Eigendecomposition of Images Correlated on $S^{1}$, $S^{2}$, and $SO(3)$ Using Spectral Theory

Eigendecomposition represents one computationally efficient approach for dealing with object detection and pose estimation, as well as other vision-based problems, and has been applied to sets of correlated images for this purpose. The major drawback in using eigendecomposition is the off line computational expense incurred by computing the desired subspace. This off line expense increases drastically as the number of correlated images becomes large (which is the case when doing fully general 3-D pose estimation). Previous work has shown that for data correlated on S ¹ , Fourier analysis can help reduce the computational burden of this off line expense. This paper presents a method for extending this technique to data correlated on S ² as well as SO(3) by sampling the sphere appropriately. An algorithm is then developed for reducing the off line computational burden associated with computing the eigenspace by exploiting the spectral information of this spherical data set using spherical harmonics and Wigner-D functions. Experimental results are presented to compare the proposed algorithm to the true eigendecomposition, as well as assess the computational savings.     

A Comparative NBTI Study of $hbox{HfO}_{2}$, $hbox{HfSiO}_{x}$, and SiON p-MOSFETs Using UF-OTF $I_{rm DLIN}$ Technique

The time, temperature, and oxide-field dependence of negative-bias temperature instability is studied in $hbox{HfO}_{2}/hbox{TiN}$, $ hbox{HfSiO}_{x}/hbox{TiN}$, and SiON/poly-Si p-MOSFETs using ultrafast on-the-fly $I_{rm DLIN}$ technique capable of providing measured degradation from very short (approximately microseconds) to long stress time. Similar to rapid thermal nitrided oxide (RTNO) SiON, $hbox{HfO}_{2}$ devices show very high temperature-independent degradation at short (submilliseconds) stress time, not observed for plasma nitrided oxide (PNO) SiON and $hbox{HfSiO}_{x}$ devices. $hbox{HfSiO}_{x}$ shows lower overall degradation, higher long-time power-law exponent, field acceleration, and temperature activation as compared to $hbox{HfO}_{2}$, which are similar to the differences between PNO and RTNO SiON devices, respectively. The difference between $ hbox{HfSiO}_{x}$ and $hbox{HfO}_{2}$ can be attributed to differences in N density in the $hbox{SiO}_{2}$ IL of these devices.      

Impacts of $hbox{N}_{2}$ and $hbox{NH}_{3}$ Plasma Surface Treatments on High-Performance LTPS-TFT With High-$kappa$ Gate Dielectric

Low-temperature polycrystalline-silicon thin-film transistors (LTPS-TFTs) with high- $kappa$ gate dielectrics and plasma surface treatments are demonstrated for the first time. Significant field-effect mobility $mu_{rm FE}$ improvements of $sim$86.0% and 112.5% are observed for LTPS-TFTs with $hbox{HfO}_{2}$ gate dielectric after $hbox{N}_{2}$ and $ hbox{NH}_{3}$ plasma surface treatments, respectively. In addition, the $hbox{N}_{2}$ and $ hbox{NH}_{3}$ plasma surface treatments can also reduce surface roughness scattering to enhance the field-effect mobility $mu_{rm FE}$ at high gate bias voltage $V_{G}$, resulting in 217.0% and 219.6% improvements in driving current, respectively. As a result, high-performance LTPS-TFT with low threshold voltage $V_{rm TH} sim hbox{0.33} hbox{V}$, excellent subthreshold swing S.S. $sim$0.156 V/decade, and high field-effect mobility $mu_{rm FE} sim hbox{62.02} hbox{cm}^{2}/hbox{V} cdot hbox{s}$ would be suitable for the application of system-on-panel.      

Pulsed $I_{d}$– $V_{g}$ Methodology and Its Application to Electron-Trapping Characterization and Defect Density Profiling

The pulsed current–voltage ($I$– $V$) measurement technique with pulse times ranging from $sim$17 ns to $sim$ 6 ms was employed to study the effect of fast transient charging on the threshold voltage shift $Delta V_{t}$ of MOSFETs. The extracted $Delta V_{t}$ values are found to be strongly dependent on the band bending of the dielectric stack defined by the high-$kappa$ and interfacial layer dielectric constants and thicknesses, as well as applied voltages. Various hafnium-based gate stacks were found to exhibit a similar trap density profile.      

