TYPO3\CMS\Extbase\Persistence\Generic\QueryResult prototype object (5 items)
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description => protected '<p>Our research addresses new <strong>semiconductor materials</strong> and n ew <strong>spectroscopic methods</strong> for their characterization. For qu antum information processing, we develop new tools based on magnetic resonan ce which allow to manipulate and detect the spin state of quantum bits via e lectrical transport measurements. As qubits, we in particular study the nucl ear spins of ionized donors, which based on our pioneering work have been de monstrated to have coherence times of the order of an hour at room temperatu re, by far exceeding any other solid-state-based qubit system.</p> ' (598 chars)
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description => protected '<p class="text-justify">Martin Brandt is a Professor at the Walter Schottky Institut and at the Physik-Department of the Technische Universität München in Garching, Germany. After studying physics at Universität Bonn, University of Oxford and TU München, he joined the group of Manuel Cardona at the Max- Planck-Institut für Festkörperforschung and received his Dr. rer. nat. degre e from Universität Stuttgart in 1992. In 1993, he was a postdoc at Xerox Pal o Alto Research Center supported by a Feodor Lynen fellowship of the Alexand er von Humboldt foundation. Also that year, Martin Brandt was awarded the Ot to-Hahn-Medal of the Max-Planck-Society. In 1994, he joined the Schottky Ins titut, where he became Privatdozent in 1999 and was appointed außerplanmäßig er Professor in 2006. His work focuses on the physics and applications of do pants and defects in semiconductors, including silicon, diamond, nitrides an d oxides. The main research tool of his group is magnetic resonance, spearhe ading the development of alternative detection methods such as via electroni c transport measurements to increase the sensitivity of this type of spectro scopy. Martin Brandt has published more than 250 papers, mostly in peer-revi ewed journals, and holds 16 patents. He has been a member of the DFG-funded Collaborative Research Centers 348, 563 and 631 and of the Research Unit 149 3 “Diamond Materials for Quantum Applications”. Furthermore, he was initiato r and member of the Priority Program 1602 “New Frontiers in Sensitivity for EPR Spectroscopy”. Currently, Martin Brandt is a core member of the Munich C enter for Quantum Science and Technology. He is a member of the editorial bo ard of the journal physica status solidi and has served on numerous conferen ce program committees, including chairing the 2016 Gordon Conference on Defe cts in Semiconductors.</p> ' (1850 chars)
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shortdescription => protected 'Photonic and optoelectronic phenomena on the nanometer scale are at the hear t of fundamental science and technology. The institute explores various opto electronic systems. ' (171 chars)
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shortdescription => protected 'In the WSI, we develop new semiconductors, catalytic assemblies, and nanosys tems that are the engines of advanced energy conversion devices. ' (140 chars)
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shortdescription => protected 'Today, we are witnessing a scientific and technological revolution in which information science and quantum mechanics have been united into the common f ield of Quantum Information Science and Technology. We work on building next generation quantum devices and materials and explore their applications ran ging from inherently secure communication and processing of information, to ultrasensitive sensors and transducers for precision metrology. ' (443 chars)
description => protected '<p>Today, we are witnessing a scientific and technological revolution in whi ch information science and quantum mechanics have been united into the commo n field of Quantum Information Science and Technology. We work on building n ext generation quantum devices and materials and explore their applications ranging from inherently secure communication and processing of information, to ultrasensitive sensors and transducers for precision metrology.</p> ' (450 chars)
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<p>Our research in nanofabrication focuses on the precise manipula tion of materials at the atomic and molecular levels. By employing cutting-e dge techniques such as electron and ion beam lithography as well as atomic l ayer deposition, we can create intricate patterns and structures with unprec edented accuracy even down to the single atom level. These techniques allow us to fabricate components that are smaller, faster, and more efficient than ever before.</p> ' (777 chars)
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paragraph2 => protected '<h3>The Center for Nanotechnology and Nanomaterials</h3>
<p>The Walter Scho ttky institute of the TUM operates the Center for Nanotechnologies and Nanom aterials (ZNN), as a shared nanofabrication facility. Students, researchers, and scholars from the greater scientific Munich area have access to state-o f-the-art nanolithography and -analytic instruments for building and charact erizing nanoscale electronic, optoelectronic, and photonic circuits. The nan ofabrication methodologies include ebeam-, focused-ion-beam-, and helium-ion -lithography.</p> ' (549 chars)
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description => protected '<p>Atomic-level control over composition, crystal structure, and defects all ows us to realize functionalities that go beyond the limits of bulk material s. In the WSI, we design and grow a diverse range of nanomaterials, includin g structured III–V semiconductors, (oxy)nitrides, and 2D van der Waals heter ostructures. These low-dimensional and nanoscale systems are created using h ighly precise growth techniques such as MBE, MOCVD, sputtering, ALD, and CVD . Advanced microscopic and spectroscopic characterization provides the criti cal feedback needed to tune interfaces, control disorder, and stabilize meta stable phases over multiple length scales. These engineered building blocks provide the basis for next-generation optoelectronics, quantum devices, sens ors, and energy conversion systems.</p> ' (799 chars)
