Hot carrier effects in n-MOSFETs with SiO2/HfO2/HfSiO gate stack and TaN metal gate

Charge trapping and trap generation in field-effect transistors with SiO₂/HfO₂/HfSiO gate stack and TaN metal gate electrode are investigated under uniform and non-uniform charge injection along the channel. Compared to constant voltage stress (CVS), hot carrier stress (HCS) exhibits more severe degradation in transconductance and subthreshold swing. By applying a detrapping bias, it is demonstrated that charge trapping induced degradation is reversible during CVS, while the damage is permanent for hot carrier injection case.     

Germanium FETs and capacitors with rare earth CeO2/HfO2 gates

Long channel Ge FETs and capacitors with CeO₂/HfO₂/TiN gates were fabricated by photolithography and gate wet etch. Rare earth CeO₂ in direct contact with Ge was used as a passivating layer producing lowest D_it values in the mid 10¹¹ eV⁻¹ cm⁻² range. HfO₂ cap reduces leakage and improves equivalent oxide thickness scaling of the whole gate stack. The p-FETs show exceptionally high I_ON/I_OFF ratio 10⁶, mainly due to low OFF current, and peak channel mobility around 80 cm²/V s. The n-FETs, although functional, show inferior performance producing ON currents an order of magnitude lower compared to p-FETs.     

Comparison of electrical stress-induced charge carrier generation/trapping and related degradation of SiO2 and HfO2/SiO2 gate dielectric stacks

We compare charge carrier generation/trapping related degradation in control oxide (SiO₂) and HfO₂/SiO₂ stack of an identical equivalent-oxide-thickness (EOT) during constant gate voltage stress of n-type metal-oxide-semiconductor (nMOS) capacitors. Irrespective of these two dielectrics, the kinetics of generation of both surface states and oxide-trapped positive charges are found to be similar. Our analysis shows that the positive oxide charge buildup during CVS is due to trapping of protons by the strained SiOSi bonds in either of the devices. We demonstrate that compared to SiO₂ devices, HfO₂ devices with an equal EOT better perform in CMOS logic applications. On the other hand, our results indicate that the control oxide is better in charge trapping memory devices. Furthermore, the lifetime of the control oxide devices is observed longer than that of HfO₂ devices at a given operating voltage.     

Effects of the metal gate on the stress-induced traps in Ta2O5/SiO2 stacks

The degradation of Ta₂O₅-based (10 nm) stacked capacitors with different top electrodes, (Al, W, Au) under constant current stress has been investigated. The variation of electrical characteristics after the stress is addressed to gate-induced defects rather than to poor-oxidation related defects. The main wearout parameter in Ta₂O₅ stacks is bulk-related and a generation only of bulk traps giving rise to oxide charge is observed. The post-stress current–voltage curves reveal that stress-induced leakage current (SILC) mode occurs in all capacitors and the characteristics of pre-existing traps define the stress response. The results are discussed in terms of simultaneous action of two competing processes: negative charge trapping in pre-existing electron traps and stress-induced positive charge generation, and the domination of one of them in dependence on both the stress level and the gate used. The charge build-up and the trapping/detrapping processes modify the dominant conduction mechanism and the gate-induced defects are precursors for device degradation. It is concluded that the impact of the metal gate on the ultimate reliability of high-k stacked capacitors should be strongly considered.     

Constant current stress-induced leakage current in mixed HfO2-Ta2O5 stacks

The electrical characteristics of HfO₂-Ta₂O₅ mixed stacks under constant current stress (CCS) at gate injection with 20 mA/cm² and stressing times of 50 and 200 s have been investigated. A very weak effect of the stress on the global dielectric constant, on fast and slow states in the stack as well as on the dominant conduction mechanism is detected. The most sensitive parameter to the CCS is the leakage current. The stress-induced leakage current (SILC) is voltage and thickness dependent. The pre-existing traps govern the trapping kinetics and are a key parameter to evaluate the stress response. Two processes - positive charge build-up and new bulk traps generation - are suggested to be responsible for SILC: the domination of one of them depends on both the film thickness and the stressing time. The positive charge build-up is localized close to the gate electrode implying gate-induced defects could be precursors for it. It is established that unlike the case of single SiO₂ layer, the bulk traps closer to the gate electrode control SILC in the mixed Ta₂O₅-HfO₂-based capacitors.     

