Coordinators: Eduardo Hernández, Rafael Roldán

13 December 2018, 12:00 h. Sala de Seminarios, 182

Instituto de Ciencia de Materiales (ICMM, CSIC)

The dynamics of a qubit that is swept repeatedly through an avoided crossing is known as Landau-Zener-Stückelberg-Majorana (LZSM) interference. Lately it is used for demonstrating quantum coherence as well as for determining qubit parameters such as the T2 time. One method for recording these interference patterns is dispersive readout performed by measuring the transmission of a cavity coupled to the qubit. In this talk, I present a universal theory for dispersive readout of quantum systems in and out of equilibrium. It is based on the backaction of the measured system to the cavity obtained with non-equilibrium linear response theory, which provides the signal in terms of a system susceptibility [1] as well as resonance conditions that relate the cavity transmission to spectral properties and Berry phases [2]. Examples are the readout of detuned qubits and thermally excited multi-level systems. For ac-driven quantum systems, we identify the relevant Fourier component of the susceptibility and introduce a computational scheme based on Floquet theory. The theory is applied to LZSM interference in Si/SiGe double quantum dots, where the interference patterns exhibit a harp-like structure stemming from the valley degree of freedom [3]. The theoretical and experimental interference patterns show a striking agreement.

[1] S. Kohler, Phys. Rev. A 98, 023849 (2018).

[2] S. Kohler, Phys. Rev. Lett. 119, 196802 (2017).

[3] X. Mi, S. Kohler, J.R. Petta, Phys. Rev. B 98, 161404(R) (2018).

29 November 2018, 12:00 h. Sala de Seminarios, 182

Universidad Complutense de Madrid

Active matter systems are composed of constituents, each one in nonequilibrium, that consume energy in order to move [1,2]. To unravel the physics of active matter, two prototype self-propelled particles have mainly been considered: the so called Active Brownian Particles (ABP) [3] and the Vicsek particles [4]. The former are particles that move at a given speed while undergoing a rotational diffusion. Whereas the latter consists of self-propelled point particles whose orientation is dictated by the average orientation of their first neighbours.

Depending on the balance between active and equilibrium forces, self- propelled particles can assemble into living clusters [5-11] (in the presence of isotropic forces) or into functional finite size aggregates [12] (in the presence of non-adsorbing polymers).

When interacting via micro-phase separation inducing potentials, self- propelled spherical or dumbbellar particles can form functional active states such as a spinning cluster crystal or a fluid of living clusters [13]. When interacting with an amphiphilic Janus interaction potential, self- propelled spherical particles self-assemble into aggregates whose morphology depends on active forcesʼ strength and direction [14].

A characteristic feature of active matter is collective motion, that can lead to nonequilibrium phase transitions or large scale directed motion [15]. A number of recent works have featured active particles interacting with obstacles [16-18].

When n active particles encounter an asymetric obstacle ratchet effects, responsible for translating particlesʼ motion into work, appear originated by the particlesʼ persistence length [19]. Interestingly, depending on the nature of activity (whether represented as run- and-tumble or Vicsek), self-propelled particles

encountering a funnelled wall can be trapped on the narrow (the former [20,21]) or the wide (the latter [22])

opening side of the funnels.

15 November 2018, 12:00 h. Sala de Seminarios, 182

University of Göttingen

The question of how one can reconcile the second law of thermodynamics with microscopic time-reversal invariance goes back to the very beginning of statistical mechanics and the dispute between Boltzmann and Loschmidt. While the answer to this question is nowadays very well understood for classical systems, its quantum mechanical version has until recently hardly been explored. Besides its importance for the foundations of quantum statistical mechanics, the understanding of reversibility and irreversibility in quantum systems also plays an important role for example in spin echo experiments. In my talk I will give an overview of recent progress on this topic.

08 November 2018, 12:00 h. Salón de Actos

Northeastern University

In the past decade we have witnessed enormous progress in experiments that consist of placing magnetic atoms at predetermined positions on substrates and building magnetic nanostructures, one atom at a time. The interactions between magnetic moments are mediated by the conduction electrons through a mechanism understood in terms of a theory developed decades ago by Ruderman, Kittel, Kasuya, and Yosida, dubbed "RKKY theory", which applies when the spins are classical. The quantum nature of the electronic spin introduces another degree of complexity and competition with other quantum phenomena: the Kondo effect. This competition is quite subtle and non-trivial, and can only be studied by numerical means. We explore these phenomena on different lattice geometries in 1,2 and 3 dimensions by introducing an exact mapping onto an effective one-dimensional problem that we can solve with the density matrix renormalization group method (DMRG). We show a clear departure from conventional RKKY theory and important differences that can be attributed to dimensionality and geometry. In particular, for the square and cubic lattices at half filling, Kondo physics dominates even at short distances, while the ferromagnetic RKKY state is energetically unfavorable, translating into a finite range for the RKKY interaction. In the case of larger spin S=1, RKKY correlations can coexist with (partial) screening.