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description => protected '<p>Our research is focused on developing optoelectronic and integrated photo nics solutions in the mid-infrared (mid-IR, λ ≈ 2.5-30 µm) and terahertz (TH z, λ ≈ 30-300 µm) spectral regions. These spectral regions host numerous wel l-established applications, such as vibrational spectroscopy and microscopy, chemical and biomedical imaging and sensing, free-space communications, ter ahertz imaging and many others. However, most of the present-day mid-IR and THz instrumentation relies on thermal sources or bulky nonlinear optics syst ems, mechanical devices for beam modulation and control, and free-space opti cal setups. We work to facilitate the transition of these bulky systems to c ompact solid-state systems based on widely-tunable electrically-pumped semic onductor light sources, fiber-optics, and integrated photonics platforms. We also exploit opportunities offered by the new mid-IR and THz photonics tech nologies for applications.<br /><br />Many of the devices that we create are based on the concepts of engineered electron quantum states in semiconducto rs, plasmonics, nonlinear optics, metamaterials, and 2D materials. These con cepts are particularly useful in the mid-IR and THz spectral range owing to relaxed fabrication tolerances, low loss of metals, controllable plasmonic a nd nonlinear optical properties of semiconductors and 2D materials, and our ability to engineer intersubband transitions in semiconductor heterostructur es. A combination of novel science, important applications, and the current rudimental state of mid-IR and THz photonics technology (compared to that in near-infrared and visible) provides a fruitful environment for high-impact research.</p>
<p>Please refer to the Research section for the list of curre nt research projects in the Chair.</p> ' (1786 chars)
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researchgroup => protected Dasoe\Wsi\Domain\Model\Researchgroup prototype persistent entity see above (uid=2, pid=80)
role => protected Dasoe\Wsi\Domain\Model\Role prototype persistent entity see above (uid=2, pid=80)
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00000000000017d70000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=139, pid=80)
uid => protected 147 (integer)
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researchgroup => protected Dasoe\Wsi\Domain\Model\Researchgroup prototype persistent entity see above (uid=2, pid=80)
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000000000000179b0000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=140, pid=80)
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researchgroup => protected Dasoe\Wsi\Domain\Model\Researchgroup prototype persistent entity see above (uid=2, pid=80)
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00000000000017620000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=141, pid=80)
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00000000000017330000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=142, pid=80)
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phone => protected '(+49) 089 289 12763 ' (19 chars)
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googlescholar => protected ' ' (0 chars)
arxiv => protected ' ' (0 chars)
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00000000000016d80000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=145, pid=80)
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phone => protected '(+49) 089 289 11373 ' (19 chars)
email => protected 'Marin.Weigel@tum.de ' (19 chars)
tuemail => protected ' ' (0 chars)
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orcid => protected ' ' (0 chars)
googlescholar => protected ' ' (0 chars)
arxiv => protected ' ' (0 chars)
external => protected FALSE
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00000000000016a80000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=146, pid=80)
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researchgroup => protected Dasoe\Wsi\Domain\Model\Researchgroup prototype persistent entity see above (uid=2, pid=80)
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link => protected ' ' (0 chars)
roomnumber => protected 'S111 ' (4 chars)
phone => protected 'Tel.: (+49) 089 289 12763 ' (25 chars)
email => protected 'Xiaoxuan.Ji@wsi.tum.de ' (22 chars)
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orcid => protected ' ' (0 chars)
googlescholar => protected ' ' (0 chars)
arxiv => protected ' ' (0 chars)
external => protected FALSE
showemail => protected FALSE
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000000000000164f0000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=147, pid=80)
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researchgroup => protected Dasoe\Wsi\Domain\Model\Researchgroup prototype persistent entity see above (uid=2, pid=80)
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lastname => protected 'Sergl ' (5 chars)
firstname => protected 'Barbara ' (7 chars)
middlename => protected ' ' (0 chars)
fullname => protected ' ' (0 chars)
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link => protected ' ' (0 chars)
roomnumber => protected 'S320 ' (4 chars)
phone => protected '(+49) 089 289 12789 ' (19 chars)
email => protected 'Barbara.Sergl@wsi.tum.de ' (24 chars)
tuemail => protected ' ' (0 chars)
researcherid => protected ' ' (0 chars)
orcid => protected ' ' (0 chars)
googlescholar => protected ' ' (0 chars)
arxiv => protected ' ' (0 chars)
external => protected FALSE
showemail => protected FALSE
showtuemail => protected FALSE
researchgroups => protected (1 items)
00000000000016140000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=148, pid=80)
uid => protected 156 (integer)
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researchgroup => protected Dasoe\Wsi\Domain\Model\Researchgroup prototype persistent entity see above (uid=2, pid=80)
