首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 843 毫秒
1.
The eigenvalue characteristics of a ferrimagnetic tridisk-coupled (TDC) resonator are described first. A TDC resonator is made of three AlYIG ferrite disks partially scraped and mutually attached on a center conductor. The EM field is treated with a consistent theory. The eigenvalue characteristics computed with stress on the mode of ν=1 are represented by the Z10 versus Z0 and Z1 versus κ/μ relationships, where Z10 is a degenerate eigenvalue, Z0 is a wavenumber-eccentric radius product, and Z1 is a continuously varying eigenvalue dependent on κ/μ with a given value of Z0. Z10 is distinguished by either a single- or double-value region as a function of Z0. The computed Z1 versus κ/μ graph belonging to the double-value region demonstrates a contradiction to the physical reality, which is resolved by introducing an equivalent circular resonant mode. The equivalent resonant mode is definitely identified by a degenerate eigenvalue and its modal curve with large modal separation. Experiments were carried out with various center conductors. The experimental results support the equivalent resonant mode. Finally, discussions are presented  相似文献   

2.
We investigate the breakdown (Vbr) enhancement potential of the field plate (FP) technique in the context of AlGaN/GaN power HEMTs. A comprehensive account of the critical geometrical and material variables controlling the field distribution under the FP is provided. A systematic procedure is given for designing a FP device, using two-dimensional (2-D) simulation, to obtain the maximum Vbr , with minimum degradation in on-resistance and frequency response. It is found that significantly higher Vbr can be achieved by raising the dielectric constant (εi) of the insulator beneath the FP. Simulation gave the following estimates. The FP can improve the Vbr by a factor of 2.8-5.1, depending on the 2-DEG concentration (ns) and εi. For n s=1×1013/cm2, the Vbr can be raised from 123 V to 630 V, using a 2.2 μm FP on a 0.8 μm silicon nitride, and 4.7 μm gate-drain separation. The methodology of this paper can be extended to the design of FP structures in other lateral FETs, such as MESFETs and LD-MOSFETs  相似文献   

3.
This paper presents a new approach to model the 2DEG concentration (ns) versus gate voltage (VG) behavior and the equilibrium 2DEG concentration (ns0) in a HEMT. The approach results in a model which is “comprehensive” in the following sense. It is valid for both delta-doped and uniformly doped HEMTs. It captures all the three ns-VG nonlinearities (subthreshold, gradual pinchoff, and gradual saturation), and the effects of all the device parameters including temperature, in relation expressing ns as an explicit closed-form integrable function of VG having continuous first derivatives; thus, the function readily yields a device current-voltage/capacitance-voltage (I-V/C-V) model which can be incorporated in software meant for simulation of circuits, particularly of the analog variety. The simple model is shown to predict the results of complex numerical calculations and experiments. The closed-form ns0 expression of the model is the first of its kind reported for delta-doped HEMT's, and reveals an interesting feature unexposed by earlier ns0 models: the reciprocal of ns0 in both delta-doped and uniformly doped devices decreases linearly with reduction in spacer width, and saturates at low spacer widths in some delta-doped devices. It is shown that the measured ns0 in delta-doped devices is predicted correctly if the electrons in the V-shaped well are assumed to be trapped at the donor sites rather than to be filling the conduction subbands  相似文献   

4.
A new decoupled C-V method is proposed to determine the intrinsic (effective) channel region and extrinsic overlap region for miniaturized MOSFET's. In this approach, a unique channel-length-independent extrinsic overlap region is extracted at a critical gate bias, so bias-independent effective channel lengths (Leff) are achieved. Furthermore, the two-dimensional (2D) charge sharing effect is separated from the effective channel region. Based on this Leff and the associated bias-dependent channel mobility, μeff , the drain-and-source series resistance (RDS) can be derived from the I-V characteristics for each device individually. For the first time, the assumption or approximation for RDS and μeff can be avoided, thus the difficulties and controversy encountered in the conventional I-V method can be solved. The 2D charge sharing effect is incorporated into the bias-dependent RDS. This bias dependence is closely related to the drain/source doping profile and the channel dopant concentration. The proposed Leff and RDS extraction method has been verified by an analytical I-V model which shows excellent agreements with the measured I-V characteristics  相似文献   

