Collective Vibration In general, forbidden – density change! forbidden – CM moves! OK... λ=0 λ=1 λ=2 λ=3 time.

Slides:



Advertisements
Similar presentations
MP-41 Teil 2: Physik exotischer Kerne, SS-2012 MP-41 Teil 2: Physik exotischer Kerne 13.4.Einführung, Beschleuniger 20.4.Schwerionenreaktionen, Synthese.
Advertisements

Quantum Harmonic Oscillator
Some (more) Nuclear Structure
Does instruction lead to learning?. A mini-quiz – 5 minutes 1.Write down the ground state wavefunction of the hydrogen atom? 2.What is the radius of the.
Coulomb excitation with radioactive ion beams
HL-5 May 2005Kernfysica: quarks, nucleonen en kernen1 Outline lecture (HL-5) Collective excitations of nuclei photo-excitation of GDR particle-hole excitations.
A Cool Party Trick. Fundamentals of Schroedinger Notation Schroedinger notation is usually called “position representation” However, Schroedinger notation.
Goldstone Bosons in Condensed Matter System Outline of lectures: 1. Examples (Spin waves, Phonon, Superconductor) 2. Meissner effect, Gauge invariance.
Atomic Vibrations in Solids: phonons
Second Quantization -- Fermions Do essentially the same steps as with bosons. Order all states and put in ones and zeros for filled and unfilled states.
Nuclear Radiation Basics Empirically, it is found that --
9. Interacting Relativistic Field Theories 9.1. Asymptotic States and the Scattering Operator 9.2. Reduction Formulae 9.3. Path Integrals 9.4. Perturbation.
NUCLEAR STRUCTURE PHENOMENOLOGICAL MODELS
Crystal Lattice Vibrations: Phonons
Formal Second Quantization Shrödinger Equation for a Many Particle System F&W – Chapter 1 Expand multiparticle wave function in terms of a complete set.
P460 - square well1 Square Well Potential Start with the simplest potential Boundary condition is that  is continuous:give: V 0 -a/2 a/2.
P460 - many particles1 Many Particle Systems can write down the Schrodinger Equation for a many particle system with x i being the coordinate of particle.
The Harmonic Oscillator
IBA Lecture part 2. Most general IBA Hamiltonian in terms with up to four boson operators (given N) IBA Hamiltonian Mixes d and s components of the wave.
Vibrational Spectroscopy
6. Second Quantization and Quantum Field Theory
Monday, Oct. 22, 2012PHYS , Fall 2012 Dr. Jaehoon Yu 1 PHYS 3313 – Section 001 Lecture #14 Monday, Oct. 22, 2012 Dr. Jaehoon Yu Infinite Potential.
Chapters 9, 11, 12 Concepts covered that will also be candidates for exam questions.
Lecture 24 Collective Excitations in nuclei Introduction: Over half the known nuclei have configurations (Z,N) even, J  = 0 + Recall that an empirical.
Operators A function is something that turns numbers into numbers An operator is something that turns functions into functions Example: The derivative.
Physics 451 Quantum mechanics I Fall 2012 Nov 5, 2012 Karine Chesnel.
Absorption and Emission of Radiation:
Wednesday, Oct. 30, 2013PHYS , Fall 2013 Dr. Jaehoon Yu 1 PHYS 3313 – Section 001 Lecture #14 Wednesday, Oct. 30, 2013 Dr. Jaehoon Yu Infinite.
Physics 451 Quantum mechanics I Fall 2012 Nov 7, 2012 Karine Chesnel.
(1) Experimental evidence shows the particles of microscopic systems moves according to the laws of wave motion, and not according to the Newton laws of.
Chapter 40.
Nuclear Collective Excitation in a Femi-Liquid Model Bao-Xi SUN Beijing University of Technology KITPC, Beijing.
Simple Harmonic Oscillator (SHO) Quantum Physics II Recommended Reading: Harris: chapter 4 section 8.
How do nuclei rotate? The nucleus rotates as a whole.
MS310 Quantum Physical Chemistry
Lecture 23: Applications of the Shell Model 27/11/ Generic pattern of single particle states solved in a Woods-Saxon (rounded square well)
Lecture 11. Hydrogen Atom References Engel, Ch. 9
4. Phonons Crystal Vibrations
MS310 Quantum Physical Chemistry
Some (more) High(ish)-Spin Nuclear Structure Paddy Regan Department of Physics Univesity of Surrey Guildford, UK Lecture 2 Low-energy.
Chapter 5: Quantum Mechanics
Physical Chemistry III (728342) The Schrödinger Equation
2.1Application of the Schrödinger Equation to the Hydrogen Atom 2.2Solution of the Schrödinger Equation for Hydrogen 2.3Quantum Numbers 2.4Magnetic Effects.
Vibrational Motion Harmonic motion occurs when a particle experiences a restoring force that is proportional to its displacement. F=-kx Where k is the.
Second Quantization of Conserved Particles Electrons, 3He, 4He, etc. And of Non-Conserved Particles Phonons, Magnons, Rotons…
Schrödinger Equation – Model Systems: We have carefully considered the development of the Schrödinger equation for important model systems – the one, two.
Monday, April 13, 2015PHYS , Spring 2015 Dr. Jaehoon Yu 1 PHYS 3313 – Section 001 Lecture # 19 Monday, April 13, 2015 Dr. Jaehoon Yu Refresher:
Lecture 21 More on singlet and triplet helium (c) So Hirata, Department of Chemistry, University of Illinois at Urbana-Champaign. This material has been.
Chapter 3 Postulates of Quantum Mechanics. Questions QM answers 1) How is the state of a system described mathematically? (In CM – via generalized coordinates.
Raman Effect The Scattering of electromagnetic radiation by matter with a change of frequency.
Quantum Theory of Hydrogen Atom
Quantum optics Eyal Freiberg.
UNIT 1 Quantum Mechanics.
CHAPTER 5 The Schrodinger Eqn.
Solid State Physics Lecture 11
THREE DIMENSIONAL SHROEDINGER EQUATION
CHAPTER 5 The Schrodinger Eqn.
PHL424: Nuclear surface vibration
Quantized Electron Orbits
Hydrogen Atom Returning now to the hydrogen atom we have the radial equation left to solve The solution to the radial equation is complicated and we must.
Lecture 21 More on singlet and triplet helium
Quantum Theory of Hydrogen Atom
Perturbation Theory Lecture 5.
PHL424: Nuclear surface vibration
Carbon Nanomaterials and Technology
Chapter 5 - Phonons II: Quantum Mechanics of Lattice Vibrations
Chapter II Klein Gordan Field Lecture 3 Books Recommended:
Chapter II Klein Gordan Field Lecture 1 Books Recommended:
Linear Vector Space and Matrix Mechanics
Second Quantization and Quantum Field Theory
Presentation transcript:

