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shortdescription => protected'In the WSI, we develop new semiconductors, catalytic assemblies, and nanosys
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title => protected'Widely-tunable room-temperature THz quantum cascade laser sources' (65 chars)
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shortdescription => protected'<p>THz spectral range is teeming with mainstream concepts. However, it is st
 ill in need of a convenient and compact semiconductor source and detector te
 chnology. In particular, THz radiation sources are bulky, complex in operati
 on, and expensive to manufacture. Real-world applications require <i>room-te
 mperature</i> broadly-tunable or frequency-comb THz sources that are similar
  in operation simplicity and mass producibility to diode lasers and mid-IR q
 uantum cascade lasers (QCLs).<br /><br />We have recently achieved significa
 nt progress in the development of such sources [1,2]. Our devices are based
 on efficient frequency mixing inside of dual-wavelength mid-IR QCLs. Their a
 ctive regions are quantum-engineered to provide a giant nonlinearity for dif
 ference-frequency generation (DFG) with population inversion [1,2] and their
  waveguides are designed for Cherenkov phase-matching of DFG that enables TH
 z extraction through the substrate [3]. As a result, these devices (referred
  to as THz DFG-QCLs) can now provide up to nearly 2 mW of peak THz power out
 put and over 10 µW of continuous-wave THz power at room temperature [1,2]. A
  schematic of a Cherenkov THz DFG-QLC is shown in the figure on the right.&n
 bsp;</p>
' (1224 chars)
description => protected'<p>A typical single mode device performance is shown in Fig. 1(a). We have a
 lso demonstrated that THz DFG-QCL chips can be continuously tuned over nearl
 y the entire 1-6 THz range using an external cavity setup [3-5] or in monoli
 thic configurations [6,7], see Fig. 2(b). We have further recently confirmed
  that, in continuous-wave operation, these devices provide a narrow (sub-MHz
 ) emission linewidth which makes them suitable to be used as local oscillato
 rs for heterodyne spectroscopy [8]. The THz DFG-QCL platform holds a high pr
 omise for developing efficient broadband THz frequency comb sources for spec
 troscopic and metrological applications.<br /><br />Our ongoing work is aime
 d at improving the THz radiation outcouping efficiency (estimated to be belo
 w ~5% in the current devices) [9,10], enhancing the optical nonlinearity in
 the QCL active regions to increase THz output power, improving device therma
 l packaging, generating THz frequency combs, developing miniature broadly-tu
 nable THz systems, and demonstrating compact semiconductor-based THz instrum
 entation such as spectroscopy and imaging systems, dual-comb spectrometers,
 and microscopy systems.</p>
' (1167 chars)
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paragraph2 => protected'<p class="text-center">REFERENCES</p> <ol><li>K. Fujita, S. Jung, Y. Jiang,
  J.H. Kim, A Nakanishi, A. Ito, M. Hitaka, T. Edamura, and M.A. Belkin, “Rec
 ent progress in terahertz difference-frequency quantum cascade laser sources
 ,” <i>Nanophoton.</i> <strong>7</strong>, 1795-1817 (2018).</li><li>M.A. Bel
 kin and F. Capasso, “New frontiers in quantum cascade lasers: high performan
 ce room temperature terahertz sources,” <i>Phys. Scr.</i> <strong>90</strong
 >, 118002 (2015).</li><li>K. Vijayraghavan, Y. Jiang, M. Jang, A. Jiang, K.
 Choutagunta, A. Vizbaras, F. Demmerle, G. Boehm, M. C. Amann, and M. A. Belk
 in, “Broadly tunable terahertz generation in mid-infrared quantum cascade la
 sers,” <i>Nature Commun.</i> <strong>4</strong>, 2021 (2013).</li><li>Y. Jia
 ng, K. Vijayraghavan, S. Jung, F. Demmerle, G. Boehm, M.-C. Amann, and M.A.
