@article{33965,
author = {{Bocchini, Adriana and Gerstmann, Uwe and Bartley, Tim and Steinrück, Hans-Georg and Henkel, Gerald and Schmidt, Wolf Gero}},
journal = {{Phys. Rev. Materials}},
pages = {{105401}},
publisher = {{American Physical Society}},
title = {{{Electrochemical performance of KTiOAsO_4 (KTA) in potassium-ion batteries from density-functional theory}}},
doi = {{10.1103/PhysRevMaterials.6.105401}},
volume = {{6}},
year = {{2022}},
}
@article{31254,
author = {{Bocchini, Adriana and Gerstmann, Uwe and Schmidt, Wolf Gero}},
journal = {{Phys. Rev. B}},
pages = {{205118}},
publisher = {{American Physical Society}},
title = {{{Oxygen vacancies in KTiOPO_4: Optical absorption from hybrid DFT}}},
doi = {{10.1103/PhysRevB.105.205118}},
volume = {{105}},
year = {{2022}},
}
@inproceedings{46484,
abstract = {{Efficient third-harmonic generation control is theoretically studied. Dielectric nanostructures placed on the metallic substrate could offer effective geometric-phase modulation on third-harmonic signals by selecting proper structure rotational symmetry.}},
author = {{Liu, Bingyi and Huang, Lingling and Zentgraf, Thomas}},
booktitle = {{Conference on Lasers and Electro-Optics}},
location = {{San Jose, USA}},
publisher = {{Optica Publishing Group}},
title = {{{Efficient Third-harmonic Generation Control with Ultrathin Dielectric Geometric-phase Metasurface}}},
doi = {{10.1364/cleo_qels.2022.fth1a.7}},
year = {{2022}},
}
@article{32088,
abstract = {{Subwavelength dielectric resonators assembled into metasurfaces have become a versatile tool for miniaturizing optical components approaching the nanoscale. An important class of metasurface functionalities is associated with asymmetry in both the generation and transmission of light with respect to reversals of the positions of emitters and receivers. The nonlinear light–matter interaction in metasurfaces offers a promising pathway towards miniaturization of the asymmetric control of light. Here we demonstrate asymmetric parametric generation of light in nonlinear metasurfaces. We assemble dissimilar nonlinear dielectric resonators into translucent metasurfaces that produce images in the visible spectral range on being illuminated by infrared radiation. By design, the metasurfaces produce different and completely independent images for the reversed direction of illumination, that is, when the positions of the infrared emitter and the visible light receiver are exchanged. Nonlinearity-enabled asymmetric control of light by subwavelength resonators paves the way towards novel nanophotonic components via dense integration of large quantities of nonlinear resonators into compact metasurface designs.}},
author = {{Kruk, Sergey S. and Wang, Lei and Sain, Basudeb and Dong, Zhaogang and Yang, Joel and Zentgraf, Thomas and Kivshar, Yuri}},
issn = {{1749-4885}},
journal = {{Nature Photonics}},
keywords = {{Atomic and Molecular Physics, and Optics, Electronic, Optical and Magnetic Materials}},
pages = {{561–565}},
publisher = {{Springer Science and Business Media LLC}},
title = {{{Asymmetric parametric generation of images with nonlinear dielectric metasurfaces}}},
doi = {{10.1038/s41566-022-01018-7}},
volume = {{16}},
year = {{2022}},
}
@article{44088,
abstract = {{Hole polarons and defect-bound exciton polarons in lithium niobate are investigated by means of density-functional theory, where the localization of the holes is achieved by applying the +U approach to the oxygen 2p orbitals. We find three principal configurations of hole polarons: (i) self-trapped holes localized at displaced regular oxygen atoms and (ii) two other configurations bound to a lithium vacancy either at a threefold coordinated oxygen atom above or at a two-fold coordinated oxygen atom below the defect. The latter is the most stable and is in excellent quantitative agreement with measured g factors from electron paramagnetic resonance. Due to the absence of mid-gap states, none of these hole polarons can explain the broad optical absorption centered between 2.5 and 2.8 eV that is observed in transient absorption spectroscopy, but such states appear if a free electron polaron is trapped at the same lithium vacancy as the bound hole polaron, resulting in an exciton polaron. The dielectric function calculated by solving the Bethe–Salpeter equation indeed yields an optical peak at 2.6 eV in agreement with the two-photon experiments. The coexistence of hole and exciton polarons, which are simultaneously created in optical excitations, thus satisfactorily explains the reported experimental data.}},