Suppression of Ge–O and Ge–N bonding at Ge–HfO2 and Ge–TiO2 interfaces by deposition onto plasma-nitrided passivated Ge substrates: Integration issues Ge gate stacks into advanced devices

A study of changes in nano-scale morphology of thin films of nano-crystalline transition metal (TM) elemental oxides, HfO₂ and TiO₂, on plasma-nitrided Ge(1 0 0) substrates, and Si(1 0 0) substrates with ultra-thin (0.8 nm) plasma-nitrided Si suboxide, SiO_x, x < 2, or SiON interfacial layers is presented. Near edge X-ray absorption spectroscopy (NEXAS) has been used to determine nano-scale morphology of these films by Jahn-Teller distortion removal of band edge d-state degeneracies. These results identify a new and novel application for NEXAS based on the resonant character of the respective O K₁ and N K₁ edge absorptions. This paper also includes a brief discussion of the integration issues for the introduction of this Ge breakthrough into advanced semiconductor circuits and systems. This includes a comparison of nano-crystalline and non-crystalline dielectrics, as well as issues relative to metal gates.     

Constant current stress of lightly Al-doped Ta2O5

The response of lightly Al-doped Ta₂O₅ stacked films (6 nm) to constant current stress (CCS) under gate injection (current stress in the range of 1 to 30 mA/cm² and stressing time of 50–400 s) has been investigated. The stress creates positive oxide charge, which is assigned to oxygen vacancies but it does not affect the dielectric constant of the films. The most sensitive parameter to the stress is the leakage current. Different degradation mechanisms control the stress-induced leakage current (SILC) in dependence on both the stress conditions and the applied measurement voltage. The origin of SILC is not the same as that in pure and Ti- or Hf-containing Ta₂O₅. The well known charge trapping in pre-existing traps operates only at low level stress resulting in small SILC at accumulation. The new trap generation plays a key role in the SILC degradation and is the dominant mechanism controlling the SILC in lightly Al-doped Ta₂O₅ layers.     

Atomic-layer-deposited silicon-nitride/SiO2 stack––a highly potential gate dielectrics for advanced CMOS technology

An extremely thin (2 monolayers) silicon nitride layer has been deposited on thermally grown SiO₂ by an atomic-layer-deposition (ALD) technique and used as gate dielectrics in metal–oxide–semiconductor (MOS) devices. The stack dielectrics having equivalent oxide thickness (T_eq=2.2 nm) efficiently reduce the boron diffusion from p⁺ poly-Si gate without the pile up of nitrogen atoms at the SiO₂/Si interface. The ALD silicon nitride is thermally stable and has very flat surface on SiO₂ especially in the thin (<0.5 nm) thickness region.An improvement has been obtained in the reliability of the ALD silicon-nitride/SiO₂ stack gate dielectrics compared with those of conventional SiO₂ dielectrics of identical thickness. An interesting feature of soft breakdown free phenomena has been observed only in the proposed stack gate dielectrics. Possible breakdown mechanisms are discussed and a model has been proposed based on the concept of localized physical damages which induce the formation of conductive filaments near both the poly-Si/SiO₂ and SiO₂/Si-substrate interfaces for the SiO₂ gate dielectrics and only near the SiO₂/Si-substrate interface for the stack gate dielectrics.Employing annealing in NH₃ at a moderate temperature of 550 °C after the ALD of silicon nitride on SiO₂, further reliability improvement has been achieved, which exhibits low bulk trap density and low trap generation rate in comparison with the stack dielectrics without NH₃ annealing.Because of the excellent thickness controllability and good electronic properties, the ALD silicon nitride on a thin gate oxide will fulfill the severe requirements for the ultrathin stack gate dielectrics for sub-0.1 μm complementary MOS (CMOS) transistors.     