 Belkin “External cavity terahertz quantum cascade laser sources based on int
 racavity frequency mixing with 1.2-5.9 THz tuning range,” <i>J. Opt.</i> <st
 rong>16</strong>, 094002 (2014).</li><li>Y. Jiang, K. Vijayraghavan, S. Jung
 , A. Jiang, J.H. Kim, F. Demmerle, G. Boehm, M.C. Amann, and M.A. Belkin, “S
 pectroscopic study of terahertz generation in mid-infrared quantum cascade l
 asers,” <i>Sci. Rep.</i> <strong>6</strong>, 21169 (2016).</li><li>S. Jung,
 A. Jiang, Y. Jiang, K. Vijayraghavan, X. Wang, M. Troccoli, and M.A. Belkin,
  “Broadly tunable monolithic room-temperature terahertz quantum cascade lase
 r sources,” <i>Nature Commun.</i> <strong>5</strong>, 4267 (2014).</li><li>A
 . Jiang, S. Jung, Y. Jiang, K. Vijayraghavan, J. Kim, and M.A. Belkin, “Wide
 ly tunable terahertz source based on intra-cavity frequency mixing in quantu
 m cascade laser arrays,” <i>Appl. Phys. Lett.</i> <strong>106</strong>, 2611
 07 (2015).</li><li>L. Consolino, S. Jung, A. Campa, M. De Regis, S. Pal, K.
 Fujita, A. Ito, M. Hitaka, S. Bartalini, P. De Natale, M.A. Belkin, and M.S.
  Vitiello, “Spectral purity and tunability of terahertz quantum cascade lase
 r sources based on intra...
' (2573 chars)
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title => protected'Integrated mid-infrared photonics' (33 chars)
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shortdescription => protected'<p>Near-infrared (wavelengths approximately in the range of 1-2.5 microns) p
 hotonic integrated circuits (PICs) based on the silicon-on-insulator (SOI) o
 r III-V platforms have undergone a tremendous expansion in recent years, dri
 ven initially by applications in fiber-optics communications and optical int
 erconnects and later expanding to beam combining and steering, chemical and
 biological sensing, and frequency comb generation. Near-infrared PIC systems
  are now commercialized for several different applications by companies such
  as Infinera, Sisco Systems, SICOYA, and many others.<br /><br />In contrast
  to the near-infrared spectral range, mid-IR laser-based systems have so far
  been designed around free-space optics. Integration of a semiconductor lase
 r with a suitable mid-IR photonics platform will enable the development of m
 id-IR PICs for a wide range of applications from spectroscopy and sensing to
  beam steering aund ab nd new frequency generation. We have recently started
  investigating approaches for developing mid-IR PICs using both silicon and
 III-V platforms.</p>
' (1084 chars)
description => protected'<p>Figure 2(a) shows the electron microscope image of a mid-IR QCL epi-trans
 ferred to Silicon-on-Sapphire (SOS) wafers using 250-nm-thick SU-8 epoxy as
 an adhesive. Efficient coupling of mid-IR light from the laser cavity to sil
 icon waveguides was achieved using tapered QCL waveguides as shown in Fig. 3
 (a) after Ref. [1]. Similar transfer-printing methods can be used to integra
 te other mid-IR light sources, such as diode lasers and interband cascade la
 sers (ICLs) with silicon waveguides.<br /><br />Hybrid mid-IR systems based
 on III-V laser materials transferred to silicon photonic waveguides are expe
 cted to perform well with mid-IR diode lasers and ICLs that have relatively
 low (few tens of milliwatts) optical powers and thermal power dissipation. H
 owever, long-wavelength room-temperature operation of these devices is limit
 ed to the 5-6 microns spectral range. In addition, the use of the Si-based p
 latforms limits the spectral range of mid-IR PICs to below 7 μm due to optic
 al absorption in Si.<br /><br />QCLs are currently the only room-temperature
  electrically pumped semiconductor light sources that can operate in the ent
 ire mid-IR range (from 3 to 15 microns) with optical powers over 1 W. Given
 the very high thermal dissipation in QCL active regions, achieving long-term
  reliability and continuous-wave operation of heterogeneously integrated dev
 ices on silicon platforms is challenging. Therefore, we have recently starte
 d working on homogeneous integration of mid-IR QCLs with low-loss III-V pass
 ive waveguides epitaxially grown on InP substrates, see Fig. 2(b). The homog
 eneous integration approach uses materials, growth, and processing steps nea
 rly identical to those used for conventional high-performance mid-IR QCLs, w
 hich offers superior reliability and performance of photonic integrated circ
 uits. Devices integrated with III-V waveguides show more than an order of ma
 gnitude higher output power from passive waveguides, compared to devices int
 egrated with the SOS wav...
