Effects of interstitial oxygen defects at HfO/sub x/N/sub y//Si interface on electrical characteristics of MOS devices

Effects of the defects at high-/spl kappa/ dielectric/Si interface on the electrical characteristics of MOS devices are important issues. To study these issues, a low defect (denuded zone) at Si surface was formed by a high-temperature annealing in hydrogen atmosphere in this paper. Our results reveal that HfO/sub x/N/sub y/ demonstrates significant improvement on the electrical properties of MOS devices due to its low amount of the interstitial oxygen [O/sub i/] and the crystal-originated particles defects as well as small surface roughness at HfO/sub x/N/sub y//Si interface. The current-conduction mechanism of the HfO/sub x/N/sub y/ film at the low- and high-electrical field and high-temperature (T>100/spl deg/C) is dominated by Schottky emission and Frenkel-Poole (FP) emission, respectively. The trap energy level involved in FP conduction was estimated to be around 0.5eV. Reduced gate leakage current, stress-induced leakage current and defect generation rate, attributable to the reduction of defects at HfO/sub x/N/sub y//Si interface, were observed for devices with denuded zone. The variable rise and fall time bipolar-pulse-induced current technique was used to determine the energy distribution of interface trap density (D/sub it/). The results exhibit that relatively low D/sub it/ can be attributed to the reduction of defects at Si surface. By using denuded zone at the Si surface, HfO/sub x/N/sub y/ has demonstrated significant improvement on electrical properties as compared to SiO/sub x/N/sub y/.     

Modeling of tunneling currents through HfO/sub 2/ and (HfO/sub 2/)/sub x/(Al/sub 2/O/sub 3/)/sub 1-x/ gate stacks

We present a physical modeling of tunneling currents through ultrathin high-/spl kappa/ gate stacks, which includes an ultrathin interface layer, both electron and hole quantization in the substrate and gate electrode, and energy band offsets between high-/spl kappa/ dielectrics and Si determined from high-resolution XPS. Excellent agreements between simulated and experimentally measured tunneling currents have been obtained for chemical vapor deposited and physical vapor deposited HfO/sub 2/ with and without NH/sub 3/-based interface layers, and ALD Al/sub 2/O/sub 3/ gate stacks with different EOT and bias polarities. This model is applied to more thermally stable (HfO/sub 2/)/sub x/(Al/sub 2/O/sub 3/)/sub 1-x/ gate stacks in order to project their scalability for future CMOS applications.     

Ultrathin Al/sub 2/O/sub 3/ and HfO/sub 2/ gate dielectrics on surface-nitrided Ge

We have studied ultrathin Al/sub 2/O/sub 3/ and HfO/sub 2/ gate dielectrics on Ge grown by ultrahigh vacuum-reactive atomic-beam deposition and ultraviolet ozone oxidation. Al/sub 2/O/sub 3/-Ge gate stack had a t/sub eq//spl sim/23 /spl Aring/, and three orders of magnitude lower leakage current compared to SiO/sub 2/. HfO/sub 2/-Ge allowed even greater scaling, achieving t/sub eq//spl sim/11 /spl Aring/ and six orders of magnitude lower leakage current compared to SiO/sub 2/. We have carried out a detailed study of cleaning conditions for the Ge wafer, dielectric deposition condition, and anneal conditions and their effect on the electrical properties of metal-gated dielectric-Ge capacitors. We show that surface nitridation is important in reducing hysteresis, interfacial layer formation and leakage current. However, surface nitridation also introduces positive trapped charges and/or dipoles at the interface, resulting in significant flatband voltage shifts, which are mitigated by post-deposition anneals.     

