In the AdS/CFT correspondence, states obtained by Hamiltonian evolution of the thermofield doubled state are also dual to an eternal black-hole geometry, which is glued to the boundary with a time shift generated by a large diffeomorphism. We describe gauge-invariant relational observables that probe the black hole interior in these states and constrain their properties using effective field theory. By adapting recent versions of the information paradox we show that these observables are necessarily described by state-dependent bulk-boundary maps, which we construct explicitly.</p
We provide a simple and explicit construction of local bulk operators that describe the interior of ...
We provide a simple and explicit construction of local bulk operators that describe the interior of ...
We provide a simple and explicit construction of local bulk operators that describe the interior of ...
In the AdS/CFT correspondence, states obtained by Hamiltonian evolution of the thermofield doubled s...
In the AdS/CFT correspondence, states obtained by Hamiltonian evolution of the thermofield doubled s...
In the AdS/CFT correspondence, states obtained by Hamiltonian evolution of the thermofield doubled s...
We show that, in the AdS/CFT correspondence, states obtained by Hamiltonian evolution of the thermof...
In the AdS/CFT correspondence, states obtained by Hamiltonian evolution of the thermofield doubled s...
We revisit the "state-dependence" of the map that we proposed recently between bulk operators in the...
We revisit the "state-dependence" of the map that we proposed recently between bulk operators in the...
We revisit the "state-dependence" of the map that we proposed recently between bulk operators in the...
We revisit the "state-dependence" of the map that we proposed recently between bulk operators in the...
We revisit the "state-dependence" of the map that we proposed recently between bulk operators in the...
We provide a simple and explicit construction of local bulk operators that describe the interior of ...
We provide a simple and explicit construction of local bulk operators that describe the interior of ...
We provide a simple and explicit construction of local bulk operators that describe the interior of ...
We provide a simple and explicit construction of local bulk operators that describe the interior of ...
We provide a simple and explicit construction of local bulk operators that describe the interior of ...
In the AdS/CFT correspondence, states obtained by Hamiltonian evolution of the thermofield doubled s...
In the AdS/CFT correspondence, states obtained by Hamiltonian evolution of the thermofield doubled s...
In the AdS/CFT correspondence, states obtained by Hamiltonian evolution of the thermofield doubled s...
We show that, in the AdS/CFT correspondence, states obtained by Hamiltonian evolution of the thermof...
In the AdS/CFT correspondence, states obtained by Hamiltonian evolution of the thermofield doubled s...
We revisit the "state-dependence" of the map that we proposed recently between bulk operators in the...
We revisit the "state-dependence" of the map that we proposed recently between bulk operators in the...
We revisit the "state-dependence" of the map that we proposed recently between bulk operators in the...
We revisit the "state-dependence" of the map that we proposed recently between bulk operators in the...
We revisit the "state-dependence" of the map that we proposed recently between bulk operators in the...
We provide a simple and explicit construction of local bulk operators that describe the interior of ...
We provide a simple and explicit construction of local bulk operators that describe the interior of ...
We provide a simple and explicit construction of local bulk operators that describe the interior of ...
We provide a simple and explicit construction of local bulk operators that describe the interior of ...
We provide a simple and explicit construction of local bulk operators that describe the interior of ...