' (2275 chars)
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paragraph2 => protected'<p class="text-center">REFERENCES</p> <ol><li>S. Jung, J. Kirch, J.H. Kim,
 L.J. Mawst, D. Botez, and M.A. Belkin, “Quantum cascade lasers transfer-prin
 ted on silicon-on-sapphire,” <i>Appl. Phys. Lett.</i> <strong>111</strong>,
 211102 (2017).</li><li>S. Jung, D. Palaferri, K. Zhang, F. Xie, Y. Okuno, C.
  Pinzone, K. Lascola, and M.A. Belkin, “Homogeneous photonic integration of
 mid-infrared quantum cascade lasers with low-loss passive waveguides on InP
 platform,” <i>Optica</i> <strong>6</strong>, 1023-1030 (2019).</li></ol>
' (528 chars)
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title => protected'Quantum-engineered nonlinear metamaterials' (42 chars)
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shortdescription => protected'<p>The mid-IR and THz regions are particularly suitable for creating enginee
 red materials based on the concepts of quantum-engineering of electron state
 s, plasmonics, and metamaterials. We have recently demonstrated the potentia
 l of this approach by creating large-area ultrathin metasurfaces with record
 -high nonlinear optical response. The metasurfaces operate by coupling modes
  in electromagnetically-engineered plasmonic nanoresonators with quantum-eng
 ineered intersubband nonlinearities in a thin semiconductor heterostructure.
 <br /><br />Subwavelength thickness of our metasurfaces precludes phase matc
 hing constrains associated with traditional nonlinear optical crystals and t
 hus allows for broadband frequency conversion. Furthermore, since very low o
 ptical intensity is required to produce strong nonlinear effects, our metasu
 rfaces may be pumped using compact continuous-wave semiconductor lasers such
  as QCLs or diode lasers. Continuously-pumped metasurfaces may be used, for
 example, to achieve self-referencing and frequency shift of low-power micror
 esonator-based optical frequency comb sources to anywhere in mid-IR and THz,
  to generate large amounts of THz radiation using high-power mid-IR pump las
 ers (e.g., CO<sub>2</sub> lasers or high-power QCLs), and to up-convert mid-
 IR and THz optical signals for focal-plane-array imaging.</p>
' (1353 chars)
description => protected'<p>The basic schematic of the metasurface is given in Fig. 4 and its operati
 on is explained in the figure caption. We achieved over 0.075 % of mid-IR se
 cond-harmonic power conversion efficiency using only 15 kW/cm<sup>2</sup> of
  pump intensity [1,2]. The second-order nonlinear susceptibility of our late
 st metasurfaces at low pump intensity is estimated to be over 10<sup>6</sup>
  pm/V, 4 orders of magnitude higher than that of traditional nonlinear mater
 ials such as LiNbO3. From the fundamental standpoint, our metasurfaces provi
 de the foundation for the “flat nonlinear optics paradigm” in which we can s
 imultaneously produce high nonlinear conversion efficiency and achieve full
 control of the wavefront of the nonlinear output, as demonstrated by us in R
 ef. [3].<br /><br />We are now investigating numerous directions in which th
 e effective nonlinearity and conversion efficiency of the metasurfaces may b
 e further improved, particularly, by optimizing plasmonic nanoresonator desi
 gns to achieve higher field enhancement and higher nonlinear overlap integra
 l [4,5] and by increasing the intersubband nonlinearity and saturation inten
 sity of the semiconductor heterostructure using more sophisticated MQW desig
 ns. Theoretical simulations indicate that up to 10% of power conversion effi
 ciency is possible in fully-optimized structures using input intensities ~10
 -100 kW/cm<sup>2</sup>. Additional ongoing and planned future research on th
 is topic include<br /><br />&nbsp;</p> <ul><li>Design and experimental test
 ing of metasurfaces for THz difference-frequency generation [6];</li><li>Met
 asurfaces for efficient up-conversion of mid-IR and THz signals for detectio
 n and imaging;</li><li>Nonlinear metasurfaces for mid-IR and THz Raman lasin
 g and other four-wave mixing processes such as phase conjugation and all-opt
 ical control;</li><li>Investigating quantum effects in individual highly-non
 linear nanoscale optical resonators [7].</li></ul>
' (1950 chars)
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paragraph2 => protected'<p class="text-center">REFERENCES</p> <ol><li>J. Lee, M. Tymchenko, C. Argy
 ropoulos, P. Y. Chen, F. Lu, F. Demmerle, G. Boehm, M. C. Amann, A. Alu, and
  M.A. Belkin, “Giant nonlinear response from plasmonic metasurfaces coupled
 to intersubband transitions,” <i>Nature</i> <strong>511</strong>, 65 (2014).