Electrical and physical characterization of remote plasma oxidized HfO/sub 2/ gate dielectrics

Bi-layer gate stacks consisting of a HfO/sub 2/ and an interfacial layer are fabricated by remote plasma oxidation (RPO) of Hf metal deposited on an Si substrate. Hf metal is fully oxidized by the RPO even at a temperature as low as 400/spl deg/C due to radical oxygens, leading to an improvement in the quality of HfO/sub 2/ with less impact to the interfacial layer growth. An insufficient oxidation leads to a deterioration of mobility with increasing interface traps and positive bias temperature instability, which is likely caused by the oxygen vacancies acting as traps induced by the remaining Hf metal. The SiO/sub 2/-like interface improves the mobility with reduced interface states. Full oxidation and the controlled SiO/sub 2/-like interface demonstrate RPO as a promising way for gate-stack optimization.     

Mobility enhancement in TaN metal-gate MOSFETs using tantalum incorporated HfO/sub 2/ gate dielectric

TaN metal-gate nMOSFETs using HfTaO gate dielectrics have been investigated for the first time. Compared to pure HfO/sub 2/, a reduction of one order of magnitude in interface state density (D/sub it/) was observed in HfTaO film. This may be attributed to a high atomic percentage of Si-O bonds in the interfacial layer between HfTaO and Si. It also suggests a chemical similarity of the HfTaO-Si interface to the high-quality SiO/sub 2/-Si interface. In addition, a charge trapping-induced threshold voltage (V/sub th/) shift in HfTaO film with constant voltage stress was 20 times lower than that of HfO/sub 2/. This indicates that the HfTaO film has fewer charged traps compared to HfO/sub 2/ film. The electron mobility in nMOSFETs with HfO/sub 2/ gate dielectric was significantly enhanced by incorporating Ta.     

Process optimization for high electron mobility in nMOSFETs with aggressively scaled HfO/sub 2//metal stacks

The performance of aggressively scaled (1.4nm相似文献   

Low-frequency noise behavior of SiO/sub 2/--HfO/sub 2/ dual-layer gate dielectric nMOSFETs with different interfacial oxide thickness

The low-frequency noise has been studied in nMOSFETs with an HfO/sub 2/--SiO/sub 2/ gate stack, for different thickness of the SiO/sub 2/ interfacial layer (IL). It is observed that the 1/f-like noise in linear operation, is about 50 times higher in the HfO/sub 2/ devices with a 0.8-nm chemical oxide IL, compared with the 4.5-nm thermal oxide reference n-channel transistors. This is shown to relate to the correspondingly higher trap density in the dielectric material. In addition, it is demonstrated that the noise rapidly reduces with increasing thickness of the IL. From the results for a 2.1-nm SiO/sub 2/ IL, it is derived that at a certain gate voltage range, electron tunneling to a defect band in the HfO/sub 2/ layer may contribute to a pronounced increase in the flicker noise.     

Fabrication and mobility characteristics of SiGe surface channel pMOSFETs with a HfO/sub 2//TiN gate stack

This paper describes an extensive experimental study of TiN/HfO/sub 2//SiGe and TiN/HfO/sub 2//Si cap/SiGe gate stacked-transistors. Through a careful analysis of the interface quality (interface states and roughness), we demonstrate that an ultrathin silicon cap is mandatory to obtain high hole mobility enhancement. Based on quantum mechanical simulations and capacitance-voltage characterization, we show that this silicon cap is not contributing any silicon parasitic channel conduction and degrades by only 1 /spl Aring/ the electrical oxide thickness in inversion. Due to this interface optimization, Si/sub 0.72/Ge/sub 0.28/ pMOSFETs exhibit a 58% higher mobility at high effective field (1 MV/cm) than the universal SiO/sub 2//Si reference and a 90% higher mobility than the HfO/sub 2//Si reference. This represents one of the best hole mobility results at 1 MV/cm ever reported with a high-/spl kappa//metal gate stack. We thus validate a possible solution to drastically improve the hole mobility in Si MOSFETs with high-/spl kappa/ gate dielectrics.     