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lastname => protected 'Rieder ' (6 chars)
firstname => protected 'Markus ' (6 chars)
middlename => protected ' ' (0 chars)
fullname => protected ' ' (0 chars)
title => protected ' ' (0 chars)
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link => protected ' ' (0 chars)
roomnumber => protected 'S320 ' (4 chars)
phone => protected '(+49) 089 289 12789 ' (19 chars)
email => protected ' ' (0 chars)
tuemail => protected ' ' (0 chars)
researcherid => protected ' ' (0 chars)
orcid => protected ' ' (0 chars)
googlescholar => protected ' ' (0 chars)
arxiv => protected ' ' (0 chars)
external => protected FALSE
showemail => protected FALSE
showtuemail => protected FALSE
researchgroups => protected (1 items)
00000000000015d60000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=149, pid=80)
uid => protected 157 (integer)
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researchgroup => protected Dasoe\Wsi\Domain\Model\Researchgroup prototype persistent entity see above (uid=2, pid=80)
role => protected Dasoe\Wsi\Domain\Model\Role prototype persistent entity see above (uid=3, pid=80)
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lastname => protected 'Schmidt ' (7 chars)
firstname => protected 'Simon ' (5 chars)
middlename => protected ' ' (0 chars)
fullname => protected ' ' (0 chars)
title => protected ' ' (0 chars)
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link => protected ' ' (0 chars)
roomnumber => protected 'S320 ' (4 chars)
phone => protected '(+49) 089 289 12789 ' (19 chars)
email => protected ' ' (0 chars)
tuemail => protected ' ' (0 chars)
researcherid => protected ' ' (0 chars)
orcid => protected ' ' (0 chars)
googlescholar => protected ' ' (0 chars)
arxiv => protected ' ' (0 chars)
external => protected FALSE
showemail => protected FALSE
showtuemail => protected FALSE
researchgroups => protected (1 items)
000000000000159d0000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=150, pid=80)
uid => protected 158 (integer)
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researchgroup => protected Dasoe\Wsi\Domain\Model\Researchgroup prototype persistent entity see above (uid=2, pid=80)
role => protected Dasoe\Wsi\Domain\Model\Role prototype persistent entity see above (uid=3, pid=80)
uid => protected 150 (integer)
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researchareas => protected (6 items)
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researcharea => protected Dasoe\Wsi\Domain\Model\Researcharea prototype persistent entity see above (uid=2, pid=79)
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researcharea => protected Dasoe\Wsi\Domain\Model\Researcharea prototype persistent entity see above (uid=3, pid=79)
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weight => protected '0 ' (1 chars)
researcharea => protected Dasoe\Wsi\Domain\Model\Researcharea prototype persistent entity see above (uid=5, pid=79)
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00000000000015480000000000000000 => (uid=28, pid=80)
weight => protected '15 ' (2 chars)
researcharea => protected Dasoe\Wsi\Domain\Model\Researcharea prototype persistent entity see above (uid=6, pid=79)
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000000000000156a0000000000000000 => (uid=29, pid=80)
weight => protected '15 ' (2 chars)
researcharea => protected Dasoe\Wsi\Domain\Model\Researcharea prototype persistent entity see above (uid=4, pid=79)
uid => protected 29 (integer)
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00000000000015220000000000000000 => (uid=30, pid=80)
weight => protected '40 ' (2 chars)
researcharea => protected Dasoe\Wsi\Domain\Model\Researcharea prototype persistent entity see above (uid=1, pid=79)
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topicsets => protected (1 items)
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title => protected 'Our research topics ' (19 chars)
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pid => protected 80 (integer)
researchgroup => protected Dasoe\Wsi\Domain\Model\Researchgroup prototype persistent entity see above (uid=2, pid=80)
topics => protected (4 items)
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title => protected 'Widely-tunable room-temperature THz quantum cascade laser sources ' (65 chars)
image => protected (uid=413, pid=79)
uidLocal => protected 389 (integer)
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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 /> </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 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> ' (479 chars)
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<p class="text-justify">A very warm welcome to the chair for <strong>Semiconductor Nanostructures and Quantum Systems (SN QS)</strong> at the <strong>Walter Schottky Institute</strong>&nbs p;of the <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 & 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. </p>
<p class="text-jus tify"><strong>Quantum Photonics & 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)
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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)
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<p>Following his doctoral studies, Dr. Esmaielpour continued his resea rch career at the Institut Photovoltaïque d’Île-de-France (IPVF) and the Cen tre national de la recherche scientifique (CNRS) in France. There, he explor ed the ultrafast thermalization of hot carriers using advanced optical spect roscopy techniques, gaining critical insights into carrier dynamics and thei r influence on photovoltaic performance. </p>
<p>He was awarded a Mari e Skłodowska-Curie Fellowship and subsequently relocated to the Walter Schot tky Institute. His current research focuses on semiconductor nanowires and q uantum wells grown through molecular beam epitaxy, aimed at advancing quantu m structures for valley-photovoltaic devices. His expertise encompasses non- equilibrium carrier generation and control, ultrafast spectroscopy of nanost ructures, and the epitaxial growth of one- and two-dimensional materials.</p > ' (1369 chars)