Optimal $ Sigma Delta$ Modulator Architectures for Fractional-$ {N}$ Frequency Synthesis

This paper presents a comparative study of $Sigma Delta$ modulators for use in fractional-$ {N}$ phase-locked loops. It proposes favorable modulator architectures while taking into consideration not only the quantization noise of the modulator but also other loop nonidealities such as the charge pump current mismatch that contributes to the degradation in the synthesized tone's phase noise. The proper choice of the modulator architecture is found to be dependent upon the extent of the nonideality, reference frequency, and loop bandwidth. Three modulator architectures are then proposed for low, medium, and high levels of nonidealities.      

High-Performance $hbox{In}_{0.7}hbox{Ga}_{0.3}hbox{As}$ -Channel MOSFETs With High-$kappa$ Gate Dielectrics and $alpha$-Si Passivation

Long and short buried-channel $hbox{In}_{0.7}hbox{Ga}_{0.3}hbox{As}$ MOSFETs with and without $alpha$-Si passivation are demonstrated. Devices with $alpha$-Si passivation show much higher transconductance and an effective peak mobility of 3810 $hbox{cm}^{2}/ hbox{V} cdot hbox{s}$. Short-channel MOSFETs with a gate length of 160 nm display a current of 825 $muhbox{A}/muhbox{m}$ at $V_{g} - V_{t} = hbox{1.6} hbox{V}$ and peak transconductance of 715 $muhbox{S}/muhbox{m}$. In addition, the virtual source velocity extracted from the short-channel devices is 1.4–1.7 times higher than that of Si MOSFETs. These results indicate that the high-performance $hbox{In}_{0.7}hbox{Ga}_{0.3} hbox{As}$-channel MOSFETs passivated by an $alpha$ -Si layer are promising candidates for advanced post-Si CMOS applications.      

High-Performance Poly-Silicon TFTs Using a High-$k$ $hbox{PrTiO}_{3}$ Gate Dielectric

In this letter, a polycrystalline-silicon thin-film transistor (poly-Si TFT) with a high- $k$ $hbox{PrTiO}_{3}$ gate dielectric is proposed for the first time. Compared to TFTs with a $hbox{Pr}_{2}hbox{O}_{3}$ gate dielectric, the electrical characteristics of poly-Si TFTs with a $hbox{PrTiO}_{3}$ gate dielectric can be significantly improved, such as lower threshold voltage, smaller subthreshold swing, higher $I_{rm on}/I_{rm off}$ current ratio, and larger field-effect mobility, even without any hydrogenation treatment. These improvements can be attributed to the high gate capacitance density and low grain-boundary trap state. All of these results suggest that the poly-Si TFT with a high- $k$ $hbox{PrTiO}_{3}$ gate dielectric is a good candidate for high-speed and low-power display driving circuit applications in flat-panel displays.      

High Density and Low Leakage Current in $ hbox{TiO}_{2}$ MIM Capacitors Processed at 300 $^{circ} hbox{C}$

We report Ir/TiO₂/TaN metal-insulator-metal capacitors processed at only 300degC, which show a capacitance density of 28 fF/mum² and a leakage current of 3 times 10^-8 (25degC) or 6 times 10^-7 (125degC) A/cm² at -1 V. This performance is due to the combined effects of 300degC nanocrystallized high-kappa TiO₂, a high conduction band offset, and high work-function upper electrode. These devices show potential for integration in future very-large-scale-integration technologies.     

22.7-dB Gain $-$19.7-dBm $ICP_{1{rm dB}}$ UWB CMOS LNA

A fully differential CMOS ultrawideband low-noise amplifier (LNA) is presented. The LNA has been realized in a standard 90-nm CMOS technology and consists of a common-gate stage and two subsequent common-source stages. The common-gate input stage realizes a wideband input impedance matching to the source impedance of the receiver (i.e., the antenna), whereas the two subsequent common-source stages provide a wideband gain by exploiting RLC tanks. The measurements have exhibited a transducer gain of 22.7 dB at 5.2 GHz, a 4.9-GHz-wide B _3dB, an input reflection coefficient lower than -10.5 dB, and an input-referred 1-dB compression point of -19.7 dBm, which are in excellent agreement with the postlayout simulation results, confirming the approach validity and the design robustness.     

InP DHBT Process in Transferred-Substrate Technology With $f_{t}$ and $f_{max}$ Over 400 GHz

In this paper, a double heterojunction bipolar transistor (DHBT) process has been developed in transferred-substrate (TS) technology to optimize high-frequency performance. It provides an aligned lithographic access to frontside and backside of the device to eliminate dominant transistor parasitics. The transistors of $hbox{0.8} times hbox{5}hbox{-}muhbox{m}^{2}$ emitter mesa feature $f_{t} = hbox{410} hbox{GHz}$ and $f_{max} = hbox{480} hbox{GHz}$ at a $hbox{BV}_{rm ceo} = hbox{5.5} hbox{V}$. Parallel to the device setup, a multilevel metallization scheme is established. It serves as construction kit for 3-D configurations of active and passive elements. High yield of the TS DHBTs, consistent large-signal modeling, and accurate simulation of complex passive elements have been demonstrated and have proved the availability of the technology for advanced millimeter-wave circuit design.      