TDDB and polarity-dependent reliability of high-quality, ultrathin CVD HfO/sub 2/ gate stack with TaN gate electrode

In this letter, we present a comprehensive study on longterm reliability of ultrathin TaN-gated chemical vapor deposition gate stack with EOT=8.5-10.5. It is found that, due to the asymmetric band structure of HfO/sub 2/ gate stack with an interfacial layer, the HfO/sub 2/ gate stack shows polarity-dependent leakage current, critical defect density, and defect generation rate, under gate and substrate injection. However, no such polarity dependence of time-to-breakdown (T/sub BD/) is observed when T/sub BD/ is plotted as a function of gate voltage. The 10-year lifetime of an HfO/sub 2/ gate stack is projected to be Vg=-1.63 V for the equivalent oxide thickness (EOT) =8.6 and Vg=-1.88 V for EOT=10.6 at 25/spl deg/C. These excellent reliability characteristics are attributed to reduced leakage current of HfO/sub 2/ gate stack with physically thicker films that result in larger critical defect density and Weibull slope to that of SiO/sub 2/ for the same EOT. However, at 150/spl deg/C, and with area scaling to 0.1 cm/sup 2/ and low percentile of 0.01%, the maximum allowed voltages are projected to Vg=-0.6 V and -0.75 V for EOT of 8.6, and 10.6, respectively.     

Mechanism of positive-bias temperature instability in sub-1-nm TaN/HfN/HfO/sub 2/ gate stack with low preexisting traps

In this letter, the positive-bias temperature instability (PBTI) characteristics of a TaN/HfN/HfO/sub 2/ gate stack with an equivalent oxide thickness (EOT) of 0.95 nm and low preexisting traps are studied. The negligible PBTI at room temperature, the so-called "turn-around" phenomenon, and the negative shifts of the threshold voltage (V/sub t/) are observed. A modified reaction-diffusion (R-D) model, which is based on the electric stress induced defect generation (ESIDG) mechanism, is proposed to explain the above-mentioned PBTI characteristics. In this modified R-D model, PBTI is attributed to the electron-induced breaking of Si-O bonds at interfacial layer (IL) between HfO/sub 2/ and Si substrate and the diffusion/drift of oxygen ions (O/sup -/) from Si-O bonds into HfO/sub 2/ layer under positive-bias temperature stressing. The ESIDG mechanism is responsible for the breaking of Si-O bonds. The measured activation energy (E/sub a/) is consistent with the one predicted by the ESIDG mechanism.     

Characterization and reliability of dual high-k gate dielectric stack (poly-Si-HfO/sub 2/-SiO/sub 2/) prepared by in situ RTCVD process for system-on-chip applications

We investigate for the first time the possibility of integrating chemical vapor deposition (CVD) HfO/sub 2/ into the multiple gate dielectric system-on-a-chip (SoC) process in the range of 6-7 nm, which supports higher voltage (2.5-5 V operation/tolerance). Results show that CVD HfO/sub 2/-SiO/sub 2/ stacked gate dielectric (EOT =6.2 nm) exhibits lower leakage current than that of SiO/sub 2/ (EOT =5.7 nm) by a factor of /spl sim/10/sup 2/, with comparable interface quality (D/sub it//spl sim/1/spl times/10/sup 10/ cm/sup -2/eV/sup -1/). The presence of negative fixed charge is observed in the HfO/sub 2/-SiO/sub 2/ gate stack. In addition, the addition of HfO/sub 2/ on SiO/sub 2/ does not alter the dominant conduction mechanism of Fowler-Nordheim tunneling in the HfO/sub 2/-SiO/sub 2/ gate stack. Furthermore, the HfO/sub 2/-SiO/sub 2/ gate stack shows longer time to breakdown T/sub BD/ than SiO/sub 2/ under constant voltage stress. These results suggest that it may be feasible to use such a gate stack for higher voltage operation in SoC, provided other key requirements such as V/sub t/ stability (charge trapping under stress) can be met and the negative fixed charge eliminated.     