25 October 2018, 12:00 h. Sala de Seminarios, 182

IMDEA Nanociencia

Electrolytes consist of positively and negatively charged ions even in an equilibrium situation. Hence, plasmonic behavior can be observed in ionic systems and interaction effects between the charge carriers may play a sizable role as compared to the quantum effects observed for metal nanoparticles beyond a classical Maxwellian description. We study ionic plasmon effects, i. e. collective charge oscillations, in electrolytes in the scope of a nonlocal, two-fluid model using the hydrodynamic theory of charges. Notably, nonlocal quenching is observed for particle sizes spanning orders of magnitude, tunable via ion concentration, their mass and charge through choice of material. A plasmonic theory for ions in solution can bridge hard and soft matter theory and allow studying interaction effects from a photonic perspective in full analogy to solid metal particles. The semi-classical approach presented here can be fully integrated into standard nano-optic simulation frameworks and is considered to be of great interest for plasmonic photo-catalysis introducing nonlocal aspects into electrolyte-electrode interactions [1].

[1] C. David, Scientific Reports 8, 7544 (2018)

18 October 2018, 12:00 h. Sala de Seminarios, 182

Understanding heat exchange via thermal radiation beyond Planck´s law is key for many areas of science and engineering [1]. In this talk, I will present an overview of our efforts devoted to explore the limits of Planck’s law in two situations in which it is no longer valid. First, I will discuss the radiative heat transfer between two objects in situations in which they are separated by a distance smaller than thermal wavelength (λTh) and the thermal exchange is dominated by evanescent waves [2-4]. Then, I will discuss the radiative heat transfer between objects with some of their dimensions being smaller than λTh. In particular, I will show that in this case it is possible to overcome the blackbody limit by orders of magnitude even in the far-field regime [5], i.e., when they are separated by macroscopic distances. I will illustrate this phenomenon in the case of micron-sized dielectric devices [5,6] and 2D materials such as graphene [7].

[1] J.C. Cuevas and F.J. García-Vidal, Radiative Heat Transfer, ACS Photonics (2018).

[2] B. Song et al., Nature Nanotechnol. 10, 253 (2015).

[3] K. Kim et al., Nature 528, 387 (2015).

[4] L. Cui et al., Nature Commun. 8, 14479 (2017).

[5] V. Fernández-Hurtado et al., Phys. Rev. B 97, 045408 (2018).

[6] D. Thompson et al., Nature 561, 216 (2018).

[7] V. Fernández-Hurtado et al., ACS Photonics 5, 3082 (2018).

11 October 2018, 12:00 h. Sala de Seminarios, 182

By having access to the microscopic details of a system, a Maxwell demon is able to extract power from an equilibrium situation without doing any work or injecting energy. Analogue systems can be defined in multiterminal mesoscopic devices where electrons propagate without thermalizing. This way, a finite power can be generated in two terminals of a conductor by maintaining a non-equilibrium situation in other two, defining a thermoelectric engine which does not absorb heat. Several realizations with quantum Hall edge states or Coulomb blockade quantum dots [1] will be discussed. In the same way, photonic systems can be used to cool a black body. Needless to say that the second law of thermodynamics is safe with us!

[1] R. S. Whitney, R. Sánchez, F. Haupt, J. Splettstoesser, Physica E 75, 257 (2016)

04 October 2018, 12:00 h. Sala de Seminarios, 182

University of Konstanz

Spin qubits in dilute nuclear-spin materials such as silicon and carbon are currently among the most coherent systems for quantum information processing. Yet, while the small magnetic moment associated with electron spins provides excellent shielding of the quantum information from external noise, it also limits the controllability of spin qubits with magnetic fields. In this talk, we address the prospects for quantum control of spin qubits using electric fields from a theory point of view. We discuss various physical mechanisms that endow electron spins with an electric dipole, such as the spin-orbit coupling, magnetic field gradients, and the exclusion principle for multi-electron qubits. In this context we report on the progress in realizing electrically driven quantum gates in silicon and the achievement of the strong coupling regime between spin qubits and a superconducting microwave resonator. Electric controllability comes at the price of an increased sensitivity of the spin qubit; to counteract this, we show that theoretical analysis can provide new shielding techniques against electric noise.

