The structural and electrical properties of the SrTa2O6/In0.53Ga0.47As/InP system

The structural and electrical properties of SrTa₂O₆(SrTaO)/n-In_0.53GaAs_0.47(InGaAs)/InP structures where the SrTaO was grown by atomic vapor deposition, were investigated. Transmission electron microscopy revealed a uniform, amorphous SrTaO film having an atomically flat interface with the InGaAs substrate with a SrTaO film thickness of 11.2 nm. The amorphous SrTaO films (11.2 nm) exhibit a dielectric constant of ∼20, and a breakdown field of >8 MV/cm. A capacitance equivalent thickness of ∼1 nm is obtained for a SrTaO thickness of 3.4 nm, demonstrating the scaling potential of the SrTaO/InGaAs MOS system. Thinner SrTaO films (3.4 nm) exhibited increased non-uniformity in thickness. From the capacitance-voltage response of the SrTaO (3.4 nm)/n-InGaAs/InP structure, prior to any post deposition annealing, a peak interface state density of ∼2.3 × 10¹³ cm⁻² eV⁻¹ is obtained located at ∼0.28 eV (±0.05 eV) above the valence band energy (E_v) and the integrated interface state density in range E_v + 0.2 to E_v + 0.7 eV is 6.8 × 10¹² cm⁻². The peak energy position (0.28 ± 0.05 eV) and the energy distribution of the interface states are similar to other high-k layers on InGaAs, such as Al₂O₃ and LaAlO₃, providing further evidence that the interface defects in the high-k/InGaAs system are intrinsic defects related to the InGaAs surface.     

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.     

Band offsets at the (1 0 0)GaSb/Al2O3 interface from internal electron photoemission study

From electron internal photoemission and photoconductivity measurements at the (1 0 0)GaSb/Al₂O₃ interface, the top of the GaSb valence band is found to be 3.05 ± 0.10 eV below the bottom of the Al₂O₃ conduction band. This interface band alignment corresponds to conduction and valence band offsets of 2.3 ± 0.10 eV and 3.05 ± 0.15 eV, respectively, indicating that the valence band in GaSb lies energetically well above the valence band of In_xGa_1−xAs (0 ? x ? 0.53) or InP.     

Comparison of short and long wavelength absorption electron donor materials in C60-based planar heterojunction organic photovoltaics

Buckminsterfullerene, C₆₀-based planar heterojunction (PHJ) organic photovoltaics (OPVs) have been created using a short wavelength absorption (λ_max = 490 nm) electron-donating bis(naphthylphenylaminophenyl)fumaronitrile (NPAFN). NPAFN exhibits a hole mobility greater than 0.07 cm² V⁻¹ s⁻¹ as determined by its field-effect transistor. It can be attributed to such hole mobility that enables a thin layer (<10 nm) NPAFN in PHJ OPV, ITO/NPAFN/C₆₀/bathocuproine/Al. Because of the low lying HOMO energy level (5.75 eV) of NPAFN and relatively high ionization potential ITO (∼5.58 eV), such OPVs exhibit a very high open circuit voltage of ∼1.0 V, relatively high fill factor of 0.60, and a relatively high shunt resistance of 1100 Ω cm⁻², which all compensate for a relatively low short circuit current of 3.15 mA cm⁻² due to the short absorption wavelength and inferred short exciton diffusion length of NPAFN. Altogether, NPAFN OPVs display a power conversion efficiency (η_PC) of 2.22%, which is better than other long wavelength absorption materials in similar PHJ OPVs, such as pentacene (λ_max 670 nm, HOMO 5.12 eV, η_PC 1.50%) and copper phthalocyanine (λ_max 624, 695 nm, HOMO 5.17 eV, η_PC 1.43%).     

