1 FK7003 Lecture 17 – Interactions in Matter ● Electromagnetic interactions in material ● Hadronic interactions in material ● Electromagnetic and hadronic.

Slides:



Advertisements
Similar presentations
Experimental Particle Physics
Advertisements

Gaseous Particle Detectors:
HEP Experiments Detectors and their Technologies Sascha Marc Schmeling CERN.
Lecture 3 – neutrino oscillations and hadrons
Детектори - II 4-ти курс УФЕЧ Спирачно лъчение (bremsstrahlung) Z 2 electrons, q=-e 0 M, q=Z 1 e 0 A charged particle of mass M and charge q=Z.
Particle interactions and detectors
Laura Gilbert How We Study Particles. The basics of particle physics! Matter is all made up of particles… Fundamental particle: LEPTON Fundamental particles:
Calorimetry and Showers Learning Objectives Understand the basic operation of a calorimeter (Measure the energy of a particle, and in the process, destroy.
Neutral Particles. Neutrons Neutrons are like neutral protons. –Mass is 1% larger –Interacts strongly Neutral charge complicates detection Neutron lifetime.
Introduction to Hadronic Final State Reconstruction in Collider Experiments Introduction to Hadronic Final State Reconstruction in Collider Experiments.
Introduction to Hadronic Final State Reconstruction in Collider Experiments Introduction to Hadronic Final State Reconstruction in Collider Experiments.
Counting Cosmic Rays through the passage of matter By Edwin Antillon.
Fundamental principles of particle physics
Particle Interactions
Exploring the Universe with Particles and Rays: α, β, γ, X, Cosmic, … Toby Burnett Prof, UW.
The CMS Muon Detector Thomas Hebbeker Aachen July 2001 Searching for New Physics with High Energy Muons.
Calorimeters A User’s Guide Elizabeth Dusinberre, Matthew Norman, Sean Simon October 28, 2006.
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.
March 2011Particle and Nuclear Physics,1 Experimental tools accelerators particle interactions with matter detectors.
My Chapter 30 Lecture.
Lecture 1.3: Interaction of Radiation with Matter
Tools for Nuclear & Particle Physics Experimental Background.
From Luigi DiLella, Summer Student Program
NEUTRON OPTICS & SHIELDING GROUP NATALIIA CHERKASHYNA TAP MEETING 23 RD OF JANUARY, 2014 Latest Developments on Shielding and Backgrounds.
LHC Detectors 101 Vivek Sharma (with slides stolen from talks of several people ) 1 Good review article: ARNPS 2006, “General purpose detectors for large.
Physics Modern Lab1 Electromagnetic interactions Energy loss due to collisions –An important fact: electron mass = 511 keV /c2, proton mass = 940.
Calorimeters Chapter 4 Chapter 4 Electromagnetic Showers.
Experimental Particle Physics PHYS6011 Joel Goldstein, RAL 1.Introduction & Accelerators 2.Particle Interactions and Detectors (2/2) 3.Collider Experiments.
NESTOR SIMULATION TOOLS AND METHODS Antonis Leisos Hellenic Open University Vlvnt Workhop.
Calorimeters Chapter 21 Chapter 2 Interactions of Charged Particles - With Focus on Electrons and Positrons -
Electrons Electrons lose energy primarily through ionization and radiation Bhabha (e+e-→e+e-) and Moller (e-e-→e-e-) scattering also contribute When the.
P ARTICLE D ETECTORS Mojtaba Mohammadi IPM-CMPP- February
Radiation Detectors In particular, Silicon Microstrip Detectors by Dr. Darrel Smith.
April 23, 2008 Workshop on “High energy photon collisions at the LHC 1 Cem Güçlü İstanbul Technical University Physics Department Physics of Ultra-Peripheral.
Interactions of Particles with Matter
Fundamental principles of particle physics G.Ross, CERN, July08.
Introduction to CERN Activities
1 Methods of Experimental Particle Physics Alexei Safonov Lecture #15.
Validation of EM Part of Geant4
PRELIMINARY RESULTS OF SIMULATIONS L.G. Dedenko M.V. Lomonosov Moscow State University, Moscow, Russia.
Neutrino-Nucleus Reactions at Medium and Low Energies [contents] 1. Neutrino and weak interaction 2. Cross section for ν-A and e-A reactions 3. EMC effect.
The Hybrid Scheme of Simulations of the Electron- photon and Electron-hadron Cascades In a Dense Medium at Ultra-high Energies L.G. Dedenko M.V. Lomonosov.
1 Methods of Experimental Particle Physics Alexei Safonov Lecture #9.
1 LHCb CMS ALICE ATLAS The ATLAS experiment at the LHC 27 km.
INTERACTIONS OF RADIATION WITH MATTER. twCshttp:// twCs
Eduardo Nebot del Busto (1) CERN, Geneva, Switzerland (2) The University of Liverpool, Department of physics, Liverpool, U. K (3) The Cockcroft Institute,
Learning Objectives Calorimetry and Showers
CMS Masterclass It’s a time of exciting new discoveries in particle physics! At CERN, the LHC succesfully completed Run I at 8 TeV of collision.
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.
Lecture 8 – Detectors - II
Lecture 18 - Detectors Detector systems
Particle accelerators
CMS Masterclasses 2017 S’Cool LAB
Calorimeters at CBM A. Ivashkin INR, Moscow.
Methods of Experimental Particle Physics
PHYS 3446 – Lecture #14 Energy Deposition in Media Particle Detection
Lecture 14 – Neutral currents and electroweak unification
Calorimeters in HEP Add hermiticity CC event - calibration
Spectrometry of high energy gamma ray
Experimental Particle Physics
Particle physics.
CMS Masterclass 2017.
Particle Detection 1. Costituents of Matter 2. Fundamental Forces
Experimental Particle Physics
PHYS 3446, Spring 2012 Andrew Brandt
PHYS 3446 – Lecture #17 Particle Detection Particle Accelerators
Particles going through matter
PHYS 3446 – Lecture #18 Monday ,April 9, 2012 Dr. Brandt Calorimeter
PHYS 3446 – Lecture #14 Energy Deposition in Media Particle Detection
Presentation transcript:

1 FK7003 Lecture 17 – Interactions in Matter ● Electromagnetic interactions in material ● Hadronic interactions in material ● Electromagnetic and hadronic showers

2 FK7003 Why we can neglect weak interactions E (TeV) Neutrino interaction lengthi In water/km Probability of interaction ~ / km water at 100 TeV energy 100 billion neutrinos pass through your thumbnail each second but only 1-2 will interact in your body during your lifetime. From lecture 3 Mean distance between interactions of neutrino + water molecule as neutrinos pass through water (interaction length).

3 FK7003 Strategy Energy loss of particles in matter  Electromagnetic energy loss ● Energy loss through collisions (ionisation) ● Radiation loss ● Electromagnetic shower  Hadronic energy loss ● Energy loss through nuclear collisions ● Hadronic shower

4 FK7003 Ionisation energy loss M

5 FK7003 M l Semi-classical derivation (skip)

6 FK7003

7 M

8

9

10 FK7003 Interaction between two particles

11 FK7003 Bethe-Bloch formula (17.23)

12 FK7003 Bethe-Bloch formula

13 FK7003 Measurements of ionisation energy loss e

14 FK7003 Strategy Energy loss of particles in matter  Electromagnetic energy loss ● Energy loss through collisions (ionisation) ● Radiation loss ● Electromagnetic shower  Hadronic energy loss ● Energy loss through nuclear collisions ● Hadronic shower

15 FK7003 Radiation energy loss E0E0 x

16 FK7003 Energy loss of an electron in copper ECEC

17 FK7003 Question

18 FK7003 Strategy Energy loss of particles in matter  Electromagnetic energy loss ● Energy loss through collisions (ionisation) ● Radiation loss ● Electromagnetic shower  Hadronic energy loss ● Energy loss through nuclear collisions ● Hadronic shower

19 FK7003 Photons

20 FK7003 Photon absorption in lead Lead

21 FK

22 FK (i) (ii)

23 FK7003 Electromagnetic shower E0E0 E 0 /2 E 0 /4 t=No. X 0 No. e + No. e - No.  No. particles

24 FK7003 Electromagnetic shower Observed electromagnetic shower (next lecture)

25 FK7003 Strategy Energy loss of particles in matter  Electromagnetic energy loss ● Energy loss through collisions (ionisation) ● Radiation loss ● Electromagnetic shower  Hadronic energy loss ● Energy loss through nuclear collisions ● Hadronic shower

26 FK7003 Hadronic energy loss p xx 

27 FK7003 Nuclear shower EM Cascade Nuclear cascade

28 FK7003 A simple model for hadronic scattering in material p   p L xx

29 FK7003 p   L Interaction Length xx 1 23 p

30 FK7003 Proton-nucleon cross sections p p

31 FK7003 Nuclear interaction length

32 FK7003 Stopping in iron

33 FK7003 Strategy Energy loss of particles in matter  Electromagnetic energy loss ● Energy loss through collisions (ionisation) ● Radiation loss ● Electromagnetic shower  Hadronic energy loss ● Energy loss through nuclear collisions ● Hadronic shower

34 FK7003 Energy loss mechanisms Important energy loss mechanisms for collider experiments (next lecture). ParticleIonisation energy loss Radiation energy loss Hadronic energy loss e + e - pair production e-e- Important only for low energies (<30 MeV) † xx  Important only at high energies (E >several hundred GeV ) † xx Charged hadrons (p,    K  …) Important only at high energies (E > several hundred GeV:    K - ; E> 1 TeV: p ) † x Neutral hadrons (n,K 0 ) xx x Photon xxx † Not important for these lectures

35 FK7003 Summary ● Interactions of particle in material ● Electromagnetic and hadronic energy loss  Ionisation and radiation energy loss (em)  Hadronic energy loss (strong) ● Now ready to design an detector for a collider experiment (next lecture).