27 September 2018, 12:00 h. Sala de Seminarios, 182

Instituto de la Estructura de la Materia (IEM-CSIC)

The non-equilibrium dynamics of a strongly correlated quantum system is one of the most fascinating problems in physics, with open questions regarding when and how thermalization occurs and what the equilibrium state is like. Unusual phenomena are observed when the system exhibits conserved quantities that constrain its evolution in phase space, invalidating the predictions of standard quantum thermodynamics. We have derived generalized versions of the quantum Jarzynski equality and the Tasaki-Crooks relation for these systems, and provide numerical simulations showing that these novel quantum fluctuation relations can be tested with available technology in trapped ion setups. Our results pave the way for a deeper understanding of the role of conserved quantities in non-equilibrium processes.

References:

[1] J. Mur-Petit, A. Relaño, R. A. Molina, D. Jacksch, Nature Communications 9, 2006 (2018)

20 September 2018, 12:00 h. Sala de Seminarios, 182

IFISC (CSIC-UIB)

The archetypal two-impurity Kondo problem in a serially coupled double quantum dot is investigated in the presence of a thermal bias θ. The slave-boson formulation is employed to obtain the nonlinear thermal and thermoelectrical responses. When the Kondo correlations prevail over the antiferromagnetic coupling J between dot spins, we demonstrate that the setup shows negative differential thermal conductance regions behaving as a thermal diode. In addition, we report a sign reversal of the thermoelectric current controlled by t=Γ (t and Γ denote the interdot tunnel and reservoir-dot tunnel couplings, respectively) and θ. All these features are attributed to the fact that at large θ both the heat current and the thermoelectric current are suppressed regardless of the value of t=Γ because the double dot decouples at high thermal biases. Finally, for a finite J, we investigate how the Kondo-to-antiferromagnetic crossover is altered by θ.

05 July 2018, 12:00 h. Sala de Seminarios, 182

Universidad de Budapest

Weyl semimetals, three dimensional materials with gapless excitations characterized by an effective Weyl Hamiltonian, are the tree dimensional generalizations of graphene. In connection with the recent rush to find condensed matter realizations of this new phase of matter another equally intriguing novel topological phase has been discovered: nodal line semimetals. In these systems the conduction and valence band touch each other along a line. This line can take a form of a loop or extend trough the whole Brillouin zone. Systems with many lines entangled with each other were also predicted to exist.

In this talk we shall first review how this novel phase was discovered in the turbulent rush towards finding novel topological phases. We conclude by examining experimental signatures characteristic to this exotic state of matter mainly focusing on magnetic oscillation spectra.

28 June 2018, 12:00 h. Sala de Seminarios, 182

ICMM

The study of open quantum systems has a long story, however most of the advances are related with oscillator bath models (typically describe phonons, photons, magnons, electron-hole pairs, etc). Another universality class corresponds to spin bath models, where the bath is described by a discrete set of localised n-level systems. Importantly, in certain regimes, the behaviour of the spin bath can be radically different from the oscillator bath models (some examples of bath spins are lattice defects, dislocation modes, spin impurities, dangling bonds nuclear spins and localised phonons/vibrons).

In this talk I will motivate the importance of these models in present experiments, discuss some well known results and some of the important questions not yet fully addressed. I will also discuss some of the different approaches that one can use to study these models and their limitations.

07 June 2018, 12:00 h. Sala de Seminarios, 182

Instituto de Ciencia de Materiales de Madrid ICMM-CSIC

The recently observed insulating and superconducting states upon doping a graphene bilayer with a small twist angle have created a lot of excitement in the scientific community[1,2]. The stacking misorientation creates a moiré pattern with a superlattice modulation corresponding to thousands of atoms per unit cell. The insulating states, arise when the charge per moiré cell is ± 2. Superconductivity emerges from one of these insulating states.

Understanding the nature of the insulating states is key to uncover the origin of the superconductivity. The filling at which the insulating character appears is consistent with the ones of a Mott insulator and suggests a posible relation with the physics of cuprate high-Tc superconductors.