 </li><li>J. Lee, N. Nookala, J. S. Gomez-Diaz, M. Tymchenko, F. Demmerle, G.
  Boehm, M.-C. Amann, A. Alù, and M.A. Belkin “Ultrathin second-harmonic meta
 surfaces with record-high nonlinear optical response,” <i>Adv. Opt. Mat.</i>
  <strong>4</strong>, 664-670 (2016).</li><li>N. Nookala, J. Lee, J.S. Gomez-
 Diaz, M. Tymchenko, F. Demmerle, G. Boehm, K. Lai, G. Shvets, M.-C. Amann, A
 . Alù, and M.A. Belkin, “Ultrathin gradient nonlinear metasurface with a gia
 nt nonlinear response,” <i>Optica</i> <strong>3</strong>, 283-288 (2016).</l
 i><li>N. Nookala, J. Xu, O. Wolf, S. March, R. Sarma, S. Bank, J. Klem, I. B
 rener, and M. A. Belkin, “Mid-infrared second-harmonic generation in ultra-t
 hin plasmonic metasurfaces without a full-metal backplane,” <i>Appl. Phys. B
 .</i> <strong>124</strong>, 132 (2018).</li><li>R. Sarma, D. de Ceglia, N. N
 ookala, M. Vincenti, S. Campione, O. Wolf, M. Scalora, M. Sinclair, M. Belki
 n and I. Brener, "Broadband and efficient second-harmonic generation from a
 hybrid dielectric metasurface/semiconductor quantum-well structure," <i>ACS
 Photon.</i> <strong>6</strong>, 1458 (2019).</li><li>M. Tokman, Z. Long, S.
 Al Mutairi, Y. Wang, V. Vdovin, M. Belkin, and A. Belyanin, “Purcell enhance
 ment of the parametric down-conversion in two-dimensional nonlinear material
 s,” <i>APL Photonics</i> <strong>4</strong>, 034403 (2019).</li><li>M. Tymch
 enko, J. S. Gomez-Diaz, J. Lee, M.A. Belkin, and A. Alù, “Highly-efficient T
 Hz generation using nonlinear plasmonic metasurfaces,” <i>J. Opt.</i> <stron
 g>19</strong>, 104001 (2017).</li></ol>
' (1863 chars)
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title => protected'Mid-infrared vertical cavity surface emitting lasers (VCSELs)' (61 chars)
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shortdescription => protected'<p>Gas sensing based on direct laser diode absorption spectroscopy is one of
  the most sensitive and selective detection methods and it is widely used in
  industry. Because of their geometry, vertical cavity surface emitting laser
 s (VCSELs) are known to have significant advantages over edge-emitting diode
  lasers, including extreme compactness, about two orders of magnitude lower
 power consumption (due to smaller active region volume), round (rather than
 elliptical) beam shape, and intrinsic single-mode operation without the need
  for complex distributed feedback gratings used in single-mode edge-emitting
  lasers (due to much smaller laser cavity size).<br /><br />Mid-IR spectral
 range is often called the ‘molecular fingerprint region’ because any chemica
 l compound can be uniquely described by its molecular absorption fingerprint
 . The development of continuous-wave (CW) mid-IR VCSELs is highly desired fo
 r the creation of compact chemical sensors with high detectivity and specifi
 city. Currently, however, such VCSELs do not exist. We are working on the de
 velopment of CW room-temperature mid-IR VCSELs in the wavelength range 3-5 µ
 m.</p>
' (1146 chars)
description => protected'<p>Due to current unavailability of CW VCSELs operating in the wavelength ra
 nge of the fundamental molecular roto-vibrational absorption lines, devices
 operating at shorter near-infrared (near-IR) wavelengths (often around 1550
 nm) are used to target the absorption lines corresponding to “overtones” (hi