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shortdescription => protected '<p>Underlying almost all of the science we do at SNQS is the availability of precise nanostructures created by design using controlled synthesis methods . We employ high-purity molecular beam epitaxy (MBE) dedicated to III-V comp ound semiconductors (group-III arsenides & antimonides), group-III nitri des and, most recently, ultra-pure 2D materials and their heterostructures. Currently, a substantial effort in synthesis is on III-V nanowires (NW), whi ch offer unique capabilities in heterostructure and crystal phase engineerin g, as well as site-selective growth and deterministic incorporation of atomi cally engineered low-dimensional quantum systems.</p> ' (661 chars)
description => protected '<div class="abstract"><p>Underlying almost all of the science we do at SNQS is the availability of precise nanostructures created by design using contro lled synthesis methods. We employ high-purity molecular beam epitaxy (MBE) d edicated to III-V compound semiconductors (group-III arsenides & antimon ides), group-III nitrides and, most recently, ultra-pure 2D materials and th eir heterostructures. Currently, a substantial effort in synthesis is on III -V nanowires (NW), which offer unique capabilities in heterostructure and cr ystal phase engineering, as well as site-selective growth and deterministic incorporation of atomically engineered low-dimensional quantum systems.</p>< /div> ' (689 chars)
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paragraph2 => protected '<p>Underlying almost all of the science we do at SNQS is the availability of precise nanostructures created by design using controlled synthesis methods . We employ high-purity molecular beam epitaxy (MBE) dedicated to III-V comp ound semiconductors (group-III arsenides & antimonides), group-III nitri des and, most recently, ultra-pure 2D materials and their heterostructures. Currently, a substantial effort in synthesis is on III-V nanowires (NW), whi ch offer unique capabilities in heterostructure and crystal phase engineerin g, as well as site-selective growth and deterministic incorporation of atomi cally engineered low-dimensional quantum systems.</p>
<div class="abstract" ><p>Underlying almost all of the science we do at SNQS is the availability o f precise nanostructures created by design using controlled synthesis method s. We employ high-purity molecular beam epitaxy (MBE) dedicated to III-V com pound semiconductors (group-III arsenides & antimonides), group-III nitr ides and, most recently, ultra-pure 2D materials and their heterostructures. Currently, a substantial effort in synthesis is on III-V nanowires (NW), wh ich offer unique capabilities in heterostructure and crystal phase engineeri ng, as well as site-selective growth and deterministic incorporation of atom ically engineered low-dimensional quantum systems.</p></div> ' (1352 chars)
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shortdescription => protected '<p>Semiconductor lasers promise to have improved performance and novel prope rties as their physical size is scaled down to the quantum limit for electro ns and photons. One of the major research directions at SNQS focuses on deve loping high-performance integrated (quantum)photonic and optoelectronic devi ces based on monolithically integrated nanowires (NWs). Specific examples in clude NW-based lasers and non-classical single photon emitters based on NW-Q D devices. Hereby, an important task is to explore the optical and photonic responses of the respective systems using advanced confocal luminescence spe ctroscopy, where e.g. the effects of the quantized electronic structure, lig ht-matter interactions, or the coupling of light to on-chip photonic circuit s are explored.</p> ' (779 chars)
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title => protected 'Strongly Correlated 2D Quantum Systems ' (38 chars)
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shortdescription => protected '<p class="text-justify">Superlattices are artificial, periodic potentials wh ich are used to confined particles and quasiparticles such as atoms, electro ns, or excitons. If the trapped quasiparticles are allowed to interact, the 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 e often hard to describe or predict theoretically, so our quantum simulators provide a route to benchmark leading theories and discover new phases of ma tter beyond current theoretical predictions.</p> ' (960 chars)
description => protected '<p class="text-justify">Our approach to quantum simulation is to create supe rlattices in 2D semiconductors by engineering an artificial electrostatic po tential. This is accomplished by applying a bias voltage between a monolayer semiconductor and a nearby thin graphite layer which has been patterned wit 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. </p>
<p class="text-justify"><br /> </p> ' (897 chars)
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title => protected 'Neuromorphic Photonic Systems ' (29 chars)
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shortdescription => protected '<p>Besides their spectacular optical, spin and electronic properties 2D mate rials can also exhibit ferroelectric order that arises as a consequence of t he stacking order of van-der-Waals (vdW) layered materials and polarisation fields that emerge within the unit cell of the crystal. Such ferroelec tricity can be controlled by strain & sliding of the component vdW layer s of the materials. We explore high-quality 3R-stacked polytypes of TM Ds that exhibit out-of-plane ferroelectricity. 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. Such materials are deal for nanoscale systems in whi ch ferroelectric order can be controlled with light, providing exciting new opportunities for optoelectronics, neuromorphic photonics, and sensing.</p>