Electrical reliability aspects of HfO2 high-k gate dielectrics with TaN metal gate electrodes under constant voltage stress

The dielectric breakdown property of ultrathin 2.5 and 5.0 nm hafnium oxide (HfO₂) gate dielectric layers with metal nitride (TaN) gate electrodes for metal oxide semiconductor (MOS) structure has been investigated. Reliability studies were performed with constant voltage stressing to verify the processing condition effects (film thicknesses and post metal annealing temperatures) on times to breakdown. The leakage current characteristics are improved with post metal annealing temperatures (PMA) for both 2.5 and 5.0 nm HfO₂ physical thicknesses. However, it is more prominent (2 orders of magnitudes) for 2.5 nm HfO₂ film thickness. The values of oxide-trapped charge density and interface-state density are also improved for 2.5 nm HfO₂ film. The different stages of charge-trapping behaviors, i.e., stress-induced leakage current, soft and hard breakdown mechanisms have been detected. During constant voltage stress of the MOS capacitors, an increase in the time-dependent gate current is observed, followed by the occurrence of several fluctuations. The amplitude of the fluctuations is much larger in the 5.0 nm HfO₂ gate dielectric layer compared to the 2.5 nm HfO₂ layer. After the occurrence of such fluctuations, the current–voltage characteristics exhibited an increased in gate current compared to the fresh (unstressed) devices.     

Degradation behavior of Ta2O5 stacks and its dependence on the gate electrode

Response of 8 nm Ta₂O₅ stacks with Al and Au gate electrodes to voltage stress at room temperature and at 100 °C is investigated. Stress-induced leakage current (SILC) reveals significant gate dependence and distinct difference to SILC in SiO₂. The mechanisms for SILC generation and stress degradation are discussed. Unlike SiO₂, pre-existing traps and positive charge build-up are recognized as a key factor for generation of SILC in Ta₂O₅ stacks.     

Distribution and generation of traps in SiO2/Al2O3 gate stacks

In this work we combine charge-pumping measurements with positive constant voltage stress to investigate trap generation in SiO₂/Al₂O₃ n-MOSFET. Trap density has been scanned either in energy or in position based on charge-pumping (CP) measurements performed under different operating conditions in terms of amplitude and frequency of the gate pulse. Our results have revealed that the traps are meanly localized shallow in energy level, deeper in spatial position and they are mostly generated near the Si/SiO₂ interface.     

A study on the improved programming characteristics of flash memory with Si3N4/SiO2 stacked tunneling dielectric

The programming characteristics of memories with different tunneling-layer structures (Si₃N₄, SiO₂ and Si₃N₄/SiO₂ stack) dielectrics are investigated using 2-D device simulator of MEDICI. It is theoretically confirmed that the memory with the SiO₂/Si₃N₄ stacked tunneling layer exhibits better programming characteristics than ones with single tunneling layer of SiO₂ or Si₃N₄ for programming by channel hot electron (CHE) injection. A 10-μs programming time with a threshold-voltage shift of 5 V can be obtained for the memory with SiO₂/Si₃N₄ stacked tunneling layer at V_cg = 10 V and V_ds = 3.3 V. This is attributed to the fact that the floating-gate voltage is close to drain voltage for the stacked tunneling dielectric (TD), and thus the CHE injection current is the largest. Furthermore, optimal substrate concentration is determined to be 5 × 10¹⁶–2 × 10¹⁷ cm⁻³, by considering a trade-off between the programming characteristics and power dissipation/lifetime of the devices. Lastly, the effects of interface states on the programming characteristics are investigated. Low interface-state density gives short programming time and small post-programming control-gate current.     