 gher-order harmonics) of fundamental molecular vibrations. However, these li
 nes are typically about 2 orders of magnitude weaker than the fundamental ab
 sorption lines. Figure 5(a) shows the absorption spectrum of methane display
 ing both fundamental absorption lines around 3300&nbsp;nm and overtone lines
  at 1550 nm and 2300 nm. Additionally, the overtone line spectrum of molecul
 ar compounds is more complex and spectrally dense compared to the spectrum o
 f the fundamental lines. As a result, it is often difficult to select an ove
 rtone absorption line of a target molecule that is free from interference pr
 oduced by overtone lines of other gases.<br /><br />Our research efforts foc
 us on developing CW room-temperature mid-IR VCSELs operating in the 3-5 µm w
 avelength range using InAlGaAsSb heterostructures grown on GaSb substrates.
 The schematic of a VCSEL structure is shown in Fig. 5(b). The Chair has prod
 uced devices that define the current state of the art in the mid-IR VCSEL te
 chnology, including CW VCSELs at 3 µm wavelength [1] and at 4 µm wavelength
 [2] with near-room-temperature operation, see Fig. 6.<br /><br />Current res
 earch efforts are focused on improving the active region design of the devic
 es using both type-I and type-II active region schemes, improving the mirror
  design and the current injection aperture design in these devices, optimizi
 ng thermal packaging and more. The development of the first CW mid-IR VCSELs
  is also expected to lead to various opportunities in application of these d
 evices for gas sensing and spectroscopy.</p>
' (1868 chars)
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paragraph2 => protected'<p class="text-center">REFERENCES</p> <ol><li>A. Andrejew, S. Sprengel, and
  M.-C. Amann, "GaSb-based vertical-cavity surface-emitting lasers with an em
 ission wavelength at 3 μm", <i>Opt. Lett.</i> <strong>41</strong>, 2799 (201
 6).</li><li>G.K. Veerabathran, S. Sprengel, A. Andrejew, and M.-C. Amann, "R
 oom-temperature vertical-cavity surface-emitting lasers at 4 μm with GaSb-ba
 sed type-II quantum wells", <i>Appl. Phys. Lett.</i> <strong>110</strong>, 0
 71104 (2017).</li></ol>
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title => protected'Finley Group' (12 chars)
descriptivename => protected'Semiconductor Nanostructures and Quantum Systems (SNQS)' (55 chars)
description => protected'<p class="text-justify"><strong>Semiconductor Nanostructures and Quantum Sys
 tems (SNQS)</strong></p> <p class="text-justify">A very warm welcome to the
  chair for&nbsp;<strong>Semiconductor Nanostructures and Quantum Systems (SN
 QS)</strong>&nbsp;at the&nbsp;<strong>Walter Schottky Institute</strong>&nbs
 p;of the&nbsp;<strong>Technical University of Munich</strong>. We perform cu
 tting-edge research and teaching in <strong>experimental condensed matter ph
 ysics</strong>, with a particular focus on <strong>emergent quantum material
 s based on semiconductors</strong>, the development of <strong>advanced spec
 troscopic tools</strong>, and the exploration of <strong>novel quantum phase
 s of matter</strong>.</p>
' (709 chars)
description2 => protected'<p class="text-justify"><strong>Quantum Materials &amp; Epitaxy: </strong>We
  synthesise a wide range of quantum nano-materials, including group-III arse
 nide and antimonide semiconductors as well as atomically thin 2D materials.
