Positron. Pair Production  Photons above twice the electron rest mass energy can create a electron positron pair. Minimum = 0.012 ÅMinimum = 0.012 Å.

Slides:



Advertisements
Similar presentations
X-RAY INTERACTION WITH MATTER
Advertisements

Radioactive Decay. - Alpha Decay The emission of an particle from the nucleus of an atom is called alpha decay An alpha particle is just a helium nucleus.
4/2003 Rev 2 I.3.4 – slide 1 of 24 Session I.3.4 Part I Review of Fundamentals Module 3Interaction of Radiation with Matter Session 4Photon Interactions.
Intermediate Physics for Medicine and Biology Chapter 15: Interaction of Photons and Charged Particles with Matter Professor Yasser M. Kadah Web:
Gamma-Ray Spectra _ + The photomultiplier records the (UV) light emitted during electronic recombination in the scintillator. Therefore, the spectrum collected.
Early Quantum Theory and Models of the Atom
Isotope characteristics differ U U
Alpha decay parent nucleus daughter nucleus Momentum conservation decides how the energy is distributed. r E 30 MeV 5 MeV.
LECTURE 6 RELATIVISTIC MOMENTUM AND ENERGY PHYS 420-SPRING 2006 Dennis Papadopoulos.
Interactions with Matter
Particle Interactions
Physical Modeling – Fall MOMENTUM For a particle, momentum is: p = mv and.
Atomic Mass & Number Isotopes The Periodic Table.
Physics 334 Modern Physics Credits: Material for this PowerPoint was adopted from Rick Trebino’s lectures from Georgia Tech which were based on the textbook.
Electrons are in energy levels or electron shells. Electrons closest to the nucleus have the lowest energy. First level can hold.
Aim: How can we apply mathematics to the photoelectric effect? In the photoelectric effect, how do you increase: The number of ejected electrons? The KE.
Radiation therapy is based on the exposure of malign tumor cells to significant but well localized doses of radiation to destroy the tumor cells. The.
Radiation Detection and Measurement, JU, First Semester, (Saed Dababneh). 1 Spectrum if all energy is captured in detector. Allows identification.
Light particles and matter waves?
Lecture 1.3: Interaction of Radiation with Matter
Tools for Nuclear & Particle Physics Experimental Background.
1. ALL POSSIBLE BASIC PARTICLES 2 Vector Electron and Positron 3.
Photo of Particles Interacting within a Bubble Chamber Fermilab bubble chamber: 4.6 m in diameter in a 3 T magnetic field How does a bubble chamber work.
 Problem : Imagine that somewhere in deep space a rock with mass 12kg is moving in the +x direction with v = 4/5 in some inertial frame. This rock then.
Chapter 29 Particles and Waves.
Calorimeters Chapter 3 Chapter 3 Interactions of Photons.
Interactions of high energy photons with matter
Monday, Oct. 16, 2006PHYS 3446, Fall 2006 Jae Yu 1 PHYS 3446 – Lecture #11 Monday, Oct. 16, 2006 Dr. Jae Yu 1.Energy Deposition in Media Total Electron.
Gamma ray interaction with matter A) Primary interactions 1) Coherent scattering (Rayleigh scattering) 2) Incoherent scattering (Compton scattering) 3)
By Dr: Nahla Nagy Assistant Professor Radiological Science Interactions of X-Rays with matter.
Chapter 5 Interactions of Ionizing Radiation. Ionization The process by which a neutral atom acquires a positive or a negative charge Directly ionizing.
Interactions of EM Radiation with Matter
Antimatter And Annihilation. Remember Photons? What are photons?
Appendix G1: Chapter 12: X-Ray Interaction with Matter
Compton Effect and Matter Waves
C.T.R. Wilson. Charles Wilson is 2nd from right in the front row. Can you find Paul Langevin and O.W. Richardson?
Accelerator Physics, JU, First Semester, (Saed Dababneh). 1 In the figure: Photoelectric suppressed. Single Compton (effect of crystal dimensions).
Electromagnetic radiation behaves as particles 1. Notes of the problem discussed Tuesday. 2. Quiz 9.11 and a few comments on quiz Topics in EM.
Modern Physics Chapters Wave-Particle Duality of Light Young’s Double Slit Experiment (diffraction) proves that light has wave properties So does.
Basic photon interactions
Dr. Mohammed Alnafea Radiation Interaction with matter.
THE COMPTON EFFECT Energy and momentum are conserved when a photon collides with an electron.
Interactions of Ionizing Radiation
Pair Production and photon-matter interactions Contents: Photoelectric effect Compton scattering Absorption Pair production Whiteboards.
EMR 2 The Compton Effect. Review of Photoelectric Effect: Intensity Matters - the greater the intensity/brightness, the greater the photoelectric current.
Compton Effect Objective:
Interaction of Radiation with Matter
Photoelectric Effect. Lenard 1902: Studied energy of the photoelectrons with intensity of light. He could increase the intensity thousand fold. 1.Noticed.
SEMICONDUCTOR PHOTONICS LAB., HANYANG UNIV 3.1 Photons Compton Scattering Scattering of an x-ray photon by a free electron in a conductor When the.
Jan 13 th Posters due Friday Interactions of Photons with matter.
Chapter 2 Radiation Interactions with Matter East China Institute of Technology School of Nuclear Engineering and Technology LIU Yi-Bao Wang Ling.
Wednesday, Mar. 2, 2005PHYS 3446, Spring 2005 Jae Yu 1 PHYS 3446 – Lecture #11 Wednesday, Mar. 2, 2005 Dr. Jae Yu 1.Energy Deposition in Media Photon energy.
PHYS 3446 – Lecture #13 Energy Deposition in Media
Interaction of gamma rays with matter
Special Theory of Relativity
Quiz_14 Previous material – Compton scattering, pair production New material – Wave-Particle duality, probability, Uncertainty Principle Physics 274 9/30/2016.
Unit - 2 Compton effect Dual nature of EM radiation
Thomson Scattering How does a photon (light) scatter from an electron?
Scattering of light Physics /15/2018 Lecture XI.
Photoelectric Effect.
I.Larin, PrimEx Analysis meeting
Interaction of gamma rays with matter
Chapter 29: Particles and Waves
Photoelectric Effect Maximum kinetic energy of the electron:
Photon-Matter Interactions
Electroweak bosons  .
Pair Production and photon-matter interactions
Interaction of Electromagnetic Radiation with Matter
PHYS 3446 – Lecture #13 Energy Deposition in Media
Atomic Physics Compton scattering Renjith Mathew Roy George Christopher Saqib Majeed Lone Dr.JOHANAN CHRISTAIN PRASANA.
Presentation transcript:

Positron

Pair Production  Photons above twice the electron rest mass energy can create a electron positron pair. Minimum = ÅMinimum = Å  The nucleus is involved for momentum conservation. Probability increases with ZProbability increases with Z  This is a dominant effect at high energy. ee  ee Z

Total Photon Cross Section  Photon cross sections are the sum of all effects. Photoelectric , Compton  incoh, pair Photoelectric , Compton  incoh, pair  J. H. Hubbell (1980) Carbon Lead