Difference between revisions of "Forest NucPhys I"
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=Introduction= | =Introduction= | ||
− | The interaction of charged particles (electrons and positrons) by the exchange of photons is described by a fundamental theory known as Quantum ElectroDynamics | + | The interaction of charged particles (electrons and positrons) by the exchange of photons is described by a fundamental theory known as Quantum ElectroDynamics. QED has perturbative solutions which are limited in accuracy only by the order of the perturbation you have expanded to. As a result the theory is quite useful in describing the interactions of electrons that are prevalent in Atomic physics. |
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+ | as | ||
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+ | Nuclear physics, however, encompases the interaction of charged pointlike particles (Dirac particles) in terms of the exchange of photons. | ||
Nuclear physics is described by quantum chromodynamics (QCD). | Nuclear physics is described by quantum chromodynamics (QCD). |
Revision as of 02:52, 23 January 2008
Advanced Nuclear Physics
References:
Krane:
Catalog Description:
PHYS 609 Advanced Nuclear Physics 3 credits. Nucleon-nucleon interaction, bulk nuclear structure, microscopic models of nuclear structure, collective models of nuclear structure, nuclear decays and reactions, electromagnetic interactions, weak interactions, strong interactions, nucleon structure, nuclear applications, current topics in nuclear physics. PREREQ: PHYS 624 OR PERMISSION OF INSTRUCTOR.
PHYS 624-625 Quantum Mechanics 3 credits. Schrodinger wave equation, stationary state solution; operators and matrices; perturbation theory, non-degenerate and degenerate cases; WKB approximation, non-harmonic oscillator, etc.; collision problems. Born approximation, method of partial waves. PHYS 624 is a PREREQ for 625. PREREQ: PHYS g561-g562, PHYS 621 OR PERMISSION OF INSTRUCTOR.
NucPhys_I_Syllabus
Introduction
The interaction of charged particles (electrons and positrons) by the exchange of photons is described by a fundamental theory known as Quantum ElectroDynamics. QED has perturbative solutions which are limited in accuracy only by the order of the perturbation you have expanded to. As a result the theory is quite useful in describing the interactions of electrons that are prevalent in Atomic physics.
as
Nuclear physics, however, encompases the interaction of charged pointlike particles (Dirac particles) in terms of the exchange of photons.
Nuclear physics is described by quantum chromodynamics (QCD).
QED has
Nomenclature
Variable | Definition |
Z | Atomic Number |
A | Atomic Mass |
L | Angular Momentum |
L | Angular Momentum |
L | Angular Momentum |
Nuclide | A specific nuclear species |
Isotope | Nuclides with same Z but different N |
Isotones | Nuclides with same N but different Z |
Isobars | Nuclides with same A |
Nuclide | A specific nuclear species |
Nucelons | Either a neutron or a proton |
J | Nuclear Angular Momentum |
Notation
= An atom identified by the Chemical symbol with protons and neutrons.
Notice that
and are redundant since can be identified by the chemical symbol and can be determined from both and the chemical symbol (N=A-Z).- example