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Wydział Fizyki UW > Badania > Seminaria i konwersatoria > Seminarium "Teoria i Modelowanie Nanostruktur"

Seminarium "Teoria i Modelowanie Nanostruktur"

2014/2015 | 2015/2016 | 2016/2017 | 2017/2018 | 2018/2019

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2015-05-07 (Czwartek)
Zapraszamy do sali 1.02, ul. Pasteura 5 o godzinie 17:15  Calendar icon
mgr Mateusz Wlazło (IFT UW)

Modeling adsorption processes on graphene via ab initio molecular dynamics

In my talk I will describe the application of Car-Parrinello molecular dynamics technique to the study of adsorption processes on graphene. Chemi- and physisorption has been simulated on pristine and defected graphene monolayers. Microcanonical (NVE) and canonical (NVT) ensemble simulations are being used to provide insight about the geometry and stability of those layers in finite temperatures. Adsorption energies are being determined utilizing density functional theory calculations with plane waves as the basis set. The exchange-correlation functional includes the semi-empirical DFT-D2 dispersion correction to account for van der Waals bonding necessary for physisorption. This correction has been tested by quantitative evaluation of exfoliation energies in the graphite bilayer system.
2015-04-23 (Czwartek)
Zapraszamy do sali 1.02, ul. Pasteura 5 o godzinie 17:15  Calendar icon
Łukasz Gładczuk (IFT UW)

First-principles study of group IV honeycomb layers and their binary alloys

Graphene, a two dimensional system exhibits exceptional electronic and physical properties, which have led to the extremely extensive research activities and wide range of proposed applications in nano-electronics and other fields. However, it has been recently predicted theoretically that other group IV elements (Si, Ge, Sn) can be stabilized in the form of honeycomb two-dimensional lattices and soon such materials have been really synthetized and silicene, germacene, and stanene have been born. Soon has been reported that the binary alloys of group IV elements (SiC, SiGe, etc.) can be also stabilized in a form of honeycomb monolayers. Motivated by these developments, we have undertaken extensive ab initio (in the frame work of the density functional theory) studies of cohesive and electronic properties of the whole plethora of the honeycomb monoatomic systems. We have employed the VASP numerical package to compute phase diagrams and electronic band structures of the following systems: Si-Si (silicene), Ge-Ge (germacene), Sn-Sn (stanene) and the binary alloys Si-C, Ge-C, Sn-C, Si-Ge, Si-Sn, and Ge-Sn. For the phase diagram calculations, we consider so-called high buckled and low buckled structures.The alloys containing C, Si-C, Ge-C, and Sn-C, have nearly flat low buckled equilibrium phase and the equilibrium energy of this phase is considerably lower than of the high buckled phase. It is in contrary to all other alloys where the energetic differences are rather small. It strongly suggests that such structures could be transformed into each other under suitable stress. Si-C, Ge-C, and Sn-C alloys have also large energy gap (roughly 2 eV), whereas all other systems have zero or minimal energy gap.
2015-04-16 (Czwartek)
Zapraszamy do sali 1.02, ul. Pasteura 5 o godzinie 17:15  Calendar icon
Michał Papaj (FUW)

Quantum Spin Hall Effect in Tungsten Ditelluride

During the last decade research on topological effects in condensed matter physics became one of the hottest areas of study. However, even though the experimental observation of the quantum spin Hall effect (QSHE) was reported for 2D non-magnetic topological insulators, the accuracy of conductance quantization is rather unsatisfactory and thus their applicability is limited. Therefore, it is important to look for new materials, whose properties would match the theoretical predictions. Recently, QSHE was proposed for 2D transition metal dichalcogenides in 1T’ structure[1]. The most stable compound of this class, tungsten ditelluride, is studied using numerical quantum transport simulations. Without strain, it is a semimetal with 0.1 eV band overlap, but if small strain is applied, the overlap can be removed. Atight-binding model is prepared in order to reproduce low-energy band structure obtained from first principles calculations. It is then used to study properties of the edge states, which reveals features such as a short decay length (about 5 nm). The simulations are performed for both unstrained and strained material and the topological protection of the edge states from disorder is shown. It results in quantized conductance for a broad range of disorder magnitudes, which confirms the viability of this material for device application.Reference:[1] X. Qian, J. Liu, L. Fu, and J. Li, Science 346, 1344 (2014)
2015-04-09 (Czwartek)
Zapraszamy do sali 1.02, ul. Pasteura 5 o godzinie 17:15  Calendar icon
mgr Jan Skolimowski (IFT UW)

Anderson and Mott transitions in presence of the spin-dependent disorder

Recent experiments with ultra cold atoms in optical lattices [1] has drawn us to investigate the phase diagram of correlated lattice fermions at half-filling in the presence of the spin-dependent random potential [2],[3]. The corresponding Anderson-Hubbard model is solved within the dynamical mean field theory with geometrically averaged local density of states [4], which makes our theory sensitive to the Anderson localization. A complete paramagnetic phase diagram for the ground state is determined. The spin-dependent disorder tends to destabilize the metallic solution in contrast to the normal disorder [6]. For strong disorder, above the critical point for the Mott transition, novel spin-dependent localized phases are found. Preliminary results for a magnetic ground state phase diagram at half-filling will be presented as well.[1] D. McKay and B. DeMarco, New J. Phys. 12, 055013 (2010). [2] K. Makuch, J. Skolimowski, P. B. Chakraborty, K. Byczuk and D. Vollhardt, New J. Phys. 15, 045031 (2013) [3] R. Nanguneri, M. Jiang, T. Cary, G. G. Batrouni and R.T. Scalettar, Phys. Rev. B 85, 134506 (2012) [4] V. Dobrosavljevic ,A. A. Pastor and B. K. Nikolic, Europhys. Lett. 62, 76 (2003)[6] K. Byczuk, W. Hofstetter, D. Vollhardt, Phys. Rev. Lett. 94, 056404 (2005).
2015-03-26 (Czwartek)
Zapraszamy do sali 1.02, ul. Pasteura 5 o godzinie 17:15  Calendar icon
Katja Plotnikova (IFW Dresden, Germany)

Propagation of the spin-orbit exciton due to the Jahn-Teller eff ect in systems with strong on-site spin-orbit coupling

2015-03-12 (Czwartek)
Zapraszamy do sali 1.02, ul. Pasteura 5 o godzinie 17:15  Calendar icon
Banhi Chatterjee (IFT UW)

Friedel oscillations in correlated fermionic systems

Friedel oscillations(FO) are quantum mechanical phenomenon observed in metals in presence of charged impurities. FO in the Fermi liquid phase, Mott insulating phase, and at the Mott transition is studied in one and two dimensional lattice models. Electronic correlations are accounted for using different models, approximations, and by solving the dynamical mean-field theory equations, using numerical renormalization group for infinite homogeneous system. Different types of impurity potentials are considered. The problem is solved numerically by exact diagonalization. We observe that in the metallic phase the amplitudes of FO are damped with increasing the interactions while the period remains unchanged. FO almost disappear close to the Mott transition and completely beyond it. An additional bound state is observed in the spectral function at the impurity site which splits along with the sub-bands on increasing the interactions.
2015-03-05 (Czwartek)
Zapraszamy do sali 1.37, ul. Pasteura 5 o godzinie 17:15  Calendar icon
mgr Andrzej Skierkowski (IFT UW)

Rashba spin splitting in 2D systems

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