How do nuclei rotate? 1. The molecular picture.

Slides:



Advertisements
Similar presentations
Molecular Bonds Molecular Spectra Molecules and Solids CHAPTER 10 Molecules and Solids Johannes Diderik van der Waals (1837 – 1923) “You little molecule!”
Advertisements

Electromagnetic Properties of
The Collective Model and the Fermi Gas Model
How do nuclei rotate? 5. Appearance of bands. Deformed mean field solutions This is clearly the case for a well deformed nucleus. Deformed nuclei show.
II. Spontaneous symmetry breaking. II.1 Weinberg’s chair Hamiltonian rotational invariant Why do we see the chair shape? States of different IM are so.
The Collective Model Aard Keimpema.
Chemistry 2 Lecture 10 Vibronic Spectroscopy. Learning outcomes from lecture 9 Excitations in the visible and ultraviolet correspond to excitations of.
CHEM 515 Spectroscopy Vibrational Spectroscopy II.
Light: oscillating electric and magnetic fields - electromagnetic (EM) radiation - travelling wave Characterize a wave by its wavelength,, or frequency,
W. Udo Schröder, 2005 Rotational Spectroscopy 1. W. Udo Schröder, 2005 Rotational Spectroscopy 2 Rigid-Body Rotations Axially symmetric nucleus 
Lesson 9 Gamma Ray Decay. Electromagnetic decay There are two types of electromagnetic decay,  -ray emission and internal conversion (IC). In both of.
Dr. Jie ZouPHY Chapter 43 Molecules and Solids.
Classical Model of Rigid Rotor
Microwave Spectroscopy II
Molecular transitions and vibrations
Vibrational and Rotational Spectroscopy
The Shell Model of the Nucleus 5. Nuclear moments
NSDD Workshop, Trieste, February 2006 Nuclear Structure (II) Collective models P. Van Isacker, GANIL, France.
Lecture 24 Collective Excitations in nuclei Introduction: Over half the known nuclei have configurations (Z,N) even, J  = 0 + Recall that an empirical.
5. Exotic modes of nuclear rotation Tilted Axis Cranking -TAC.
Electronic Spectroscopy
Revisit vibrational Spectroscopy
4. The rotating mean field. The mean field concept A nucleon moves in the mean field generated by all nucleons. The mean field is a functional of the.
MOLECULAR SPECTROSCOPY  SPECTROSCOPY IS THAT BRANCH OF SCIENCE WHICH DEALS WITH THE STUDY OF INTERACTION OF ELECTROMAGNETIC RADIATION WITH MATTER.  ELECTROMAGNETIC.
Chirality of Nuclear Rotation S. Frauendorf Department of Physics University of Notre Dame, USA IKH, Forschungszentrum Rossendorf Dresden, Germany.
Collective Model. Nuclei Z N Character j Q obs. Q sp. Qobs/Qsp 17 O 8 9 doubly magic+1n 5/ K doubly magic -1p 3/
MOLECULAR SPECTROSCOPY  SPECTROSCOPY IS THAT BRANCH OF SCIENCE WHICH DEALS WITH THE STUDY OF INTERACTION OF ELECTROMAGNETIC RADIATION WITH MATTER.  ELECTROMAGNETIC.
1 New symmetries of rotating nuclei S. Frauendorf Department of Physics University of Notre Dame.
ROTATIONAL SPECTROSCOPY
Spontaneous symmetry breaking and rotational bands S. Frauendorf Department of Physics University of Notre Dame.
Surrey Mini-School Lecture 2 R. F. Casten. Outline Introduction, survey of data – what nuclei do Independent particle model and residual interactions.
Quantum Chemistry: Our Agenda (along with Engel)
How do nuclei rotate? The nucleus rotates as a whole.
MS310 Quantum Physical Chemistry
Partition functions of ideal gases. We showed that if the # of available quantum states is >> N The condition is valid when Examples gases at low densities.
Petrică Buganu, and Radu Budaca IFIN-HH, Bucharest – Magurele, Romania International Workshop “Shapes and Dynamics of Atomic Nuclei: Contemporary Aspects”
Nuclear and Radiation Physics, BAU, 1 st Semester, (Saed Dababneh). 1 Shell model Notes: 1. The shell model is most useful when applied to closed-shell.
Nuclear and Radiation Physics, BAU, First Semester, (Saed Dababneh). 1 Extreme independent particle model!!! Does the core really remain inert?
A close up of the spinning nucleus S. Frauendorf Department of Physics University of Notre Dame, USA IKH, Forschungszentrum Rossendorf Dresden, Germany.
Left-handed Nuclei S. Frauendorf Department of Physics University of Notre Dame, USA IKH, Forschungszentrum Rossendorf Dresden, Germany.
Symmetries of the Cranked Mean Field S. Frauendorf Department of Physics University of Notre Dame USA IKH, Forschungszentrum Rossendorf, Dresden Germany.
Triaxiality in nuclei: Theoretical aspects S. Frauendorf Department of Physics University of Notre Dame, USA IKH, Forschungszentrum Rossendorf Dresden,
Rotation and vibration spectra. Rotational States Molecular spectroscopy: We can learn about molecules by studying how molecules absorb, emit, and scatter.
Chapter 8. Molecular Motion and Spectroscopy
How do nuclei rotate? 3. The rotating mean field.
W. Udo Schröder, 2005 Gamma Decay 1. W. Udo Schröder, 2005 Gamma Decay 2 Photons Photons: generated by moving charge distributions. Distributions can.
Nordita Workshop on chiral bands /04/2015 Multiple chiral bands associated with the same strongly asymmetric many- particle nucleon configuration.
Rotational energy term in the empirical formula for the yrast energies in even-even nuclei Eunja Ha and S. W. Hong Department of Physics, Sungkyunkwan.
Harmonic Oscillator and Rigid Rotator
Determining Reduced Transition Probabilities for 152 ≤ A ≤ 248 Nuclei using Interacting Boson Approximation (IBA-1) Model By Dr. Sardool Singh Ghumman.
Molecular Spectroscopy
Shape parameterization
oblate prolate l=2 a20≠0, a2±1= a2±2= 0 Shape parameterization
20/30.
PHL424: Nuclear rotation.
CHAPTER 9 Molecules Rotations Spectra Complex planar molecules
CHAPTER 9 Molecules Rotations Spectra Complex planar molecules
Diatomic molecules
Interactions of Electromagnetic Radiation
Quantal rotation Molecules
How do nuclei rotate? 2. High Spin.
High spin physics- achievements and perspectives
Rotational Spectroscopy
Interactions of Elm. Radiation: Extended Task
20/30.
Molecular Spectra By – P.V.Koshti.
How do nuclei rotate? 5. Appearance of bands.
II. Spontaneous symmetry breaking
How do nuclei rotate? 1. The molecular picture.
Quantal rotation Molecules
Presentation transcript:

How do nuclei rotate? 1. The molecular picture

The classical rotor 1 2 3

Axial rotor Classical motion of J K J orbit

Small E Triaxial rotor Classical motion of J wobbling motion Intermediate E Large E

Euler angles

Quantization

The molecular rotor Axial rotor 1 2 3

K J orbit

Centrifugal stretching Stiff bonds

1 2 3 Triaxial rotor Small E wobbling motion

Born-Oppenheimer Approximation . Electronic motion Vibrations Rotations CO

Adiabatic approximation el rot vib

HCl Microwave absorption spectrum

Band Spectrum

Indistinguishable Particles . Upper particles Lower particles 2 Restriction of orientation

The nuclear rotor Most nuclei have a deformed axial shape. Unified Model (Bohr and Mottelson): The nucleus rotates as a whole. (collective degrees of freedom) The nucleons move independently inside deformed potential (intrinsic degrees of freedom) The nucleonic motion is much faster than the rotation (adiabatic approximation)

Nucleons are indistinguishable The nucleus does not have an orientation degree of freedom with respect to the symmetry axis. Axial symmetry

symmetry

Electromagnetic Transitions Emitted photon has multipolarity E1, E2, E2, ... or M1, M2, ... Multipole moments of the nucleus

Reduced transition probabilities in the Unified Model

Limitations of the molecular picture rigid rotor HCl Nucleons are not on fixed positions. The nuclear surface What is rotating?

More like a liquid, but what kind of? Ideal “irrotational flow” moment of inertia viscous

rigid irrotational

Breakdown of adiabatic approximation

Summary Molecules are the protoype of quantal rotors. Electronic and vibrational motion are much faster than rotation. Rotational bands consist of states with different angular momentum and the same intrinsic state (elec., vib.). Indistiguishability leads to restrictions in the possible values of the angular momentum. Nuclei at low spin are are similar to molecules. The nuclear surface is rotating. Unified model: intrinsic states correspond to the motion of nucleons in the deformed potential. Nuclei are liquid-like. The flow pattern is dominated by quantal effects. Microscopic theory needed for calculating them.