Quantized Brans Dicke Theory: Phase Transition and Strong Coupling (Large $\omega$) Limit & General Relativity
Sridip Pal

TL;DR
This paper explores the phase structure of quantized Brans-Dicke theory, revealing how quantum effects lead to symmetry breaking and a transition to General Relativity in the strong coupling limit, contrasting classical predictions.
Contribution
It demonstrates that quantized Brans-Dicke theory exhibits anomalous symmetry breaking and a phase transition, with the theory reducing to General Relativity at strong coupling, unlike classical expectations.
Findings
Quantum Brans-Dicke theory shows symmetry breaking due to anomalies.
In the strong coupling limit, BD theory reduces to GR.
Quantum effects induce a phase transition absent classically.
Abstract
We show that Friedmann-Robertson-Walker (FRW) geometry with flat spatial section in quantized (Wheeler deWitt quantization) Brans Dicke (BD) theory reveals a rich phase structure owing to anomalous breaking of a classical symmetry, which maps the scale factor for some constant . In the weak coupling () limit, the theory goes from a symmetry preserving phase to a broken phase. The existence of phase boundary is an obstruction to another classical symmetry [arXiv:gr-qc/9902083] (which relates two BD theory with different coupling) admitted by BD theory with scale invariant matter content i.e . Classically, this prohibits the BD theory to reduce to General Relativity (GR) for scale invariant matter content. We show that strong coupling limit of BD and GR both preserves the symmetry involving scale factor. We also show that with a…
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