Starke Licht-Materie-Wechselwirkung in Halbleiter-Mikroresonatoren führt zur Ausbildung von Eigenmoden mit gemischtem Licht-Materie-Charakter, die als Polaritonen bezeichnet werden. Die besonderen Eigenschaften dieser bosonischen Quasiteilchen können zur Realisierung neuartiger Bauteile genutzt werden, wie etwa des Polariton-Lasers, der auf stimulierter Streuung beruht anstatt auf stimulierter Emission, durch die Photon-Lasing ausgelöst wird. Durch den direkten Zugang zu Polariton-Zuständen in spektroskopischen Experimenten, sowie durch die Möglichkeit mit vielfältigen Mitteln nahezu beliebige Potentiallandschaften definieren zu können, eröffnen sich zahlreiche weitere Anwendungsgebiete, etwa in der Quantensimulation bzw. -emulation. Mittels externer elektrischer und magnetischer Felder können Erkenntnisse über Polaritonen gewonnen werden, die in rein optischen Experimenten nicht zugänglich sind. Durch die Felder, die nicht mit rein photonischen Moden wechselwirken, kann auf den Materie-Anteil der Hybridmoden zugegriffen werden. Weiterhin können die Felder zur in-situ Manipulation der Polariton-Energie genutzt werden, was für die Erzeugung dynamischer Potentiale relevant werden könnte. Der Fokus dieser Arbeit liegt daher auf der Betrachtung verschiedener Phänomene der Licht-Materie-Wechselwirkung unter dem Einfluss äußerer Felder. Dazu wurden auf das jeweilige Experiment abgestimmte Strukturen und Bauteile hergestellt und in magneto-optischen oder elektro-optischen Messungen untersucht. Um elektrische Felder entlang der Wachstumsrichtung anlegen zu können, d.h. in vertikaler Geometrie, wurden dotierte Resonatoren verwendet, die mit elektrischen Kontakten auf der Probenoberfläche und -rückseite versehen wurden. In diesen Bauteilen wurde die Energieverschiebung im elektrischen Feld untersucht, der sogenannte Stark-Effekt. Dieser im linearen Regime bereits mehrfach demonstrierte Effekt wurde systematisch auf den nichtlinearen Bereich des Polariton-Lasings erweitert. Dabei wurde besonderes Augenmerk auf die Probengeometrie und deren Einfluss auf die beobachteten Energieverschiebungen gelegt. Die Untersuchungen von Proben mit planarer, semi-planarer und Mikrotürmchen-Geometrie zeigen, dass ein lateraler Einschluss der Ladungsträger, wie er im Mikrotürmchen erzielt wird, zu einer Umkehrung der Energieverschiebung führt. Während in dieser Geometrie mit zunehmender Feldstärke eine Blauverschiebung des unteren Polaritons gemessen wird, die durch Abschirmungseffekte erklärt werden kann, wird in planarer und semi-planarer Geometrie die erwartete Rotverschiebung beobachtet. In beiden Fällen können, je nach Verstimmung, Energieverschiebungen im Bereich von einigen hundert µeV gemessen werden. Die gemessenen Energieverschiebungen zeigen gute Übereinstimmung mit den Werten, die nach einem Modell gekoppelter Oszillatoren berechnet wurden. Weiterhin werden vergleichbare Energieverschiebungen unter- und oberhalb der Schwelle zum Polariton-Lasing beobachtet, sodass der Polariton-Stark-Effekt als eindeutiges Merkmal erachtet werden kann, anhand dessen optisch angeregte Polariton- und Photon-Laser eindeutig unterschieden werden können. Wird das elektrische Feld nicht entlang der Wachstumsrichtung angelegt, sondern senkrecht dazu in der Ebene der Quantenfilme, dann kommt es schon bei geringen Feldstärken zur Feldionisation von Elektron-Loch-Paaren. Um diese Feldgeometrie zu realisieren, wurde ein Verfahren entwickelt, bei dem Kontakte direkt auf die durch einen Ätzvorgang teilweise freigelegten Quantenfilme eines undotierten Mikroresonators aufgebracht werden. Durch das Anlegen einer Spannung zwischen den lateralen Kontakten kann die Polariton-Emission unterdrückt werden, wobei sich die Feldabhängigkeit der Polariton-Besetzung durch ein Modell gekoppelter Ratengleichungen reproduzieren lässt. Die neuartige Kontaktierung erlaubt es weiterhin den Photostrom in den Quantenfilmen zu untersuchen, der proportional zur Dichte freier Ladungsträger ist. Dadurch lässt sich zeigen, dass die zwei Schwellen mit nichtlinearem Anstieg der Emission, die in derartigen Proben häufig beobachtet werden, auf grundsätzlich verschiedene Verstärkungsmechanismen zurückgehen. An der zweiten Schwelle wird ein Abknicken des leistungsabhängigen Photostroms beobachtet, da dort freie Ladungsträger als Reservoir des Photon-Lasings dienen, deren Dichte an der Schwelle teilweise abgeklemmt wird. Die erste Schwelle hingegen, die dem Polariton-Lasing zugeordnet wird, hat keinen Einfluss auf den linear mit der Anregungsleistung ansteigenden Photostrom, da dort gebundene Elektron-Loch-Paare als Reservoir dienen. Mittels angepasster Ratengleichungsmodelle für Polariton- und Photon-Laser lässt sich der ermittelte Verlauf der Ladungsträgerdichte über den gesamten Leistungsbereich qualitativ reproduzieren. Abschließend wird durch ein magnetisches Feld der Einfluss der Licht-Materie-Wechselwirkung auf die Elektron-Loch-Bindung im Regime der sehr starken Kopplung beleuchtet. Durch die Messung der diamagnetischen Verschiebung wird der mittlere Elektron-Loch-Abstand von unterem und oberem Polariton für zwei Resonatoren mit unterschiedlich starker Licht-Materie-Wechselwirkung bestimmt. Bei geringer Kopplungsstärke werden die Hybridmoden in guter Näherung als Linearkombinationen der ungekoppelten Licht- und Materie-Moden beschrieben. Für den Resonator mit großer Kopplungsstärke wird eine starke Asymmetrie zwischen unterem und oberem Polariton beobachtet. Die diamagnetische Verschiebung des oberen Polaritons steigt mit zunehmender Verstimmung auf bis etwa 2,1 meV an, was fast eine Größenordnung über der Verschiebung des unteren Polaritons (0,27 meV) bei derselben Verstimmung liegt und die Verschiebung des ungekoppelten Quantenfilms um mehr als den Faktor 2 übersteigt. Das bedeutet, dass das untere Polariton