5.
To transmit information by timing arrivals to a single-server queue, we consider using the exponential server channel's maximum likelihood decoder. For any server with service times that are stationary and ergodic with mean 1/μ seconds, we show that the rate e -1μ nats per second (capacity of the exponential server timing channel) is achievable using this decoder. We show that a similar result holds for the timing channel with feedback. We also show that if the server jams communication by adding an arbitrary amount of time to the nominal service time, then the rate e-1μ1μ2/(μ12) nats per second is achievable with random codes, where the nominal service times are stationary and ergodic with mean 1/μ1 seconds, and the arithmetic mean of the delays added by the server does not exceed 1/μ2 seconds. This is a model of an arbitrarily varying channel where the current delay and the current input can affect future outputs. We also show the counterpart of these results for single-server discrete-time queues  相似文献   

6.
Hammons et al. (see ibid., vol.40, p.301-19, 1994) showed that, when properly defined, the binary nonlinear Preparata code can be considered as the Gray map of a linear code over Z4, the so called Preparata code over Z4. We consider the rth generalized Hamming weight dr(m) of the Preparata code of length 2m over Z4. For any m⩾3, dr(m) is exactly determined for r=0.5, 1, 1.5, 2, 2.5 and 3.0. For a composite m, we give an upper bound on dr(m) using the lifting technique. For m=3, 4, 5, 6 and 8, the weight hierarchy is completely determined. In the case of m=7, the weight hierarchy is completely determined except for d4(7)  相似文献   

7.
A fully analytical model for the current-voltage (I-V) characteristics of HEMT's is presented. It uses a polynomial expression to model the dependence of sheet carrier concentration (ns) in the two-dimensional electron gas (2-DEG) on gate voltage (VG ). The resultant I-V relationship incorporates a correction factor α analogous to SPICE MOSFET Level 3 model and is therefore more accurate than models assuming a linear ns-VG dependence leading to square law type I-V characteristics. The model shows excellent agreement with experimental data over a wide range of bias. Further, unlike other models using nonlinear ns-VG dependence, it neither uses fitting parameters nor does it resort to iterative methods at any stage. It also includes the effects of the extrinsic source and drain resistances. Due to its simplicity and similarity in formulation to the SPICE MOSFET Level 3 model, it is ideally suited for circuit simulation purposes  相似文献   

8.
A macroscopic model is proposed for nonlinear electromagnetic phenomena in superconductors. Nonlinear constitutive relations are derived by modifying the linear London's equations. The superelectron number density as a function of applied macroscopic current density, n s(J), is derived from a distribution of electron velocities at a certain temperature T. At temperature T≠0 K, the function ns(J) has a smooth variation near the macroscopic critical current density Jc. Agreement has been found between this n s(J,T) model and the temperature dependence of ns in the two-fluid model. The nonlinear conductivities σs(J) and σn(J) are obtained from the London's equation with the modified ns(J) function. Nonlinear resistance R(I), kinetic inductance Lk(I) and surface impedance Zs(I) in thin wire, slab, and strip geometries are calculated  相似文献   

9.
In this letter, we propose a low complexity Maximum Likelihood (ML) decoding algorithm for quasi-orthogonal space-time block codes (QOSTBCs) based on the real-valued lattice representation and QR decomposition. We show that for a system with rate r = ns/T, where ns is the number of transmitted symbols per T time slots; the proposed algorithm decomposes the original complex-valued system into a parallel system with ns 2 × 2 real-valued components, thus allowing for a simple joint decoding of two real symbols. For a square QAM constellation with L points (L-QAM), this algorithm achieves full diversity by properly incorporating two-dimensional rotation using the optimal rotation angle and the same rotating matrix for any number of transmit antennas (N ⩾4). We show that the complexity gain becomes greater when N or L becomes larger. The complexity of the proposed algorithm is shown to be linear with the number of transmitted symbols ns.  相似文献   