author = {{Schmidt, Falko and Kozub, Agnieszka L. and Gerstmann, Uwe and Schmidt, Wolf Gero and Schindlmayr, Arno}},
issn = {{2073-4352}},
journal = {{Crystals}},
number = {{11}},
publisher = {{MDPI AG}},
title = {{{A density-functional theory study of hole and defect-bound exciton polarons in lithium niobate}}},
doi = {{10.3390/cryst12111586}},
volume = {{12}},
year = {{2022}},
}
@article{34094,
author = {{Gao, Ying and Li, Yao and Ma, Xuekai and Gao, Meini and Dai, Haitao and Schumacher, Stefan and Gao, Tingge}},
issn = {{0003-6951}},
journal = {{Applied Physics Letters}},
keywords = {{Physics and Astronomy (miscellaneous)}},
number = {{20}},
publisher = {{AIP Publishing}},
title = {{{Tilting nondispersive bands in an empty microcavity}}},
doi = {{10.1063/5.0093908}},
volume = {{121}},
year = {{2022}},
}
@article{31937,
author = {{Li, Yao and Ma, Xuekai and Hatzopoulos, Zaharias and Savvidis, Pavlos G. and Schumacher, Stefan and Gao, Tingge}},
issn = {{2330-4022}},
journal = {{ACS Photonics}},
number = {{6}},
pages = {{2079--2086}},
publisher = {{American Chemical Society (ACS)}},
title = {{{Switching Off a Microcavity Polariton Condensate near the Exceptional Point}}},
doi = {{10.1021/acsphotonics.2c00288}},
volume = {{9}},
year = {{2022}},
}
@article{37713,
author = {{Murzakhanov, Fadis F. and Mamin, Georgy Vladimirovich and Orlinskii, Sergei Borisovich and Gerstmann, Uwe and Schmidt, Wolf Gero and Biktagirov, Timur and Aharonovich, Igor and Gottscholl, Andreas and Sperlich, Andreas and Dyakonov, Vladimir and Soltamov, Victor A.}},
issn = {{1530-6984}},
journal = {{Nano Letters}},
keywords = {{Mechanical Engineering, Condensed Matter Physics, General Materials Science, General Chemistry, Bioengineering}},
number = {{7}},
pages = {{2718--2724}},
publisher = {{American Chemical Society (ACS)}},
title = {{{Electron–Nuclear Coherent Coupling and Nuclear Spin Readout through Optically Polarized VB– Spin States in hBN}}},
doi = {{10.1021/acs.nanolett.1c04610}},
volume = {{22}},
year = {{2022}},
}
@article{33080,
author = {{Long, Teng and Ma, Xuekai and Ren, Jiahuan and Li, Feng and Liao, Qing and Schumacher, Stefan and Malpuech, Guillaume and Solnyshkov, Dmitry and Fu, Hongbing}},
issn = {{2198-3844}},
journal = {{Advanced Science}},
keywords = {{General Physics and Astronomy, General Engineering, Biochemistry, Genetics and Molecular Biology (miscellaneous), General Materials Science, General Chemical Engineering, Medicine (miscellaneous)}},
number = {{29}},
publisher = {{Wiley}},
title = {{{Helical Polariton Lasing from Topological Valleys in an Organic Crystalline Microcavity}}},
doi = {{10.1002/advs.202203588}},
volume = {{9}},
year = {{2022}},
}
@article{32310,
author = {{Li, Yao and Ma, Xuekai and Zhai, Xiaokun and Gao, Meini and Dai, Haitao and Schumacher, Stefan and Gao, Tingge}},
issn = {{2041-1723}},
journal = {{Nature Communications}},
keywords = {{General Physics and Astronomy, General Biochemistry, Genetics and Molecular Biology, General Chemistry, Multidisciplinary}},
number = {{1}},
publisher = {{Springer Science and Business Media LLC}},
title = {{{Manipulating polariton condensates by Rashba-Dresselhaus coupling at room temperature}}},
doi = {{10.1038/s41467-022-31529-4}},
volume = {{13}},
year = {{2022}},
}
@article{32148,
author = {{Gao, Xinghui and Hu, Wei and Schumacher, Stefan and Ma, Xuekai}},
issn = {{0146-9592}},
journal = {{Optics Letters}},
keywords = {{Atomic and Molecular Physics, and Optics}},
number = {{13}},
pages = {{3235--3238}},
publisher = {{Optica Publishing Group}},
title = {{{Unidirectional vortex waveguides and multistable vortex pairs in polariton condensates}}},
doi = {{10.1364/ol.457724}},
volume = {{47}},
year = {{2022}},
}
@inbook{30288,