Bulk oxide charge and slow states in Si–SiO2 structures generated by RIE-mode plasma

The damage induced in the thin SiO₂–Si system after an exposure to O₂ and N₂ plasma working in reactive ion etching (RIE) mode has been studied. A generation of high density (up to 5×10¹² cm⁻² in the first 15 s plasma exposure) of positive oxide charge in bulk traps as well as in slow states has been established. The RIE damage effects become highly process dependent as the plasma time increases, the fixed oxide charge first increases and then slows down or even turns around depending on discharge conditions. It is suggested that the relative contribution of the two main plasma components (ion bombardment and vacuum UV photons) at different discharge regimes is the reason for the appearance or the absence of the “turn-around” effect. It is established that the combination O₂ plasma and low pressure is critical for the degradation of the plasma treated samples. The results reveal a strong linear correlation between the leakage current detected and plasma created positive charge.     

Charge trapping and reliability characteristics of ultra-thin HfYOx films on n-GaAs substrates

Ultra-thin layers of the HfYO_x gate dielectric were deposited on n-GaAs substrates by employing radio frequency (rf) sputter deposition system with a Si interface control layer sandwiched between the dielectric and semiconductor. The trapping/detrapping behaviour of charge carriers in the ultra-thin HfYO_x/Si gate dielectric stack has been extensively studied during constant-voltage stressing (CVS) and compared with the results obtained from directly deposited HfYO_x films on n-GaAs. The increase in gate leakage current observed during electrical stress is estimated and explained by taking into account the build up of trap charges and stress induced trap generation. Also, the capture cross-section of the generated traps is estimated. The variation of the trap centroid and the trapped charge density with injected influences have been investigated using constant current stressing (CCS) measurements. The dielectric breakdown and reliability of the dielectric films have been studied using constant-voltage stressing. A high time-dependent dielectric breakdown (TDDB, t_bd  1700 s) is observed for HfYO_x gate dielectric with a silicon inter-layer under a high constant-voltage stress (8 V).     

Interfacial layer quality effects on low-frequency noise (1/f) in p-MOSFETs with advanced gate stacks

The effects of interfacial layer quality on the low-frequency noise behavior of p-channel MOSFETs with high-κ gate dielectric and metal gate are investigated. Devices with chemically grown SiO₂ interfacial layers (0.8 nm) are compared with N₂O (0.8 nm) interfacial oxides. A 0.4 nm SiO₂ interfacial layer device is used for comparison purposes. A cross-over kind of behavior has been observed in N₂O devices, which occur at lower gate voltages (1.2–1.3 V) when normalized spectral densities and input referred noise are investigated. This behavior is found to be closely related to the observed transconductance variation in these devices. The dominant mechanism of 1/f noise is found to be Hooge’s mobility fluctuations. Hooge’s parameter, as a figure of merit, shows an increase for 0.4 nm devices when compared to 0.8 nm devices, while 0.8 nm N₂O devices confirm their cross-over nature.     

Investigation of atomic vapour deposited TiN/HfO2/SiO2 gate stacks for MOSFET devices

HfO₂ films were grown by atomic vapour deposition (AVD) on SiO₂/Si (1 0 0) substrates. The positive shift of the flat band voltage of the HfO₂ based metal-oxide-silicon (MOS) devices indicates the presence of negative fixed charges with a density of 5 × 10¹² cm⁻². The interface trap charge density of HfO₂/SiO₂ stacks can be reduced to 3 × 10¹¹ eV⁻¹ cm⁻² near mid gap, by forming gas annealing. The extracted work function of 4.7 eV preferred the use of TiN as metal gate for PMOS transistors. TiN/HfO₂/SiO₂ gate stacks were integrated into gate-last-formed MOSFET structures. The extracted maximum effective mobility of HfO₂ based PMOS transistors is 56 cm²/Vs.     

Electrical measurements of voltage stressed Al2O3/GaAs MOSFET

Electrical characteristics of GaAs metal–oxide–semiconductor field effect transistor with atomic layer deposition deposited Al₂O₃ gate dielectric have been investigated. The IV characteristics were studied after various constant voltage stress (CVS) has been applied. A power law dependence of the gate leakage current (I_g) on the gate voltage (V_g) was found to fit the CVS data of the low positive V_g range. The percolation model well explains the degradation of I_g after a high positive V_g stress. A positive threshold voltage (V_th) shift for both +1.5 V and +2 V CVS was observed. Our data indicated that positive mobile charges may be first removed from the Al₂O₃ layer during the initial CVS, while the trapping of electrons by existing traps in the Al₂O₃ layer is responsible for the V_th shift during the subsequent CVS.     

