By Ben Simons
Quantum mechanics underpins quite a few huge topic components inside of physics
and the actual sciences from excessive strength particle physics, good country and
atomic physics via to chemistry. As such, the topic is living on the core
of each physics programme.
In the subsequent, we record an approximate “lecture by means of lecture” synopsis of
the diversified issues handled during this path.
1 Foundations of quantum physics: evaluate after all constitution and
organization; short revision of historic historical past: from wave mechan-
ics to the Schr¨odinger equation.
2 Quantum mechanics in a single measurement: Wave mechanics of un-
bound debris; strength step; capability barrier and quantum tunnel-
ing; certain states; oblong good; !-function power good; Kronig-
Penney version of a crystal.
3 Operator tools in quantum mechanics: Operator methods;
uncertainty precept for non-commuting operators; Ehrenfest theorem
and the time-dependence of operators; symmetry in quantum mechan-
ics; Heisenberg illustration; postulates of quantum concept; quantum
4 Quantum mechanics in additional than one size: inflexible diatomic
molecule; angular momentum; commutation relatives; elevating and low-
ering operators; illustration of angular momentum states.
5 Quantum mechanics in additional than one size: important po-
tential; atomic hydrogen; radial wavefunction.
6 movement of charged particle in an electromagnetic ﬁeld: Classical
mechanics of a particle in a ﬁeld; quantum mechanics of particle in a
ﬁeld; atomic hydrogen – common Zeeman influence; diamagnetic hydrogen and quantum chaos; gauge invariance and the Aharonov-Bohm impression; loose electrons in a magnetic ﬁeld – Landau levels.
7-8 Quantum mechanical spin: background and the Stern-Gerlach experi-
ment; spinors, spin operators and Pauli matrices; pertaining to the spinor to
spin path; spin precession in a magnetic ﬁeld; parametric resonance;
addition of angular momenta.
9 Time-independent perturbation idea: Perturbation sequence; ﬁrst and moment order enlargement; degenerate perturbation concept; Stark impression; approximately unfastened electron model.
10 Variational and WKB process: floor country power and eigenfunc tions; software to helium; excited states; Wentzel-Kramers-Brillouin method.
11 exact debris: Particle indistinguishability and quantum statis-
tics; house and spin wavefunctions; effects of particle statistics;
ideal quantum gases; degeneracy strain in neutron stars; Bose-Einstein
condensation in ultracold atomic gases.
12-13 Atomic constitution: Relativistic corrections; spin-orbit coupling; Dar-
win constitution; Lamb shift; hyperﬁne constitution; Multi-electron atoms;
Helium; Hartree approximation and past; Hund’s rule; periodic ta-
ble; coupling schemes LS and jj; atomic spectra; Zeeman effect.
14-15 Molecular constitution: Born-Oppenheimer approximation; H2+ ion; H2
molecule; ionic and covalent bonding; molecular spectra; rotation; nu-
clear records; vibrational transitions.
16 box conception of atomic chain: From debris to ﬁelds: classical ﬁeld
theory of the harmonic atomic chain; quantization of the atomic chain;
17 Quantum electrodynamics: Classical conception of the electromagnetic
ﬁeld; conception of waveguide; quantization of the electromagnetic ﬁeld and
18 Time-independent perturbation conception: Time-evolution operator;
Rabi oscillations in point structures; time-dependent potentials – gen-
eral formalism; perturbation conception; surprising approximation; harmonic
perturbations and Fermi’s Golden rule; moment order transitions.
19 Radiative transitions: Light-matter interplay; spontaneous emis-
sion; absorption and motivated emission; Einstein’s A and B coefficents;
dipole approximation; choice principles; lasers.
20-21 Scattering conception I: fundamentals; elastic and inelastic scattering; method
of particle waves; Born approximation; scattering of exact particles.
22-24 Relativistic quantum mechanics: historical past; Klein-Gordon equation;
Dirac equation; relativistic covariance and spin; loose relativistic particles
and the Klein paradox; antiparticles and the positron; Coupling to EM
ﬁeld: gauge invariance, minimum coupling and the relationship to non- relativistic quantum mechanics; ﬁeld quantization.
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Extra resources for Advanced Quantum Physics
SYMMETRY IN QUANTUM MECHANICS 26 This is clearly a discrete transformation. Application of parity twice returns the initial state implying that Pˆ 2 = 1. Therefore, the eigenvalues of the parity operation (if such exist) are ±1. A wavefunction will have a defined parity if and only if it is an even or odd function. For example, for ψ(x) = cos(x), Pˆ ψ = cos(−x) = cos(x) = ψ; thus ψ is even and P = 1. Similarly ψ = sin(x) is odd with P = −1. Later, in the next chapter, we will encounter the spherical harmonic functions which have the following important symmetry under parity, Pˆ Y m = (−1) Ylm .
Previously, we have seen that a symmetric attractive potential always leads to a bound state in one-dimension. However, odd parity states become bound only at a critical strength of the interaction. 4 Atomic hydrogen The Hydrogen atom consists of an electron bound to a proton by the Coulomb potential, V (r) = − 1 e2 . 4π 0 r We can generalize the potential to a nucleus of charge Ze without complication of the problem. Since we are interested in finding bound states of the proton-electron system, we are looking for solutions with E negative.
3). Therefore, a quantum system has spatial translation as an invariance group if and only if the following condition holds, ˆ (a)H ˆ =H ˆU ˆ (a), U ˆ =H ˆp ˆH ˆ. e. p ˆ = H(ˆ ˆ p), This demands that the Hamiltonian is independent of position, H as one might have expected! Similarly, the group of unitary transformaˆ (b) = exp[− i b · ˆr], performs translations in momentum space. tions, U ˆ (b) = Moreover, spatial rotations are generated by the transformation U i ˆ ˆ ˆ denotes the angular momentum operator.
Advanced Quantum Physics by Ben Simons