abstract = {{Lithium niobate (LiNbO3), a material frequently used in optical applications, hosts different kinds of polarons that significantly affect many of its physical properties. In this study, a variety of electron polarons, namely free, bound, and bipolarons, are analyzed using first-principles calculations. We perform a full structural optimization based on density-functional theory for selected intrinsic defects with special attention to the role of symmetry-breaking distortions that lower the total energy. The cations hosting the various polarons relax to a different degree, with a larger relaxation corresponding to a larger gap between the defect level and the conduction-band edge. The projected density of states reveals that the polaron states are formerly empty Nb 4d states lowered into the band gap. Optical absorption spectra are derived within the independent-particle approximation, corrected by the GW approximation that yields a wider band gap and by including excitonic effects within the Bethe-Salpeter equation. Comparing the calculated spectra with the density of states, we find that the defect peak observed in the optical absorption stems from transitions between the defect level and a continuum of empty Nb 4d states. Signatures of polarons are further analyzed in the reflectivity and other experimentally measurable optical coefficients.}},
author = {{Schmidt, Falko and Kozub, Agnieszka L. and Gerstmann, Uwe and Schmidt, Wolf Gero and Schindlmayr, Arno}},
booktitle = {{New Trends in Lithium Niobate: From Bulk to Nanocrystals}},
editor = {{Corradi, Gábor and Kovács, László}},
isbn = {{978-3-0365-3340-7}},
pages = {{231--248}},
publisher = {{MDPI}},
title = {{{Electron polarons in lithium niobate: Charge localization, lattice deformation, and optical response}}},
doi = {{10.3390/books978-3-0365-3339-1}},
year = {{2022}},
}
@article{40371,
abstract = {{Multimode integrated interferometers have great potential for both spectral engineering and metrological applications. However, the material dispersion of integrated platforms constitutes an obstacle that limits the performance and precision of such interferometers. At the same time, two-colour nonlinear interferometers present an important tool for metrological applications, when measurements in a certain frequency range are difficult. In this manuscript, we theoretically developed and investigated an integrated multimode two-colour SU(1,1) interferometer operating in a supersensitive mode. By ensuring the proper design of the integrated platform, we suppressed the dispersion, thereby significantly increasing the visibility of the interference pattern. The use of a continuous wave pump laser provided the symmetry between the spectral shapes of the signal and idler photons concerning half the pump frequency, despite different photon colours. We demonstrate that such an interferometer overcomes the classical phase sensitivity limit for wide parametric gain ranges, when up to 3×104 photons are generated.}},
author = {{Ferreri, Alessandro and Sharapova, Polina R.}},
issn = {{2073-8994}},
journal = {{Symmetry}},
keywords = {{Physics and Astronomy (miscellaneous), General Mathematics, Chemistry (miscellaneous), Computer Science (miscellaneous)}},
number = {{3}},
publisher = {{MDPI AG}},
title = {{{Two-Colour Spectrally Multimode Integrated SU(1,1) Interferometer}}},
doi = {{10.3390/sym14030552}},
volume = {{14}},
year = {{2022}},
}
@article{30210,
abstract = {{Lithium niobate on insulator (LNOI) has a great potential for photonic integrated circuits, providing substantial versatility in design of various integrated components. To properly use these components in the implementation of different quantum protocols, photons with different properties are required. In this paper, we theoretically demonstrate a flexible source of correlated photons built on the LNOI waveguide of a special geometry. This source is based on the parametric down-conversion (PDC) process, in which the signal and idler photons are generated at the telecom wavelength and have different spatial profiles and polarizations, but the same group velocities. Distinguishability in polarizations and spatial profiles facilitates the routing and manipulating individual photons, while the equality of their group velocities leads to the absence of temporal walk-off between photons. We show how the spectral properties of the generated photons and the number of their frequency modes can be controlled depending on the pump characteristics and the waveguide length. Finally, we discuss special regimes, in which narrowband light with strong frequency correlations and polarization-entangled Bell states are generated at the telecom wavelength.}},
author = {{Ebers, Lena and Ferreri, Alessandro and Hammer, Manfred and Albert, Maximilian and Meier, Cedrik and Förstner, Jens and Sharapova, Polina R.}},
issn = {{2515-7647}},