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title => protected '2D Magnetic Semiconductors ' (26 chars)
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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 gnetic order in CrXH compounds and the excitons they host. The unique magnet ic and optical properties of CrXH materials present unique opportunities to develop spintronic devices with magnetic and optical controllability.</p> ' (529 chars)
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<p>Duis at sodales sapien. Donec nec justo dictum, vulputate tortor vitae, placerat dui. Pellentesque cursus ultricies mauris rutrum tristique. Nam sit amet leo ut dui tincidunt pretium eget qui s sem. Morbi et nisi tellus. Vestibulum ullamcorper, elit ac sollicitudin bl andit, risus risus egestas mauris, eu sagittis dolor lorem et ligula. Duis o dio purus, rhoncus vitae nisl at, accumsan egestas sem. Aliquam erat volutpa t. Morbi est ipsum, sollicitudin sit amet finibus at, sollicitudin ut purus. Duis varius eget quam a dictum. Cras in eleifend justo. Etiam vel aliquam o dio.</p> ' (1224 chars)
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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 ementation of quantum technologies and their transition from a laboratory to 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. </p> ' (1215 chars)
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title => protected 'Quantum Photonics & Light-Matter Interactions ' (45 chars)
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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 ly addressed. They are used as deterministic and highly efficient sources of single photons, entangled photon pairs and streams of polarisation entangle d photons for quantum photonic technologies. Single spins can create t imed strings of entangled photons. Pairs of tunnel coupled spins in QD-molec ules can be used to generate non-classical states of light with 2D entanglem ent structures needed for measurement based quantum information processing t echnologies. </p> ' (555 chars)
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title => protected 'Quantum Transduction ' (20 chars)
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shortdescription => protected '<p>A <strong>quantum transducer</strong> converts quantum information betwee n different physical systems, such as photons, phonons, or spins. It enables communication across platforms that operate at distinct, and frequently dis parate frequency or energy scales. Such devices are essential for link ing quantum processors to long-distance quantum communication networks. &nbs p;Working as part of the <a href="https://www.munich-quantum-valley.de">Muni ch Quantum Valley</a> project, WSI groups are working on the development of high bandwidth, semiconductor based quantum transducer modules capable of ef ficiently mapping between microwave quantum states of light and photons in t he telecommunications band that can be distributed over optical fibers. &nbs p;</p> ' (766 chars)
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title => protected 'Superconducting Nanowire Single Photon Detectors (SNSPDs) ' (57 chars)
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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. When operated at cryogenic temperatures, they deliver unmatched per formance for quantum light detection with high efficiency, low noise, phonon -number resolution and picosecond photon timing precision. Thanks to their s peed and sensitivity across a wide range of wavelengths spanning the visible to infrared, SNSPDs are a key technology for quantum communication, secure data transfer, advanced imaging, and fundamental scientific research. In the WSI we work closely with <a href="https://munich-quantum-instruments. com" title="Munich Quantum Instruments">Munich Quantum Instruments GmbH</a> and the QEC Group led by <a href="https://www.ee.cit.tum.de/qec/home/" title ="Kai Müller">Kai Müller</a> in the framework of several third-party researc h projects developing the materials technologies for SNSPDs made from polycr ystalline superconducting thin films such as MoSi and NbTiN, as well as emer gent van der Waals superconductors like NbSe<sub>2</sub>. We aim to un derstand the microscopic mechanisms governing the photo-detection process an d apply e.g. local He-ion irradiation to enhance detector performance.   ;Detectors are integrated into quantum photonic circuits with much scope for emergent quantum photonic technologies. </p> ' (1501 chars)
description => protected '<p>Longer Text Description</p> ' (30 chars)
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title => protected 'Quantum Sensing ' (15 chars)
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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. 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>. 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). It prov ides nanoscale access to magnetic properties of nano-materials subject to el ectrical / optical perturbations. Feel free to reach out to <a href="m ailto:jj.finley@tum.de?subject=Interest%20in%20SQLM" title="SQLM">Prof. Finl ey</a> if you are interested!</p> ' (1097 chars)
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title => protected 'Nanoscale quantum magnetometry ' (30 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. </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> ' (862 chars)
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title => protected 'Group-IV Quantum Emitters ' (25 chars)
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title => protected 'Hexagonal Silicon Germanium ' (27 chars)
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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. However, a newly discovered allotrope of Si Ge - <strong>hexagonal SiGe </strong>- efficiently emits light, holding much promise for silicon based classical and quantum photonic technologies.  ;</p> ' (613 chars)
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title => protected 'Holleitner Group ' (16 chars)