Correlation between infrared transmission spectra and the interface trap density of SiO2 films

This work is an attempt to estimate the electrical properties of SiO₂ thin films by recording and analyzing their infrared transmission spectra. In order to study a big variety of films having different infrared and electrical properties, we studied SiO₂ films prepared by low pressure chemical vapor deposition (LPCVD) from SiH₄ + O₂ mixtures at 425 °C and annealed at 750 °C and 950 °C for 30 min. In addition thermally grown gate quality SiO₂ films of similar thickness were studied in order to compare their infrared and electrical properties with the LPCVD oxides. It was found that all studied SiO₂ films have two groups of Si–O–Si bridges. The first group corresponds to bridges located in the bulk of the film and far away from the interfaces, the grain boundaries and defects and the second group corresponds to all other bridges located near the interfaces, the grain boundaries and defects. The relative population of the bulk over the boundary bridges was found equal to 0.60 for the LPCVD film after deposition and increased to 4.0 for the LPCVD films after annealing at 950 °C. Thermally grown SiO₂ films at 950 °C were found to have a relative population of Si–O–Si bridges equal to 3.9. The interface trap density of the LPCVD film after deposition was found equal to 5.47 × 10¹² eV⁻¹ cm⁻² and decreases to 6.50 × 10¹⁰ eV⁻¹ cm⁻² after annealing at 950 °C for 30 min. The interface trap density of the thermally grown film was found equal to 1.27 × 10¹¹ eV⁻¹ cm⁻² showing that films with similar Si–O–Si bridge populations calculated from the FTIR analysis have similar interface trap densities.     

Breakdown characteristics of nFETs in inversion with metal/HfO2 gate stacks

Time zero and time dependent dielectric breakdown (TZBD and TDDB) characteristics of atomic layer deposited (ALD) TiN/HfO₂ high-κ gate stacks are studied by applying ramped and constant voltage stress (RVS and CVS), respectively, on the n-channel MOS devices under inversion conditions. For the gate stacks with thin high-κ layers (?3.3 nm), breakdown (BD) voltage during RVS is controlled by the critical electric field in the interfacial layer (IL), while in the case of thicker high-κ stacks, BD voltage is defined by the critical field in the high-κ layer. Under low gate bias CVS, one can observe different regimes of the gate leakage time evolution starting with the gate leakage current reduction due to electron trapping in the bulk of the dielectric to soft BD and eventually hard BD. The duration of each regime, however, depends on the IL and high-κ layer thicknesses. The observed strong correlation between the stress-induced leakage current (SILC) and frequency-dependent charge pumping (CP) measurements for the gate stacks with various high-κ thicknesses indicates that the degradation of the IL triggers the breakdown of the entire gate stack. Weibull plots of time-to-breakdown (T_BD) suggest that the quality of the IL strongly affects the TDDB characteristics of the Hf-based high-κ gate stacks.     

The separation of generation lifetimes of Si and SiGe using capacitance-transient measurements on MOS capacitors formed by plasma anodisation of Si:Si0.9Ge0.1:Si substrates

A simple technique leading to the measurement of minority carrier lifetimes of UHV compatible LPCVD Si and SiGe by C–t depth profiling of Metal:Oxide:Si:SiGe:Si structures is reported. A high quality gate oxide is realised by low temperature (<100°C) plasma anodisation thereby reducing any oxidation effects on the underlying epitaxial layer quality. Capacitance response times were observed for an impurity concentration of 2.5×10¹⁷ cm⁻³, giving rise to generation lifetimes of the Si and Si_0.9Ge_0.1 of >0.55 and 2.6 μs respectively, reflective of very high quality epitaxial semiconductor material.