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2023年度:理論ゼミ [2023/10/02 05:44] p1 |
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^ 担当順 ^ 担当 | ^ 担当順 ^ 担当 | ||
- | |1|大澤| 1 |{{ : | + | |1|大澤| 1 Attempts at relativistic quantum mechanics |
- | |2|鴛原| 2 |{{ : | + | |2|鴛原| 2 Lorentz Invariance |
- | |3|斎藤(一)| 3 | {{ : | + | |3|斎藤(一)| 3 Canonical Quantization of Scalar Fields |
- | |4|齊藤(巧)| 4 | {{ : | + | |4|齊藤(巧)| 4 The Spin-Statistics Theorem |
- | |5|篠田| 5 | {{ : | + | |5|篠田| 5 The LSZ Reduction Formula |
- | |6|佐々木| 6 |{{ : | + | |6|佐々木| 6 Path Integrals in Quantum Mechanics |
- | |7|中島| 7 | {{ : | + | |7|中島| 7 The Path Integral for the Harmonic Oscillator |
- | |8|林| 8 |{{ : | + | |8|林| 8 The Path Integral for Free Field Theory |
- | |9|藤木| 9 |{{ : | + | |9|藤木| 9 The Path Integral for Interacting Field Theory |
- | |10|松井| 10 |{{ : | + | |10|松井| 10 Scattering Amplitudes and the Feynman Rules |{{ : |
- | |11|中村| 11 | {{ : | + | |11|中村| 11 Cross Sections and Decay Rates | {{ : |
- | |12|三木| 12 |{{ : | + | |12|三木| 12 Dimensional Analysis with hbar = c = 1 |{{ : |
- | |13|堀| 13 | {{ : | + | |13|堀| 13 The Lehmann-Kallen Form of the Exact Propagator |
- | |14|溝添|14|{{ : | + | |14|溝添| 14 Loop Corrections to the Propagator |
- | |15|大澤| 15 |{{ : | + | |15|大澤| 15 The One-Loop Correction in Lehmann-Kallen Form |{{ : |
- | |16|鴛原| 16 |{{ : | + | |16|鴛原| 16 Loop Corrections to the Vertex |
- | |17|齊藤(巧)| 17 |はよ資料あげてもろて | + | |17|齊藤(巧)| 17 Other 1PI Vertices |
- | |18|齊藤(巧)| 18 | {{ : | + | |18|齊藤(巧)| 18 Higher-Order Corrections and Renormalizability |
- | |19|篠田| 19 |{{ : | + | |19|篠田| 19 Perturbation Theory to All Orders |
- | |20|佐々木| 20 |{{ : | + | |20|佐々木| 20 Two-Particle Elastic Scattering at One Loop |{{ : |
- | |21|中島| 21 |{{ : | + | |21|中島| 21 The Quantum Action |
- | |22|林| 22 | {{ : | + | |22|林| 22 Continuous Symmetries and Conserved Currents |
- | |23|中村|23|{{ : | + | |23|中村| 23 Discrete Symmetries: P , T , C , and Z |{{ : |
- | |24|松井| 24 |{{ : | + | |24|松井| 24 Nonabelian Symmetries |
- | |25|藤木| 25 |{{ : | + | |25|藤木| 25 Unstable Particles and Resonances |
- | |26|三木| 26 |{{ : | + | |26|三木| 26 Infrared Divergences |
- | |27|堀| 27 |{{ : | + | |27|堀| 27 Other Renormalization Schemes |
+ | |28|溝添| 28 The Renormalization Group |{{ : | ||
+ | |29|大澤| 29 Effective field theory |{{ : | ||
+ | |30|鴛原| 30 Spontaneous Symmetry Breaking |{{ : | ||
+ | |31|篠田| 31 Broken Symmetry and Loop Corrections |{{ : | ||
+ | |32|齊藤(巧)| 32 Spontaneous Breaking of Continuous Symmetries |{{ : | ||
+ | |33|中島| 33 Representations of the Lorentz Group |{{ : | ||
+ | |34|佐々木| 34 Left- and Right-Handed Spinor Fields |{{ : | ||
+ | |35|中村| 35 Manipulating Spinor Indices |{{ : | ||
+ | |36|林| 36 Lagrangians for Spinor Fields |{{ : | ||
+ | |37|藤木| 37 Canonical Quantization of Spinor Fields I |{{ : | ||
+ | |38|松井| 38 Spinor Technology |{{ : | ||
+ | |39|堀| 39 Canonical Quantization of Spinor Fields II |{{ : | ||
+ | |40|三木| 40 Parity, Time Reversal, and Charge Conjugation |{{ : | ||
+ | |41|大澤| 41 LSZ Reduction for Spin-One-Half Particles |{{ : | ||
+ | |42|溝添| 42 The Free Fermion Propagator |{{ : | ||
+ | |43|篠田| 43 The Path Integral for Fermion Fields |{{ : |