durch eine Wellenfunktion beschrieben wird, dessen Materie-Anteil einen verringerten mittleren Elektron-Loch-Abstand aufweist. Im oberen Polariton ist dieser mittlere Radius deutlich größer als der eines Elektron-Loch-Paars im ungekoppelten Quantenfilm, was sich durch eine von Photonen vermittelte Wechselwirkung mit angeregten und Kontinuumszuständen des Quantenfilms erklären lässt. / Strong light-matter interaction in semiconductor microcavities leads to the formation of eigenmodes with mixed light-matter characteristics, so-called polaritons. The unique properties of these bosonic quasiparticles may be exploited to realize novel devices, such as polariton-lasers which rely on stimulated scattering instead of stimulated emission, which in turn triggers photon-lasing. Polariton states are directly accessible in spectroscopic experiments and can be subjected to almost arbitrary potential landscapes which could lead to numerous applications, for instance in quantum simulation or emulation. External electric and magnetic fields can be used to gain insights into polaritons that are not available in all-optical experiments. The matter part of the hybrid modes is accessed by the external fields that do not interact with purely photonic modes. Furthermore, in-situ manipulation of the polariton energy by external fields could be used to create dynamic potentials. This thesis is therefore focussed on studying different aspects of light-matter coupling under the influence of external fields. To this end, structures and devices tailored to the specific experiments were fabricated and investigated in electro-optical or magneto-optical measurements. Doped microcavities with electrical contacts on the sample surface and back side were used to apply electric fields along the growth direction, i.e. in vertical geometry. The energy shift in an electric field, the so-called Stark effect, was investigated in these devices. In this work, measurements of the polariton Stark effect, which has previously been demonstrated in the linear regime, were systematically extended to the nonlinear regime of polariton-lasing with special attention paid to the sample geometry and its influence on the observable energy shifts. Investigations of samples with planar, semi-planar and micropillar geometries show that lateral carrier confinement in a micropillar leads to an inversion of the energy shift. While in this geometry a blueshift with increasing field strength is measured, which can be explained by screening effects, the expected redshift is restored in planar and semi-planar geometries. In both cases, detuning-dependent energy shifts of up to hundreds of µeV are observed in good agreement with values calculated with a model of coupled harmonic oscillators. Furthermore, comparable shifts below and above the polariton-lasing threshold are observed both in the semi-planar and in the micropillar geometry. The polariton Stark effect may therefore be considered as criterion to unambiguously distinguish optically excited polariton- and photon-lasers. If the electric field is not oriented along the growth direction but perpendicular to it, i.e. in the plane of the quantum wells, then field ionization of electron-hole pairs occurs already at low field strengths. To realize this field geometry, a process was developed to deposit electrical contacts directly onto the quantum wells of an undoped microcavity which are partially exposed in an etching step. The polariton emission can be suppressed by applying voltage to the lateral contacts and the dependency of the polariton occupation upon the electric field is reproduced using a set of coupled rate equations. This novel contacting technique furthermore allows to measure the photocurrent in the quantum wells which is proportional to the free carrier density. The two thresholds of nonlinear emission, which are commonly observed in similar samples, can then be shown to rely on fundamentally different gain mechanisms. A kink in the power dependence of the photocurrent is observed at the second threshold, where free carriers act as reservoir for photon-lasing which is why their density is partially clamped at threshold. The first threshold on the other hand, which is attributed to polariton-lasing, has no influence on the linear increase of the photocurrent with increasing excitation power, since there bound electron-hole pairs act as reservoir. The experimentally determined power dependence of the photocurrent is reproduced qualitatively over the whole range of excitation powers using adapted rate equation models for polariton- and photon-lasers. Finally, a magnetic field is used to reveal the impact of light-matter interactions on electron-hole coupling in the regime of very strong coupling. By measuring the diamagnetic shift, the average electron-hole separations of lower and upper polariton are determined for two microcavities with different light-matter coupling strengths. At small coupling strength, describing the hybrid modes as linear combinations of uncoupled light and matter modes is a valid approximation. At large coupling strength, significant asymmetries between lower and upper polariton are observed. With increasing detuning, the upper polariton diamagnetic shift increases up to 2.1 meV, almost an order of magnitude larger than the lower polariton shift (0.27 meV) at the same detuning and more than twice as large as the bare quantum well diamagnetic shift. Thus, the lower polariton is described by a wavefunction with a matter part exhibiting a decreased average electron-hole separation. For the upper polariton, this average radius is much larger than that of an electron-hole pair in the uncoupled quantum well which can be explained by photon-mediated interactions with excited and continuum states of the quantum well.

