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The Immirzi parameter in quantum general relativity

Carlo Rovelli, Thomas Thiemann

TL;DR

The paper identifies a fundamental one-parameter quantization ambiguity in loop quantum gravity, arising from Barbero's scale transformation $U(\iota)$ that is canonical but not unitarily implementable in the quantum theory. By analyzing the scaled variables $A_\iota$ and $E_\iota$ and their effect on geometric spectra (e.g., area $A(S)=\iota\,f(S,E_\iota)$), the authors show that different $\iota$ yield unitarily inequivalent quantum theories with spectra scaled by $\iota$. They debunk several incorrect interpretations and illustrate the phenomenon with toy models, including a simple system where eigenvalues scale as $\iota^{2}$. The result clarifies the status and physical significance of the Immirzi parameter, indicating it as a potentially measurable quantum gravity parameter that introduces a second fundamental length scale alongside the Planck length.

Abstract

Barbero has generalized the Ashtekar canonical transformation to a one-parameter scale transformation $U(ι)$ on the phase space of general relativity. Immirzi has noticed that in loop quantum gravity this transformation alters the spectra of geometrical quantities. We show that $U(ι)$ is a canonical transformation that cannot be implement unitarily in the quantum theory. This implies that there exists a one-parameter quantization ambiguity in quantum gravity, namely a free parameter that enters the construction of the quantum theory. The purpose of this letter is to elucidate the origin and the role of this free parameter.

The Immirzi parameter in quantum general relativity

TL;DR

The paper identifies a fundamental one-parameter quantization ambiguity in loop quantum gravity, arising from Barbero's scale transformation that is canonical but not unitarily implementable in the quantum theory. By analyzing the scaled variables and and their effect on geometric spectra (e.g., area ), the authors show that different yield unitarily inequivalent quantum theories with spectra scaled by . They debunk several incorrect interpretations and illustrate the phenomenon with toy models, including a simple system where eigenvalues scale as . The result clarifies the status and physical significance of the Immirzi parameter, indicating it as a potentially measurable quantum gravity parameter that introduces a second fundamental length scale alongside the Planck length.

Abstract

Barbero has generalized the Ashtekar canonical transformation to a one-parameter scale transformation on the phase space of general relativity. Immirzi has noticed that in loop quantum gravity this transformation alters the spectra of geometrical quantities. We show that is a canonical transformation that cannot be implement unitarily in the quantum theory. This implies that there exists a one-parameter quantization ambiguity in quantum gravity, namely a free parameter that enters the construction of the quantum theory. The purpose of this letter is to elucidate the origin and the role of this free parameter.

Paper Structure

This paper contains 12 sections, 26 equations.