H, He and heavy nuclei up to 1000 TeV.∼ The instrument will also monitor solar activity and search for gamma ray transients. The phase B study has started, aimed at a launch in 2013 by H-II Transfer Vehicle (HTV) for a 5 year observation period on JEM/EF. -
Chapter 11.Pdf
Chapter 11. Kinematics of Particles Contents Introduction Rectilinear Motion: Position, Velocity & Acceleration Determining the Motion of a Particle Sample Problem 11.2 Sample Problem 11.3 Uniform Rectilinear-Motion Uniformly Accelerated Rectilinear-Motion Motion of Several Particles: Relative Motion Sample Problem 11.5 Motion of Several Particles: Dependent Motion Sample Problem 11.7 Graphical Solutions Curvilinear Motion: Position, Velocity & Acceleration Derivatives of Vector Functions Rectangular Components of Velocity and Acceleration Sample Problem 11.10 Motion Relative to a Frame in Translation Sample Problem 11.14 Tangential and Normal Components Sample Problem 11.16 Radial and Transverse Components Sample Problem 11.18 Introduction Kinematic relationships are used to help us determine the trajectory of a snowboarder completing a jump, the orbital speed of a satellite, and accelerations during acrobatic flying. Dynamics includes: Kinematics: study of the geometry of motion. Relates displacement, velocity, acceleration, and time without reference to the cause of motion. Fdownforce Fdrive Fdrag Kinetics: study of the relations existing between the forces acting on a body, the mass of the body, and the motion of the body. Kinetics is used to predict the motion caused by given forces or to determine the forces required to produce a given motion. Particle kinetics includes : • Rectilinear motion: position, velocity, and acceleration of a particle as it moves along a straight line. • Curvilinear motion : position, velocity, and acceleration of a particle as it moves along a curved line in two or three dimensions. Rectilinear Motion: Position, Velocity & Acceleration • Rectilinear motion: particle moving along a straight line • Position coordinate: defined by positive or negative distance from a fixed origin on the line. -
Charged-Particle (Proton Or Helium Ion) Radiotherapy for Neoplastic Conditions
Charged-Particle (Proton or Helium Ion) Radiotherapy for Neoplastic Conditions Policy Number: Original Effective Date: MM.05.005 07/01/2009 Line(s) of Business: Current Effective Date: HMO; PPO; QUEST Integration 07/28/2017 Section: Radiology Place(s) of Service: Outpatient I. Description Charged-particle beams consisting of protons or helium ions are a type of particulate radiation therapy (RT). Treatment with charged-particle radiotherapy is proposed for a large number of indications, often for tumors that would benefit from the delivery of a high dose of radiation with limited scatter that is enabled by charged-particle beam radiotherapy. For individuals who have uveal melanoma(s) who receive charged-particle (proton or helium ion) radiotherapy, the evidence includes RCTs and systematic reviews. Relevant outcomes are overall survival, disease-free survival, change in disease status, and treatment-related morbidity. Systematic reviews, including a 1996 TEC Assessment and a 2013 review of randomized and non- randomized studies, concluded that the technology is at least as effective as alternative therapies for treating uveal melanomas and is better at preserving vision. The evidence is sufficient to determine qualitatively that the technology results in a meaningful improvement in the net health outcome. For individuals who have skull-based tumor(s) (i.e., cervical chordoma and chondrosarcoma) who receive charged-particle (proton or helium ion) radiotherapy, the evidence includes observational studies and systematic reviews. Relevant outcomes are overall survival, disease-free survival, change in disease status, and treatment-related morbidity. A 1996 TEC Assessment concluded that the technology is at least as effective as alternative therapies for treating skull-based tumors. -
Beam-Transport Systems for Particle Therapy
Beam-Transport Systems for Particle Therapy J.M. Schippers Paul Scherrer Institut, Villigen, Switzerland Abstract The beam transport system between accelerator and patient treatment location in a particle therapy facility is described. After some general layout aspects the major beam handling tasks of this system are discussed. These are energy selection, an optimal transport of the particle beam to the beam delivery device and the gantry, a device that is able to rotate a beam delivery system around the patient, so that the tumour can be irradiated from almost any direction. Also the method of pencil beam scanning is described and how this is implemented within a gantry. Using this method the particle dose is spread over the tumour volume to the prescribed dose distribution. Keywords Beam transport; beam optics; degrader; beam analysis; gantry; pencil beam scanning. 1 Introduction The main purpose of the beam-transport system is to aim the proton beam, with the correct diameter and intensity, at the tumour in the patient and to apply the correct dose distribution. The beam transport from the accelerator to the tumour in the patient consists of the following major sections (see Fig. 1): – energy setting and energy selection (only for cyclotrons); – transport system to the treatment room(s), including beam-emittance matching; – per treatment room—a gantry or a fixed beam line aiming the beam from the correct direction; – beam-delivery system in the treatment room, by which the dose distribution is actually being applied. These devices are combined in the so called ‘nozzle’ at the exit of the fixed beam line or of the gantry. -