 Material growth uses molecular beam epitaxy (MBE) systems, equipped with adv
 anced <i>in-situ</i> diagnostics. These include low-temperature optical spec
 troscopy performed inside the UHV environment, enabling real-time characteri
 sation of material properties.</p> <p class="text-justify"><strong>Strongly
  Correlated 2D Quantum Systems: </strong>We explore heterostructures formed
 by stacking van der Waals materials, where strong charge and spin correlatio
 ns lead to rich optical, electronic, and magnetic phenomena. Our research fo
 cuses on probing such correlated quantum states, with the goal of discoverin
 g and exploring new quantum states of matter. &nbsp;</p> <p class="text-jus
 tify"><strong>Quantum Photonics &amp; Light–Matter Interactions: </strong>We
  develop quantum photonic technologies, including sources of entangled photo
 ns for quantum communication and computation. Working closely with the QEC g
 roup led by <a href="https://www.ee.cit.tum.de/qec/home/"><u>Kai Müller at T
 UM-CIT</u></a> we also study fundamental aspects of light–matter interaction
  in such systems. In partnership with <a href="https://munich-quantum-instru
 ments.com/"><u>Munich Quantum Instruments</u></a> GmbH, we work on supercond
 ucting single-photon detectors.</p> <p class="text-justify"><strong>Group-I
 V Quantum Emitters: </strong>We develop hexagonal SiGe quantum heterostructu
 res in an ERC Synergy project with <a href="https://www.tue.nl/en/research/r
 esearch-groups/advanced-nanomaterials-devices"><u>Erik Bakkers (TU Eindhoven
 )</u></a> and <a href="https://www.utwente.nl/en/eemcs/ne/"><u>Floris Zwanen
 burg (University of Twente)</u></a>. Hex-SiGe has a direct bandgap, opening
 exciting possibilities for group-IV nanolasers, quantum light sources, and s
 pin–photon interfaces.</...
' (2399 chars)
description3 => protected'' (0 chars)
description4 => protected'<p>We are always interested to hear from highly motivated undergraduates, Ph
 D-candidates and postdocs who might be interested in joining our laboratorie
 s. Please send an email to <a class="group_submenu" href="mailto:jj.finley@t
 um.de" target="new_mail">Jonathan Finley</a> with a copy of your CV and a br
 ief (10 line) motivation for joining us.</p>
' (348 chars)
description5 => protected'<p>We very gratefully acknowledge third-party funding for the research condu
 cted at SNQS – it supports a lot of talented postdocs, grad and undergraduat
 e students and creates an environment that makes science enjoyable for all o
 f us!</p>
' (237 chars)
description6 => protected'<p>Our funding sources include the German Science Foundation (DFG) via vario
 us individual projects and we are proud members of the DFG Excellence Cluste
 rs (<a href="http://mcqst.de/" target="_blank">MCQST</a>) and <a href="https
 ://www.e-conversion.de/" target="_blank">e-conversion</a>. Other major resea
 rch efforts include the German Federal Ministry of Education and Research (B
 MBF), the European Union (EU) via Horizon 2020 and the Quantum Flagship, the
  Bavarian Science Ministry (ExQM), the Max-Planck-Society (IMPRS), the Inter
 national Graduate school of Science and Engineering (IGSSE), the TUM Institu
 te of Advanced Study (TUM-IAS) and various industrial partners. We were deli
 ghted that Gregor Koblmüller was successful in his application for the prest
 igious ERC Consolidator Grant.</p>
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shortdescription => protected'<p class="text-justify">Superlattices are artificial, periodic potentials wh
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 resulting many-body state can capture essential behaviors of canonical quant
 um many-body theories (e.g. the Hubbard model). Such artificial quasiparticl
 e lattices are often called <strong>analogue</strong> <strong>quantum simula
 tors</strong>. A bit like a quantum wind tunnel, the quantum simulator serve
 s as an engineerable scale model of a real physical system (electrons or oth
 er particles in a real crystalline solid) which allows us to probe complicat
 ed many-body physics with a high level of control. Such many-body physics ar
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 h a periodic array of holes, generating a periodic potential/electric field
 profile in the 2D semiconductor layer which can trap charges. The depth of t
 he superlattice potential can be easily tuned, and any lattice geometry can
 be implemented due to our top-down fabrication approach. We probe the superl
 attice devices using a combination of optical spectroscopy, relying on the n
 atural sensitivity of the optically-active excitons to the correlated behavi
 or of the charges in the superlattice, complemented by charge transport meas
 urements.&nbsp;</p> <p class="text-justify"><br />&nbsp;</p>