In the seminar I will review some aspects of the experimental results and introduce the physics and properties of Mott insulators. Common wisdom about Mott insulators is generally built upon techniques which only take into account local correlations. We will see that the expectations including only local correlations are not compatible with the experimentally observed behaviour of the insulating states with temperature and magnetic field [3]. I will then argue that including non-local correlations can reverse these predictions and discuss other possible consequences of non-local correlations.

[1] Cao et al, Nature 556, p. 80-84 (2018)

[2] Cao et al, Nature 556, p. 43-50 (2018)

[3] J.M. Pizarro, M.J. Calderón, E. Bascones, arXiv:1805.07303

31 May 2018, 12:00 h. Sala de Seminarios, 182

Instituto de Ciencia de Materiales de Madrid ICMM-CSIC

Iron superconductors were discovered 10 years ago giving rise to the second family of high temperature superconductors with unknown superconducting mechanism. Most undoped pnictides present columnar magnetism and a puzzling electronic nematic phase that upon doping or pressure become superconducting. Over these years the spin scenario has shown to be a strong candidate to explain the mechanism of antiferromagnetism, nematicity and superconductivity. Notably exception is FeSe lacking the magnetic phase and presenting a peculiar orbital ordering. This situation has motivated the orbital ordering scenario for FeSe. In our work, we have taken a different route: we have derived a low energy effective model– the orbital selective spin fluctuations (OSSF)- model that allows to address spin-orbital interplay. [1,2]

So far, with this model we have been able to give a mechanism to understand (i) the difference between magnetism and nematicity in pnictides and FeSe, [1] (ii) the odd orbital ordering observed in ARPES in FeSe [3] (iv) The enigmatic anisotropy of the superconducting gaps in FeSe revealed by STM and ARPES experiments [4](vi) the renormalization of the velocity and the scattering rate due to self-energy effects reflected in the resistivity anisotropy. [5]

[1] L. Fanfarillo, A. Cortijo, and B. Valenzuela, Phys. Rev. B 91, 214515 (2015)

[2] L. Fanfarillo, L. Benfatto, and B. Valenzuela, Phys. Rev. B 97, 121109(R) (2018).

[3] L. Fanfarillo, et al., Phys. Rev. B 94, 155138 (2016).

[4] L. Fanfarillo, B. Valenzuela, L. Benfatto, arXiv:1804.05800.

[5] R. Fernández, L. Fanfarillo, L. Benfatto, B. Valenzuela, arXiv:1804.07293.

17 May 2018, 12:00 h. Sala de Seminarios, 182

IFIMAC

The excited state properties of nanoscale semiconductors are dominated by the dynamics of quantum confined electron-hole pairs known as excitons. Thanks to recent advances in the size and shape control of semiconductor nanomaterials, this confinement can now be tuned with high precision which has resulted in a rapidly expanding family of high-quality excitonic building blocks. However, while extensive research has been done to understand and control the excitonic properties of the isolated building blocks, comparatively little is known about exciton dynamics in nanoscale assemblies.

In the first part of the talk, I will present some of our efforts in trying to understand and control the exciton dynamics in nanomaterial assemblies. Specifically, I will discuss transient microscopy techniques which allow us to spatially resolve exciton diffusion in colloidal quantum-dot films. In addition, I will present our findings of anomalous excitonic energy-transfer dynamics between zero-dimensional colloidal quantum-dots and two-dimensional MoS2 monolayers.

In the second part of the talk, I will present new strategies for the assembly of excitonic building blocks into high quality wavelength-scale patterns using template stripping of colloidal quantum-dot films. I will show that this technique can produce high-quality photonic structures composed solely out of colloidal quantum dots.

Finally, I will briefly highlight some recent work on the use of plasmonic antennas to structure the fluorescence of colloidal quantum-dot emitters, specifically by mapping spectral information to the polarization state of light. Based on this concept, we propose polarization-resolved spectroscopy scheme that may benefit high-speed readout of fluorescent signatures.

10 May 2018, 12:00 h. Sala de Seminarios, 182

University of Lancaster

Topological photonics aims to replicate fermionic symmetries as feats of precision engineering. Here I show how to enhance these systems via effects such as gain, loss and nonlinearities that do not have a direct electronic counterpart. This leads to a topological mechanism of mode selection [1,2,3], formation of compactons in flat band condensates [4], and topological excitations in lasers when linearized around their working point [5]. The resulting effects show a remarkable practical robustness against disorder, which arises from the increased spectral isolation of the manipulated states.

[1] Topologically protected midgap states in complex photonic lattices, H. Schomerus, Opt. Lett. 38, 1912 (2013).