No / Two Cylindrical Dielectric Resonators DR asymmetrically placed on a thin dielectric substrate and fed by a single rectangular slot for wideband wireless applications are presented. Optimized design procedures were applied within a well-known electromagnetic solver to achieve the improved elements dimensions of the antenna geometry. The simulated and measured results show that the proposed DRA can achieve 29% relative bandwidth at 10 dB return loss covering the spectrum range from 9.62 GHz to 12.9 GHz with a maximum gain of 8 dB.

Yes / A compact dielectric resonator antenna for ultra-wideband vehicular communication applications is proposed. Two cylindrical dielectric resonators are asymmetrically located with respect to the center of an offset rectangular coupling aperture, through which they are fed. Optimizing the design parameters results in an impedance bandwidth of 21%, covering the range from 5.9 to 7.32 GHz in the lower-band and a 53% relative bandwidth from 8.72 to 15 GHz in the upper-band. The maximum achieved gain is 12 dBi. Design details of the proposed antenna and the results of both simulations and experiment are presented and discussed.

No / A small dielectric resonator antenna has been designed for ultra wideband (UWB) communication system applications. The antenna element is a rectangular low permittivity ceramic block, with a dielectric constant of 9.4, and the modified T-shaped feed network includes a 50 ohm microstrip line to achieve strong coupling, and some bandwidth enhancement. The antenna performance is simulated and measured over a frequency band extending from 3100 MHz to 5500 MHz; the impedance bandwidth over this interval is 55.8% with VSWR <; 2, making the antenna suitable for UWB applications.

Цель работы заключается в теоретическом и экспериментальном исследовании новых типов электрических антенн. Проведено исследование в среде электромагнитного моделирования Ansoft HFSS, по результатам моделирования изготовлены прототипы и проведены измерения их характеристик. Новые типы антенны имеют большие перспективы дальнейшего развития, возможно изготовление активной антенны или использование ее в качестве элемента фазированной антенной решетки. / The purpose of work consists in theoretical and experimental research of new types of electric antennas. Study of electromagnetic environment simulation Ansoft HFSS, the simulation results of fabricated prototypes and measured their characteristics. New types of antennas have great potential for further development, it is possible to manufacture an active antenna or use it as element of a phased antenna array.