Nonvolatile-Memory Characteristics of $hbox{AlO}^{-}$ -Implanted $hbox{Al}_{2}hbox{O}_{3}$

The nonvolatile-memory (NVM) characteristics of $hbox{AlO}^{-}$ -implanted $hbox{Al}_{2}hbox{O}_{3}$ structures are reported and shown to exhibit promising behaviors, including fast program/erase speeds and high-temperature data retention. Photoconductivity spectra show the existence of two dominant trap levels, located at around 2 and 4 eV below the conduction band minimum of $hbox{Al}_{2}hbox{O}_{3}$, and our calculations show that these levels are likely attributed to the defects in the $hbox{Al}_{2}hbox{O}_{3}$, such as the Al–O divacancy. The relative concentrations of these defects vary with the implant fluence and are shown to explain the NVM characteristics of the samples irradiated to different fluences.      

The Performance of Acoustic-Optical $Q$-switched Mode-Locking 1.34 $mu$m Nd:GdVO$_{4}$ Laser

A diode-end-pumped $Q$ -switched mode-locking $hbox{Nd:GdVO}_{4}$ laser operating at 1.34 $mu{hbox {m}}$ with an acousto-optical (AO) Q-switch in a compact V-type cavity was realized in our experiment for the first time. When the AO Q-switch repetition rate was 10 kHz, the maximum average output power of 750 mW and the pulse energy of 75 $muhbox{J}$ were obtained at the maximum incident pump power of 9 W. The mode-locking modulation depth of about 100% was obtained at certain pump power over the threshold. The mode-locked pulse inside in the $Q$-switched pulse had a repetition rate of 341 MHz, and its average pulsewidth was estimated to be about 350 ps. A developed rate equation model for the $Q$ -switched and mode-locked lasers with an AO Q-switch were proposed by using the hyperbolic secant functional methods. The results of numerical calculations of the rate equations were in good agreement with the experimental results.      

Scaling Properties of $hbox{Ge}$ –$hbox{Si}_{x}hbox{Ge}_{1 - x}$ Core–Shell Nanowire Field-Effect Transistors

We demonstrate the fabrication of high-performance $hbox{Ge}$ –$hbox{Si}_{x}hbox{Ge}_{1 - x}$ core–shell nanowire (NW) field-effect transistors with highly doped source (S) and drain (D) and systematically investigate their scaling properties. Highly doped S and D regions are realized by low-energy boron implantation, which enables efficient carrier injection with a contact resistance much lower than the NW resistance. We extract key device parameters, such as intrinsic channel resistance, carrier mobility, effective channel length, and external contact resistance, as well as benchmark the device switching speed and on/off current ratio.      

2 MHz AO $Q$ -switched ${rm TEM}_{00}$ Grazing Incidence Laser With 3 at.% Neodymium Doped Nd:YVO$_{4}$

We present a detailed experimental and theoretical study of the ultrahigh repetition rate AO $Q$ -switched ${rm TEM}_{00}$ grazing incidence laser. Up to 2.1 MHz $Q$-switching with ${rm TEM}_{00}$ output of 8.6 W and 2.2 MHz $Q$ -switching with multimode output of 10 W were achieved by using an acousto-optics $Q$ -switched grazing-incidence laser with optimum grazing-incidence angle and cavity configuration. The crystal was 3 at.% neodymium doped Nd:YVO$_{4}$ slab. The pulse duration at 2 MHz repetition rate was about 31 ns. The instabilities of pulse energy at 2 MHz repetition rate were less than ${pm}6.7hbox{%}$ with ${rm TEM}_{00}$ operation and ${pm}3.3hbox{%}$ with multimode operation respectively. The modeling of high repetition rate $Q$-switched operation is presented based on the rate equation, and with the solution of the modeling, higher pump power, smaller section area of laser mode, and larger stimulated emission cross section of the gain medium are beneficial to the $Q$-switched operation with ultrahigh repetition rate, which is in consistent with the experimental results.      

