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description => protected'<p class="text-justify">Martin Brandt is a Professor at the Walter Schottky
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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
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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
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Belkin Group
Welcome to the Chair of Semiconductor Technology!
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nics solutions in the mid-infrared (mid-IR, λ ≈ 2.5-30 µm) and terahertz (TH
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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
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s to achieve specific functionality and explore interactions where solid mat
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ques such as electron beam lithography, atomic layer deposition, and nanoimp
rint lithography, we can create intricate patterns and structures with unpre
cedented accuracy even down to the single atom level. These techniques allow
us to fabricate components that are smaller, faster, and more efficient tha
n ever before. </p>
<p>Nanofabrication is a cornerstone of modern semi
conductor technology, enabling the creation of devices and structures at the
nanometer scale. The research is crucial for the advancement of various tec
hnologies, including micro- and nanoelectronics, photonics, energy conversio
n and quantum computing. We are dedicated to pushing the boundaries of nanof
abrication to develop innovative solutions that address the corresponding ch
allenges of the future.</p>
<p>At our institute, we are committed to advanc
ing the field of nanofabrication through interdisciplinary collaboration and
cutting-edge research. Our work not only contributes to the scientific comm
unity but also has a profound impact on industry and society. By training th
e next generation of scientists and engineers, we are ensuring that the inno
vations of today will lead to the technological breakthroughs of tomorrow.</
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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
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ofabrication methodologies include ebeam-, focused-ion-beam-, and helium-ion
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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)
description => protected'<p>Photonic and optoelectronic phenomena on the nanometer scale are at the h
eart of fundamental science and technology. The institute explores various o
ptoelectronic systems.</p>' (178 chars)
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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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000000000000149d0000000000000000 => Dasoe\Wsi\Domain\Model\Topicprototypepersistent entity (uid=33, pid=79)
title => protected'Integrated mid-infrared photonics' (33 chars)
image => protectedTYPO3\CMS\Extbase\Domain\Model\FileReferenceprototypepersistent entitymax depth (uid=359, pid=79)
link => protected'' (0 chars)
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)
image2 => protectedTYPO3\CMS\Extbase\Persistence\ObjectStorageprototypeobjectmax depth (2 items)
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)
institution => protectedTYPO3\CMS\Extbase\Persistence\ObjectStorageprototypeobjectmax depth (empty)
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00000000000014510000000000000000 => Dasoe\Wsi\Domain\Model\Topicprototypepersistent entity (uid=34, pid=79)
title => protected'Quantum-engineered nonlinear metamaterials' (42 chars)
image => protectedTYPO3\CMS\Extbase\Domain\Model\FileReferenceprototypepersistent entitymax depth (uid=362, pid=79)
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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)
image2 => protectedTYPO3\CMS\Extbase\Persistence\ObjectStorageprototypeobjectmax depth (1 items)
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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00000000000013ef0000000000000000 => Dasoe\Wsi\Domain\Model\Topicprototypepersistent entity (uid=35, pid=79)
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)
image2 => protectedTYPO3\CMS\Extbase\Persistence\ObjectStorageprototypeobjectmax depth (2 items)
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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title => protected'Finley Group' (12 chars)
descriptivename => protected'Semiconductor Nanostructures and Quantum Systems (SNQS)' (55 chars)
description => protected'<p>Mi, nia sit, ex ex et arum ideliquis apel erum quod esed ut ut aliquosae
sinvel moluptas consedit volore culparum ad que rendionest quisitatet aborat
endis et aliberum facea is as susam iume vellitaquis sim untum ressit maximu
s rem. Itas consent quas cus qui aut liqui archicae volut re as autemped qua
turitas voluptatet, ulles et omnita nonsequo qui blaboriam ut rerepre ommolu
ptur, idit hit fugia coresci aspelles utatusda nis expla</p>' (440 chars)
description2 => protected'<p>Researchers at SNQS currently explore a wide-range of research themes in
condensed matter physics, including <br /> </p>
<ol><li><i><stron
g>Growth and Functional Properties of Ultrapure Nanomaterials:</strong> III-
V semiconductor nanostructures (nanowires, QD-nanostructures), 2D-nanomateri
als and diamond grown using methods such as MBE and CVD.</i></li><li><i><str