[2] Selective enhancement of topologically induced interface states in a dielectric resonator chain, C. Poli, M. Bellec, U.Kuhl, F. Mortessagne, H. Schomerus, Nat. Commun. 6, 6710 (2015).

[3] Topological Hybrid Silicon Microlasers, H. Zhao et al., Nat. Commun. 9, 981 (2018)

[4] Exciton-polaritons in a two-dimensional Lieb lattice with spin-orbit coupling, C. E. Whittaker et al., Phys. Rev. Lett. 120, 097401 (2018)

[5] Topological phases in nonlinear complex-wave equations with a time-preserving symmetry, S. Malzard, E. Cancellieri, and H. Schomerus, arXiv:1705.06895

07 May 2018, 12:00 h. Sala de Seminarios, 182

Princeton University

One hallmark of topological phases with broken time reversal symmetry is the appearance of quantized non-dissipative transport coefficients, the archetypical example being the quantized Hall conductivity in quantum Hall states. Here I will talk about a new non-dissipative transport coefficients that appear in such systems - the Hall viscosity. In the first part of the talk, I will start by reviewing previous results concerning the Hall viscosity, including its relation to a topological invariant known as the shift when rotational symmetry is preserved. Next, I will show how the Hall viscosity can be computed from a Kubo formula. For Galilean invariant systems, the Kubo formula implies a relationship between the viscosity and conductivity tensors which may have relevance for experiment. In the second part of the talk, I will examine the fate of the Hall viscosity when rotational symmetry is broken. Through a combination of field theory and numerical techniques, I will show that rotational symmetry breaking allows for the introduction of a new topological quantum number characterizing quantum Hall states.

26 April 2018, 12:00 h. Sala de Seminarios, 182

Instituto de Ciencia de Materiales de Madrid ICMM-CSIC

Following recent reports of superconductivity and Mott transitions in twisted graphene bilayers, the field of moiré patterns in stacked 2D crystals has seen a surge of interest. I will review the rich phenomenology associated to moiré patterns in various heterostructures of 2D crystals, both from an electronic and from an elastic point of view. I will focus on the case of twisted graphene bilayer and graphene on hexagonal boron nitride. The elastic aspect of the problem, which has received comparatively little attention, will be analysed within a simple continuum description. This model is sufficient to capture the formation and properties of stacking solitons, which dramatically affect the electronic properties in some systems. It will also be employed to explain and the characteristic the spontaneous rippling of some van der Waals materials, such as Franckeite and Cylindrite, whose large scale structure is thus shown to be a consequence of interlayer moiré patterns.

19 April 2018, 12:00 h. Salón de Actos

Instituto de Ciencia de Materiales de Madrid ICMM-CSIC

In 2008, Hosono’s group discovered superconductivity in the iron-based superconductors. In this family, a quasi-2D layer is formed by arranging the iron atoms in a square pattern, with pnictogen or chalcogen atoms tetrahedrally coordinating these iron positions. The superconducting phase appears when a antiferromagnetic phase is supressed by doping or by applying pressure. Superconductivity is unconventional but its origin is not well established. The phase diagram of this family is similar to the one of cuprate superconductors. However, a striking difference is that the parent compound of iron superconductors is a metal in which the Hund’s coupling seems to play an important role, while for the cuprates it is a Mott insulator. The metallic nature of the iron superconductors has led to a never ending debate about the role of local correlations on superconductivity.

In 2015 a new kind of iron superconductor with a quasi-one dimensional two leg ladder structure was discovered. BaFe2S3 becomes superconductor with T_c^max≈24K when pressure is applied ≈10GPa and an antiferromagnetic phase is supressed. In 2017, another related compound, BaFe2Se3, was also reported to be a superconductor with T_c^max≈11Kat ≈12.7GPa. Interestingly, at zero pressure these systems are insulators, and what has led some authors to propose that they are Mott insulators.

In this talk I will briefly review some of the phenomenology of iron superconductors, as well as the Hund metal paradigm. In the main part, I will present the calculations that we have performed to clarify the role of electronic interactions in the superconductor BaFe2S3.

05 April 2018, 12:00 h. Salón de Actos

Universidad del País Vasco

The inversion symmetry breaking at the interface between different materials generates strong spin-orbit coupling (SOC). We will study through theoretical models various transport phenomena in metal-metal and metal-oxide and ferromagnet-oxide junctions induced by this interaction. This type of interaction is responsible of the greatest spin-to-charge conversion. We will show that apart from this spin-to-charge conversion this SOC is also responsible of spin swapping, (spin-to-spin conversion) and anomalous Hall effects in the presence of ferromagnetic materials.