Etching characteristics and plasma-induced damage of Ba0.65Sr0.35TiO3 thin films etched in CF4/Ar/O2 plasma

Sol-gel-derived Ba_0.65Sr_0.35TiO₃ (BST) thin films were etched in CF₄/Ar/O₂ plasma using magnetically enhanced reactive ion etching technology. The maximum etch rate of BST film is 8.47 nm/min when CF₄/Ar/O₂ gas mixing ratio is equal to 9/36/5. X-ray photoelectron spectroscopy analysis indicates the accumulation of fluorine-containing by-products on the etched surface due to their poor volatility, resulting in (Ba,Sr)-rich and (Ti,O)-deficient etched surface. Compared to the unetched counterparts, the etched Ba 3d_5/2, Ba 3d_3/2, Sr 3d_5/2, Sr 3d_3/2, Ti 2p_3/2, Ti 2p_1/2 and O 1s photoelectron peaks shift towards higher binding energy regions by amounts of 1.31, 1.30, 0.60, 0.79, 0.09, 0.46 and 0.50 eV, respectively. X-ray diffraction (XRD) analysis reveals that intensities of the etched BST (1 0 0), (1 1 0), (2 0 0) and (2 1 1) peaks are lowered and broadened. Raman spectra confirm that the Raman peaks of the etched film shift towards lower wave number regions with the values of 7, 6, 4 and 4 cm⁻¹, and the corresponding phonon lifetimes are longer than those of the unetched film because of the plasma-induced damage. When the etched films are postannealed at 650 °C for 20 min under an O₂ ambience, the chemical shifts of Ba 3d, Sr 3d, Ti 2p and O 1s peaks, the variations for atomic concentrations of Ba, Sr, Ti and O, and the Raman redshifts are reduced, while the corresponding XRD peak intensities increase. It is conceivable that the plasma-induced damage of the etched film could be partially recovered during the postannealing process.     

Optical characteristics of Si/SiO2 multilayers prepared by magnetron sputtering

Si/SiO₂ multilayers have been successfully prepared by magnetron sputtering and subsequently thermal annealed in an Ar atmosphere at a temperature of more than 500 °C. The surface of the as-deposited films is compact and smooth, and the distribution of grain size estimated to be 20 nm is uniform. For Si/SiO₂ multilayers annealed at 1100 °C, the Si sublayer sandwiched between potential barrier SiO₂ is crystalline structure by means of the analysis of Raman spectra and XRD data. The visible PL peak accompanying to a blue-shift with the decrease of Si sublayer thickness has been observed, and the intensity of this peak enhances with the increase of annealing temperature. The visible luminescence properties of Si/SiO₂ multilayers can be ascribed to quantum confinement of electron-hole pairs in quantum wells with grain size lower than 4.5 nm. In Si/SiO₂ multilayers, not only quantum confinement but also Si-SiO₂ interface states play an important role in the optical transition. The PL peak located at 779 nm is independent of the thickness of Si sublayer, so it may be ascribed to interface mediated transition. Typical Si dangling bonds defect could be a dominating obstacle to high luminescence efficiencies.     

Structural and electrical characteristics of RF-sputtered HfO2 high-k based MOS capacitors

The HfO₂ high-k thin films have been deposited on p-type (1 0 0) silicon wafer using RF magnetron sputtering technique. The XRD, AFM and Ellipsometric characterizations have been performed for crystal structure, surface morphology and thickness measurements respectively. The monoclinic structured, smooth surface HfO₂ thin films with 9.45 nm thickness have been used for Al/HfO₂/p-Si metal-oxide-semiconductor (MOS) structures fabrication. The fabricated Al/HfO2/Si structure have been used for extracting electrical properties viz dielectric constant, EOT, barrier height, doping concentration and interface trap density through capacitance voltage and current-voltage measurements. The dielectric constant, EOT, barrier height, effective charge carriers, interface trap density and leakage current density are determined are 22.47, 1.64 nm, 1.28 eV, 0.93 × 10¹⁰, 9.25 × 10¹¹ cm⁻² eV⁻¹ and 9.12 × 10⁻⁶ A/cm² respectively for annealed HfO₂ thin films.     

Characterization of UV photodetectors with MgxZn1−xO thin films

In this study the metal-semiconductor-metal (MSM) structure ultraviolet (UV) photodetectors (PDs) based on Mg_xZn_1−xO thin films were fabricated. The Mg_xZn_1−xO thin films were grown on glass substrates by sol-gel method. The results show that the optical absorption has a blue shift and higher transmittance with increasing Mg dopant. The optical band gap were modified by 3.28-3.52 eV, which corresponded to x = 0 and x = 0.16. For a 10 V applied bias, the dark currents of the Mg_xZn_1−xO MSM-PDs were 637 nA (x = 0) to 0.185 nA (x = 0.16) and showed good Schottky contacts. This UV-visible rejection ratio of the Mg_xZn_1−xO UV PDs at x = 0, 0.16, 0.21 and 0.33 were 18.82, 35.36, 40.91 and 42.92, respectively.     

