Methods of excitation: nuclear reactions

Slides:



Advertisements
Similar presentations
Day 15: Electric Potential due to Point Charges The Electric Potential of a Point Charge Work done to bring two point charges together The Electric Potential.
Advertisements

When we have two charged particles interacting, there is a difference between potential energy and electric potential. A.True B.False.
Coulomb excitation with radioactive ion beams
An electromagnetic analog of gravitational wave memory Midwest Relativity Meeting Milwaukee, WI Oct. 25, 2013.
The Multipole Expansion of the Electric Potential and Non-Spherical Nuclei John Karkheck Marquette University Summer Meeting American Association of Physics.
8/5/08Lecture 2 Part 21 Maxwell’s Equations of the Electromagnetic Field Theory Gauss’s Law – charge makes an electric field The magnetic field is solenoidal.
21-1 Physics I Class 21 Thinking About Electric Fields and Electric Potential.
Week 11 Lecture 27 Monday, Oct 30, 2006 NO CLASS : DPF06 conference Lecture 28 Wednesday, Nov 1, 2006 GammaDecaysGammaDecays Lecture 29 Friday, Nov 3,
Nuclear de-excitation Outline of approach… Source of radiation Propagation of radiation field Detection of radiation ?? nucleus.
Nuclear Electromagnetic Moments
NUCLEAR STRUCTURE PHENOMENOLOGICAL MODELS
02/03/2014PHY 712 Spring Lecture 81 PHY 712 Electrodynamics 10-10:50 AM MWF Olin 107 Plan for Lecture 8: Start reading Chapter 4 Multipole moment.
© 2012 Pearson Education, Inc. { Chapter 23 Electric Potential (cont.)
Day18: Electric Dipole Potential & Determining E-Field from V
PHYS 580 Nuclear Structure Chapter5-Lecture1 GAMMA DECAY
6-1 RFSS: Lecture 6 Gamma Decay Part 1 Readings: Modern Nuclear Chemistry, Chap. 9; Nuclear and Radiochemistry, Chapter 3 Energetics Decay Types Transition.
Chapter 27 Magnetism. Introduction Our approach –Review of E&M interaction ideas –Magnetic fields & magnets (initial ideas) –Magnetic field and currents.
 Somnath Bharadwaj and Pratik Khastgir, Department of Physics and Meteorology, IIT Kharagpur, India Electromagnetic.
3. 3 Separation of Variables We seek a solution of the form Cartesian coordinatesCylindrical coordinates Spherical coordinates Not always possible! Usually.
Lecture 20: More on the deuteron 18/11/ Analysis so far: (N.B., see Krane, Chapter 4) Quantum numbers: (J , T) = (1 +, 0) favor a 3 S 1 configuration.
Intermolecular Forces:Electrostatics “Dielectrics Different classical electrostatic interactions.
abrasion ablation  σ f [cm 2 ] for projectile fragmentation + fission  luminosity [atoms cm -2 s -1 ]  70% transmission SIS – FRS  ε trans transmission.
The Exciting Scavenger Hunt By: Elyssa, Bella and the Two Others.
02/05/2014PHY 712 Spring Lecture 91 PHY 712 Electrodynamics 11-11:50 AM MWF Olin 107 Plan for Lecture 9: Continue reading Chapter 4 Dipolar fields.
§3.4. 1–3 Multipole expansion Christopher Crawford PHY
Energy Kinetic Energy Potential Energy.
Chapter 5 Interactions of Ionizing Radiation. Ionization The process by which a neutral atom acquires a positive or a negative charge Directly ionizing.
PARALLEL PLATES. From previous work, the electric field strength can be found from the electric force on a test charge.
Finish EM Ch. 5: Magnetostatics Methods of Math
Jan 2001AFOSR San Antonio Meeting Inverse Source Problem A.J. Devaney and Mei-Li, “The inverse source problem in non-homogeneous background media”, accepted.
Nuclear and Radiation Physics, BAU, First Semester, (Saed Dababneh). 1 Extreme independent particle model!!! Does the core really remain inert?
11. Radiation. What is radiation? Radiation sources Antenna: radio waves, microwaves Atoms, molecules: light, infrared light, UV, X-rays Nuclei: Gamma.
 Somnath Bharadwaj and Pratik Khastgir, Department of Physics and Meteorology, IIT Kharagpur, India Electromagnetic.
Authorization and Inspection of Cyclotron Facilities Radiation Fields.
Finish EM Ch.5: Magnetostatics Methods of Math. Physics, Thus. 10 March 2011, E.J. Zita Lorentz Force Ampere’s Law Maxwell’s equations (d/dt=0) Preview:
3.3 Separation of Variables 3.4 Multipole Expansion
Move It, Move It!!!! Forms of Energy. Mechanical Energy Energy of movement(can be in a potential or kinetic state)
Nuclear and Radiation Physics, BAU, 1 st Semester, (Saed Dababneh). 1 Electromagnetic moments Electromagnetic interaction  information about.
ELECTROMAGNETIC PARTICLE: MASS, SPIN, CHARGE, AND MAGNETIC MOMENT Alexander A. Chernitskii.
Intermolecular Forces “Review” of electrostatics -> today Force, field, potentials, and energy Dipoles and multipoles Discussion of types of classical.
Multipole Moments Section 41. Expand potential  in powers of 1/R 0.
W. Udo Schröder, 2005 Gamma Decay 1. W. Udo Schröder, 2005 Gamma Decay 2 Photons Photons: generated by moving charge distributions. Distributions can.
System of charges in an external field
Magnets and Electromagnetic Induction
Christopher Crawford PHY
Electric Dipole and Equipotential Surfaces
Forms of Energy Foldable
Forms of Energy Foldable
Studies of Pear Shaped Nuclei using rare isotope beams
§5.3: Magnetic Multipole Expansion
PHL424: γ-decay γ-decay is an electromagnetic process where the nucleus decreases in excitation energy, but does not change proton or neutron numbers This.
§3.4.1–3 Multipole expansion
Types of energy By: Brian Jome.
Interactions of Electromagnetic Radiation
The Mysterious Magnetic Field
Energy and Electrons energy
Christopher Crawford PHY
Related OSE's.
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 9:
individual excitations of nucleons
Electrical Energy & Capacitance Pgs
Forms of energy Chapter 5 section 2.
Interaction of Radiation with Matter
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 9:
Symmetry Concept: Multipolar Electric and Magnetic Fields
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 8:
Forms of Energy Vocabulary.
Three kinds of particle emission
Electricity and Magnetism
Cold Atom project 12/02/2019.
Presentation transcript:

Methods of excitation: nuclear reactions

Electromagnetic excitation 208Pb beam 238U target energy of gamma radiation (keV) log (intensity)

Electric fields of multipoles In general the electric potential due to an arbitrary charge distribution is expansion special case: electric monopole

Electric fields of multipoles In general the electric potential due to an arbitrary charge distribution is homogenous charge distribution special case: electric monopole

Electric field lines of two interacting charges

Monopole, dipole, quadrupole, ... octopole

Monopole, dipole, quadrupole, ...

Electric fields of multipoles In general the electric potential due to an arbitrary charge distribution is expansion multipole moments special case: electric quadrupole potential special case: electric quadrupole matrixelement B(E2)-value: