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Spontaneously broken spacetime symmetries and Goldstone's theorem
1Jefferson Physical Laboratory, Harvard University, Cambridge, Massachusetts 02138, USA.
Physical Review Letters
|March 23, 2002
Summary
Goldstone's theorem correctly predicts massless particles for broken symmetries. This study resolves discrepancies in counting these particles for spontaneously broken spacetime symmetries, including Poincaré and conformal invariance.
Area of Science:
- Theoretical Physics
- High Energy Physics
- Condensed Matter Theory
Background:
- Goldstone's theorem links broken symmetry generators to massless modes.
- The standard theorem fails for spontaneously broken spacetime symmetries.
- Existing methods do not consistently yield the correct count of massless modes.
Purpose of the Study:
- To provide a general method for correctly counting massless modes.
- To resolve the failure of naive generalizations of Goldstone's theorem.
- To analyze massless modes in spontaneously broken Poincaré and conformal symmetries.
Main Methods:
- Revisiting the theoretical framework of spontaneous symmetry breaking.
- Developing a generalized counting procedure for massless modes.
- Applying the method to specific examples of spacetime symmetries.
Main Results:
- A corrected method for enumerating massless modes in spontaneously broken theories.
- Demonstration of the method's efficacy for Poincaré and conformal symmetries.
- Resolution of the long-standing issue with naive mode counting.
Conclusions:
- The generalized method accurately predicts massless modes for broken spacetime symmetries.
- This work clarifies the application of Goldstone's theorem in complex symmetry breaking scenarios.
- The findings have implications for understanding particle physics and condensed matter systems.