Hossenfelder's beautiful idea resolves QG/QFT tension

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Discussion Overview

The discussion revolves around Sabine Hossenfelder's proposal for resolving the tensions between quantum gravity (QG) and quantum field theory (QFT). Participants explore the implications of her idea, which suggests a mechanism where gravity can be treated classically at high energies while remaining perturbatively quantized at low energies. The conversation includes theoretical implications, comparisons to historical ideas, and critiques of the proposal.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Hossenfelder's proposal suggests that gravity can decouple from matter fields at high energies due to a change in the quantization condition, making Planck's constant a field that undergoes symmetry breaking.
  • Some participants express enthusiasm for the potential of Hossenfelder's idea to yield testable predictions and to unify quantum geometry with QFT.
  • Others draw parallels between Hossenfelder's approach and historical ideas, such as David Finkelstein's notion of quantizing the imaginary unit, suggesting that it may offer a new algebraic structure.
  • Concerns are raised regarding the ad hoc nature of Hossenfelder's postulated commutation relation, with some participants questioning its convincingness and appeal.
  • A participant highlights a potential issue with distinguishing between the c-number field and the operator in Hossenfelder's equations, raising questions about the implications for high-energy states not in thermodynamic equilibrium.
  • Another participant suggests that Hossenfelder's theory could be likened to the Higgs effect, proposing a new scalar particle, and humorously suggests naming it "HHH theory."

Areas of Agreement / Disagreement

Participants express a mix of enthusiasm and skepticism regarding Hossenfelder's proposal. While some find it original and potentially groundbreaking, others raise significant concerns about its foundations and implications. No consensus is reached on the validity or appeal of the idea.

Contextual Notes

Participants note limitations regarding the clarity of the relationship between the c-number field and the operator in Hossenfelder's framework, particularly at high energies. The discussion reflects a range of interpretations and uncertainties about the proposal's implications.

  • #31
What exactly are the consequences of [STRIKE]h[/STRIKE] going to zero at high energies?
 
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  • #32
Berlin said:
If at high energies h --> 0 it would also mean that the big bang would consist of a near classical bose gas of spin-0 particles without Pauli exclusion.
This suggests another argument against the hossi's proposal. If at high energies quantum fluctuations vanish, then the early inflationary phase of the Universe expansion cannot explain the primordial density fluctuations, which are needed to explain the observed inhomogenities in the spectrum of cosmic microwave background.
 
  • #33
Berlin said:
But what would happen with the fermi statistics kicking in? Could we calculate the pressure of a developing fermi gas, maybe mimicking inflation?
Fermi-Dirac statistics in the limit h->0 is still a Fermi-Dirac statistics. This limit does not turn the anti-commutator into a commutator.
 

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