Measurement of As diffusivity in Ni2Si thin films

The lattice and grain boundary diffusion coefficients of As in 260 nm-thick Ni₂Si films were measured. The Ni₂Si layers were prepared via the reaction between a Si layer deposited by low pressure chemical vapor deposition and a Ni layer deposited by magnetron sputtering on a Si substrate covered with a SiO₂ film. As was implanted in the silicide. Its concentration profiles were measured using secondary ion mass spectroscopy before and after annealing (550-700 °C). 2D finite element diffusion simulations taking into account lattice diffusion and grain boundary (GB) diffusion were performed based on the microstructure of the samples. They were found to fit accurately the measured profiles and allowed to measure the diffusion coefficients for each temperature. Lattice diffusion is characterized by a pre-exponential factor D⁰v ∼ 1.5 × 10⁻¹ cm² s⁻¹ and an activation energy Qv ∼ 2.72 eV. In the case of GB diffusion P⁰ = sδD⁰gb = 9.0 × 10⁻³ cm³ s⁻¹ and the activation energy was found to be higher than for lattice diffusion with Qgb ∼ 3.07 eV. Existing data concerning diffusion in silicides and other materials is used to discuss these results. The diffusion of As in Ni₂Si could be reduced due to impurity segregation in GBs.     

MOCVD fluorine free WSix metal gate electrode on high-k dielectric for NMOS technology

We report material and electrical properties of tungsten silicide metal gate deposited on 12 in. wafers by chemical vapor deposition (CVD) using a fluorine free organo-metallic (MO) precursor. We show that this MOCVD WSi_x thin film deposited on a high-k dielectric (HfSiO:N) shows a N+ like behavior (i.e. metal workfunction progressing toward silicon conduction band). We obtained a high-k/WSi_x/polysilicon “gate first” stack (i.e. high thermal budget) providing stable equivalent oxide thickness (EOT) of ∼1.2 nm, and a reduction of two decades in leakage current as compared to SiO₂/polysilicon standard stack. Additionally, we obtained a metal gate with an equivalent workfunction (EWF) value of ∼4.4 eV which matches with the +0.2 eV above Si midgap criterion for NMOS in ultra-thin body devices.     

Optical properties of nanostructured lead sulfide films with a <Emphasis Type="Italic">D</Emphasis>0<Subscript>3</Subscript> cubic structure

The optical transmittance of nanostructured cubic PbS (lead sulfide) films with a D0₃ structure is measured in the wavelength range 300 to 3200 nm. The film thicknesses are in the range ∼120 to ∼400 nm. Electron microscopy of the microstructure shows that about half of the films’ particles are 60 nm or smaller in size. As the average particle size is decreased, the band gap E _g increases from 0.85 to 1.5 eV, being noticeably larger than the band gap of coarse-grained PbS, 0.41 eV. This is indicative of a blue shift of the optical absorption band in nanostructured PbS films.     

Effect of RuO2 electrode on laser-MBE prepared HfO2 gate dielectrics

In this paper, we report our recent study of the effect of RuO₂ as an alternative top electrode for pMOS devices to overcome the serious problems of polysilicon (poly-Si) gate depletion, high gate resistance and dopant penetration in the trend of down to 50 nm devices and beyond. The conductive oxide RuO₂, prepared by RF sputtering, was investigated as the gate electrode on the Laser MBE (LMBE) fabricated HfO₂ for pMOS devices. Structural, dielectric and electric properties were investigated. RuO₂/HfO₂/n-Si capacitors showed negligible flatband voltage shift (<10 mV), very strong breakdown strength (>10 MV cm⁻¹). Compared to the SiO₂ dielectric with the same EOT value, RuO₂/HfO₂/n-Si capacitors exhibited at least 4 orders of leakage current density reduction. The work function value of the RuO₂ top electrode was calculated to be about 5.0 eV by two methods, and the effective fixed oxide charge density was determined to be 3.3 × 10¹² cm⁻². All the results above indicate that RuO₂ is a promising alternative gate electrode for LMBE grown HfO₂ gate dielectrics.     

