A two-probe system of the heterojunction formed by an (8, 0) carbon nanotube (CNT) and an (8, 0) silicon carbide nanotube (SiCNT) was established based on its optimized structure. By using a method combining n...
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A two-probe system of the heterojunction formed by an (8, 0) carbon nanotube (CNT) and an (8, 0) silicon carbide nanotube (SiCNT) was established based on its optimized structure. By using a method combining nonequilibrium Green's function (NEGF) with density functional theory (DFF), the transport properties of the het-erojunction were investigated. Our study reveals that the highest occupied molecular orbital (HOMO) has a higher electron density on the CNT section and the lowest unoccupied molecular orbital (LUMO) mainly concentrates on the interface and the SiCNT section. The positive and negative threshold voltages are +1.8 and -2.2 V, respectively.
Ga_(2)O_(3)is difficult to achieve p-type doping,which further hinders the development of Ga_(2)O_(3)-based power devices and is not conducive to the development of new devices with high power density and low power **...
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Ga_(2)O_(3)is difficult to achieve p-type doping,which further hinders the development of Ga_(2)O_(3)-based power devices and is not conducive to the development of new devices with high power density and low power *** paper expounds aβ-Ga_(2)O_(3)/4H-SiC heterojunction lateral metal–oxide–semiconductor field-effect transistor(HJFET),which can make better use of the characteristics of PN junction by adding p-doped SiC in the channel *** with the conventional devices,the threshold voltage of the heterojunction metal–oxide–semiconductor field-effect transistor(MOSFET)is greatly improved,and normally-off operation is realized,showing a positive threshold voltage of 0.82 ***,the off-state breakdown voltage of the device is up to 1817 V,and the maximum transconductance is 15.3 mS/*** optimal PFOM is obtained by simulating the thickness,length and doping of the SiC in each region of the epitaxial *** structure provides a feasible idea for high performanceβ-Ga_(2)O_(3)MOSFET.
The structure of a heterojunction made up of an (8, 0) carbon nanotube and an (8, 0) boron nitride nanotube is achieved through geometry optimization implemented in the CASTEP package. Based on the optimized geome...
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The structure of a heterojunction made up of an (8, 0) carbon nanotube and an (8, 0) boron nitride nanotube is achieved through geometry optimization implemented in the CASTEP package. Based on the optimized geometry, the model of the heterojunction is established. Its transport properties are investigated by combining the nonequilibrium Green's function with density functional theory. Results show that both the lowest unoccupied molecular orbital and the highest occupied molecular orbital mainly locate on the carbon nanotube section. In the current-voltage characteristic of the heterojunction, a rectification feature is revealed.
The design and test results of a 6-bit 3-Gsps analog-to-digital converter (ADC) using 1 μm GaAs het- erojunction bipolar transistor (HBT) technology are presented. The monolithic folding-interpolating ADC makes u...
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The design and test results of a 6-bit 3-Gsps analog-to-digital converter (ADC) using 1 μm GaAs het- erojunction bipolar transistor (HBT) technology are presented. The monolithic folding-interpolating ADC makes use of a track-and-hold amplifier (THA) with a highly linear input buffer to maintain a highly effective number of bits (ENOB). The ADC occupies an area of 4.32 × 3.66 mm2 and achieves 5.53 ENOB with an effective resolution bandwidth of 1.l GHz at a sampling rate of 3 Gsps. The maximum DNL and INL are 0.36 LSB and 0.48 LSB, respectively.
Metal-organic chemical vapor deposition was applied to fabricate YBa2Cu3OT-a (YBCO) films on singlecrystal LaA103 (001) substrates for its high deposition rate, easy adjustment on film composition, and low require...