<p dir="ltr">Gyroscopes have become an integral part of many application spaces ranging from consumer electronics to navigation. As navigation and movement tracking becomes necessary through inertial measurement units (that comprises gyroscopes and accelerometers) in myriad of scenarios especially when global navigation and satellite system (GNSS) is not available, stability of gyroscopes plays a detrimental role in the accuracy of navigation. Recent developments in micro-electromechanical systems (MEMS) based gyroscopes enabled them to penetrate into navigation grade application spaces. MEMS based miniaturization approach also revived the interest in nuclear magnetic resonance gyroscopes (NMRGs). In parallel, emerging atomic gyroscope technologies are getting attention such as using quantum defects in single crystal diamond. </p><p><br></p><p dir="ltr">Considering innovative ways MEMS can improve gyroscopes, we investigate solid state gyroscope technologies in piezoelectric MEMS and nuclear spin based platforms for next generation rotation sensing that is shock and vibration insensitive. For the first part of this study, we explore a piezoelectric resonator that can excite wine-glass mode (WGM) and tangential mode. WGM is used for rotation sensing applications in various excitation mechanisms in literature. However, we demonstrate the capability of exciting WGM without the need for segmented electrodes in piezoelectric domain that allows self-alignment of the excitation electrodes using a unique property of Lead Magnesium Niobate-Lead Titanate (PMN-PT). In the second part of the study, we explore Nitrogen-Vacancy (NV) centers in diamond to be used as gyroscopes exploiting the rotation sensitivity of nuclear spins. NV center-based gyroscopes provide solid-state solution with comparable or superior performance without any moving parts. We propose mechanical coupling to NV centers in diamond using piezoelectrically excited bulk acoustic waves (BAW) to extend the coherence time of nuclear spins by dynamical decoupling. We explore piezoelectric coupling design space of AlN thin film BAW resonators (FBARs) to enable efficient mechanical drive to improve Rabi oscillations in diamond to overcome one of the most important bottlenecks of realizing a gyroscope, which is the mitigation and control of nuclear spin and electron spin interaction in diamond NV center system.</p>

Silicon Nanowire-based biosensors owe their sensitivity to the large surface area to volume ratio of the nanowires. However, presently they have only been shown to detect specific bio-markers in low-salt buffer environments. The first part of this thesis presents a pertinent next step in the evolution of these sensors by presenting the specific detection of a target analyte (NT-ProBNP) in a physiologically relevant solution such as serum. By fabrication of the nanowires down to widths of 60 nm, choosing appropriate design parameters, optimization of the silicon surface functionalization recipe and using a reduced gate oxide thickness of 5 nm; these sensors are shown to detect the NT-ProBNP bio-marker down to 2ng/ml in serum. The observed high background noise in the measured response of the sensor is discussed and removed experimentally by the addition of an extra microfabrication step to employ a differential measurement scheme. It is also shown how the modulation of the local charge density via external static electric fields (applied by on-chip patterned electrodes) pushes the sensitivity threshold by more than an order of magnitude. These demonstrations bring the silicon nanowire-based biosensor platform one step closer to being realized for point-of-care (POC) applications. In the second half of the thesis, it is demonstrated how silicon micromechanical piezoelectric resonators could be tasked to provide wireless power to such POC bio-systems. At present most sensing and actuation platforms, especially in the implantable format, are powered either via onboard battery packs which are large and need periodic replacement or are powered wirelessly through magnetic induction, which requires a proximately located external charging coil. Using energy harnessed from electric fields at distances over a meter; comprehensive distance, orientation, and power dependence for these first-generation devices is presented. The distance response is non-monotonic and anomalous due to multi-path interferences, reflections and low directivity of the power receiver. This issue is studied and evaluated using COMSOL Multiphysics simulations. It is shown that the efficiency of these devices initially evaluated at 3% may be enhanced up to 15% by accessing higher frequency modes.

No description available.

Small scale renewable energy harvesting is an attractive solution to the growing need for power in remote technological applications. For this purpose, localized thermal gradients on-chip—created via radiative cooling—could be exploited to produce microscale renewable heat engines running on environmental heat. This could allow self-powering in small scale portable applications, thus reducing the need for non-renewable sources of electricity and hazardous batteries. In this work, we demonstrate the creation of a local thermal gradient on-chip by radiative cooling of a 90 nm thick freestanding silicon nitride nanomechanical resonator integrated on a silicon substrate at ambient temperature. The reduction in temperature of the thin film is inferred by tracking its mechanical resonance frequency, under high vacuum, using an optical fiber interferometer. Experiments were conducted on 15 different days during fall and summer months, resulting in successful radiative cooling in each case. Maximum temperature drops of 9.3 K and 7.1 K are demonstrated during the day and night, respectively, in close correspondence with our heat transfer model. Future improvements to the experimental setup could enhance the temperature reduction to 48 K for the same membrane, while emissivity engineering potentially yields a maximum theoretical cooling of 67 K with an ideal emitter. This thesis first elaborates a literature review on the field of radiative cooling, along with a theoretical review of relevant thermal radiation concepts. Then, a heat transfer model of the radiative cooling experiment is detailed, followed by the experimental method, apparatus, and procedures. Finally, the experimental and theoretical results are presented, along with future work and concluding remarks.

No description available.