ong>Heterostructures of 2D-Materials:</strong> two-dimensional materials suc
h as graphene, transition metal dichalcogenides and layered perovskites and
the exploration of their novel optical, electronic and magnetic properties.<
/i></li><li><i><strong>Quantum-Photonics*:</strong> quantum spin-systems in
III-V semiconductors and diamond and their use for quantum technologies.</i>
</li><li><i><strong>Photonic Nanomaterials*:</strong> understanding and cont
rolling light-matter-interactions by engineering materials to trap, route an
d focus light at the nanoscale.</i></li><li><i><strong>Quantum Sensing:</str
ong> development of quantum sensors with a particular focus on applications
in the life-sciences and ultra-sensitive photon detection at the quantum lim
it.</i></li></ol>
<p><br />*SNQS collaborates closely with the <a href="htt
ps://www.wsi.tum.de/views/groups.php?group=Mueller">Photonic Quantum Enginee
ring</a> group at <a href="https://www.ei.tum.de/en/welcome/" target="_new"
rel="nofollow">TUM-ECE</a> led by <a href="https://www.wsi.tum.de/views/user
.php?user=180113077">Kai Müller</a>.</p>' (1484 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:jonathan.fi
nley@wsi.tum.de" target="new_mail">Jonathan Finley</a> with a copy of your C
V and a brief (10 line) motivation for joining us.</p>' (358 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>' (794 chars)
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shortdescription => protected'In the WSI, we develop new semiconductors, catalytic assemblies, and nanosys
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shortdescription => protected'We aim at structuring materials down to the atomic level or to dimensions sp
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shortdescription => protected'Photonic and optoelectronic phenomena on the nanometer scale are at the hear
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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
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des and, most recently, ultra-pure 2D materials and their heterostructures.
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description => protected'<div class="abstract"><p>Underlying almost all of the science we do at SNQS
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<div class="abstract"
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shortdescription => protected'<p>Semiconductor lasers promise to have improved performance and novel prope
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ns and photons. One of the major research directions at SNQS focuses on deve
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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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shortdescription => protected'<p>The optical properties of 2D transition-metal dichalcogenides (TMDs) such
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um number. Because 2D materials are so thin materials directly adjacent to t
he TMD layer can influence spin and magneto-optical properties. SNQS researc
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citonic-excitations in TMDs? How does the dielectric / magnetic / topologica
l environment influence the excitons?</p>' (573 chars)
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shortdescription => protected'<p>Localized excitons in 2D materials have shown to be sources of non-classi
cal light. SNQS researchers follow three avenues for exciton localization: (
i) dielectric engineering, (ii) strain-induced exciton localization and (iii
) site-selective generation of native defects via He-ion irradiation. Our go
als are to understand the mechanisms of localization for couple light from s
uch localized emitters into photonic structures and explore interesting phas
es of interacting excitations in defined trapping potentials. Here, we work
closely with the Ultrafast Optoelectronics group led by <a href="https://www
.wsi.tum.de/views/sub_group.php?group=Holleitner">Alexander Holleitner</a> a
t WSI, the <a href="https://www.wsi.tum.de/views/groups.php?group=sharp">Exp
erimental Semiconductor Physics</a> group led by <a href="https://www.wsi.tu
m.de/views/user.php?user=180113215">Ian Sharp</a> and the <a href="https://w
ww.wsi.tum.de/views/groups.php?group=Mueller">Photonic Quantum Engineering</
a> group at TUM-ECE led by <a href="https://www.wsi.tum.de/views/user.php?us
er=180113077">Kai Müller</a>.</p>' (1097 chars)
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title => protected'Novel heterostructures with 2D perovskites' (42 chars)
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shortdescription => protected'Similar to conventional III-V semiconductor superlattices, Ruddlesden-Popper
halide perovskites are quantum well-like structures formed by two-dimension
al layers of halide perovskites semiconductors, separated by organic spacer
layers. This layered structure can be tuned by varying the perovskite layer
thickness and the composition of the organic layer. Although efficient opto-
electronic devices were made from such materials, fundamental questions conc
erning the nature of optical resonances remain. SNQS researchers strive to u
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ontrolled, especially when they are combined with other 2D-materials.' (677 chars)
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title => protected'Quantum optics and spin-photon interfaces in single and coupled-QDs' (67 chars)
