Pair Production and photon-matter interactions

Slides:



Advertisements
Similar presentations
X-RAY INTERACTION WITH MATTER
Advertisements

The Modern Quantum Atom The nucleus and the discovery of the neutron What are electron-volts ? The Quantum atom.
_______________physics 1.Matter is a____________________ 2.Light is a _________________. particle wave Classical This is "everyday" physics that deals.
Early Quantum Theory and Models of the Atom
Isotope characteristics differ U U
Early Quantum Mechanics
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Chapter.
10-1 CHEM 312 Lecture 10: Part 1 Radiation Reactions: Dosimetry and Hot Atom Chemistry Readings: §Reading: Modern Nuclear Chemistry, Chap. 17; Nuclear.
Compton Effect 1923 Compton performed an experiment which supported this idea directed a beam of x-rays of wavelength  onto a carbon target x-rays are.
Homework due Monday. Use Compton scattering formula for Ch5 Q8 An electron volt (eV) is a unit of energy = work done moving an electron down one volt =
Interactions with Matter
Particle Interactions
Antimatter  The mass of a p is 938MeV/c 2 and its charge is +e. The mass of a  p is __ and its charge is ___ a ) 938MeV/c 2, +e b ) - 938MeV/c 2, +e.
AP Physics 12 – Class Starter FR Question Please grab a whiteboard, markers and a couple friends to answer the following question!
Early Quantum Theory and Models of the Atom
Interaction of Gamma-Rays - General Considerations uncharged transfer of energy creation of fast electrons.
Stopping Power The linear stopping power S for charged particles in a given absorber is simply defined as the differential energy loss for that particle.
Modern Physics Previously we showed that Light behaves like sound. It has characteristics of waves Now we get to see how it also behaves like a particle.
Modern Physics Wave Particle Duality of Energy and Matter Is light a particle or a wave? We have see that light acts like a wave from polarization, diffraction,
Resident Physics Lectures Christensen, Chapter 4 Basic Interactions Between X-Rays and Matter George David Associate Professor Medical College of Georgia.
Of Photons and Electrons Compton Effect, Pair Production and X-Rays.
Interactions of radiation with Matter
De Broglie wavelengths
Chapter 5 Interactions of Ionizing Radiation. Ionization The process by which a neutral atom acquires a positive or a negative charge Directly ionizing.
Appendix G1: Chapter 12: X-Ray Interaction with Matter
Goal: To understand how light acts like a particle Objectives: 1)To learn about Quantization 2)To understand Blackbody radiation 3)To learn more about.
Physics 102: Lecture 23, Slide 1 De Broglie Waves, Uncertainty, and Atoms Physics 102: Lecture 23.
Gamma and X ray interactions
INTERACTIONS OF RADIATION WITH MATTER. twCshttp:// twCs
Relativistic Mechanics Momentum and energy. Momentum p =  mv Momentum is conserved in all interactions.
Dr. Mohammed Alnafea Radiation Interaction with matter.
Alhanouf Alshedi Basic Interactions of Radiation with Matter 2 ed Lecture.
THE COMPTON EFFECT Energy and momentum are conserved when a photon collides with an electron.
Interactions of Ionizing Radiation
Lecture 5. Particle Properties of Waves (cont’d)
Compton Scattering When light encounters charged particles, the particles will interact with the light and cause some of the light to be scattered. incident.
Pair Production and photon-matter interactions Contents: Photoelectric effect Compton scattering Absorption Pair production Whiteboards.
Jan 13 th Posters due Friday Interactions of Photons with matter.
CH Explaining a Continuous Spectrum (called a blackbody spectrum)
Chapter 2 Radiation Interactions with Matter East China Institute of Technology School of Nuclear Engineering and Technology LIU Yi-Bao Wang Ling.
The photoelectric effect Contents: Einstein’s proposed experiment Solving photoelectric problems Example 1 | Example 2Example 1Example 2 Whiteboard Photon.
The photoelectric effect Contents: Einstein’s proposed experiment Solving photoelectric problems Example 1 | Example 2Example 1Example 2 Whiteboard Photon.
2.4.2 interaction of x-rays with matter
Chapter 5 Interactions of Ionizing Radiation
Relativity of Mass According to Newtonian mechanics the mass of a body is unaffected with change in velocity. But space and time change…….. Therefore “mass”
Interaction of gamma rays with matter
Quiz_14 Previous material – Compton scattering, pair production New material – Wave-Particle duality, probability, Uncertainty Principle Physics 274 9/30/2016.
Herriman High AP Physics 2
Interactions of Radiation With Matter
Unit - 2 Compton effect Dual nature of EM radiation
De Broglie Waves, Uncertainty, and Atoms
Thomson Scattering How does a photon (light) scatter from an electron?
Scattering of light Physics /15/2018 Lecture XI.
Photoelectric Effect.
De Broglie Waves, Uncertainty, and Atoms
The photoelectric effect
Unit 11 – Modern Physics.
Interaction of gamma rays with matter
Photon-Matter Interactions
Basic Physics Processes in a Sodium Iodide (NaI) Calorimeter
Resident Physics Lectures (year 1)
Review Lepton Number Particle Lepton number (L) electron 1 neutrino
AS Physics Unit 1 1 Matter and Radiation Ks5 AS Physics AQA 2450
Quantization of light, charge and energy Chapter 2-Class5
Absorption & Emission.
Lecturer Radiological Science
Electronic Physics Dr. Ghusoon Mohsin Ali E    8.857eV  1400
The Wave-Particle Duality
256 nm light strikes a metal and the ejected electrons have a stopping potential of 1.15 V. What is the work function of the metal in eV? (2) E = hf =
Atomic Physics Compton scattering Renjith Mathew Roy George Christopher Saqib Majeed Lone Dr.JOHANAN CHRISTAIN PRASANA.
Presentation transcript:

Pair Production and photon-matter interactions Contents: Photoelectric effect Compton scattering Absorption Pair production Whiteboards                                

Photoelectric effect Photon knocks electron from atom Photon disappears in the process

Compton Scattering Photon bounces off electron Electron absorbs some energy Photon has longer wavelength after collision

Absorption Photon hits electron in orbital Electron moves to excited state Photon disappears in the process Only for photons with the right energy

Help me! I’m going to be annihilated presently! Pair production Photon with sufficient energy passes near nucleus Energy of photon turns into matter Pair of matter/anti matter is created Nucleus must carry off some momentum Help me! I’m going to be annihilated presently! Positron m = 9.11 x 10-31 kg Charge = +e Electron m = 9.11 x 10-31 kg Charge = -e

Example 1: What energy photon (in MeV) is needed to create a electron-positron pair each with a kinetic energy of 0.34 MeV? What is the wavelength of that photon? Photon energy = energy to create matter + kinetic energy

Example 2: A 0. 00025 nm photon creates a electron positron pair Example 2: A 0.00025 nm photon creates a electron positron pair. What is the kinetic energy of each particle?

Whiteboards: Pair production 1 | 2 | 3

A photon creates a electron-positron pair each with a kinetic energy of 0.170 MeV. What is the energy of the photon? (in MeV) photon energy = energy to create mass + kinetic energy = .511 MeV + .511 MeV + .170 MeV + .170 MeV = 1.362 MeV 1.362 MeV

A 2134 MeV photon creates a proton, antiproton pair, each with how much kinetic energy? (2) Proton rest mass = 938 MeV photon energy = energy to create mass + kinetic energy 2134 MeV = 938 MeV + 938 MeV + kinetic energy kinetic energy = 258 MeV/(2 particles) = 129 MeV 129 MeV

A photon with a wavelength of 5 A photon with a wavelength of 5.27113x 10-13 m creates a electron-positron pair with how much kinetic energy each? (answer in keV) E = hf = hc/ E = hc/, = (6.626 x 10-34 Js)(3.00 x 108 m/s)/(5.27113x 10-13 m) = (3.77111x 10-13 J)/(1.602 x 10-19 J/eV) = 2354000 eV = 2354 keV photon energy = energy to create mass + kinetic energy 2354 keV= 511 keV + 511 keV + kinetic energy kinetic energy = 1332 keV/(2 particles) = 666 keV 666 keV

Solving pair production E = hf = hc/ E = mc2 E - Energy m - mass c = 3.00 x 108 m/s 1 eV = 1.602 x 10-19 J Example 1: What energy photon (in MeV) is needed to create a electron-positron pair each with a kinetic energy of 0.34 MeV? What is the wavelength of that photon? Photon energy = energy to create matter + kinetic energy

Solving pair production E = hf = hc/ E = mc2 E - Energy m - mass c = 3.00 x 108 m/s 1 eV = 1.602 x 10-19 J Example 3: A 0.00025 nm photon creates a electron positron pair. What is the kinetic energy of each particle?