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description => protected '<p>Structuring materials with atomic precision is the ultimate goal of nanot echnology and is becoming increasingly relevant as an enabling technology fo r quantum electronics, spintronics, optoelectronics, and photonics, as well as for energy conversion applications. Our chair explores the possibility to structure materials on an atomic level and to explore the fundamental physi cal properties of atomistic 2D materials with a specific focus on semiconduc ting nanomaterials for future information and energy conversion technologies .</p>
<p>We follow four main research directions:</p>
<ul><li><a href="t3: //record?identifier=topic&uid=20"><span>Single-atom circuits</span></a>< /li><li><a href="t3://record?identifier=topic&uid=23"><span>Topological electronics and materials</span></a></li><li><a href="t3://record?identifier =topic&uid=21"><span>Excitonic many-body states towards Bose-Einstein co ndensates</span></a></li><li><a href="t3://record?identifier=topic&uid=2 2"><span>Femtosecond on-chip electronics</span></a></li></ul> ' (1049 chars)
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description7 => protected '<p>We are always looking for interested Bachelor, Master and PhD students. P lease, contact Prof. Holleitner and/or Dr. Kastl for position openings.</p> ' (151 chars)
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title => protected 'DigiQ ' (5 chars)
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0000000000006dfc0000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=77, pid=80)
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00000000000070340000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=183, pid=80)
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title => protected 'Excitonic Many-Body States towards Bose-Einstein Condensates ' (60 chars)
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shortdescription => protected '<p>Increasing the interaction strength between quasi-particles in solid-stat e materials can cause strong correlations, collective phenomena and the tran sition to macroscopic quantum phases, such as a Bose-Einstein condensate. He terostructures made of semiconducting 2D materials, such as MoSe<sub>2</sub> and WSe<sub>2</sub>, are ideal systems to realize interacting exciton ensem bles, because they provide large exciton binding energies, long photolumines cence lifetimes, as well as a permanent exciton dipole. The latter allows th e manipulation of the exciton ensembles, e.g. via electric fields. Recently, we have reported on several signatures regarding photoluminescence intensit y, linewidth, as well as spatial and temporal coherences in accordance with the predicted degeneracy of an exciton ensemble at low temperature. The ongo ing studies want to explore further predicted phases, such as an excitonic s uperfluidity and possible condensation phenomena in momentum space.</p>
<p> Collaborators: Ursula Wurstbauer (University of Münster), Andreas Knorr (TU Berlin).</p> ' (1076 chars)
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shortdescription => protected '<p>We generate optically active defects in atomically thin 2D materials on a spatial scale of below 10 nm, such that scalable opto/electronics based on individual atomic states seems at reach. We use a helium-ion microscope (HIM ) to generate individual defects, e.g. in semiconducting MoS<sub>2</sub>. Ou r single-defect technology is principally applicable to the wide range of 2D materials with more than a thousand different materials and is compatible w ith standard cleanroom manufacturing steps. This combination makes it possib le to realize first devices based on single defects, such as gate-switchable single photon emitters and photodetectors or even solar cells based on indi vidual atomic defects. At the same time, fundamental processes, such as the coherent single electron tunneling dynamics and many-body interactions of lo calized states in a Fermion boson mixture are experimentally accessible.</p>
<p>Collaborators: Jonathan Finley (TUM), Kai Müller (TUM), Nicolas Leither er-Stenger (DTU), Sivan Refaely-Abramson (Weizmann), Alex Weber-Bargioni (Be rkeley)</p> ' (1075 chars)
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shortdescription => protected '<p>We are heading the Center for Nanotechnologies and Nanomaterials (ZNN), w hich is a shared nanofabrication facility of the Walter Schottky Institute o f TUM. Students, researchers, and scholars from the greater scientific Munic h area have access to state-of-the-art nanolithography and nanoanalytic inst ruments for building nanoscale electronic, optoelectronic, and photonic circ uits. The methodologies include electron beam-, focused-ion-beam-, and heliu m-ion-beam lithography.</p> ' (483 chars)
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title => protected 'Towards femtosecond on-chip electronics ' (39 chars)
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shortdescription => protected '<p>The vision of this research topic is to generate electric current pulses with a duration of only a few femtoseconds for an on-chip signal conversion at the interface between electronics and optics, the so-called THz-gap. For signal generation we use amongst others, photo-emission processes, such as m ultiphoton absorption and strong field tunnel processes in plasmonic nanocon tacts; but also femtosecond processes within solid state materials. The sign al propagation occurs via electromagnetic THz modes in coplanar strip conduc tors. For the on-chip THz-detection, we are working on an electrical detecti on on the 100 fs scale and faster. Currently we reach 350 fs by using the re laxation dynamics in amorphous silicon photo-switches. Our group manufacture s all circuits in our own laboratory, and we use phase-stable femtosecond la sers to drive the on-chip THz circuits coherently. Intriguingly, atomically thin 2D materials can be integrated into the THz circuits without much effor t, such that the 2D materials can act as functional THz modulators. In the s ame way, the electron and heat dynamics in the 2D materials can be investiga ted on a femto- to picosecond timescale.</p>