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shortdescription => protected'<p>SNQS researchers investigate quantum optical methods to prepare, manipula
te and readout optically active quantum spin-states in semiconductor QDs. Du
e to their strong optical transitions with almost transform-limited linewidt
h, QDs are ideal prototypes for solid-state quantum emitters. Among our curr
ent experiments are resonance fluorescence investigations of quantum optical
properties of QDs, investigations of the complex <a href="https://www.wsi.t
um.de/views/user.php?user=180113106">dynamics</a> of single electron and hol
e spins confined to QDs and the use of QD-molecules for solid-state quantum
repeaters. SNQS works closely with the <a href="https://www.wsi.tum.de/views
/groups.php?group=Mueller">Photonic Quantum Engineering</a> group at TUM-ECE
led by <a href="https://www.wsi.tum.de/views/user.php?user=180113077">Kai M
üller</a>.</p>' (850 chars)
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äußerlich den Spitzmäusen. Allen Maulwürfen ist ein dichtes Fell mit überwie
gend dunkler Fellfarbe zu eigen. Bis auf die Spitzmausmaulwürfe haben die
meisten Vertreter keine äußerlich sichtbaren Ohren ausgebildet, die ebenso w
ie die Augen häufig verkümmert sind. Eine Besonderheit stellen die Eimersc
hen Organe als feinfühliges Tastwerkzeug dar. – <a href="https://de.w
ikipedia.org/wiki/Maulw%C3%BCrfe" title="Maulwürfe"><i>Zum Artikel …</i
></a></p>' (1605 chars)
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Die Tiere besitzen vielfältige Anpassungen an untersch
iedliche Lebensweisen. Dementsprechend variabel ist auch ihr äußeres Ersc
heinungsbild. Allgemein kennzeichnend sind ein walzen- bis spindelförmige
r Körper mit kurzem Hals, auf dem ein spitz zulaufender Kopf sitzt. Die mei
sten Arten, so die Eurasischen Maulwürfe und die Neuweltmaulwürfe' (371 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
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ging from inherently secure communication and processing of information, to
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description => protected'<p>Controlling how materials interact with complex environments enables adva
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otosynthesis. In the WSI, we create hybrid organic/inorganic interfaces, sem
iconductor/electrolyte junctions, and engineered solid state heterostructure
s to achieve specific functionality and explore interactions where solid mat
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shortdescription => protected'In the WSI, we develop new semiconductors, catalytic assemblies, and nanosys
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description => protected'<p>In the WSI, we develop new semiconductors, catalytic assemblies, and nano
systems that are the engines of advanced energy conversion devices.</p>' (147 chars)
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shortdescription => protected'We aim at structuring materials down to the atomic level or to dimensions sp
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description => protected'<p>Our research in nanofabrication focuses on the precise manipulation of ma
terials at the atomic and molecular levels. By employing cutting-edge techni
ques such as electron beam lithography, atomic layer deposition, and nanoimp
rint lithography, we can create intricate patterns and structures with unpre
cedented accuracy even down to the single atom level. These techniques allow
us to fabricate components that are smaller, faster, and more efficient tha
n ever before. </p>
<p>Nanofabrication is a cornerstone of modern semi
conductor technology, enabling the creation of devices and structures at the
nanometer scale. The research is crucial for the advancement of various tec
hnologies, including micro- and nanoelectronics, photonics, energy conversio
n and quantum computing. We are dedicated to pushing the boundaries of nanof
abrication to develop innovative solutions that address the corresponding ch
allenges of the future.</p>
<p>At our institute, we are committed to advanc
ing the field of nanofabrication through interdisciplinary collaboration and
cutting-edge research. Our work not only contributes to the scientific comm
unity but also has a profound impact on industry and society. By training th
e next generation of scientists and engineers, we are ensuring that the inno
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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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shortdescription => protected'In the WSI, we develop new semiconductors, catalytic assemblies, and nanosys
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title => protected'Nanophotonics and Optoelectronics' (33 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)
description => protected'<p>Photonic and optoelectronic phenomena on the nanometer scale are at the h
eart of fundamental science and technology. The institute explores various o
ptoelectronic systems.</p>' (178 chars)
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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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title => protected'Single-atom circuits' (20 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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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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