22 March 2018, 12:00 h. Sala de Seminarios, 182

Departamento de Física Teórica de la Materia Condensada (UAM) and IFIMAC

There is an increasing interest on the interface between Plasmonics and electron transport phenomena, mainly motivated by the ability of localized surface plasmons to concentrate light in sub-nanometric ìhot spotsî in a controllable manner. This offers unique opportunities in the design of novel molecular-scale optoelectronic devices exhibiting highly tuneable operativeness. Systems comprising plasmonic nanostructures bridged by tunnel junctions constitute a natural route towards the realization of such devices. Among those, simple vacuum sub-nanometric gaps in metallic nanoparticle dimers have been addressed experimentally and analysed theoretically using classical-optics prescriptions. However, only recently fully ab-initio simulations of the optical response have been carried out for such archetypical systems. In this case, the detailed atomic structure in the junction has to be necessarily considered since, for instance, small distortions of the around-gap geometry not only affect to the intensity of the photoinduced current, but also lead to qualitative changes in the optical absorption spectrum.

More interesting is the case of hybrid systems, where metallic nanostructures are bridged by atomic or molecular junctions. In this talk, we shall discuss the effects of different single-atom junctions on the optical properties of bridged nanoparticle dimers, as well as the corresponding plasmon-induced electric currents through the junctions. We show that, besides the appearance of well-defined signatures in the infrared absorption spectrum associated to a photoinduced quantized electric current, the plasmonic response is affected by such a current. A deeper understanding of the physical process is given via a simple model system.

02 March 2018, 10:30 h. Sala de Seminarios, 182

University of Twente. The Netherlands.

Ge/Si core/shell nanowires are proposed candidates for observing Majorana fermions where a hard superconducting gap is essential for topological protection at zero energy. In double quantum dots, we observe shell filling of new orbitals and corresponding Pauli spin blockade. In nanowires with superconducting Al leads we create a Josephson junction via proximity-induced superconductivity. A gate-tuneable supercurrent is observed with a maximum of ~60 nA. We identify two different regimes: Cooper pair tunnelling via multiple subbands in the open regime and, while near depletion a supercurrent is carried by single-particle levels of a quantum dot operating in the few-hole regime.

Secondly, we create ambipolar quantum dots in silicon nanoMOSFETs. After passivation of charge defects we can electrostatically define hole quantum dots up to 180 nm in length. In recent devices, we have characterized the conformity of aluminium, titanium and palladium nanoscale gates by means of transmission electron microscopy (TEM). Subsequently, we have defined low-disorder quantum dots with Pd gates. Finally, we have made depletion-mode hole quantum dots in intrinsic silicon. We use fixed charge in a SiO2/Al2O3 dielectric stack to induce a 2DHG at the Si/SiO2 interface. This depletion-mode design avoids complex multilayer architectures requiring precision alignment and allows directly adopting best practices already developed for depletion dots in other material systems.

01 March 2018, 12:00 h. Sala de Seminarios, 182

Laboratoire de Physique des Solides. Université Paris Saclay.

Motivated by experimental findings [1], we study theoretically smooth topological interfaces, i.e. interfaces between a topological and a normal insulator. In addition to the usual topologically protected chiral surface states, which do not depend on the specific form of the interface, several massive states appear if the interface width is larger than a particular intrinsic length (given by the bulk gap and the Fermi velocity). These states, first described by Volkov and Pankratov in the 1990ies [2], are intrinsically relativistic and can be related to Landau bands of relativistic fermions. We show that the gap variation can be interpreted precisely as a vector potential that is affected by an additional electric field in a relativistic manner [3]. The electric field can thus be used not only to dope electronically these massive surface states, but they become even more accessible due to the reduction of the Landau gap in the presence of an electric field. The effect is at the origin of an oscillating resistance measured as a function of the electric field in high-frequency experiments [1]. We finish with a short discussion of how this "Landau-level approach" can also be used in the framework of Weyl semimetals and the description of Fermi arcs that play the role of chiral Landau bands here [4]

[1] A.Inhofer et al. PRB 96, 195104 (2017)

[2] V.Volkov and O. Pankratov, JETP Lett 42, 178 (1985)

[3] S.Tchoumakov et al. PRB 96, 201302 (2017)

[4] S.Tchoumakov et al. PRB 95, 125306 (2017)

22 February 2018, 12:00 h. Sala de Seminarios, 182

Universidad Carlos III

Recent scanning tunneling microscope (STM) experiments have shown that a soft rippled flat state coexists with a hard buckled state in suspended graphene sheets. For small values of the STM current, the transition between these states is reversible, whereas it becomes irreversible when the STM current surpasses a certain threshold. We present phenomenological models of graphene as a membrane coupled to pseudo-spins that undergo Glauber dynamics. These models allow us to understand the STM induced transitions between rippled flat and buckled states as driving the spin-membrane system through a first order phase transition.

