Novel dual-metal gate technology using Mo-MoSi/sub x/ combination

A novel dual-metal gate technology that uses a combination of Mo-MoSi/sub x/ gate electrodes is proposed. An amorphous-Si/Mo stack was fabricated as a gate electrode for the n-channel device. It was thermally annealed to form MoSi/sub x/. Pure Mo served as the gate electrode for the p-channel device. The work functions of MoSi/sub x/ and pure Mo gates on SiO/sub 2/ are 4.38 and 4.94 eV, respectively, which are appropriate for devices with advanced transistor structures. The small increase in the work function (< 20 meV) and the negligible equivalent oxide thickness variation (< 0.08 nm) after rapid thermal annealing at 950 /spl deg/C for 30 s also demonstrate the excellent thermal stabilities of Mo and MoSi/sub x/ on SiO/sub 2/. Additional arsenic ion implantation prior to silicidation was demonstrated further to lower the work function of MoSi/sub x/ to 4.07 eV. This approach for modulating the work function makes the proposed combination of Mo-MoSi/sub x/ gate electrodes appropriate for conventional bulk devices. The developed dual-metal-gate technology on HfO/sub 2/ gate dielectric was also evaluated. The effective work functions of pure Mo and undoped MoSi/sub x/ gates on HfO/sub 2/ are 4.89 and 4.34 eV, respectively. A considerable work-function shift was observed on the high-/spl kappa/ gate dielectric. The effect of arsenic preimplantation upon the work function of the metal silicide on HfO/sub 2/ was also demonstrated, even though the range of modulation was a little reduced.     

Thermal stability of Hf/sub x/Ta/sub y/N metal gate electrodes for advanced MOS devices

In this letter, the composition effects of hafnium (Hf) and tantalum (Ta) in Hf/sub x/Ta/sub y/N metal gate on the thermal stability of MOS devices were investigated. The work function of the Hf/sub x/Ta/sub y/N metal gate can reach a value of /spl sim/4.6 eV (midgap of silicon) by suitably adjusting the Hf and Ta compositions. In addition, with a small amount of Hf incorporated into a TaN metal gate, excellent thermal stability of electrical properties, including the work function, the equivalent oxide thickness, interface trap density and defect generation rate characteristics, can be achieved after a post-metal anneal up to 950/spl deg/C for 45 s. Experimental results indicate that Ta-rich Hf/sub x/Ta/sub y/N is a promising metal gate for advanced MOS devices.     

Fermi-level pinning induced thermal instability in the effective work function of TaN in TaN/SiO/sub 2/ gate stack

In this letter, we demonstrate for the first time that the Fermi-level pinning caused by the formation of Ta(N)-Si bonds at the TaN/SiO/sub 2/ interface is responsible for the thermal instability of the effective work function of TaN in TaN/SiO/sub 2/ devices after high temperature rapid thermal annealing (RTA). Because of weak charge transfer between Hf and Ta(N) and hence negligible pinning effect at the TaN/HfO/sub 2/ interface, the effective work function of TaN is significantly more thermally stable on HfO/sub 2/ than on SiO/sub 2/ dielectric during RTA. This finding provides a guideline for the work function tuning and the integration of metal gate with high-/spl kappa/ dielectric for advanced CMOS devices.     

Characteristics of HfO/sub 2/ pMOSFET prepared by B/sub 2/H/sub 6/ plasma doping and KrF excimer laser annealing

The electrical characteristics of HfO/sub 2/ pMOSFETs prepared by B/sub 2/H/sub 6/ plasma doping and excimer laser annealing were investigated. Various metal gate electrodes were evaluated to protect the high-/spl kappa/ oxide during laser irradiation. Although the aluminum gate electrode showed superior reflectivity to the laser, the equivalent oxide thickness was increased due to the interaction between aluminum and HfO/sub 2/, which resulted in reduced capacitance. In contrast, the Al-TaN stacked gate showed good reflectivity up to laser energy of 500 mJ/cm/sup 2/ and improved capacitance was obtained compared with the Al gate. For the first time, the electrical characteristics of a HfO/sub 2/ pMOSFET with an Al-TaN gate fabricated by plasma doping and excimer laser annealing were demonstrated. It was also demonstrated that plasma doping and excimer laser annealing combined with a metal gate could be applied for high-/spl kappa/ oxide MOSFET fabrication.     

