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About Lecture 13 Summary
1. The Lagrangian and Hamiltonian formulations of classical mechanics possess certain symmetries. Specifically, the Lagrangian can be multiplied by a constant, a constant can be added to it, or a total derivative can be added without changing the physics or equations of motion. 2. In classical mechanics, the Hamiltonian cannot depend on odd combinations of coordinates like rjk × rlm · rno since these change sign under a parity transformation, while even combinations like rjk · rlm are invariant. 3. However, in processes involving the weak interaction, parity is not a symmetry and the Hamiltonian can depend on terms that change sign, like the dot product of an electron's momentum and a muon's angular momentum in muon decay.
Detailed Information
| Author: | ['Raúl Hugo'] |
|---|---|
| Publication Year: | 2019 |
| Pages: | 2 |
| Language: | English |
| Format: | |
| Price: | FREE |
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