15 February 2018, 12:00 h. Sala de Seminarios, 182

Instituto de Ciencia de Materiales de Madrid ICMM-CSIC

This talk will be structured in two parts.

In the first part, we investigate the electromagnetic response of staggered two-dimensional materials of the graphene family, including graphene, silicene, germanene, and stanene, as they are driven through various topological phase transitions using external fields [1] [2]. Utilizing Kubo formalism, we compute their optical conductivity tensor taking into account the frequency and wave vector of the electromagnetic excitations, and study its behavior over the full electronic phase diagram of the materials. We compute the Plasmon dispersion relation for different phases.

In the second part of the talk, we revisit the atom-plate quantum friction and Casimir force with a full-relativistic formalism for atoms modelled as Unruh-deWitt detectors in exited, relaxed and coherent superposition close to a plate [3]. We show that, for relative velocities close to c, the quantum friction diverges while the Casimir force is almost independent of the velocity. We are able to include the effect of the finite size of the detector, then we also obtain quantum friction when the detector is isolated but follows a non-inertial trajectory and we obtain a more realistic result for short distance interactions.

Those studies open the venue to understand the role of non-local response in quantum friction.

[1] P. Rodriguez-Lopez, et al., Nature Communications 8, 14699 (2017)

[2] P. Rodriguez-Lopez, et al., Phys. Rev. Materials 2, 014003 (2018)

[3] P. Rodriguez-Lopez and E. Martin-Martinez. Casimir Forces and Quantum friction of finite-size atoms in relativistic trajectories. Submitted

08 February 2018, 12:00 h. Sala de Seminarios, 182

G. Millán Institute, Universidad Carlos III Madrid

Let us consider two identical beakers of water, initially at two different temperatures, put in contact with a thermal reservoir at subzero (on the Celsius scale) temperature. While one may intuitively expect that the initially cooler sample would freeze first, it has been observed that this is not always the case. This paradoxical behavior named the Mpemba effect (ME) [1] has been known since antiquity and discussed by philosophers like Aristotle, Roger Bacon, Francis Bacon, and Descartes [2].

There is no consensus on the underlying physical mechanisms that bring about the ME. Specifically, water evaporation, differences in the gas composition of water, natural convection, or the influence of supercooling, either alone or combined with other causes, have been claimed to have an impact on the ME. Conversely, the own existence of the ME in water has been recently put in question [3]. Notwithstanding, Mpemba-like effects have also been observed in different physical systems, such as carbon nanotube resonators or clathrate hydrates.

In this seminar, we show that the Mpemba effect and its inverse are present in granular fluids [4], both in uniformly heated and in freely cooling systems. In both cases, the system remains homogeneous, and no phase transition is present. Analytical quantitative predictions are given for how differently the system must be initially prepared to observe the Mpemba effect, the theoretical predictions being confirmed by both molecular dynamics and Monte Carlo simulations. Possible implications of our analysis for other systems are also discussed.

01 February 2018, 12:00 h. Sala de Seminarios, 182

Universidad Autónoma de Madrid

Hybrid devices that couple superconductors and semiconductor nanowires have attracted considerable attention in recent years owing to their potential to realize topological superconductivity and Majorana zero modes. The topological phase is predicted to result from a combination of induced superconductivity, spin-orbit coupling and spin polarization in the semiconductor nanowire. Crucially, the one-dimensional character of such a system must be preserved over micron-length scales for the topological phase to the established - a requirement that is not so straightforward to meet in realistic materials. In this talk, I will address experiments performed in InAs-based hybrid superconductor-semiconductor nanowire devices, in which clear signatures of charge localization are detected. I will discuss different effects associated with the resulting superconductor-quantum dot system whose signatures could be mistakenly interpreted in favor of Majorana zero modes. In particular, I will address zero-bias peaks related to the Kondo effect and the Zeeman splitting of Andreev levels. Finally, I will discuss how, even when seemingly absent, charge localization plays a crucial role in the transport properties of quasi-ballistic nanowire quantum point contacts.

