Discussion Overview
The discussion revolves around Thomas Larsson's post regarding the implications of Thiemann's "Loop-String" paper, particularly focusing on the differences between Loop Quantum Gravity (LQG) representations and lowest-energy representations. The scope includes theoretical considerations and algebraic structures within quantum gravity frameworks.
Discussion Character
- Exploratory
- Technical explanation
- Debate/contested
Main Points Raised
- Larsson argues that the algebraic differences between LQG representations and lowest-energy representations explain the absence of anomalies in Thiemann's approach, suggesting that this may establish LQG as a quantum theory.
- K-H Rehren highlights that quantizing classical invariant observables via normal ordering leads to a quantum algebra that differs from classical relations, introducing additional generators and potentially violating the correspondence principle.
- Some participants propose that the correspondence principle may not be violated if classical physics is expressed in terms of Taylor data, although convergence issues may arise.
- Rehren mentions a no-go theorem by V. Kac, indicating that maintaining non-triviality, anomaly freedom, positive energy, unitarity, and ghost freedom simultaneously is problematic, suggesting that sacrificing anomaly freedom might be the least damaging option.
- Larsson distinguishes between "lowest-A-number" representations in LQG and lowest-energy representations, asserting that the former is essentially classical and thus lacks anomalies.
- Participants discuss the implications of different vacuum states in relation to normal ordering and the algebraic structures generated by bilinears in LQG, noting that the absence of anomalies in LQG may stem from its classical nature.
Areas of Agreement / Disagreement
Participants express differing views on the implications of Larsson's arguments, with some agreeing on the inequivalence of LQG quantization to standard quantization, while others challenge or refine these points. The discussion remains unresolved regarding the broader implications for LQG and its relationship to established quantum theories.
Contextual Notes
There are limitations regarding the assumptions made about the correspondence principle and the implications of the algebraic differences discussed. The dependence on specific definitions and the unresolved nature of certain mathematical steps are also noted.