Chapter 3 Motion in Two and Three Dimensions
Chapter 3 Motion in Two and Three Dimensions 3.1 The Important Stuff 3.1.1 Position In three dimensions, the location of a particle is specified by its location vector, r: r = xi + yj + zk (3.1) If during a time interval ∆t the position vector of the particle changes from r1 to r2, the displacement ∆r for that time interval is ∆r = r1 − r2 (3.2) = (x2 − x1)i +(y2 − y1)j +(z2 − z1)k (3.3) 3.1.2 Velocity If a particle moves through a displacement ∆r in a time interval ∆t then its average velocity for that interval is ∆r ∆x ∆y ∆z v = = i + j + k (3.4) ∆t ∆t ∆t ∆t As before, a more interesting quantity is the instantaneous velocity v, which is the limit of the average velocity when we shrink the time interval ∆t to zero. It is the time derivative of the position vector r: dr v = (3.5) dt d = (xi + yj + zk) (3.6) dt dx dy dz = i + j + k (3.7) dt dt dt can be written: v = vxi + vyj + vzk (3.8) 51 52 CHAPTER 3. MOTION IN TWO AND THREE DIMENSIONS where dx dy dz v = v = v = (3.9) x dt y dt z dt The instantaneous velocity v of a particle is always tangent to the path of the particle. 3.1.3 Acceleration If a particle’s velocity changes by ∆v in a time period ∆t, the average acceleration a for that period is ∆v ∆v ∆v ∆v a = = x i + y j + z k (3.10) ∆t ∆t ∆t ∆t but a much more interesting quantity is the result of shrinking the period ∆t to zero, which gives us the instantaneous acceleration, a. -
Compact LWFA-Based Extreme Ultraviolet Free Electron Laser: Design Constraints
Compact LWFA-Based Extreme Ultraviolet Free Electron Laser: design constraints Alexander Molodozhentsev∗, Konstantin O. Kruchinin Institute of Physics ASCR, v.v.i. (FZU), ELI-Beamlines, Za Radnici 835 Dolni Brezany 25241, Czech Republic Abstract Combination of advanced high power laser technology, new acceleration methods and achievements in undulator development opens a way to build compact, high brilliance Free Electron Laser (FEL) driven by a laser wakefield accelerator (LWFA). Here we present a study outlining main requirements on the LWFA based Extreme Ultra Violet (EUV) FEL setup with the aim to reach saturation of photon pulse energy in a single unit commercially available undulator with the deflection parameter K0 in a range of (1÷1.5). A dedicated electron beam transport which allows to control the electron beam slice parameters, including collective effects, required by the self-amplified spontaneous emission (SASE) FEL regime is proposed. Finally, a set of coherent photon radiation parameters achievable in the undulator section utilizing best experimentally demonstrated electron beam parameters are analyzed. As a result we demonstrate that the ultra-short (few fs level) pulse of the photon radiation with the wavelength in the EUV range can be obtained with the peak brilliance of ∼2×1030 photons/s/mm2/mrad2/0.1%bw if the driver laser operates at the repetition rate of 25 Hz. Keywords: laser wake field acceleration, free electron laser, electron beam transport 1. Introduction transport design for a compact laser based EUV-FEL. We demonstrate that proposed setup is capable to generate high In recent years linac-based FELs as a deliverer of coherent brightness coherent photon radiation reaching energy saturation X-ray pulses changed the science landscape. -
Plasma Heating by Intense Charged Particle-Beams Injected on Solid Targets T
PLASMA HEATING BY INTENSE CHARGED PARTICLE-BEAMS INJECTED ON SOLID TARGETS T. Okada, T. Shimojo, K. Niu To cite this version: T. Okada, T. Shimojo, K. Niu. PLASMA HEATING BY INTENSE CHARGED PARTICLE-BEAMS INJECTED ON SOLID TARGETS. Journal de Physique Colloques, 1988, 49 (C7), pp.C7-185-C7-189. 10.1051/jphyscol:1988721. jpa-00228205 HAL Id: jpa-00228205 https://hal.archives-ouvertes.fr/jpa-00228205 Submitted on 1 Jan 1988 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. JOURNAL DE PHYSIQUE Colloque C7, supplgment au n012, Tome 49, dbcembre 1988 PLASMA HEATING BY INTENSE CHARGED PARTICLE-BEAMS INJECTED ON SOLID TARGETS T. OKADA, T. SHIMOJO* and K. NIU* ' Department of Applied Physics, Tokyo University of Agriculture and Technology, Koganei-shi, Tokyo 184, Japan *~epartmentof Physics, Tokyo Gakugei University, Koganei-shi, Tokyo 184, Japan Department of Energy Sciences, Tokyo Institute of Technology, Midori-ku, Yokohama 227, Japan Rbsunb - La production et le chauffage du plasma sont estimbs numbriquement B l'aide d'un modele simple pour l'interaction de faisceaux intenses d'blectrons ou protons avec plusieurs cibles solides. On obtient ainsi les longueurs d'ionisation et la temperature du plasma produit.