Evaluation of NBTI in HfO/sub 2/ gate-dielectric stacks with tungsten gates

Negative-bias temperature instability (NBTI) of the threshold voltage in ultrathin HfO/sub 2/ p-type field-effect transistors (pFET) with tungsten gates is reported. The dependence of threshold voltage, transconductance peak, and interface trap density on stress time is investigated for various negative stress voltages and temperatures. The measurements show that the threshold voltage shifts with a concomitant decrease in transconductance peak and increase in interface trap density as assessed by subthreshold slope and dc current-voltage (DCIV) method. The threshold voltage shift data are fitted with a stretched exponential equation and the fits are used for estimating lifetime. The measurements show that NBTI-related degradation in HfO/sub 2/ stacks is comparable to that observed in SiO/sub 2//poly Si pFETs.     

Theoretical and experimental investigation of Si nanocrystal memory device with HfO/sub 2/ high-k tunneling dielectric

In this paper, silicon (Si) nanocrystal memory using chemical vapor deposition (CVD) HfO/sub 2/ high-k dielectrics to replace the traditional SiO/sub 2/ tunneling/control dielectrics has been fabricated and characterized for the first time. The advantages of this approach for improved nanocrystal memory operation have also been studied theoretically. Results show that due to its unique band asymmetry in programming and retention mode, the use of high-k dielectric on Si offers lower electron barrier height at dielectric/Si interface and larger physical thickness, resulting in a much higher J/sub g,programming//J/sub g,retention/ ratio than that in SiO/sub 2/ and therefore faster programming and longer retention. The fabricated device with CVD HfO/sub 2/ shows excellent programming efficiency and data-retention characteristics, thanks to the combination of a lower electron barrier height and a larger physical thickness of HfO/sub 2/ as compared with SiO/sub 2/ of the same electrical oxide thickness (EOT). It also shows clear single-electron charging effect at room temperature and superior data endurance up to 10/sup 6/ write/erase cycles.     

Low-frequency noise in submicrometer MOSFETs with HfO/sub 2/, HfO/sub 2//Al/sub 2/O/sub 3/ and HfAlO/sub x/ gate stacks

Low-frequency noise measurements were performed on p- and n-channel MOSFETs with HfO/sub 2/, HfAlO/sub x/ and HfO/sub 2//Al/sub 2/O/sub 3/ as the gate dielectric materials. The gate length varied from 0.135 to 0.36 /spl mu/m with 10.02 /spl mu/m gate width. The equivalent oxide thicknesses were: HfO/sub 2/ 23 /spl Aring/, HfAlO/sub x/ 28.5 /spl Aring/ and HfO/sub 2//Al/sub 2/O/sub 3/ 33 /spl Aring/. In addition to the core structures with only about 10 /spl Aring/ of oxide between the high-/spl kappa/ dielectric and silicon substrate, there were "double-gate oxide" structures where an interfacial oxide layer of 40 /spl Aring/ was grown between the high-/spl kappa/ dielectric and Si. DC analysis showed low gate leakage currents in the order of 10/sup -12/A(2-5/spl times/10/sup -5/ A/cm/sup 2/) for the devices and, in general, yielded higher threshold voltages and lower mobility values when compared to the corresponding SiO/sub 2/ devices. The unified number-mobility fluctuation model was used to account for the observed 1/f noise and to extract the oxide trap density, which ranged from 1.8/spl times/10/sup 17/ cm/sup -3/eV/sup -1/ to 1.3/spl times/10/sup 19/ cm/sup -3/eV/sup -1/, somewhat higher compared to conventional SiO/sub 2/ MOSFETs with the similar device dimensions. There was no evidence of single electron switching events or random telegraph signals. The aim of this paper is to present a general discussion on low-frequency noise characteristics of the three different high-/spl kappa//gate stacks, relative comparison among them and to the Si--SiO/sub 2/ system.     

