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Wydział Fizyki UW > Badania > Seminaria i konwersatoria > Seminarium Fizyki Materii Skondensowanej
2019-01-11 (Piątek)
Zapraszamy do sali 1.02, ul. Pasteura 5 o godzinie 12:15  Calendar icon
Felix Tennie (University of Oxford)

Hardcore boson N-representability

In systems of indistinguishable particles, the 1- and 2-body N-representability problems are of tantamount importance since their solution potentially offers an exponential computational advantage in determining the ground state (energy) over solving the N-particle Schroedinger equation. For fermions, this has already been thoroughly investigated and is know as Coulson's Challenge in Quantum Chemistry. The talk addresses the question of N-representability for systems of lattice hardcore bosons. A result on the maximal possible occupation number will be given which resembles a new 'Pauli principle' for hardcore bosons. In addition, the possibility of (fractional) Bose-Einstein condensation in a one-dimensional model system will be discussed.
2018-12-14 (Piątek)
Zapraszamy do sali 1.02, ul. Pasteura 5 o godzinie 12:15  Calendar icon
Krzysztof Wohlfeld (IFT UW)

Using the magnon language to describe a 1D spin problem

Quite often a 2D spin problem can be well-described in terms ofnoninteracting magnons. On the other hand, a 1D spin model is usuallysolved using the so-called spinon (magnetic domain wall) language.Here we concentrate on a specific 1D magnetic problem, described bythe Ising Hamiltonian and an electronic hopping term (the so-calledt-Jz model), and show how to solve it in the magnon language[arXiv:1809.07120]. Interestingly, the “spinon result” can bereproduced exactly only when the magnon-magnon interactions areproperly included and once an infinite number of magnons is kept inthe calculations. This result demonstrates how a single spinoncorresponds to an infinite number of magnons.
2018-12-07 (Piątek)
Zapraszamy do sali 1.02, ul. Pasteura 5 o godzinie 12:15  Calendar icon
Jacek Wojtkiewicz (KMMF UW)

On the non-existence of Bose-Einstein condensation in d=1 and 2 Bose-Hubbard model

It is argued that there is no Bose-Einstein condensation in d=1 and 2 Bose-Hubbard model. The argument is based on Bogolyubov-type inequality. The situation is more involved than in the fermionic case, as unbounded operators are present and they have to be treated carefully. The exposition is based on joint work with W. Pusz and P. Stachura.
2018-11-30 (Piątek)
Zapraszamy do sali 1.02, ul. Pasteura 5 o godzinie 12:15  Calendar icon
Piotr Witkowski (Max Planck, Dresden)

What's 'electron hydrodynamics' and how to observe it?

Around 40 years ago it was suggested, that under some conditions transport in crystalline materials should be dominated by electron-electron scattering effects and therefore governed by the equations of hydrodynamics. However,that prediction, made by Ghurzi, was far outside experimental reach in the past. Luckily in recent years advances in production of very pure materials allowed to conduct measurements, that indeed suggest presence of such 'hydrodynamic regime' in graphene.In this talk I will describe what does 'hydrodynamic regime' mean, why and when do we expect it, and what are the possible signatures of hydrodynamic behavior in transport measurements. Since the story of electron hydrodynamics(or, as some prefer to call it, viscous electronics) is far from being complete, I will also tell you about the open problems and some possibly interesting future directions.
2018-11-23 (Piątek)
Zapraszamy do sali 1.02, ul. Pasteura 5 o godzinie 12:15  Calendar icon
Maxym Dudka (National Academy of Sciences of Ukraine, Lviv, Ukraine)

Critical behavior of two-dimensional models with descrete spins in the presence of long-range correlated disorder

