An analytic static monopole solution is found in global AdS(4), in the limit of small backreaction. This solution is mapped in Poincare patch to a falling monopole configuration, which is dual to a local quench triggered by the injection of a condensate. Choosing boundary conditions which are dual to a time-independent Hamiltonian, we find the same functional form of the energy-momentum tensor as the one of a quench dual to a falling black hole. On the contrary, the details of the spread of entanglement entropy are very different from the falling black hole case, where the quench induces always a higher entropy compared to the vacuum, i.e. increment Delta S > 0. In the propagation of entanglement entropy for the monopole quench, there is instead a competition between a negative contribution to increment Delta S due to the scalar condensate and a positive one carried by the freely propagating quasiparticles generated by the energy injection.
Zenoni, N., Auzzi, R., Caggioli, S., Martinelli, M., Nardelli, G., A falling magnetic monopole as a holographic local quench, <<JOURNAL OF HIGH ENERGY PHYSICS>>, 2021; (11): 0-34. [doi:10.1007/JHEP11(2021)048] [https://hdl.handle.net/10807/201516]
A falling magnetic monopole as a holographic local quench
Zenoni, Nicolo';Auzzi, Roberto;Nardelli, Giuseppe
2021
Abstract
An analytic static monopole solution is found in global AdS(4), in the limit of small backreaction. This solution is mapped in Poincare patch to a falling monopole configuration, which is dual to a local quench triggered by the injection of a condensate. Choosing boundary conditions which are dual to a time-independent Hamiltonian, we find the same functional form of the energy-momentum tensor as the one of a quench dual to a falling black hole. On the contrary, the details of the spread of entanglement entropy are very different from the falling black hole case, where the quench induces always a higher entropy compared to the vacuum, i.e. increment Delta S > 0. In the propagation of entanglement entropy for the monopole quench, there is instead a competition between a negative contribution to increment Delta S due to the scalar condensate and a positive one carried by the freely propagating quasiparticles generated by the energy injection.File | Dimensione | Formato | |
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