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Feynman Path Integral Formulation

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Chapter 7<br />

Analytical Lattice Expansion Methods<br />

7.1 Motivation<br />

The following sections will discuss a number of instances where the lattice theory<br />

of quantum gravity can be investigated analytically, subject to some necessary simplifying<br />

assumptions.<br />

The first problem deals with the lattice weak field expansion about a flat background.<br />

It will be shown that in this case the relevant modes are the lattice analogs<br />

of transverse-traceless deformations.<br />

The second problem involves the strong coupling (large G) expansion, where the<br />

weight factor in the path integral is expanded in powers of 1/G. The domain of<br />

validity of this expansion can be regarded as somewhat complementary to the weak<br />

field limit.<br />

The third case to be discussed is what happens in lattice gravity in the limit of<br />

large dimensions d, which formally is similar in some ways to the large-N expansion<br />

discussed previously in this review. In this limit one can derive exact estimates for<br />

the phase transition point and for the scaling dimensions.<br />

7.2 Lattice Weak Field Expansion and Transverse-Traceless<br />

Modes<br />

One of the simplest possible problems that can be treated in quantum Regge calculus<br />

is the analysis of small fluctuations about a fixed flat Euclidean simplicial<br />

background (Roček and Williams, 1981; 1984). In this case one finds that the lattice<br />

graviton propagator in a De Donder-like gauge is precisely analogous to the<br />

continuum expression.<br />

To compute an expansion of the lattice Regge action<br />

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