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shortdescription => protected'<p>Besides their spectacular optical, spin and electronic properties 2D mate
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 fields that emerge within the unit cell of the crystal. &nbsp;Such ferroelec
 tricity can be controlled by strain &amp; sliding of the component vdW layer
 s of the materials. &nbsp;We explore high-quality 3R-stacked polytypes of TM
 Ds that exhibit out-of-plane ferroelectricity. &nbsp;In 3R-TMD bilayers, sli
 ding one monolayer a few Ångströms over the other flips the ferroelectric po
 larisation, a new ‘slidetronics’ concept in condensed matter physics inspire
 d by twistronics. &nbsp;Such materials are deal for nanoscale systems in whi
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 opportunities for optoelectronics, neuromorphic photonics, and sensing.</p>
 
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shortdescription => protected'<p>The chromium chalcogen halides (CrXH) are an emerging family of 2D semico
 nductors with a direct bandgap, highly anisotropic structural and electronic
  properties, and robust magnetic order with ordering temperatures up to room
  temperature. We seek to understand and engineer interactions between the ma
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title => protected'Van der Waals Materials for Integrated Nanophotonics' (52 chars)
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shortdescription => protected'<p class="text-justify">Integrated quantum photonics is pivotal for the impl
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  a real-life context. A photonic circuit may comprise one or more single pho
 ton sources and diverse components, such as waveguides, beam splitters, inte
 rferometers etc. required for steering and processing the quantum signals pr
 oduced by the sources. In order to insure performance stability, as well as
 to minimise energy consumption, photonic circuits should integrate as many c
 omponents as possible on a same chip. To this respect, a critical hurdle is
 represented by the necessity to assemble different materials that accomplish
  different tasks. In the <a href="https://cordis.europa.eu/project/id/101186
 642">VALERIA project</a> our long term vision is to realise a single-materia
 l photonic platform exploiting the nano-structuring of transition metal dich
 alcogenides. The demonstration of this vision will be the fabrication of all
 -in-one devices made of a single TMD bulk crystal embedding site-controlled
 single photon emitters integrated with photonic crystal cavities and coupled
  to waveguides, beamsplitters amd non linear optical components. &nbsp;</p>
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title => protected'Artificial Molecules as Spin-Photon Interfaces' (46 chars)
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shortdescription => protected'<p>III-V quantum dots (QDs) host ultrastable spin-qubits that can be optical
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  single photons, entangled photon pairs and streams of polarisation entangle
 d photons for quantum photonic technologies. &nbsp;Single spins can create t
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shortdescription => protected'<p>A <strong>quantum transducer</strong> converts quantum information betwee
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 p;Working as part of the <a href="https://www.munich-quantum-valley.de">Muni
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 p;</p>
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shortdescription => protected'<p>Superconducting Nanowire Single-Photon Detectors (SNSPDs) are cutting-edg
 e devices that enable the reliable detection of individual photons. They are
  formed by nano-patterning thin superconducting films to form nanowires wire
 s. &nbsp;When operated at cryogenic temperatures, they deliver unmatched per
 formance for quantum light detection with high efficiency, low noise, phonon
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 ystalline superconducting thin films such as MoSi and NbTiN, as well as emer
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 d apply e.g. local He-ion irradiation to enhance detector performance. &nbsp
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  emergent quantum photonic technologies. &nbsp;&nbsp;</p>
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title => protected'Munich Initiative for Cross-Correlative Spin Microscopy (MICroCoSM)' (67 chars)
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shortdescription => protected'<p>The overarching goal of the <strong>Munich Initiative for Cross-Correlati
