(Institute of Physics, Faculty of Physics, Astronomy and Informatics, Nicolaus Copernicus University, Toruń, Poland)
Gated multilayer graphene with rhombohedral stacking of layers exhibits a tunable energy gap. The stacking order can be changed when some layers are stretched, or delaminated and corrugated. In such cases, topological gapless states, connecting the valence and conduction band continua, appear at each valley. These states are localized at stacking domain walls (interfaces) that separate two different stacking orders. When the stacking change occurs along the zigzag direction, the Dirac cones at different valleys in the k-space are well separated. The gapless states are therefore valley-protected and provide one-dimensional and non-destructive valley currents that can flow along the stacking domain wall in opposite directions. Valley protection can be destroyed in the presence of atomic-scale defects. Here, we demonstrate the robustness of the gapless states to different defect-like perturbations of the multilayers. It is shown that some gapless states survive very strong distortions of the stacking domain walls. They persist when some layers are broken or partially removed, or even when vacancies or magnetic impurities are present at the stacking interface.
Zapraszamy do sali 0.06, ul. Pasteura 5 o godzinie 10:15

prof dr hab. Izabella Grzegory (Institute of High Pressure Physics Unipress PAS)
The discoveries of graphene, topological insulators and other novel materials have opened a whole new area, namely two-dimensional electronics. This new frontier has spurred the rediscovery of boron nitride (BN), a member of the family of III-N compounds that has much promise for modern electronics. In this talk the hexagonal BN (hBN) will be introduced. In particular the use of high pressure for its synthesis and crystal growth as well for identification of selected defect centers will be highlighted.Like carbon, BN forms crystalline structures with different atomic configurations at different pressure-temperature conditions. At relatively low pressures, BN is thermodynamically stable in its hexagonal graphite-like structure, hBN. This form features monoatomic layers strongly bound in a honeycomb pattern, like graphene, and inter-bonded with weak van der Waals forces. The hBN, is well established, having been widely deployed for many years. It has found use as a crucible material, in the form of sintered ceramics that benefit from its high thermal and chemical stability, and as a solid lubricant, thanks to its layered structure. Now new opportunities beckon, with hBN under investigation as a potential platform for 2D electronics and quantum technology.While graphite and hBN have similarities in their crystalline form, they differ in electrical conductivity, with hBN behaving as a strongly insulating crystal. This strongly insulating characteristic is to be expected, given that hBN has a wide bandgap of 6 eV. In monolayer hBN this gap is direct, but it shifts to indirect as the number of layers increases. Surprisingly, regardless of whether this material has a direct or indirect band gap, the UV optical emission produced by hBN is extremely efficient. Employed in its two-dimensional form as very thin structures, hBN can be deployed as an excellent insulator or tunnelling dielectric barrier in devices based on graphene and other 2D heterostructures.Important opportunities arise in hBN due to defects within the material. These imperfections enable very interesting physical systems that provide single-photon emitters, or centres hosting quantum spin states with a long coherence time. The results of using high pressure for identification of important ultraviolet color centers in hBN will be presented.For both fundamental studies and the pursuit of new applications, it is critical to produce high-quality crystalline hBN, as this holds the key to uncovering its fascinating properties, as well as evaluating the predictability of theoretical models. Unfortunately, it is far from easy to grow crystalline hBN. Due to a melting temperature that exceeds 3000 °C, hBN, unlike silicon and GaAs, cannot be grown from its stoichiometric melt. Due to this limitation, two leading methods have emerged for the crystallization of hBN. One of them, involves very high pressures of 5 GPa or more, and metallic solutions, containing the likes of Ba, Mg and Ni. In contrast to GaN and InN, hBN does not require a high nitrogen pressure to suppress its decomposition at high temperatures. So the alternative –is based on growth on the surfaces of molten transition metal alloys containing boron, and involves a flow of nitrogen gas at atmospheric pressure. For both approaches, crystals are limited to the order of 1 mm in size. Another concern is the very small thickness of the hBN crystals grown on metal surfaces under atmospheric N2 pressure. To avoid this, we have focused recently, on the high N2 pressure approach to the crystal growth of hBN. Our expectation is that through the controlled increase of nitrogen solubility in molten metals, we will enhance the growth of hBN in the c-direction in the case of surface crystallization, and enable the production of thicker crystals. Our ultimate goal is to establish a new approach, where in contrast to crystallization of hBN on metal surfaces, crystals will be grown in the solution volume. That’s mirroring the technique that we honed for the production of high-quality single crystals of GaN with dimensions of more than 1cm. New emerging high pressure approaches: zone melting and ammonothermal will be also introduced.