Thermally robust TaTb/sub x/N metal gate electrode for n-MOSFETs applications

In this letter, we study Terbium (Tb)-incorporated TaN (TaTb/sub x/N) as a thermally robust N-type metal gate electrode for the first time. The work function of the Ta/sub 0.94/Tb/sub 0.06/N/sub y/ metal gate is determined to be /spl sim/4.23 eV after rapid thermal anneal at 1000/spl deg/C for 30 s, and can be further tuned by varying the Tb concentration. Moreover, the TaTb/sub x/N-SiO/sub 2/ gate stack exhibits excellent thermal stability up to 1000/spl deg/C with no degradation to the equivalent oxide thickness, gate leakage, and time-dependent dielectric breakdown (TDDB) characteristics. These results suggest that Tb-incorporated TaN (TaTb/sub x/N) could be a promising metal gate candidate for n-MOSFET in a dual-metal gate Si CMOS process.     

A dual-metal gate integration process for CMOS with sub-1-nm EOT HfO/sub 2/ by using HfN replacement gate

A replacement gate process employing a HfN dummy gate and sub-1-nm equivalent oxide thickness (EOT) HfO/sub 2/ gate dielectric is demonstrated. The excellent thermal stability of the HfN-HfO/sub 2/ gate stack enables its use in high temperature CMOS processes. The replacement of HfN with other metal gate materials with work functions adequate for n- and pMOS is facilitated by a high etch selectivity of HfN with respect to HfO/sub 2/, without any degradation to the EOT, gate leakage, or time-dependent dielectric breakdown characteristics of HfO/sub 2/. By replacing the HfN dummy gate with Ta and Ni in nMOS and pMOS devices, respectively, a work function difference of /spl sim/0.8 eV between nMOS and pMOS gate electrodes is achieved. This process could be applicable to sub-50-nm CMOS technology employing ultrathin HfO/sub 2/ gate dielectric.     

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.     

High-k Al/sub 2/O/sub 3/ gate dielectrics prepared by oxidation of aluminum film in nitric acid followed by high-temperature annealing

A simple, cost-effective, and room temperature process was proposed to prepare high-k gate dielectrics. An aluminum oxide (Al/sub 2/O/sub 3/) gate dielectric was prepared by oxidation of ultrathin Al film in nitric acid (HNO/sub 3/) at room temperature then followed by high-temperature annealing in O/sub 2/ or N/sub 2/. The substrate injection current behavior and interface trap-induced capacitance were introduced to investigate the interfacial property between the gate dielectric and Si substrate. Al/sub 2/O/sub 3/ gate dielectric MOS capacitors with and without initial SiO/sub 2/ layers were characterized. It was shown that the Al/sub 2/O/sub 3/ gate dielectrics with initial oxide exhibit better electrical properties than those without. The 650/spl deg/C N/sub 2/-POA Al/sub 2/O/sub 3/-SiO/sub 2/ sample with an equivalent oxide thickness of 18 /spl Aring/ exhibits three orders of magnitude reduction in gate leakage current in comparison with the conventional thermal SiO/sub 2/ sample.     

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/.     

Threshold voltage (V/sub th/) instability in HfO/sub 2/ high-/spl kappa/ gate stacks with TiN metal gate: comparison between NH/sub 3/ and O/sub 3/ interface treatments

The impacts of O/sub 3/ or NH/sub 3/ interface treatments on the long-term V/sub th/ instability in nMOSFET HfO/sub 2/ high-/spl kappa/ gate stacks with TiN metal gate electrodes are compared. The NH/sub 3/ interface treatment is found to be beneficial to suppress the V/sub th/ shift compared to the O/sub 3/-treated samples. This is explained by an enhanced valence band electrons injection in O/sub 3/-treated samples and is experimentally confirmed through a carrier separation measurement. The dynamic stress measurement also indicates that trapped charges are more easily detrapped in NH/sub 3/-treated samples than O/sub 3/-treated samples, improving significantly the V/sub th/ stability.     

Fully silicided NiSi gate on La/sub 2/O/sub 3/ MOSFETs

We have fabricated the fully silicided NiSi on La/sub 2/O/sub 3/ for n- and p-MOSFETs. For 900/spl deg/C fully silicided CoSi/sub 2/ on La/sub 2/O/sub 3/ gate dielectric with 1.5 nm EOT, the gate dielectric has large leakage current by possible excess Co diffusion at high silicidation temperature. In sharp contrast, very low gate leakage current density of 2/spl times/10/sup -4/ A/cm/sup 2/ at 1 V is measured for 400/spl deg/C formed fully silicided NiSi and comparable with Al gate. The extracted work function of NiSi was 4.42 eV, and the corresponding threshold voltages are 0.12 and -0.70 V for respective n- and p-MOSFETs. Electron and hole mobilities of 156 and 44 cm/sup 2//V-s are obtained for respective n- and p-MOSFETs, which are comparable with the HfO/sub 2/ MOSFETs without using H/sub 2/ annealing.     