10.
高健  吕京杰 《电子学报》2018,46(7):1768-1773
定义了Z4×(F2+uF2)上的循环码,明确了一类循环码的生成元结构,给出了该类循环码的极小生成元集.利用Gray映射,构造了一些二元非线性码.  相似文献   

11.
The validity of a one- and a two-cylinder model, underlying thoracic impedance cardiography (TIC), was investigated by studying the length dependence of the impedance parameters Z0, (dZ/dt)min, and stroke volume (SV). It can be shown that, within a one-cylinder model, all parameters are directly proportional to the length, whereas, if the volume conduction of the thorax and the neck are modeled separately, Z0 and (dZ/dt)min are expected to be linear dependent and SV will he nonlinear dependent upon the length. The expectations were compared to results from in vivo measurements. Two electrode arrays were studied, in which the caudal recording electrode position was varied; SV was calculated using Kubicek's equation. Except for small distances, the results showed a nearly linear relation between the parameters and the length. Regression analysis of the linear part revealed statistically significant intercepts (p<0.05). Neither the intercept nor the nonlinear part can be explained by a one-cylinder model, whereas a model consisting of two cylinders serially connected describes the experimental results accurately. Thus SV estimation based on a one-cylinder model is biased due to the invalid one-cylinder model. Corrections for the Kubicek-equation need to be developed in future research using this two-cylinder model  相似文献   

12.
An experimental technique for accurately determining both the inversion charge and the channel mobility μ of a MOSFET is presented. With this new technique, the inversion charge is measured as a function of the gate and drain voltages. This improvement allows the channel mobility to be extracted independent of drain voltage VDS over a wide range of voltages (VDS=20-100 mV). The resulting μ(VGS) curves for different VDS show no drastic mobility roll-off at V GS near VTH. This suggests that the roll-off seen in the mobility data extracted using the split C- V method is probably due to inaccurate inversion charge measurements instead of Coulombic scattering  相似文献   

13.
Dispersive nonlinearity in amorphous Si/SiO2 quantum well structures (QW's) has been investigated. The refractive index changes obtained from the intensity-dependent reflection spectra are nonlinearly dependent on the excitation intensity and can be described by the model of the saturating nonlinearity at low pump intensities. The nonlinear refractive index reveals resonant behavior associated with the subband structure of the QW's. The saturated nonlinear index and the saturation intensity have been obtained as Δns=-0.11 and Is=1.9 MW/cm2 at the transitions between the lowest subbands, and Δns~0.3 and Is~0.5 MW/cm2 at the transitions between the second subbands of the valence and conduction bands. The nonlinearity for the second subband transitions has been found high enough to provide potentially bistable operation, but the bistability is not expected at the transitions between the ground subbands. Carrier lifetime less than 1 ps restricting the switching time of the nonlinearity has been estimated from the saturation intensity  相似文献   

14.
Let S(8) denote the set of the eight admissible signals of an 8PSK communication system. The alphabet S(8) is endowed with the structure of Z8, the set of integers taken modulo 8, and codes are defined to be Z8-submodules of Z8n. Three cyclic codes over Z8 are then constructed. Their length is equal to 6, 8, and 7, and they, respectively, contain 64, 64, and 512 codewords. The square of their Euclidean minimum distance is equal to 8, 16-4√2 and 10-2√2, respectively. The size of the codes of length 6 and 7 can be doubled while the Euclidean minimum distance remains the same  相似文献   

15.
A dramatic improvement of inversion channel mobility in 4H-SiC MOSFETs was successfully achieved by utilizing the (112¯0) face: 17 times higher (95.9 cm2/Vs) than that on the conventional (0001) Si-face (5.59 cm2/Vs). A low threshold voltage of MOSFETs on the (112¯0) face indicates that the (112¯0) MOS interface has fewer negative charges than the (0001) MOS interface. Small anisotropy of channel mobility in 4H-SiC MOSFETs (μ(11¯00)(0001)=0.85) reflects the small anisotropy in bulk electron mobility  相似文献   