The $hbox{Pd/TiO}_{2}$/ $hbox{n}$-LTPS Thin-Film Schottky Diode on Glass Substrate for Hydrogen Sensing Applications

A $hbox{Pd/TiO}_{2}$/n-type low-temperature-polysilicon (n-LTPS) MOS thin-film Schottky diode fabricated on a glass substrate for hydrogen sensing is reported. The n-LTPS is an excimer-laser-annealed and $hbox{PH}_{3}$ -gas-plasma-treated amorphous-silicon (a-Si) thin film. At room temperature and $-$2-V bias, the developed MOS Schottky diode exhibited a high signal ratio of 1540 to 50 ppm of hydrogen gas, with a fast response time of 40 s, respectively. The signal ratio is better or comparable with that of other reported MOS-type hydrogen gas sensors prepared on Si or III–V compound substrate. In addition, the signal ratio is 7.6, 14, and 30 times over other interfering gases of $ hbox{C}_{2}hbox{H}_{5}hbox{OH}$, $hbox{C}_{2}hbox{H}_{4}$ , and $hbox{NH}_{3}$ at room temperature and a concentration of 8000 ppm at $-$2-V bias, respectively. Thus, the developed MOS Schottky diode shows promise for the future development and commercialization of a low-cost hydrogen sensor.      

Improved Electrical Properties of Ge p-MOSFET With $ hbox{HfO}_{2}$ Gate Dielectric by Using $hbox{TaO}_{x} hbox{N}_{y}$ Interlayer

The electrical characteristics of germanium p-metal-oxide-semiconductor (p-MOS) capacitor and p-MOS field-effect transistor (FET) with a stack gate dielectric of HfO₂/TaOxNy are investigated. Experimental results show that MOS devices exhibit much lower gate leakage current than MOS devices with only HfO₂ as gate dielectric, good interface properties, good transistor characteristics, and about 1.7-fold hole-mobility enhancement as compared with conventional Si p-MOSFETs. These demonstrate that forming an ultrathin passivation layer of TaOxNy on germanium surface prior to deposition of high-k dielectrics can effectively suppress the growth of unstable GeOx, thus reducing interface states and increasing carrier mobility in the inversion channel of Ge-based transistors.     

ZnO Nanowire and $hbox{WS}_{2}$ Nanotube Electronics

In this paper, we report on the synthesis and applications of semiconducting nanostructures. Nanostructures of interest were zinc oxide (ZnO) nanowires and tungsten disulfide $(hbox{WS}_{2})$ nanotubes where transistors/phototransistors and photovoltaic (PV) energy conversion cells have been fabricated. ZnO nanowires were grown with both high- and low-temperature approaches, depending on the application. Individual ZnO nanowire side-gated transistors revealed excellent performance with a field-effect mobility of 928 $hbox{cm}^{2}/hbox{V} cdot hbox{s}$. ZnO networks were proposed for large-area macroelectronic devices as a less lithographically intense alternative to individual nanowire transistors where mobility values in excess of 20 $ hbox{cm}^{2}/hbox{V} cdot hbox{s}$ have been achieved. Flexible PV devices utilizing ZnO nanowires as electron acceptors and for photoinduced charge separation and transport have been presented. Phototransistors were fabricated using individual $hbox{WS}_{2}$ nanotubes, where clear sensitivity to visible light has been observed. The results presented here simply reveal the potential use of inorganic nanowires/tubes for various optoelectronic devices.      

$V_{rm th}$ Control by Complementary Hot-Carrier Injection for SONOS Multi-Level Cell Flash Memory

In this paper, a complementary hot-carrier injection programming/erasing (P/E) scheme is proposed for accurate threshold voltage $(V_{rm th})$ control for polysilicon–oxide–nitride–oxide–silicon (SONOS) multi-level cell (MLC) Flash memory. Alternate hot electrons (HEs) and hot holes (HHs) are injected by pulse gate and drain biases, and complementary HE and HH injections spontaneously correct the $V_{rm th}$ offsets via a feedback control enabled by the programming and the offset-correcting cycles. The HE and HH fluxes are balanced at a steady state induced by the tunnel oxide potential transformation. Accurate $V_{rm th}$ control is accomplished, and endurance reliability is significantly improved for SONOS MLCs.      

Dual-Gate Graphene FETs With $f_{T}$ of 50 GHz

A dual-gate graphene field-effect transistor is presented, which shows improved radio-frequency (RF) performance by reducing the access resistance using electrostatic doping. With a carrier mobility of 2700 cm²/V · s, a cutoff frequency of 50 GHz is demonstrated in a 350-nm-gate-length device. This f_T value is the highest frequency reported to date for any graphene transistor, and it also exceeds that of Si MOS field-effect transistors at the same gate length, illustrating the potential of graphene for RF applications.