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    Monolithic 4-Terminal 1.2 kV/20 A 4H-SiC Bi-Directional Field Effect Transistor (BiDFET) with Integrated JBS Diodes
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    Abstract:
    In this paper, we report successful fabrication of the first large area, monolithic, 1.2 kV 4H-SiC Bi-Directional FETs (BiDFETs) with integrated JBS diodes in a 6-inch commercial foundry for use in matrix converters. The fabricated BiDFETs support high voltage (>1.2 kV) in the first and third quadrants. They exhibit very low on-resistance of 50 mΩ in the on-state in both quadrants when the 20 V gate bias is applied to both gates, allowing conduction of 20 A with 1 V drop. Fully gate voltage controlled output characteristics are also confirmed in both quadrants.
    The authors fabricated an organic nanochannel field-effect transistor (FET) that is self-wired with highly conductive organic conductors. The advantages of the transistor are a short channel (approximately 400nm in length) and spontaneous formation of an active layer of the FET. Further, in principle, the carrier-injection barrier is absent at the interface of the organic metal and organic semiconductor. Thus, the transistor is highly conductive despite the narrow cross section of the channel. The FET characteristics of the nanochannel transistor exhibit the n-channel enhancement mode behavior.
    Organic semiconductor
    Organic field-effect transistor
    Citations (19)
    For the present work single-walled carbon nanotube (SWNT) field-effect transistors and field-effect transistors based on poly(3-hexylthiophene) were fabricated and used as protein sensors in aqueous environment. The stability of both transistor types in biological buffers was tested. Additionally the interactions of various proteins with ligands, were analyzed using SWNT transistors. Using biofunctionalized SWNT transistors the dissociation constants of a protein was probed and it was possible to distinguish between two different other proteins by their pH-dependent sensor response.
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    Differential Power Processing (DPP) converters have been recently utilized for reducing the losses in partially shaded PV systems. Through enabling new paths for currents, shaded panels have less impact on blocking higher currents from series connected PV modules. This ultimately results in harvesting more power from partially shaded PV units. Unfortunately, the number of required DPP converters increases linearly with the number of series PV units. To address this challenge, this paper investigates the possibility of reconfiguring DPP converters reducing the number of needed converters. Instead of using a complete set of DPP converters, reconfiguring DPP converters could substantially reduce the number of needed converters. The used DPP converters will be connected to shaded units and reconfigured online with changes in shadings to reduce the mismatch power losses. Validation and verification through simulation is conducted to demonstration the effectiveness of the proposed idea.
    Ac-dc power conversion can either be done with two separate converter stages or with a single converter stage. Two-stage ac-dc converters, however, can be costly and complex and the performance of single-stage converters is compromised due to a reduced number of components. Several researchers have therefore proposed adding some sort of auxiliary circuit consisting of a second switch and some passive elements to single-stage converters to improve their performance. Although these quasi-single-stage (QSS) converters may have two converters, they are not two-stage converters as they do not have two separate and independently controlled converters that are always operating to convert power from one form to another. In the paper, the operation of ac-dc single-stage converters is first reviewed and their characteristics are noted. The operation of several QSS converters, including one proposed by the authors, is then discussed, and the paper concludes by presenting experimental results that confirm the feasibility of the proposed converter.
    Single stage
    1. Terminology, specifications and evaluation techniques 2. Scaled D to A converters 3. High resolution scaled D to A converters 4. Feedback A to D converters 5. Algorithmic converters 6. Rampfunction converters 7. Delta-sigma converters 8. Fast A to D converters Appendix: simulations
    Delta-sigma modulation
    Sigma
    Citations (45)
    Room temperature magnetotransport experiments were carried out on field-effect transistors in magnetic fields up to 10 T. It is shown that measurements of the transistor magnetoresistance and its first derivative with respect to the gate voltage allow the derivation of the electron mobility in the gated part of the transistor channel, while the access/contact resistances and the transistor gate length need not be known. We demonstrate the potential of this method using GaN and Si field-effect transistors and discuss its importance for mobility measurements in transistors with nanometer gate length.
    Electron Mobility
    Static induction transistor
    Citations (12)
    Floating gate field-effect transistors (FETs) for the detection of extracellular signals from electrogenic cells were fabricated in a complementary metal oxide semiconductor process. Additional passivation layers protected the transistor gates from the electrolyte solution. To compare the signals from n- and p-FETs, two electronically separated, but locally adjacent transistors were combined to one measuring unit. The paired sensing area of this unit had the dimension of a single cell. Simultaneous recordings with n- and p-channel floating gate FETs from a single cell exhibited comparable amplitudes and identical time courses. The experiments indicate that both types of FETs express similar sensitivities.
    Passivation
    Citations (18)
    We present dc and microwave experiments on a graphene-based top-gate field effect transistor. The transistor is acting as an active device far from the Dirac point, and turns into a passive device at the Dirac point, the transistor amplification being suppressed due to lack of carriers. In this way, microwave switches can be implemented based on the specific charge carrier transport in graphene. The maximum stable gain of the transistor is maintained up to 9 GHz, and the mobility of graphene FET is greater than 8000 cm 2 /Vs far from the Dirac point.
    Static induction transistor
    Charge carrier