Here we are interested in the critical properties of two-dimensionalIsing model and $N$-'color' Ashkin-Teller model in a presence of randomquenched structural defects correlated with the distance $r$ according toa power-law $r^{-a}$. In our study we use a mapping of the mentioned spinmodels onto two-dimensional theory of complex (Dirac) fermionic fieldswith disorder. To study the critical behaviour we apply therenormalization group approach. Using two-loop approximation for Isingmodel we find that it belongs to new universality class characterized bythe correlation length exponent $\nu=2/a$. Applying bosonization, we alsocalculate the averaged square of the spin-spin correlation function andfind an estimate for the critical exponent $\eta$. Within one-loop orderwe find for $N$-'color' Ashkin-Teller model that a ``weakly universal''scaling behavior for $N = 2$ as well as the first-order phase transitionfor $N > 2$, are transformed by the correlated disorder into acontinuous phase transition sharing universality class with previouslyconsidered model.
2018-11-16 (Piątek)
Zapraszamy do sali 1.02, ul. Pasteura 5 o godzinie 12:15  Calendar icon
Magdalena Stobińska (IFT UW)

Quantum interference enables constant-time quantum information processing

It is an open question how fast information processing can be performed and whether quantum effects can speed up the best existing solutions. Signal extraction, analysis and compression in diagnostics, astronomy, chemistry and broadcasting builds on the discrete Fourier transform. It is implemented with the Fast Fourier Transform (FFT) algorithm that assumes a periodic input of specific lengths, which rarely holds true. A less-known transform, the Kravchuk-Fourier (KT), allows one to operate on finite strings of arbitrary length. It is of high demand in digital image processing and computer vision, but features a prohibitive runtime. We report a one-step computation of a fractional quantum KT. A quantum d-nary (qudit) architecture we use comprises only one gate and offers processing time independent of the input size. The gate may employ a multiphoton Hong-Ou-Mandel effect. Existing quantum technologies may scale it up towards diverse applications.
2018-11-09 (Piątek)
Zapraszamy do sali 1.02, ul. Pasteura 5 o godzinie 12:15  Calendar icon
Mircea Trif (Tsinghua University, Beijing)

Majorana fermions signatures in a cavity QED setup

One dimensional p-wave (or topological) mesoscopic superconductors are known to host zero energy end modes known as Majorana fermions, i. e. particles that are their own antiparticle. These exotic objects are robust against local perturbations and, moreover, they obey non-Abelian statistics under braiding operations, thus recommending them as qubits for the implementation of a topological quantum computer. While most of the studies of these systems pertain to electronic transport, which is invasive by nature, I will show that the cavity photons give direct access to various electronic susceptibilities of the topological superconductor, which in turn reveals some of its exotic features in a non-invasive fashion. Specifically, in my talk I will show that the the topological phase transition, the presence Majorana fermions, the fractional Josephson effect, as well as their exotic exchange statistics pertaining to their braiding can be imprinted into the electromagnetic field of the cavity.
2018-10-26 (Piątek)
Zapraszamy do sali 1.02, ul. Pasteura 5 o godzinie 12:15  Calendar icon
Krzysztof Sacha (UJ, Kraków)

Time Crystals

2018-10-19 (Piątek)
Zapraszamy do sali 1.02, ul. Pasteura 5 o godzinie 12:15  Calendar icon
Marcin Wysokiński (International Research Centre MagTop, Institute of Physics PAS, Warszawa)

Numerically efficient variational methods to strongly correlated fermion systems at and out of equilibrium

In my presentation, building upon simplest Gutzwiller ansatz, I am going to introduce two methods that can accurately describe strongly correlated fermion systems with a very low numerical effort in comparison to established, rigorous many-body tolls. First, I am going to present diagrammatic expansion of Gutzwiller wave function technique capturing finite-dimensional effects of many-body interactions and demonstrate its performance on concrete examples of topological Kondo insulators and heavy fermion superconductors. Second, I am going to present Gutzwiller wave function combined with a variational Schrieffer-Wolff transformation for a description of Mott transition and its out-of-equilibrium counterpart, dynamical Mott transition.
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