Collective Vibration In general, forbidden – density change! forbidden – CM moves! OK... λ=0 λ=1 λ=2 λ=3 time

Collective Vibration In general, λ=2: quadrupole vibrationλ=3: octupole vibration

Collective Vibration classical Hamiltonian Binding energy of a nucleus: a V = MeV a S = MeV a C = MeV a A = MeV a P = MeV constants:

Collective Vibration classical Hamiltonian quantization energy eigenvalue 0 wave function

Collective Vibration classical Hamiltonian differential equation

Second Quantization Hamilton operator rule for boson operators: creation & annihilation operators increase or decrease the number of phonons in a wave function ground state (vacuum) 1-phonon state 2-phonon state

Second Quantization Hamilton operator rule for boson operators: 1-phonon energy:

Second Quantization Hamilton operator rule for boson operators: 2-phonon energy: etc.

Second Quantization Hamilton operator rule for boson operators: 2-phonon state: normalization (approximation):

Second Quantization Hamilton operator rule for boson operators: 2-phonon state: normalization:

Collective Vibration

Example of vibrational excitations (E-E ground state) n=1, = 2, 2+ phonon n = 2, = 2, J  = 0+, 2+, 4+ ħ2ħ2 2ħ  2 3ħ  2 multiple = 2 phonon states, ideally degenerate 3- state?

Second Quantization Hamilton operator rule for boson operators: 2-phonon state: reduced transition probability:

Reduced transition probabilities 2-phonon state 3-phonon state

Reduced transition probabilities 1-phonon state 2-phonon state 3-phonon state