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Introduction to Quantum Field Theory. Autumn 2010.
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- N.B.
-
- The examination is scheduled for 19-October-2010, 9:00-12:00,
at the address: Åbogade 36 (behind Kræftens Bekæmpelse). I will not
be there, but you are allowed to call me at my office, 89423651, to
clarify the formulations of the examination problems.
- A footnote is added at note10 reminding that the operators
within the interaction lagrangian are assumed to be in the normal order.
- The running headers on the lecture notes are reformatted into a
logical sequence: note1, note2, ..., note13.
- You can ask your last
questions on October 18th, 10:15-12:00, aud. 520-516.
- The examination is scheduled for October 19th.
If this date is is really inconvenient for somebody, send me a message,
we should be able to arrange a reexamination at some later date.
-
Correction: note 5: in the discussion of the direct product of
representation the correct term for the sum of generators is Kronecker
sum, not direct
sum.
- Schedule:
-
Lectures:
Wednesday, 10:15, Aud. 1525-323; and
Thursday, 11:15, Aud. 1525-323.
-
Seminars: Monday, 10:15, Aud. 1525-323.
- Weekly notes:
-
-
Introduction.
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The subject of quantum field theory. Particles and fields.
Principle of covariance. Special theory of relativity. Four-vector notation.
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Classical Lagrangian field theory.
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Principle of least action. Euler-Lagrange
equation of motion. Translation invariance and energy-momentum tensor.
Energy and momentum conservation. Global gauge invariance and conserved
current. Charge conservation. Noether's theorem.
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Canonical quantization of a complex scalar field.
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Klein-Gordon equation. Normal modes. Energy and charge in normal mode
representation. Number-of-particles operator. Generation/annihilation
operators. Statistics.
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Transformational properties of fields.
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[Exercises:
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The group of coordinate transformations.
Group representations. Lie groups and Lie algebras. Lie algebras
of the rotation group and the Lorentz group. Irreducible representations
of the rotation group.
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Irreducible representations of the Lorentz group.
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[Exercises:
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Direct product of two representations of a group. Reduction of
a direct product of two representations of the rotation group and the
Lorentz group. Parity transformation. Finite rotation matrix.
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Spin-1/2 field.
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Bispinors. Bilinear forms of bispinors. Gamma-matrices.
Lagrangian. Dirac equation.
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Canonical quantization of spin-1/2 field.
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Normal modes (plane-waves).
Charge and energy in normal mode representation. Generation-annihilation
operators: anti-commutation relation.
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Spin-1 fields.
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Massive spin-1 field, Lorenz condition; Electromagnetic field, gauge
invariance, quantization in radiation gauge; Spin-statistics theorem.
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Interacting quantum fields.
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Interaction Lagrangian; Time development
in quantum mechanics: Heisenberg,
Schrödinger, and interaction picture; S-matrix; Time-ordered product of
operators.
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Feynman diagrams.
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Calculation of the S-matrix elements: time- and normal-products of field
operators; propagators; Wick's theorem; Feynman diagrams in coordinate space.
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CPT theorem. Gauge theories.
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CPT symmetry. Gauge theories: QED; Yang-Mills (non-abelian) theories.
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Higgs mechanism.
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Spontaneous symmetry breaking; The Higgs mechanism; The Standard Model.
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Non-relativistic limit of QFT.
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Lippmann-Schwinger equation; One boson
exchange potential.
- Literature:
- P.J. Mulders,
Quantum Field Theory,
lecture notes.
- Links:
-
A free textbook on field theory by Warren Siegel
Wikipedia
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D.V.Fedorov
(fedorov (at) phys (dot) au (dot) dk)