25 January 2018, 12:00 h. Sala de Seminarios, 182

IFIMAC & Departamento de Física Teórica de la Materia Condensada, UAM

Strong coupling is achieved when the coherent energy exchange between a confined electromagnetic field mode and material excitations becomes faster than the decay and decoherence of either constituent. This creates a paradigmatic hybrid quantum system with eigenstates that have mixed light-matter character (polaritons). It has recently been realized that polariton formation in organic molecules also affects their internal nuclear degrees of freedom, opening the possibility to manipulate and control reactions through polaritonic chemistry. I will first discuss our theoretical approach towards modeling such systems, based on extending the well-known Born-Oppenheimer approximation to describe polaritonic potential energy surfaces. I will then show various applications, including the possibility to completely suppress reactions such as photoisomerization, which surprisingly works more efficiently when many molecules are coupled to a single light mode due to a “collective protection” effect. Finally, I will show how polaritonic chemistry can be exploited to allow many-molecule reactions triggered by a single photon. Here, the collective nature of polaritons and the resulting formation of a "supermolecule", in which a single excitation is distributed over many molecules, can enable a reaction involving the nuclear degrees of freedom of most or even all coupled molecules. This process can overcome the Stark-Einstein law that applies for most common photochemical reactions, which states that a single photon will only induce a reaction in a single molecule.

Finally, I will discuss future perspectives, open questions, and remaining challenges to fully exploit the potential of polaritonic chemistry.

18 January 2018, 12:00 h. Sala de Seminarios, 182

Instituto de Ciencia de Materiales de Madrid ICMM-CSIC and IMDEA Nanociencia

In this talk I will review some of the current achievements in the pursuit of Majorana fermions, along with the major drawbacks that stand in the way of exploiting them as fundamental qubits in the field of topological quantum computation. I will introduce a novel setting for creating Majorana bound states and performing protected non-Abelian single-qubit operations without real space braiding of Majoranas and with no fine-tuning of the control parameters. The proposed platform is a two-dimensional electron gas in the Quantum Hall regime in the presence of a Zeeman field, with the Fermi level tuned to filling factor 1. I will show that, in the presence of spin-orbit coupling, contacting the 2DEG to a narrow strip of an s-wave superconductor produces a topological superconducting gap along the contact as a result of crossed Andreev reflection processes across the strip. The sign of the topological gap depends periodically on the Fermi wavelength and strip width and can be externally tuned. An interface between two halves of a long strip with topological gaps of opposite sign implements a robust π-junction that hosts a pair of protected Majorana zero modes. Such a configuration can be exploited to perform non-Abelian tunnel-braid operations that are much simpler to execute than Majorana braidings in real space, and are nevertheless topologically protected.

11 January 2018, 12:00 h. Sala de Seminarios, 182

Universidad Autónoma de Madrid

We demonstrate the possibility of modeling recent experiments in complex graphene-metal (G-M) systems by means of Density Functional Theory (DFT) calculations. Since different modification techniques are currently applied on G -and related materials- to get new functionalities, our work does not restrict to the mere description of the G-M interface but we have to reproduce all these surface modifications. More precisely, we reveal the multi-domain structure of G grown on Rh(111), an archetypical strongly interacting substrate, in which G adopts a rippled structure with corrugations larger than 1 Å [1]. Additionally, we will present different examples of surface modification; like the evolution of G properties as a function of the oxygen coverage in the interface [2]; the atomistic mechanisms involved in this intercalation process [3]; and the tailoring of the electronic properties by means of ion implantation nitrogen doping [4,5]. Finally, we will briefly discuss about some methodological aspects of DFT calculations in this kind of G-M systems and their current limitations when dealing with very large systems (like grain boundaries, G-covered metallic steps or under-cover chemical reactions).To overcome this issue, we present preliminary results of a new approach based on highly optimized localized orbital basis set to reach high-accuracy descriptions at quantum level of systems with thousands of atoms.

[1] A. Martín-Recio et al. Nanoscale 7 (2015) 11300

[2] C. Romero-Muñiz et al. Carbon 101 (2016) 129

[3] C. Romero-Muñiz et al. (submitted)

[4] A. Martín-Recio et al. Nanoscale 8 (2016) 17686

[5] A. Martín-Recio et al. (submitted)