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Approaches to Quantum Gravity

Approaches to Quantum Gravity

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2The fundamental nature of space and timeG. ’T HOOFT2.1 <strong>Quantum</strong> <strong>Gravity</strong> as a non-renormalizable gauge theory<strong>Quantum</strong> <strong>Gravity</strong> is usually thought of as a theory, under construction, where thepostulates of quantum mechanics are <strong>to</strong> be reconciled with those of general relativity,without allowing for any compromise in either of the two. As will be arguedin this contribution, this ‘conservative’ approach may lead <strong>to</strong> unwelcome compromisesconcerning locality and even causality, while more delicate and logicallymore appealing schemes can be imagined.The conservative procedure, however, must first be examined closely. The firstattempt (both his<strong>to</strong>rically and logically the first one) is <strong>to</strong> formulate the theory of‘<strong>Quantum</strong> <strong>Gravity</strong>’ perturbatively [1; 2; 3; 4; 5], as has been familiar practice in thequantum field theories for the fundamental particles, namely the Standard Model.In perturbative <strong>Quantum</strong> <strong>Gravity</strong>, one takes the Einstein–Hilbert action,∫S = ∂ 4 x √ ( R(x))−g + L matter (x) ɛ = 16πG (2.1)ɛconsiders the metric <strong>to</strong> be close <strong>to</strong> some background value: g μν = gμν Bg + √ ɛ h μν ,and expands everything in powers of ɛ, or equivalently, New<strong>to</strong>n’s constant G.Invariance under local coordinate transformations then manifests itself as a localgauge symmetry: h μν 〉h μν + D μ u ν + D ν u μ , where D μ is the usual covariant derivative,and u μ (x) generates an infinitesimal coordinate transformation. Here one canuse the elaborate machinery that has been developed for the Yang–Mills theories ofthe fundamental particles. After imposing an appropriate gauge choice, all desiredamplitudes can be characterized in terms of Feynman diagrams. Usually, these containcontributions of ‘ghosts’, which are gauge dependent degrees of freedom thatpropagate according <strong>to</strong> well-established rules. At first sight, therefore, <strong>Quantum</strong><strong>Gravity</strong> does not look al<strong>to</strong>gether different from a Yang–Mills theory. It appearsthat at least the difficulties of reconciling quantum mechanics with general coordinateinvariance have been dealt with. We understand exactly how the problem<strong>Approaches</strong> <strong>to</strong> <strong>Quantum</strong> <strong>Gravity</strong>: Toward a New Understanding of Space, Time and Matter, ed. Daniele Oriti.Published by Cambridge University Press. c○ Cambridge University Press 2009.

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