16.
Cyclic codes and self-dual codes over F2+uF2   总被引:1,自引:0,他引:1  
We introduce linear cyclic codes over the ring F2+uF 2={0,1,u,u¯=u+1}, where u2=0 and study them by analogy with the Z4 case. We give the structure of these codes on this new alphabet. Self-dual codes of odd length exist as in the case of Z4-codes. Unlike the Z4 case, here free codes are not interesting. Some nonfree codes give rise to optimal binary linear codes and extremal self-dual codes through a linear Gray map  相似文献   

17.
The correlation between gate and substrate currents in NMOSFET's with effective channel length, Leff, down to 0.1 μm is investigated within the general framework of the lucky-electron model. It Is found that the correlation coefficient, Φb/Φi, decreases with decreasing Leff in the 0.1 μm regime, where Φb is the effective Si-SiO2 barrier height for channel hot-electrons, and Φi is the effective threshold potential for impact ionization. Furthermore, this effect becomes stronger in NMOSFET's with shorter Leff. These experimental results suggest the need for further investigation on specific assumptions in the lucky-electron model to understand hot-electron behavior and impact ionization-mechanisms in 0.1 μm-scale NMOSFET's  相似文献   

18.
A novel structure Ga0.51In0.49P/GaAs MISFET with an undoped Ga0.51In0.49P layer serving as the airbridge between active region and gate pad was first designed and fabricated. Wide and flat characteristics of gm and fmax versus drain current or gate voltage were achieved. The device also showed a very high maximum current density (610 mA/mm) and a very high gate-to-drain breakdown voltage (25 V). Parasitic capacitances and leakage currents were minimized by the airbridge gate structure and thus high fT of 22 GHz and high fmax of 40 GHz for 1 μm gate length devices were attained. To our knowledge, both were the best reported values for 1 μm gate GaAs channel FET's  相似文献   

19.
Devices have been designed and fabricated in a CMOS technology with a nominal channel length of 0.15 μm and minimum channel length below 0.1 μm. In order to minimize short-channel effects (SCEs) down to channel lengths below 0.1 μm, highly nonuniform channel dopings (obtained by indium and antimony channel implants) and shallow source-drain extensions/halo (by In and Sb preamorphization and low-energy As and BF2 implant were used. Maximum high V DS threshold rolloff was 250 mV at effective channel length of 0.06 μm. For the minimum channel length of 0.1 μm, the loaded (FI=FO=3, C=240 fF) and unloaded delays were 150 and 25 ps, respectively  相似文献   

20.
The merits of InGaAs-based millimeter-wave mixer diodes are explored experimentally and theoretically. Schottky junctions on InGaAs exhibit barriers (φb) in the neighborhood of 0.25 eV. The high mobility of InGaAs contributes to the low n+ sheet resistances of 1.9-5 Ω/square for 1-μm n+ InGaAs layers (ns=1.5×1019 cm-3, μ n=1800 cm2/V·s) grown with our in-house Metalorganic Vapor Phase Epitaxy (MOVPE) system, The design, material growth, fabrication, and characterization of InGaAs integrated mixer/antennae are reported. Pt plating technology, adapted here for InGaAs Schottky contacts, has improved the ideality factor (η) and yield relative to conventional evaporated Pt. With 810 μW of local oscillator power, applied to the diode, and zero DC bias, an integrated InGaAs mixer/antenna demonstrated an excellent diode performance of 199 K RF input double-sideband noise temperature with a corresponding single-sideband (SSB) conversion loss (Lc) of 5.0 dB at LO, RF, and IF frequencies of 94 GHz, 94 GHz±1.4 GHz, and 1.4 GHz, respectively. Likewise, the diodes in an InGaAs subharmonic integrated mixer/antenna demonstrated an equivalent RF-port double-sideband (DSB) noise temperature (Tmix) of 1058 K and single-sideband conversion loss of 10.2 dB at 180 GHz with a 90-GHz LO power (PLO) of 1.6 mW. Compared to GaAs diodes with RF coupling and IF losses removed, the single-ended InGaAs noise temperature results were within 46-100 K of those for state-of-the-art GaAs mixer diodes while requiring significantly less LO power  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号