Carrier transport in HfO/sub 2//metal gate MOSFETs: physical insight into critical parameters

Electron and hole mobility in HfO/sub 2//metal gate MOSFETs is deeply studied through low-temperature measurements down to 4.2 K. Original technological splits allow the decorrelation of the different scattering mechanisms. It is found that even when charge trapping is negligible, strong remote coulomb scattering (RCS) due to fixed charges or dipoles causes most of the mobility degradation. The effective charges are found to be located in the HfO/sub 2/ near the SiO/sub 2/ interface within 2 nm. Experimental results are well reproduced by RCS calculation using 7/spl times/10/sup 13/ cm/sup -2/ fixed charges at the HfO/sub 2//SiO/sub 2/ interface. We also discuss the role of remote phonon scattering in such gate stacks. Interactions with surface soft-optical phonon of HfO/sub 2/ are clearly evidenced for a metal gate but remain of second order. All these remote interactions are significant for an interfacial oxide thickness up to 2 nm, over which, these are negligible. Finally, the metal gate (TiN) itself induces a modified surface-roughness term that impacts the low to high effective field mobility even for the SiO/sub 2/ gate dielectric references.     

Low-frequency noise in submicrometer MOSFETs with HfO/sub 2/, HfO/sub 2//Al/sub 2/O/sub 3/ and HfAlO/sub x/ gate stacks

Low-frequency noise measurements were performed on p- and n-channel MOSFETs with HfO/sub 2/, HfAlO/sub x/ and HfO/sub 2//Al/sub 2/O/sub 3/ as the gate dielectric materials. The gate length varied from 0.135 to 0.36 /spl mu/m with 10.02 /spl mu/m gate width. The equivalent oxide thicknesses were: HfO/sub 2/ 23 /spl Aring/, HfAlO/sub x/ 28.5 /spl Aring/ and HfO/sub 2//Al/sub 2/O/sub 3/ 33 /spl Aring/. In addition to the core structures with only about 10 /spl Aring/ of oxide between the high-K dielectric and silicon substrate, there were "double-gate oxide" structures where an interfacial oxide layer of 40 /spl Aring/ was grown between the high-K dielectric and Si. DC analysis showed low gate leakage currents in the order of 10/sup -12/ A(2-5 /spl times/ 10/sup -5/ A/cm/sup 2/) for the devices and, in general, yielded higher threshold voltages and lower mobility values when compared to the corresponding SiO/sub 2/ devices. The unified number-mobility fluctuation model was used to account for the observed 1/f noise and to extract the oxide trap density, which ranged from 1.8 /spl times/ 10/sup 17/ cm/sup -3/ eV/sup -1/ to 1, 3 /spl times/ 10/sup 19/ cm/sup -3/ eV/sup -1/ somewhat higher compared to conventional SiO/sub 2/ MOSFETs with the similar device dimensions. There was no evidence of single electron switching events or random telegraph signals. The aim of this paper is to present a general discussion on low-frequency noise characteristics of the three different high-K/gate stacks, relative comparison among them and to the Si-SiO/sub 2/ system.     

Low-frequency noise in TaSiN/HfO/sub 2/ nMOSFETs and the effect of stress-relieved preoxide interfacial layer

Low-frequency noise characteristics are reported for TaSiN-gated n-channel MOSFETs with atomic-layer deposited HfO/sub 2/ on thermal SiO/sub 2/ with stress-relieved preoxide (SRPO) pretreatment. For comparison, control devices were also included with chemical SiO/sub 2/ resulting from standard Radio Corporation of America clean process. The normalized noise spectral density values for these devices are found to be lower when compared to reference poly Si gate stack with similar HfO/sub 2/ dielectric. Consequently, a lower oxide trap density of /spl sim/4/spl times/10/sup 17/ cm/sup -3/eV/sup -1/ is extracted compared to over 3/spl times/10/sup 18/ cm/sup -3/eV/sup -1/ values reported for poly Si devices indicating an improvement in the high-/spl kappa/ and interfacial layer quality. In fact, this represents the lowest trap density values reported to date on HfO/sub 2/ MOSFETs. The peak electron mobility measured on the SRPO devices is over 330 cm/sup 2//V/spl middot/s, much higher than those for equivalent poly Si or metal gate stacks. In addition, the devices with SRPO SiO/sub 2/ are found to exhibit at least /spl sim/10% higher effective mobility than RCA devices, notwithstanding the differences in the high-/spl kappa/ and interfacial layer thicknesses. The lower Coulomb scattering coefficient obtained from the noise data for the SRPO devices imply that channel carriers are better screened due to the presence of SRPO SiO/sub 2/, which, in part, contributes to the mobility improvement.     