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Metal-organic chemical vapor deposition was applied to fabricate YBa2Cu3OT-a (YBCO) films on singlecrystal LaA103 (001) substrates for its high deposition rate, easy adjustment on film composition, and low requirement on vacuum apparatus. The effects of Cu(tmhd)2 concentra- tion in the precursor on the properties of YBCO films were systematically investigated. X-ray diffraction (XRD) reveals that the mole ratio of Cu/Ba in the precursor from 0.77 to 0.97 is helpful to improve the crystallization and out-of-plane orientation of YBCO films; however, it hardly affects the inplane texture. Scanning electron microscope (SEM) shows the dense, crack-free but rough surface, on which there are Cu-O and Ba-Cu-O outgrowths identified by energy-dispersive spectrometer (EDS). As the mole ratio of Cu/Ba increasing, the average size of Ba-Cu-O precipitates keeps increasing and the film composition becomes inhomoge- neous at the mole ratio of Cu/Ba of 0.97. The 250 nm thick YBCO film prepared at the mole ratio of Cu/Ba of 0.91 shows the critical current density (Jc) of 4.0 ***-2 (77 K, 0 T).
Surface acoustic wave(SAW) resonators with Pt/AlN/Si and Pt/AlN/Pt/Si configurations were fabricated by lift-off photolithography techniques. High-temperature performances of both configurations were investigated fo...
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Surface acoustic wave(SAW) resonators with Pt/AlN/Si and Pt/AlN/Pt/Si configurations were fabricated by lift-off photolithography techniques. High-temperature performances of both configurations were investigated for temperature sensor applications. AlN films grown on Ptcoated Si substrates exhibit a lower(002) preferred orientation than those grown on Si substrates. The center frequencies of Pt/AlN/Si and Pt/AlN/Pt/Si configurations at room temperature are 424.1 and 456.4 MHz, *** SAW was limited by Pt bottom electrodes to propagate in AlN layer. The temperature coefficient of frequency(TCF) values of Pt/AlN/Si and Pt/AlN/Pt/Si configurations are-51.6 × 10^-6 and-69.2 × 10^-6℃^-1, *** with that of Pt/AlN/Si configuration, the TCF value of Pt/AlN/Pt/Si configuration decreases by 34.1 %.AlN resonator with the Pt floating bottom electrodes provides a large, quasi-constant temperature sensitivity which is suitable for temperature sensor applications.
Single-layer YBa2Cu3O7-δ(YBCO) films with the thickness of over 600 nm were fabricated by modified metal organic deposition using trifluoroacetate metal organic deposition(TFA-MOD) method on LaAlO3(LAO) substra...
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Single-layer YBa2Cu3O7-δ(YBCO) films with the thickness of over 600 nm were fabricated by modified metal organic deposition using trifluoroacetate metal organic deposition(TFA-MOD) method on LaAlO3(LAO) substrates. Polyvinylbutyral(PVB) was added into the precursor solution to enhance the thickness of the single layer. The pyrolysis process was shortened to about 3 h due to the reduction of the fluorine content in the precursor *** effects of heating rate during the crystallization process on the microstructure and Jcvalues of YBCO films were investigated. The α-axis-oriented YBCO crystals dominate when the heating rate is lower than 20 °C·min^-1, while faster heating rate of 43 °C·min^-1 results in pure c-axis epitaxial growth. The Jcvalues of YBCO films increase linearly with heating rate increasing due to the increase of c-axis YBCO growth, and the critical current(Ic) value of 100 A·cm^-1 within a single-layer YBCO film is achieved.
In this paper, the Hot-Carrier (HC) degradation characteristics and mechanisms of nMOSFETs with high-k/metal gate (HK/MG) structure are systematically investigated. The Idsat shift under different Vd states obeys powe...
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Precise measurement of temperature and salinity is crucial for marine engineering, resource exploitation, and environmental protection. However, developing a compact device capable of simultaneously measuring both par...
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This paper gives a detailed analysis of the time-dependent degradation of the threshold voltage in AlGaN/GaN high electron mobility transistors(HEMTs) submitted to off-state stress. The threshold voltage shows a posit...
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This paper gives a detailed analysis of the time-dependent degradation of the threshold voltage in AlGaN/GaN high electron mobility transistors(HEMTs) submitted to off-state stress. The threshold voltage shows a positive shift in the early stress, then turns to a negative shift. The negative shift of the threshold voltage seems to have a long recovery time. A model related with the balance of electron trapping and detrapping induced by shallow donors and deep acceptors is proposed to explain this degradation mode.
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