Zapraszamy do sali 0.06, ul. Pasteura 5 o godzinie 10:15

dr inż. Konrad Wilczyński (Wydział Fizyki Politechniki Warszawskiej)
The purpose of this work is to study the vibrational properties of crystal lattices (phonons) in a choice of two-dimensional materials and their heterostructures on the grounds of quantum-mechanical simulations based on the density functional theory (DFT), with particular emphasis on the impact of the lattice temperature. The following two-dimensional structures (based on the transition metal dichalcogenides) will be considered: semiconducting single-layered 1H-MoS2 and 1H-WS2, multi-layered 2H-WS2 [1], 1H-MoS2/1H-WS2 heterostructures with different relative stacking between the layers, 1H-MoS2/graphene heterostructure, and highly anharmonic semi-metallic 1T-TiS2 material [2]. All the listed-above systems are significant from the point of view of their potential applications, enabling us to supplement physical properties of the famous graphene – from the point of view of its electrical, thermal, optical, mechanical, and chemical properties.The undertaken studies, based on rigorous theoretical grounds described in the literature of the 1960s, include the calculation of key effects induced by the anharmonicity of interatomic interactions, such as the thermal expansion of the structure and anharmonic phonon-phonon interactions (in particular three- and four-phonon processes) – affecting the temperature dependence of the effective phonon frequencies and their lifetimes. Each of the above-listed anharmonic effects has been studied separately, enabling us to better understand their nature in each studied two-dimensional material and their dependence on the structure’s geometry. The obtained theoretical temperature-dependent propagation parameters of main phonon modes agree very well with available spectroscopic measurement data, indicating the DFT calculations’ ability to well reproduce this physical property. Therefore, the proposed methodology might be successfully extended to more advanced problems such as complex multi-layered structures and other phonon-limited physical properties (e.g., thermal conductivity).Acknowledgments: Research was funded by the Warsaw University of Technology within the Excellence Initiative: Research University (IDUB) programme. We also acknowledge the usage of computer cluster DWARF at Warsaw University of Technology supported by the Polish National Science Center (NCN) under Contracts No. UMO-2017/26/E/ST3/00428 and UMO-2017/27/B/ST2/02792.References[1] K. Wilczyński, A.P. Gertych, K. Czerniak-Łosiewicz, J. Sitek, M. Zdrojek, “Phonon anharmonicity in multi-layered WS2 explored by first-principles and Raman studies”, Acta Materialia 240, 118299, (2022).[2] K. Wilczyński, A.P. Gertych, M. Zdrojek, “Explaining Mysterious “Shoulder” Raman Band in TiS2 by Temperature-dependent Anharmonicity and Defects”. J. Phys. Chem. C 127, 20870–20880 (2023).