 ve Spin Microscopy (MICroCoSM)</strong> is to facilitate the study of nanosc
 ale quantum materials and hybrid quantum systems using the high-resolution -
  and crucially - the multi-modal spectroscopy offered by tip-based nitrogen
 vacancy (NV) quantum sensing. &nbsp;The unique system installed in the labs
 of WSI moves the boundary of the experimental state-of-the-art by enabling <
 i>tip-based, time resolved single spin spectroscopy at low temperatures in h
 igh magnetic fields</i>. &nbsp;This is done using a low-temperature version
 of the <a href="https://qnami.ch/portfolio/proteusq/" title="ProteusQ LM">Pr
 oteusQ </a>scanning NV microscope from <a href="https://qnami.ch" title="Qna
 mi">Qnami</a> as a Spin-based Quantum Light Microscope (SQLM). &nbsp;It prov
 ides nanoscale access to magnetic properties of nano-materials subject to el
 ectrical / optical perturbations. &nbsp;Feel free to reach out to <a href="m
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' (1097 chars)
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shortdescription => protected'<p class="text-justify">The Nanoscale Quantum Magnetometer is a scanning pro
 be microscope based on a single nitrogen vacancy (NV) center implanted in a
 diamond tip. The spin and optical dipole of the NV center can be used to mea
 sure stray electric and magnetic fields with nanoscale spatial resolution an
 d exceptional dynamic range. The overarching goal of this instrument is to e
 nable the study of nanoscale quantum materials and hybrid quantum systems us
 ing the high-resolution - and crucially - the multi-modal spectroscopy offer
 ed by tip-based NV quantum sensing. The unique proposed system moves the bou
 ndary of the experimental state-of-the-art by enabling <i>tip-based, time re
 solved single spin spectroscopy at low temperatures in high magnetic fields<
 /i>. These capabilities are unique but necessary in order to manipulate and
 investigate the spin-and charge configurations of quantum matter. Moreover,
 the instrument has a sophisticated optical design to <i>enable advanced opti
 cal spectroscopy</i> experiments to correlate in real-time the nanoscale NV
 probe measurements with global observables. This project will enable complet
 ely new insight into the challenging but critical phase space from single pa
 rticle interactions to a global quantum phase, and therefore overcomes the m
 ain experimental roadblocks to understand emergence in quantum matter.&nbsp;
 </p>
' (1372 chars)
description => protected'<p class="text-justify">A conventional approach to study many-body systems a
 t the single-particle level would be with a series of specialized scanning t
 ip microscopes, capable of probing many of the most fundamental properties o
 f condensed matter systems, from sample morphology to magnetism, optical con
 ductivity, electronic energy levels, etc. However, this approach requires di
 fferent instruments or at least different probe tips, which practically ofte
 n times bring along incompatible system or sample requirements. <strong>Cruc
 ially, however, the conventional approach is blind to the fact that emergent
  phases are intrinsically linked to all of the above – simultaneously -</str
 ong> and most conventional methods can only probe static properties. Only an
  NV-based system is able to combine all sample properties to fully understan
 d emergence in solids.</p>
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shortdescription => protected'<p>By far the most important chip materials are silicon (Si) and germanium (
 Ge), accounting for ~90% of global demand, and entirely dominating the elect
 ronics industry. Silicon chips could be much faster and more energy efficien
 t if they operated with light. Silicon, germanium, and their alloys do not e
 fficiently emit light in their naturally occurring, cubic, crystal form due
 to their indirect bandgap. &nbsp;However, a newly discovered allotrope of Si
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 ;</p>
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WSI dev: Research overview
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Research at Walter Schottky Institute

The institute research spans a wide range of topics in quantum optics and photonic quantum engineering, nanophotonics and nanoelectronics, photocatalysis and renewable energy conversion, semiconductor optoelectronics and integrated photonics technologies. 

A unifying aspect of the research done in WSI is the use of nanofabrication and nanotechnology to unlock the full potential of solid-state materials for applications. The variety of research topics of individual WSI groups are illustrated in the interactive diagram below. Further details of the groups research can be found at the induvial group pages.