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Scattering States in AdS/CFT
(CFP Room (326 DFA), from
20190322 13:30 to
20190322 14:30)

We show that suitably regulated multitrace primary states in large N CFTs behave like `in' and `out' scattering states in the flatspace limit of AdS. Their transition matrix elements approach the exact scattering amplitudes for the bulk theory, providing a natural CFT definition of the flat space SMatrix. We study corrections resulting from the AdS curvature and particle propagation far from the center of AdS, and show that AdS simply provides an IR regulator that disappears in the flat space limit.

Entanglement and formation of Black Holes
(CFP room (326), from
20190227 14:00 to
20190227 15:00)


"Holography, higher spin and gravity"
(CFP Room (326), from
20190225 13:30 to
20190225 14:30)


A tale of three models  How annealing can give rise to localization, liquids phases, and topological order.
(CFP Room (326), from
20190130 14:00 to
20190130 15:00)

Annealed, as opposed to quenched, degrees of freedom are allowed to choose their equilibrium state rather than remaining frozen in a predetermined configuration. Models of annealed classical degrees of freedom in contact with quantum mechanical variables can emerge in the presence of quasiconserved quantities or as effective descriptions of collective excitations, valid away from the zero temperature limit. In contrast to their classical counterparts, these models can be efficiently simulated by classical Monte Carlo algorithms. The FalicovKibble (FK) model is the simplest of this kind. It has been widely studied and used as testing grounds to dynamical mean field theory methods.
In this talk, I will first show that the phase diagram of the FK model still held some surprises, including an example of a disorderedfree localized phase. Second, I will show that introducing frustration, by going to the triangular lattice, an FKlike model can support rather exotic liquid phases. Thirdly, I will show how FK interactions affect the topological properties of the Haldane model.
References:
[1] Interactiontuned Anderson versus Mott localization
A. E. Antipov, Y. Javanmard, P. Ribeiro, S. Kirchner
Phys. Rev. Lett. 117, 146601 (2016)
[2] Classical and quantum liquids induced by quantum fluctuations.
M. M. Oliveira, P. Ribeiro, S. Kirchner.
arXiv:1810.10582 (2018)
[3] Temperaturedriven gapless topological insulator.
M. Gonçalves, P. Ribeiro, R. Mondaini, E. V. Castro.
arXiv:1808.00978 (2018)

Manybody localization and Thermalization in isolated quantum systems
(, from
20190114 22:32 to
20190114 22:32)

The fundamental question of how an isolated interacting quantum
system, subjected to only unitary timeevolution, loses information about
its initial preparations has been the focus of a variety of studies [1, 2]. More recently, however,
another angle of this problem has also been investigated: When they are
influenced by quenched disorder, information of the initial conditions can
be preserved for arbitrarily long times, whose potential application to
quantum memories is immediate. This phenomenon is dubbed manybody
localization and can be seen as the generalization of the fundamental
problem of the Anderson localization when its constituents are interacting.
In this talk, I will present an overall picture of this interplay of the
manybody localization [3, 4] and thermalization [5, 6], describing the
conditions they are manifest.
Importantly, it has been the focus of not only numerical studies but also of
experimental ones, via the emulation in optical lattices trapping cold atoms
[7, 8]. I will also glance on some recent generalizations investigated by
our group showing that manybody localization may also be manifest
in systems that are translationally invariant, i.e., even in the absence of
quenched disorder [9], and the possible investigation of manybody mobility edges. [10]
[1] M. Srednicki, Phys. Rev. E 50, 888 (1994)
[2] M. Rigol, V. Dunjko, and M. Olshanii, Nature 452, 854858 (2008)
[3] R. Mondaini, M. Rigol, Phys. Rev. A 92, 041601(R) (2015)
[4] C. Cheng, R Mondaini, Phys. Rev. A 94 (5), 053610 (2016)
[5] R. Mondaini, K. R. Fratus, M. Srednicki, M. Rigol, Phys. Rev. E 93 (3),
032104 (2016)
[6] R. Mondaini and M. Rigol, Phys. Rev. E 96, 012157 (2017)
[7] M. Schreiber, S. S. Hodgman, P. Bordia, H. P. Luschen, M. H. Fischer, R.
Vosk, E. Altman, U. Schneider, I. Bloch, Science 349, 842 (2015)
[8] J.Y. Choi, S. Hild, J. Zeiher, P. Schauß, A. RubioAbadal, T. Yefsah,
V.Khemani, D. A. Huse, I. Bloch, and C. Gross, Science 352, 1547 (2015)
[9] R. Mondaini and Z. Cai, Phys. Rev. B 96, 035153 (2017)
[10] Xing Bo Wei, Chen Cheng, Gao Xianlong, Rubem Mondaini, arXiv:1810.08209

