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CCCC – p. 5<br />

Hypersurface-deformation algebra<br />

Diffeomorphism constraint D[w a ] and Hamiltonian constraint H[N].<br />

Classical algebra<br />

{D[w a 1],D[w a 2]} = −D[L w2 w a 1]<br />

{H[N],D[w a ]} = −H[w a ∇ a N]<br />

{H[N 1 ],H[N 2 ]} = D[h ab (N 1 ∇ b N 2 −N 2 ∇ b N 1 )]<br />

ensures that <strong>the</strong>ory respects<br />

→ gauge transformations for coordinate changes: space-time<br />

Lie derivative {f,H[ǫ]+D[ξ a ]} = L (ǫ/N,ξa +ǫN a /N)f if<br />

constraints satisfied and time direction t a = Nn a +N a . [Dirac]<br />

→ slicing independence: algebra amounts to deformations of<br />

hypersurfaces<br />

[Kuchar, Teiltelboim]<br />

Anomaly-free quantum-corrected constraints generate modified<br />

gauge transformations. Space-time?

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