journal = {{Journal of Physics: Photonics}},
keywords = {{tet_topic_waveguide}},
pages = {{025001}},
publisher = {{IOP Publishing}},
title = {{{Flexible source of correlated photons based on LNOI rib waveguides}}},
doi = {{10.1088/2515-7647/ac5a5b}},
volume = {{4}},
year = {{2022}},
}
@article{30921,
abstract = {{Quantum walks function as essential means to implement quantum simulators, allowing one to study complex and often directly inaccessible quantum processes in controllable systems. In this contribution, the notion of a driven Gaussian quantum walk is introduced. In contrast to typically considered quantum walks in optical settings, we describe the operation of the walk in terms of a nonlinear map rather than a unitary operation, e.g., by replacing a beam-splitter-type coin with a two-mode squeezer, being a process that is controlled and driven by a pump field. This opens previously unattainable possibilities for quantum walks that include nonlinear elements as core components of their operation, vastly extending their range of applications. A full framework for driven Gaussian quantum walks is developed, including methods to dynamically characterize nonlinear, quantum, and quantum-nonlinear effects. Moreover, driven Gaussian quantum walks are compared with their classically interfering and linear counterparts, which are based on classical coherence of light rather than quantum superpositions. In particular, the generation and boost of highly multimode entanglement, squeezing, and other quantum effects are studied over the duration of the nonlinear walk. Importantly, we prove the quantumness of the evolution itself, regardless of the input state. A scheme for an experimental realization is proposed. Furthermore, nonlinear properties of driven Gaussian quantum walks are explored, such as amplification that leads to an ever increasing number of correlated quantum particles, constituting a source of new walkers during the walk. Therefore, a concept for quantum walks is proposed that leads to—and even produces—directly accessible quantum phenomena, and that renders the quantum simulation of nonlinear processes possible.}},
author = {{Held, Philip and Engelkemeier, Melanie and De, Syamsundar and Barkhofen, Sonja and Sperling, Jan and Silberhorn, Christine}},
issn = {{2469-9926}},
journal = {{Physical Review A}},
number = {{4}},
publisher = {{American Physical Society (APS)}},
title = {{{Driven Gaussian quantum walks}}},
doi = {{10.1103/physreva.105.042210}},
volume = {{105}},
year = {{2022}},
}
@article{25605,
abstract = {{The nonlinear process of second harmonic generation (SHG) in monolayer (1L) transition metal dichalcogenides (TMD), like WS2, strongly depends on the polarization state of the excitation light. By combination of plasmonic nanostructures with 1L-WS2 by transferring it onto a plasmonic nanoantenna array, a hybrid metasurface is realized impacting the polarization dependency of its SHG. Here, we investigate how plasmonic dipole resonances affect the process of SHG in plasmonic–TMD hybrid metasurfaces by nonlinear spectroscopy. We show that the polarization dependency is affected by the lattice structure of plasmonic nanoantenna arrays as well as by the relative orientation between the 1L-WS2 and the individual plasmonic nanoantennas. In addition, such hybrid metasurfaces show SHG in polarization states, where SHG is usually forbidden for either 1L-WS2 or plasmonic nanoantennas. By comparing the SHG in these channels with the SHG generated by the hybrid metasurface components, we detect an enhancement of the SHG signal by a factor of more than 40. Meanwhile, an attenuation of the SHG signal in usually allowed polarization states is observed. Our study provides valuable insight into hybrid systems where symmetries strongly affect the SHG and enable tailored SHG in 1L-WS2 for future applications.}},
author = {{Spreyer, Florian and Ruppert, Claudia and Georgi, Philip and Zentgraf, Thomas}},
issn = {{1936-0851}},
journal = {{ACS Nano}},
number = {{10}},
pages = {{16719--16728}},
title = {{{Influence of Plasmon Resonances and Symmetry Effects on Second Harmonic Generation in WS2–Plasmonic Hybrid Metasurfaces}}},
doi = {{10.1021/acsnano.1c06693}},
volume = {{15}},
year = {{2021}},
}
@article{23815,
