Compact Variable ${rm TE}$-${rm TM}$ Polarization Splitter Based on Simplified Coherent Coupling in Lithium Niobate

A compact-sized electrically tunable ${rm TE}$- ${rm TM}$ mode splitter composed of a mode converter and an asymmetric Y-branch structure is presented. The asymmetric Y-branch consists of a straight and a bent waveguides to split two polarization modes based on the mode-sorting effect. To shorten the device length, a simplified coherently coupled-bending structure is utilized for the bent waveguide. Experimental results show that the device length is reduced about 52%, extinction ratios of both ${rm TE}$ and ${rm TM}$ modes are higher than 25 dB, yet the applied voltage is not significantly increased.      

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.      

Leakage Minimization of SRAM Cells in a Dual-$V_t$ and Dual-$T_{rm ox}$ Technology

Aggressive CMOS scaling results in low threshold voltage and thin oxide thickness for transistors manufactured in deep submicrometer regime. As a result, reducing the subthreshold and tunneling gate leakage currents has become one of the most important criteria in the design of VLSI circuits. This paper presents a method based on dual- V t and dual- T _ox assignment to reduce the total leakage power dissipation of static random access memories (SRAMs) while maintaining their performance. The proposed method is based on the observation that read and write delays of a memory cell in an SRAM block depend on the physical distance of the cell from the sense amplifier and the decoder. Thus, the idea is to deploy different configurations of six-transistor SRAM cells corresponding to different threshold voltage and oxide thickness assignments for the transistors. Unlike other techniques for low-leakage SRAM design, the proposed technique incurs neither area nor delay overhead. In addition, it results in a minor change in the SRAM design flow. The leakage saving achieved by using this technique is a function of the values of the high threshold voltage and the oxide thickness, as well as the number of rows and columns in the cell array. Simulation results with a 65-nm process demonstrate that this technique can reduce the total leakage power dissipation of a 64 times 512 SRAM array by 33% and that of a 32 times 512 SRAM array by 40%.     

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.     

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.     

$V_{rm th}$ 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.      

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.      

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.      

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.      

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.      

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.      

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.     

A Differential Clapp-VCO in 0.13 $mu{rm m}$ CMOS Technology

A new differential voltage-controlled oscillator (VCO) is designed and implemented in a 0.13 $mu{rm m}$ CMOS 1P8M process. The designed circuit topology is an all nMOS LC-tank Clapp-VCO using a series-tuned resonator. At the supply voltage of 0.9 V, the output phase noise of the VCO is $-$110.5 dBc/Hz at 1 MHz offset frequency from the carrier frequency of 18.78 GHz, and the figure of merit is $-$188.67 dBc/Hz. The core power consumption is 5.4 mW. Tuning range is about 3.43 GHz, from 18.79 to 22.22 GHz, while the control voltage was tuned from 0 to 1.3 V.      

In Situ Comparison of Si/High- $kappa$ and $hbox{Si}/ hbox{SiO}_{2}$ Channel Properties in SOI MOSFETs

Detailed measurements of front- and back-channel characteristics in advanced SOI MOSFETs (ultrathin Si film, high-kappa, metal gate, and selective epitaxy of source/drain) are used to reveal and compare the transport properties at the corresponding Si/high- kappa (HfO₂ or HfSiON) and Si/SiO₂ interfaces. Low-temperature operation magnifies the difference between these two interfaces in terms of carrier mobility, threshold voltage, and subthreshold swing. As compared with Si/SiO₂, the low-field mobility is lower at the Si/high-kappa interface and increases less rapidly at low temperature, reflecting additional scattering mechanisms governed by high-kappa and neutral defects.     

Improvement of On–Off-Current Ratio in $ hbox{TiO}_{rm x}$ Active-Channel TFTs Using $hbox{N}_{2} hbox{O}$ Plasma Treatment

Without sacrificing the on-current in the transfer characteristics, we have successfully reduced the off-current part by the optimal $hbox{N}_{2}hbox{O}$ plasma treatment to improve the on–off-current ratio in n-type titanium oxide $( hbox{TiO}_{rm x})$ active-channel thin-film transistors. While the high-power (275 W) $hbox{N}_{2}hbox{O}$ plasma treatment oxidizes the whole $hbox{TiO}_{rm x}$ channel and results in the reduction of both on- and off-current, the optimized low-power (150 W) process makes the selective oxidation of the top portion in the channel and reduces only the off-current significantly. Increase in on–off ratio by almost five orders of magnitude is achieved without change in on-current by using the presented method.      

Spectroscopy and Diode-Pumped Laser Experiments of LiLuF$_{bf 4}$:Tm$^{{bf 3}+}$ Crystals

In this work we report on the 2-${mbi mu}$m laser emission of LiLuF ${_{bf 4}}$ crystals doped with Thulium trivalent ions (Tm:LLF) at different doping density up to 16%. We will present our results regarding growth, absorption and emission spectroscopy, Judd–Ofelt analysis and room temperature diode pumping laser experiments as a function of the dopant density. The best result is 56% of slope efficiency, with a maximum output power of 280 mW. The emission wavelength ranges between 1985 and 2038 nm, exploiting the vibronic emission of Tm in LLF.      

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.      

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.