<p>Collaborator: Reinhard Kien berger (TUM).</p> ' (1233 chars)
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title => protected 'Topological electronics and materials ' (37 chars)
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shortdescription => protected '<p>Topological materials are very promising for future opto/electronic circu its, since computing schemes can be envisaged where e.g. information-carryin g surface states are protected by topology. Van der Waals materials and thei r heterostructure are an ideal platform to engineer and explore topological states. On the one hand, one can control and break the relevant symmetries o f the Hamiltonian at will by interfacing different van der Waals materials w ith different symmetries. On the other hand, we can directly address the sym metry of the electron-Bloch states in the van der Waals crystal e.g. by exte rnal electric fields. In our research, we explore a wide range of non-trivia l, i.e. topological quantum phenomena. The research is headed by Dr. Christo ph Kastl.</p>
<p>Collaborator: Marko Burghard (MPI Stuttgart).</p> ' (827 chars)
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description => protected '<p>Understanding and controlling the interaction of light, charge, and mater ials at the atomic scale is key to developing the next generation of sustain able energy technologies. To address these challenges, we design and develop advanced semiconducting materials and functional interfaces, with a focus o n thin films and their heterostructures for solar energy conversion, electro catalysis, and optoelectronics. Through our research, we aim to un cover and direct optical excitations, charge carrier transport mechanis ms, and interfacial dynamics. To gain new insights into these fund amental processes, we combine advanced deposition methods, includi ng reactive sputtering, atomic layer deposition, and molecular beam epitaxy, with a comprehensive suite of (in situ) structural, ele mental, and optoelectronic characterization tools. This integrated approach enables us to interrogate and guide complex light-to-charge and charge- to-chemical transformation pathways that underlie the functional characteris tics of emerging optoelectronic and energy conversion systems.</p> ' (1130 chars)
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An Initiative of the Bayerisches Sta atsministerium für Wissenschaft und Kunst ' (117 chars)
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phone => protected ' ' (0 chars)
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0000000000005c770000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=110, pid=80)
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0000000000005d2f0000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=114, pid=80)
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email => protected 'Julius.Kuehne@wsi.tum.de ' (24 chars)
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0000000000005e290000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=119, pid=80)
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researchgroup => protected Dasoe\Wsi\Domain\Model\Researchgroup prototype persistent entity see above (uid=9, pid=80)
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phone => protected '+49 89 289 12752 ' (16 chars)
email => protected 'sonja.matich@wsi.tum.de ' (23 chars)
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0000000000005e3f0000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=120, pid=80)
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researchgroup => protected Dasoe\Wsi\Domain\Model\Researchgroup prototype persistent entity see above (uid=9, pid=80)
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orcid => protected '0009-0007-7386-1011 ' (19 chars)
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0000000000005e970000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=121, pid=80)
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roomnumber => protected ' ' (0 chars)
phone => protected '+49 89 289 12889 ' (16 chars)
email => protected 'saswati.santra@wsi.tum.de ' (25 chars)
tuemail => protected 'saswati.santra@tum.de ' (21 chars)
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orcid => protected '0000-0003-0327-0279 ' (19 chars)
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0000000000005ead0000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=122, pid=80)
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researchgroup => protected Dasoe\Wsi\Domain\Model\Researchgroup prototype persistent entity see above (uid=9, pid=80)
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phone => protected '+49 89 289 12738 ' (16 chars)
email => protected 'Nick.Schroeder@wsi.tum.de ' (25 chars)
tuemail => protected 'Nick.Schroeder@tum.de ' (21 chars)
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orcid => protected ' ' (0 chars)
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arxiv => protected ' ' (0 chars)
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0000000000005ee70000000000000000 => Dasoe\Wsi\Domain\Model\Pgroupconnection prototype persistent entity see above (uid=123, pid=80)
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researchgroup => protected Dasoe\Wsi\Domain\Model\Researchgroup prototype persistent entity see above (uid=9, pid=80)
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roomnumber => protected 'S309 ' (4 chars)