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.     

Origin of the threshold voltage instability in SiO/sub 2//HfO/sub 2/ dual layer gate dielectrics

The magnitude of the V/sub T/ instability in conventional MOSFETs and MOS capacitors with SiO/sub 2//HfO/sub 2/ dual-layer gate dielectrics is shown to depend strongly on the details of the measurement sequence used. By applying time-resolved measurements (capacitance-time traces and charge-pumping measurements), it is demonstrated that this behavior is caused by the fast charging and discharging of preexisting defects near the SiO/sub 2//HfO/sub 2/ interface and in the bulk of the HfO/sub 2/ layer. Based on these results, a simple defect model is proposed that can explain the complex behavior of the V/sub T/ instability in terms of structural defects as follows. 1) A defect band in the HfO/sub 2/ layer is located in energy above the Si conduction band edge. 2) The defect band shifts rapidly in energy with respect to the Fermi level in the Si substrate as the gate bias is varied. 3) The rapid energy shifts allows for efficient charging and discharging of the defects near the SiO/sub 2//HfO/sub 2/ interface by tunneling.     

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.     

Composite TiSi/sub 2//n+ Poly-Si Low-Resistivity Gate Electrode and Interconnect for VLSI Device Technology

A composite polycide structure consisting of refractory metal silicide film on top of polysilicon has been considered as a replacement for polysilicon as a gate electrode and interconnect line in MOSFET integrated circuits. This paper presents fine-line patterning techniques and device characteristics of MOSFET's with a TiSi/sub 2/ polycide gate. A coevaporated TiSi/sub 2/ polycide gate was chosen for this study because it had 2 to 5 times lower resistivity as compared to other silicides. Polycide formation by electron-beam coevaporation is chosen in preference to sputtered TiSi/sub 2/ because of lower oxygen contamination. The coevaporation technique to form TiSi/sub 2/ polycide with a sheet resistivity of 1 Omega/square (bulk resistivity of 21 µOmega · cm) is described. Anisotropic etching of nominally 1-/spl mu/m lines with a 15 : 1 etch selectivity against oxide is reported. Measurements of metal-semiconductor work function, fixed oxide charge density, dielectric strength, oxide defect density, mobile-ion contamination, threshold voltage, and mobility have been made on polycide structures with 25-nm gate oxides. These MOS parameters correspond very closely to those obtained for n+ poly-Si gates. In addition, the specific contact resistivity between Al and TiSi/sub 2/ polycide is lower than the contact resistivity between Al and polysilicon by one order of magnitude.     

GaN MOS device using SiO/sub 2/-Ga/sub 2/O/sub 3/ insulator grown by photoelectrochemical oxidation method

We report on a SiO/sub 2/-Ga/sub 2/O/sub 3/ gate insulator stack directly grown on n-type GaN by the photoelectrochemical oxidation method. The resultant MOS devices are fabricated using standard photolithography and liftoff techniques. The effect of annealing temperature on the SiO/sub 2/-Ga/sub 2/O/sub 3//n-type GaN MOS devices is investigated. The properties of high breakdown field, low gate leakage current, and low interface state density are investigated for the MOS devices.     

Memory characterization of SiGe quantum dot flash memories with HfO/sub 2/ and SiO/sub 2/ tunneling dielectrics

In this study, we have developed a SiGe dot floating-gate flash memory with high-K dielectric (HfO/sub 2/) tunneling oxide. Using SiGe dots and HfO/sub 2/ tunneling oxide, a low program/erase voltage can be achieved, along with good endurance and charge retention characteristics as compared to the SiGe dots with a SiO/sub 2/ tunneling oxide. We have also examined the impact of Ge concentration in the SiGe dots on charge retention time. This demonstrates that the SiGe dots with HfO/sub 2/ tunneling oxide can be used as the floating gate to replace SiGe dots with SiO/sub 2/ tunneling oxide and have a high potential for further scaling of floating gate memory devices.     

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.     

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.     

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.