Zapraszamy do sali 0.06, ul. Pasteura 5 o godzinie 10:15

dr hab. Maciej Molas, prof. UW (Institute of Experimental Physics, Faculty of Physics, University of Warsaw, Warsaw, Poland)
Semiconducting transition metal dichalcogenides (S-TMDs) based on molybdenum andtungsten, i.e. MoS2, MoSe2, MoTe2, WS2, and WSe2, are the most well-known representativesof van der Waals materials. Their most distinguished hallmark is the transition from indirect- todirect-band gap, when thinned down from a bulk to a monolayer (ML). The optical response ofS-TMDs is caused mainly by excitonic effects, even at room temperature, due to the largeexcitonic binding energy at the level of hundreds of meV. Moreover, the exciton-phononcoupling (EPC) is significant in thin layers of S-TMDs, which leads to the rich Raman scattering(RS) spectra under their resonant excitation conditions.In my talk I will give an overview on excitons and phonons apparent in high qualityS-TMD MLs and bilayers (BLs) encapsulated in hexagonal BN. The first part of the lecturewill cover experimental and theoretical investigations of excitonic properties in ML and the BLof MoSe2 [1]. The measured magnetic field evolutions of the reflectance contrast spectra of theMoSe2 ML and BL permit one to determine g-factors of intralayer A and B excitons, as well asthe g-factor of the interlayer exciton. The dependence of g-factors on the number of layers andexcitation state will be explained using first-principles calculations. It will be demonstrated thatthe experimentally measured ladder of excitonic s states in the ML can be reproduced using thek·p approach with the Rytova–Keldysh potential that describes the electron–hole interaction.On the contrary, the analogous calculation for the BL case requires taking into account the outof-plane dielectric response of the MoSe2 BL.The second part of my talk will be devoted to the study of phonons in the four S-TMDMLs, i.e. MoS2, MoSe2, WS2, and WSe2, using Raman scattering excitation (RSE), which is anexperimental technique in which the spectrum is made up by sweeping the excitation energywhen the detection energy is fixed [2]. It will be shown that the outgoing resonant conditionsof Raman scattering reveal an extraordinary intensity enhancement of the phonon modes, whichresults in extremely rich RSE spectra. The obtained spectra are composed not only of Ramanactive peaks, i.e. in-plane E’ and out-of-plane A’1, but the appearance of 1st, 2nd, and higherorder phonon modes is recognized. Moreover, the intensity profiles of the A’1 modes in theinvestigated MLs resemble the emissions due to neutral excitons measured in the correspondingPL spectra for the outgoing type of resonant Raman scattering conditions. This results indicatesthat the strength of EPC in S-TMD MLs strongly depends on the type of their ground excitonicstate, i.e. bright or dark, resulting in different shapes of the RSE spectra.[1] Ł. Kipczak, et al., 2D Materials 10, 025014 (2023).[2] M. Zinkiewicz, et al., npj 2D Materials and Applications 8, 2 (2024)
Zapraszamy do sali 0.06, ul. Pasteura 5 o godzinie 10:15

prof. dr hab. Grzegorz Karczewski (Institute of Physics, Polish Academy of Sciences)
The wide energy gap II-VI semiconductor, CdTe, and the narrow energy gap IV-VI semiconductor, PbTe, have been studied for years, thus their properties are well known. Both crystallize in cubic lattice structures with very similar lattice constants, making epitaxy of one material on another simple. However, their crystal structures are different - for PbTe it is a rock salt structure, and for CdTe it is a zinc blende structure. The crystal structure mismatch makes PbTe and CdTe immiscible. The interfaces between areas of pure PbTe and CdTe are very sharp, however, decorated with a large number of dangling bonds that can act as traps for mobile carriers from PbTe. The goal of the seminar is to show that a mixture of nanometer-sized areas of pure PbTe and CdTe, i.e. a PbTe/CdTe nanocomposite, exhibits new or at least strongly modified features that lead to new functionalities and applications of the material. In particular, it will be recalled how perfectly shaped PbTe quantum dots are produced in a CdTe matrix and what their luminescent properties are. It will also be recalled that CdTe anti-dots introduced into PbTe improve its thermoelectric properties. The main part of the seminar will be devoted to the latest research results of high-temperature infrared detectors made of PbTe/CdTe nanocomposite. Two types of detectors will be presented: photoresistors and photodiodes. In the latter case, the p-n diodes are made of wide bandgap II-VI semiconductors with narrow bandgap PbTe nano-inclusions introduced into the depletion region during MBE growth. Such diodes can be used not only for infrared sensing, but also for two-color infrared photovoltaics.