ScN/sub x/ gate on atomic layer deposited HfO/sub 2/ and effect of high-pressure wet post deposition annealing

For nMOS devices with HfO/sub 2/, a metal gate with a very low workfunction is necessary. In this letter, the effective workfunction (/spl Phi//sub m,eff/) values of ScN/sub x/ gates on both SiO/sub 2/ and atomic layer deposited (ALD) HfO/sub 2/ are evaluated. The ScN/sub x//SiO/sub 2/ samples have a wide range of /spl Phi//sub m,eff/ values from /spl sim/ 3.9 to /spl sim/ 4.7 eV, and nMOS-compatible /spl Phi//sub m,eff/ values can be obtained. However, the ScN/sub x/ gates on conventional post deposition-annealed HfO/sub 2/ show a relatively narrow range of /spl Phi//sub m,eff/ values from /spl sim/ 4.5 to /spl sim/ 4.8 eV, and nMOS-compatible /spl Phi//sub m,eff/ values cannot be obtained due to the Fermi-level pinning (FLP) effect. Using high-pressure wet post deposition annealing, we could dramatically reduce the extrinsic FLP. The /spl Phi//sub m,eff/ value of /spl sim/ 4.2 eV was obtained for the ScN/sub x/ gate on the wet-treated HfO/sub 2/. Therefore, ScN/sub x/ metal gate is a good candidate for nMOS devices with ALD HfO/sub 2/.     

Charge trapping and dielectric reliability of SiO/sub 2/-Al/sub 2/O/sub 3/ gate stacks with TiN electrodes

A detailed study on charge trapping and dielectric reliability of SiO/sub 2/-Al/sub 2/O/sub 3/ gate stacks with TiN electrodes has been carried out. Due to the inherent asymmetry of the dual layer stack all electrical properties studied were found to be strongly polarity dependent. The gate current is strongly reduced for injection from the TiN (gate) electrode compared to injection from the n-type Si substrate. For substrate injection, electron trapping occurs in the bulk of the Al/sub 2/O/sub 3/ film, whereas for gate injection mainly hole trapping near the Si substrate is observed. Furthermore, no significant interface state generation is evident for substrate injection. In case of gate injection a rapid build up of interface states occurs already at small charge fluence (q/sub inj/ /spl sim/ 1 mC/cm/sup 2/). Dielectric reliability is consistent with polarity-dependent defect generation. For gate injection the interfacial layer limits the dielectric reliability and results in low Weibull slopes independent of the Al/sub 2/O/sub 3/ thickness. In the case of substrate injection, reliability is limited by the bulk of the Al/sub 2/O/sub 3/ layer leading to a strong thickness dependence of the Weibull slope as expected by the percolation model.     

Gate-first Germanium nMOSFET with CVD HfO/sub 2/ gate dielectric and silicon surface passivation

A gate-first self-aligned Ge n-channel MOSFET (nMOSFET) with chemical vapor deposited (CVD) high-/spl kappa/ gate dielectric HfO/sub 2/ was demonstrated. By tuning the thickness of the ultrathin silicon-passivation layer on top of the germanium, it is found that increasing the silicon thickness helps to reduce the hysteresis, fixed charge in the gate dielectric, and interface trap density at the oxide/semiconductor interface. About 61% improvement in peak electron mobility of the Ge nMOSFET with a thick silicon-passivation layer over the CVD HfO/sub 2//Si system was achieved.