Photoemission study of the Si(1 1 1)-native SiO2/copper phthalocyanine (CuPc) ultra-thin film interface

The Ultraviolet and X-ray Photoemission Spectroscopy (UPS, XPS) investigation was done to examine the interface formation between deposited copper phthalocyanine (CuPc) thin films and covered with native oxide n- and p-type silicon Si(1 1 1) substrates. The UPS results indicated the existence of small interface dipole effect for very first layer of CuPc deposited on both types of substrates. The dipoles were oriented differently depending on silicon conductivity type. In this paper we present that near the inorganic/organic interface the phthalocyanine’s molecular orbital levels shift downwards 0.20 ± 0.05 eV in the case of n-Si substrate and upwards 0.25 ± 0.05 eV for p-Si indicating the different displacement of the negative charge within the interface region. This tendency was also confirmed by conducted XPS study of the core levels. It is highly probable that band bending-like shift is provoked by the continuous change of CuPc molecule orientation induced by interface polarization layer.     

Multilevel charge storage in Si nanocrystals arranged in double-dot-layers within SiO2

We investigated charging/discharging characteristics of a MOS structure with two layers of Si-nanocrystals (NCs) embedded in the SiO₂ dielectric. The two-dimensional (2D) arrays of nanocrystals, of sizes 3 and 5 nm in the lower and upper NCs layer, respectively, were fabricated by low pressure chemical vapor deposition (LPCVD) of amorphous Si (a-Si), followed by oxidation/annealing. The tunnel oxide was 3.5 nm thick. Successive charging of the NCs layers by both electrons and holes injected from the substrate was clearly demonstrated by the observed steps in the flatband voltage shift (ΔV_FB) as a function of the applied positive (electrons) or negative (holes) pulses on the gate, thus opening the potential for multiple bit operation of the memory. Discharging of the structure by pulses of opposite sign was consistently obtained. The current-voltage (I-V) curves exhibited two transient peaks at voltages corresponding to the two steps in ΔV_FB vs. V_gate that were attributed to a displacement current from the substrate to the nanocrystal layers. Clear improvement of charge retention in the double-nanocrystal layer structure compared to the single one was obtained, opening the possibility for lowering the gate oxide thickness of the NC memory without compromising device reliability.     

Integration of low dimensional crystalline Si into functional epitaxial oxides

In this work we show that by efficiently exploiting the growth kinetics during molecular beam epitaxy (MBE) one could create Si nanostructures of different dimensions. Examples are Si quantum dots (QD) or quantum wells (QW), which are buried into an epitaxial rare-earth oxide, e.g. Gd₂O₃. Electrical measurements carried out on Pt/Gd₂O₃/Si MOS capacitors comprised with Si-QD demonstrate that such well embedded Si-QD with average size of 5 nm and density of 2×10¹² cm⁻² exhibit very good charge storage capacity with suitable retention (∼10⁵ s) and endurance (∼10⁵ write/erase cycles) characteristics. The Pt/Gd₂O₃/Si (metal-oxide-semiconductor (MOS)) basic memory cells with embedded Si-QD display large programming window (∼1.5-2 V) and fast writing speed and hence could be a potential candidate for future non-volatile memory application. The optical absorption of such Si-QD embedded into epitaxial Gd₂O₃ was found to exhibit a spectral threshold maximum up to 2.9±0.1 eV depending on their sizes, inferring a significant influence of quantum confinement on the QD/oxide interface band diagram.Ultra-thin single-crystalline Si-QW with epitaxial insulator (Gd₂O₃) as the barrier layers were grown by a novel approach based on cooperative vapor phase MBE on Si wafer with sharp interfaces between well and barriers. The current-voltage characteristics obtained for such structure exhibits negative differential resistance at lower temperature, making them a good candidate for resonant tunneling devices.     

Impact of the TiN electrode deposition on the HfO2 band gap for advanced MOSFET gate stacks

The impact of the deposition of a TiN electrode on the high-k oxide HfO₂ has been investigated, focussing on the dielectric band gap. After the gate elaboration, a non-destructive approach combining Spectroscopic Ellipsometry (SE), Reflection Electron Energy Loss Spectroscopy (REELS) and X-ray Photoelectron Spectroscopy (XPS) was developed to probe the buried metal/high-k interface. The overall optical band gap is 5.9 ± 0.1 eV with no change after the metal gate deposition. A local reduction of 1 eV is measured near the TiN layer, due to N diffusion at the interface creating N 2p states at the top of the HfO₂ valence band. Increased disorder and defects are identified in the high-k after gate elaboration by XPS, REELS and SE.     