On the energy transport in a nonintegrable Ising chain
(CFP Room (326), from
20181107 13:00 to
20181107 14:00)

Typicality arguments have been first proposed as a welldefined framework to study quantum thermodynamics, from a more fundamental point of view. The key idea of typicality is to describe thermal ensembles from a pure state formalism. The applicability of typicality extends beyond equilibrium quantum physics and possibly to other areas of physics. I will present a study of the energy transport in a nonintegrable spin1/2 Ising chain using typicality arguments, which amounts to characterizing the quench dynamics after a local perturbation. We obtained numerical results regarding transport coefficients both at finite and infinite temperature, which question the understanding in nonintegrable models. Second, I will introduce Matrix Product States (MPS) and explain the connection with typicality arguments. We obtained several results regarding typicality of MPS and showed their limitations to study quench dynamics.

Can Teleparallel gravity (TEGR) really be the Translations gauge theory?
(CFP Room (326), from
20181017 13:30 to
20181017 14:30)

I will report on my work reexamining the translation gauge aspect of Teleparallel Equivalent to GR. TEGR is presented as the gravity theory equivalent to GR that is also the gauge theory of translations. We addressed that claim and discovered that it is not tenable given that the principal fiber bundle of translation cannot be built in general and that the need for general frames entails the use of the Lorentz group. We found the solution in a WeitzenbockCartanPoincaré construction that is not yet clearly a gauge theory. This talk is funded by Fundação para a Ciência e a Tecnologia (FCT) through the project UID/FIS/04650/2013.

Planar fourpoint functions of protected operators in N=4 SYM
(CFP Room (326), from
20181015 13:30 to
20181015 14:30)

We study fourpoint functions of protected operators in planar N=4 SYM up to the fiveloop order. We use a lightcone OPE analysis to constrain the integrands and then fix the integrated correlators with input from integrability. The OPE data we extract allows us to determine the triple wrapping correction in the Hexagon approach to threepoint functions, which contributes earlier than expected.

Dark side of the seesaw
(Room 326 (CFP room), from
20181003 14:30 to
20181003 15:30)

I present a model where there is a connection between two apparently uncorrelated sectors, namely neutrino and dark matter. In the model, a scalar field acts as mediator between these two sectors, its vacuum expectation value generating the mass of the dark matter and also taking part in generating neutrino mass. A Z4 symmetry is used, broken by the scalar field vacuum to a remnant Z2 responsible for dark matter stability. The observed light neutrino masses and relic abundance constraint on the dark matter combined lead to predictions of the heavy seesaw scale. This framework to connect dark matter and neutrino sector introduced here is a generic one and can be applied to other possible neutrino mass generation mechanism and different dark matter candidate(s).
This talk is funded by Fundação para a Ciência e a Tecnologia (FCT) through the project UID/FIS/04650/2013.

Berry phases and topological physics in onedimensional systems
(CFP Room  326, from
20180726 14:00 to
20180726 15:00)

Topological systems are one of the most active research areas in condensed matter physics. The topological characterization of a condensed matter system relies on mathematical constructs such as the Berry phase, the winding number, or the Chern number. In the first part of the talk, I will explain how the Berry phase can be understood as the first cumulant of a series. We calculate higher order cumulants and reconstruct the underlying distribution of the polarization for the RiceMele model. Our approach allows the visualization of a topological transition, how a system goes between phases with different quantization. In the second part of the talk, I will go through constructing onedimensional analogs of the Haldane and KaneMele models. In the former, the overall winding number does not indicate topological behavior, but the model falls into two independent Creutz models with opposite windings, and the topological transition occurs within each one separately. The latter ladder model also consists of two Creutz models, one for each spinchannel and falls in the CII symmetry class. In its analysis, the thermodynamic derivation of the generalization of the StredaWidom formula to the quantum spin Hall effect turned out to be useful.