This woke me up...
Seems pretty topical, esp after listening to Susskind's lecture (I now get more where Condensed Matter Physics comes into this discussion). It just felt pretty concrete after reading in as far as I could...
I found it searching for Ryu Takayanagi... which seems like foundation of what Susskind and his student(s) are talking about, and for which there isn't much on wiki.
http://arxiv.org/abs/1203.4565
The quantum phases of matter
Authors:
Subir Sachdev
(Submitted on 20 Mar 2012 (
v1), last revised 22 May 2012 (this version, v4))
Abstract: I present a selective survey of the phases of quantum matter with varieties of many-particle quantum entanglement. I classify the phases as gapped, conformal, or compressible quantum matter. Gapped quantum matter is illustrated by a simple discussion of the Z_2 spin liquid, and connections are made to topological field theories. I discuss how conformal matter is realized at quantum critical points of realistic lattice models, and make connections to a number of experimental systems. Recent progress in our understanding of compressible quantum phases which are not Fermi liquids is summarized. Finally, I discuss how the strongly-coupled phases of quantum matter may be described by gauge-gravity duality. The structure of the large N limit of SU(N) gauge theory, coupled to adjoint fermion matter at non-zero density, suggests aspects of gravitational duals of compressible quantum matter.I'd sure love to understand better what they mean when they call the "vision" of the Z2 RVB state, "Dark Matter". I take it they are only being literal - in that it has neither charge nor spin, only energy.
And just in general what a "gapped quantum state" is. I have a cartoon that there is some sort of "entanglement" resonance that changes the Energy Level of the ground state for some quantum ensemble.
Seems relevant, but more trying to calculate causal relationships despite the weirdness (complexity) the the many body quantum lattice state space...
http://arxiv.org/abs/1305.2176
Elementary excitations in gapped quantum spin systems
Jutho Haegeman,
Spyridon Michalakis,
Bruno Nachtergaele,
Tobias J. Osborne,
Norbert Schuch,
Frank Verstraete
(Submitted on 9 May 2013 (
v1), last revised 13 Jun 2013 (this version, v2))
For quantum lattice systems with local interactions, the Lieb-Robinson bound acts as an alternative for the strict causality of relativistic systems and allows to prove many interesting results, in particular when the energy spectrum exhibits an energy gap. In this Letter, we show that for translation invariant systems, simultaneous eigenstates of energy and momentum with an eigenvalue that is separated from the rest of the spectrum in that momentum sector, can be arbitrarily well approximated by building a momentum superposition of a local operator acting on the ground state. The error decreases in the size of the support of the local operator, with a rate that is set by the gap below and above the targeted eigenvalue. We show this explicitly for the AKLT model and discuss generalizations and applications of our result.