Influence of oxidation temperature on the microstructure and electrical properties of Ta2O5 on Si

The effect of the oxidation temperature (673-873 K) on the microstructural and electrical properties of thermal Ta₂O₅ thin films on Si has been studied. Auger electron spectroscopy and X-ray photoelectron spectroscopy results revealed that the films are non-stoichiometric in the depth; an interfacial transition layer between tantalum oxide and Si substrate, containing presumably SiO₂ was detected. It has been found by X-ray diffraction that the amorphous state of Ta₂O₅ depends on both the oxidation temperature and the thickness of the films—the combination of high oxidation temperature (>823 K) and thickness smaller than 50 nm is critical for the appearance of a crystal phase. The Ta₂O₅ layers crystallize to the monoclinic phase and the temperature of the phase transition is between 773 and 823 K for the thinner layers (<50 nm) and very close to 873 K for the thicker ones. The electrical characterization (current/voltage; capacitance/voltage) reveals that the optimal oxidation temperature for achieving the highest dielectric constant (∼32) and the lowest leakage current (10⁻⁸ A/cm² at 1 MV/cm applied field) is 873 K. The results imply that the poor oxidation related defects are rather the dominant factor in the leakage current than the crystallization effects.     

Analytic computation of the photocurrent density in a n-6H-SiC/p-Si/n-Si/p-Si0.8Ge0.2 multilayer solar cell

In this work we conceived a model of a multilayer solar cell composed by four layers of opposite conductivities: an n-type 6H-SiC used as a frontal layer to absorb high energy photons (energy gap equals 2.9 eV), a p-type Si layer, an n-type Si layer and a p-type SiGe back layer to absorb low energy photons (Si_0.8Ge_0.2 with an energy gap equal to 0.8 eV). The impurity concentration in every layer of the model is taken equal to 10¹⁷ cm⁻³ to ensure abrupt junctions inside the cell. The optical properties of the separate layers have been fitted and tabulated to be used for thin films devices numerical simulation. We developed the equations giving the minority carrier concentration and the photocurrent density in each abscissa of the model. We used Matlab software to simulate and optimize the layers thicknesses to achieve the maximum photocurrent generated under AM0 solar spectrum. The results of simulation showed that the optimized structure could deliver, assuming 10⁵ cm/s surface recombination velocity, a photocurrent density of more than 53 mA/cm², which represents 88.3% of the ideal photocurrent (59.99 mA/cm²) that can be generated under AM0 solar spectrum.     

Phase formation and texture of nickel silicides on Si1−xCx epilayers

We investigated the phase formation and texture of nickel silicides formed during the reaction of 10 nm sputter deposited nickel with Si_1−xC_x epitaxial layers on Si(1 0 0) substrates, having a carbon content between 0 and 2.5 atomic percent. It was found that both the formation temperature as well as the texture of the metal-rich phases is influenced by the amount of carbon in the Si_1−xC_x layer. To determine the influence of the location of the carbon during the silicidation process we also investigated the reaction of 10 nm nickel on Si(1 0 0) substrates, where carbon was either alloyed in the nickel layer or deposited as an interlayer at the interface between the nickel and the substrate. Depending on the location of the carbon, a different thermal stability of the layer was found.     

Properties of ALD HfTaxOy high-k layers deposited on chemical silicon oxide

HfTa_xO_y high-k dielectric layers with different compositions were deposited using ALD on 1 nm SiO₂ generated by ozone based cleaning of 200 mm Si(1 0 0) surface. Physical characterization of blanket layers and C-V mapping demonstrates that the ALD layers have excellent uniformity and controllable compositions. The layers with a composition of HfTaO_5.5 remain amorphous after annealing at 900 °C. The C-V measurements of MOS capacitors show no hysteresis, negligible frequency dispersion and interfacial state density smaller than 3 × 10¹¹ (cm⁻² eV⁻¹). k-value of the amorphous layers varies in the range from 20 to 25, depending on layer composition. The flat band voltage does not shift with the increase of EOT, implying that the effect of fixed charge densities in the layers is negligible. The I-V measurements show a leakage reduction comparable to that of the ALD HfO₂ layers.