abstract = {{In this paper, silicon oxynitride films (SiON) grown by plasma-enhanced chemical vapor deposition are investigated. As precursor gases silane (SiH4), nitrous oxide (N2O), nitrogen (N2) and ammonia (NH3) are used with different compositions. We find that for achieving high nitrogen content adding ammonia to the precursor mix is most efficient. Moreover, we investigate the balance between adsorption and desorption processes during film growth by investigating the film growth rate as a function of the substrate temperature. From these data we are able to determine an effective activation energy for the film growth, corresponding to the difference between adsorption and desorption energy. Finally, we have thoroughly investigated the optical properties of the films using spectroscopic ellipsometry. From these measurements, we suggest a parametrized model for the refractive index and extinction coefficient in a wide range of compositions based on a Cauchy- and a Lorentz-fit.}},
author = {{Aschwanden, R. and Köthemann, R. and Albert, M. and Golla, C. and Meier, Cedrik}},
issn = {{0040-6090}},
journal = {{Thin Solid Films}},
title = {{{Optical properties of silicon oxynitride films grown by plasma-enhanced chemical vapor deposition}}},
doi = {{10.1016/j.tsf.2021.138887}},
volume = {{736}},
year = {{2021}},
}
@article{20592,
abstract = {{GaAs-(111)-nanostructures exhibiting second harmonic generation are new building blocks in nonlinear optics. Such structures can be fabricated through epitaxial lift-off using selective etching of Al-containing layers and subsequent transfer to glass substrates. Herein, the selective etching of (111)B-oriented AlxGa1−xAs sacrificial layers (10–50 nm thick) with different aluminum concentrations (x = 0.5–1.0) in 10\% hydrofluoric acid is investigated and compared with standard (100)-oriented structures. The thinner the sacrificial layer and the lower the aluminum content, the lower the lateral etch rate. For both orientations, the lateral etch rates are in the same order of magnitude, but some quantitative differences exist. Furthermore, the epitaxial lift-off, the transfer, and the nanopatterning of thin (111)B-oriented GaAs membranes are demonstrated. Atomic force microscopy and high-resolution X-ray diffraction measurements reveal the high structural quality of the transferred GaAs-(111) films.}},
author = {{Henksmeier, Tobias and Eppinger, Martin and Reineke, Bernhard and Zentgraf, Thomas and Meier, Cedrik and Reuter, Dirk}},
journal = {{physica status solidi (a)}},
keywords = {{epitaxial lift-off, GaAs/AlxGa1−xAs heterostructures, selective etching}},
number = {{3}},
pages = {{2000408}},
title = {{{Selective Etching of (111)B-Oriented AlxGa1−xAs-Layers for Epitaxial Lift-Off}}},
doi = {{https://doi.org/10.1002/pssa.202000408}},
volume = {{218}},
year = {{2021}},
}
@article{20900,
author = {{Albert, M. and Golla, C. and Meier, Cedrik}},
issn = {{0022-0248}},
journal = {{Journal of Crystal Growth}},
title = {{{Optical in-situ temperature management for high-quality ZnO molecular beam epitaxy}}},
doi = {{10.1016/j.jcrysgro.2020.126009}},
volume = {{557}},
year = {{2021}},
}
@article{22450,
abstract = {{We realize and investigate a nonlinear metasurface taking advantage of intersubband transitions in ultranarrow GaN/AlN multi-quantum well heterostructures. Owing to huge band offsets, the structures offer resonant transitions in the telecom window around 1.55 µm. These heterostructures are functionalized with an array of plasmonic antennas featuring cross-polarized resonances at these near-infrared wavelengths and their second harmonic. This kind of nonlinear metasurface allows for substantial second-harmonic generation at normal incidence which is completely absent for an antenna array without the multi-quantum well structure underneath. While the second harmonic is originally radiated only into the plane of the quantum wells, a proper geometrical arrangement of the plasmonic elements permits the redirection of the second-harmonic light to free-space radiation, which is emitted perpendicular to the surface.}},
author = {{Mundry, Jan and Spreyer, Florian and Jmerik, Valentin and Ivanov, Sergey and Zentgraf, Thomas and Betz, Markus}},
issn = {{2159-3930}},
journal = {{Optical Materials Express}},
number = {{7}},
publisher = {{OSA}},
title = {{{Nonlinear metasurface combining telecom-range intersubband transitions in GaN/AlN quantum wells with resonant plasmonic antenna arrays}}},
doi = {{10.1364/ome.426236}},
volume = {{11}},
year = {{2021}},
}