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shortdescription => protected '<p>While 2D semiconductors offer unique electronic and optical properties, r ealization of their full potential requires scalable growth and controlled i ntegration into functional assemblies. In our research, we aim to create def ined 2D/3D heterostructures using chemical vapor deposition (CVD) of transit ion metal dichalcogenides (TMDs) onto engineered substrates. These heterostr uctures include thin film junctions and laterally patterned substrates that enable precise spatial control of the 2D material and its electronic environ ment. In addition, we take advantage of low-temperature atomic layer deposit ion (ALD) processes to precisely tune interaction lengths and strengths betw een TMDs and their surroundings. A major emphasis of this work on 2D semicon ductor assemblies is devoted to elucidating interfacial mechanisms that gove rn charge transfer pathways, energetic alignment, and structural and chemica l interactions, providing a basis for future applications spanning from adva nced optoelectronics to photocatalytic energy conversion.</p> ' (1049 chars)
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title => protected 'Discovery and development of advanced thin film semiconductors ' (62 chars)
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shortdescription => protected '<p>Thin film semiconductors based on nitrides, oxynitrides, and oxides serve as versatile platforms for tailoring electronic and optical properties of m aterials. By leveraging advanced deposition techniques, such as reactive spu tter deposition, molecular beam epitaxy, and solution-based processing, we e xplore novel material compositions with precisely controlled structures. A k ey focus of our research is the comprehensive characterization of these mate rials, including their elemental composition and atomic bonding environments , electronic structures, and excited state characteristics using a combinati on of lab- and synchrotron-based techniques. With this suite of complementar y experimental tools, we investigate defects, doping strategies, and charge transport dynamics to understand and tune optical and electronic properties. These insights are crucial for controlling the functional properties of the se materials for applications that include photoelectrochemical energy conve rsion, solar cells, and sustainable electronic devices. </p> ' (1053 chars)
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title => protected 'In situ & operando spectroscopy at reactive interfaces ' (54 chars)
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shortdescription => protected '<p>To unlock the full potential of functional materials, it is essential to study their properties under realistic operating conditions. Our research fo cuses on the development of in situ and operando spectroscopic techniques th at provide real-time insights into the structural, electronic, and chemical dynamics of thin films, electrocatalysts, and semiconductor systems. In part icular, we employ near-ambient pressure X-ray photoelectron spectroscopy (NA P-XPS) to probe surface chemistry in reactive environments, transient absorp tion spectroscopy (TAS) to track charge carrier and electrochemical dynamics , Fourier-transform infrared (FTIR) spectroscopy to monitor molecular vibrat ions and reaction intermediates, and Raman spectroscopy to analyze structura l transformations of materials driven away from equilibrium. These technique s allow us to correlate key energy conversion performance metrics with the e lectronic structure, defect states, and reaction mechanisms in dynamic envir onments. Our approach bridges fundamental materials science with innovative energy conversion concepts, enabling the design of more efficient and stable energy materials.</p> ' (1162 chars)
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title => protected 'Tailored (photo)electrochemical interfaces ' (42 chars)
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shortdescription => protected '<p>The performance of advanced energy materials is critically determined by their interfaces. In (photo)electrochemical systems, efficient charge transf er relies on the precise design of both solid-solid and solid-liquid interfa ces. Our research focuses on tailoring these interfaces at the atomic- and n anoscale to precisely guide efficient energy conversion processes. A key asp ect of this research is based on the alignment of energy levels at heterojun ctions, which governs selective charge injection and extraction. In addition , we investigate semiconductor-liquid junctions, where interfacial electric fields and surface states play a crucial role in dictating reaction kinetics . Beyond material properties, we study how microenvironments around electroc atalysts – including local pH, ion distribution, and solvation effects – can influence reaction selectivity. These insights are applied to the developme nt of materials for sustainable generation of chemicals from sunlight, with tailored interfacial properties enabling accelerated charge transfer, enhanc ed reaction selectivity, and improved conversion efficiency.</p> ' (1128 chars)
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title => protected 'Ultrathin functional materials via atomic layer deposition ' (58 chars)
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shortdescription => protected '<p>From tunable dielectrics integrated into nanoscale electronic devices to multifunctional coatings that promote efficient solar-to-chemical energy con version, we make extensive use of atomic layer deposition (ALD) to precisely engineer interfaces, design novel heterostructures, and introduce defined f unctionalities at surfaces. Within this research, we develop novel ALD proce sses and materials, guided by in situ spectroscopic ellipsometry and mass sp ectrometry that offer real-time insights into nucleation dynamics, growth ki netics, defect formation, and film properties. Moving beyond traditional app roaches, we explore advanced ALD strategies by, for example, integrating pla sma-surface interactions to tune interfacial chemical and electronic propert ies, introducing external stimuli to achieve area-selective growth, and tail oring reaction conditions to shape nanoscale morphologies. By advancing ALD- based methods for precise interface and material control, our work contribut es to the development of next-generation electronic, energy, and catalytic s ystems in which nanoscale structure-property relationships are critical.</p> ' (1140 chars)
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