Duo Cao

Improvement of Al2O3 Films on Graphene Grown by Atomic Layer Deposition with Pre-H2O Treatment

We improve the surface of graphene by atomic layer deposition (ALD) without the assistance of a transition layer or surface functionalization. By controlling gas-solid physical adsorption between water molecules and graphene through the optimization of pre-H2O treatment and two-step temperature growth, we directly grew uniform and compact Al2O3 films onto graphene by ALD. Al2O3 films, deposited with 4-cycle pre-H2O treatment and 100-200 °C two-step growing process, presented a relative permittivity of 7.2 and a breakdown critical electrical field of 9 MV/cm. Moreover, the deposition of Al2O3 did not introduce any detective defects or disorders in graphene.

Property transformation of graphene with Al2O3 films deposited directly by atomic layer deposition

Al2O3 films are deposited directly onto graphene by H2O-based atomic layer deposition (ALD), and the films are pinhole-free and continuously cover the graphene surface. The growth process of Al2O3 films does not introduce any detective defects in graphene, suppresses the hysteresis effect and tunes the graphene doping to n-type. The self-cleaning of ALD growth process, together with the physically absorbed H2O and oxygen-deficient ALD environment consumes OH− bonds, suppresses the p-doping of graphene, shifts Dirac point to negative gate bias and enhances the electron mobility.

Improvement of SOI Trench LDMOS Performance With Double Vertical Metal Field Plate

In this paper, a novel high-voltage trench lateral double-diffused metal-oxide-semiconductor field effect transistor (TLDMOS) based on silicon-on-insulator technology is proposed. The new structure is characterized by a double vertical metal field plate (DVFP) in the oxide trench, which is surrounded by heavily doped N/P pillars [superjuction (SJ)]. The DVFP introduces five new electric field peaks in the bulk of drift region compared with the conventional TLDMOS, leading to the breakdown voltage (BV) increase. Furthermore, the DVFP and SJ provide an electrons accumulation layer at the interface of the N pillar and oxide trench under the ON-state, reducing the specific ON-resistance (RON). With the 2-D device simulation, a BV of 840 V and a RON of 60.2 mQ · cm2 are realized on a 25-μm-thick SOI layer and 0.5 μm buried oxide layer, and the Baligas figure of merit [(FOM), FOM = BV2/RON] of 11.4 MW/cm2 is achieved, breaking through the silicon limit.

HfO2 dielectric film growth directly on graphene by H2O-based atomic layer deposition

Due to its exceptionally high carrier mobility, International Technology Roadmap for Semiconductors considers graphene to be among the candidate materials for postsilicon electronics. In order to realize graphene-based devices, thin and uniform-coverage high-κ dielectrics without any pinholes on top of graphene is required. There are no dangling bonds on defect-free graphene surface; it is difficult to grow uniform-coverage high-κ dielectrics on graphene directly by atom layer deposition. Meanwhile, degradation of defects in graphene/high-κ structure is necessary for the optimization of high-κ dielectrics fabrication technology. Here the authors report on a H2O-based atom layer deposition method used for HfO2 growth, where physically adsorbed H2O molecules on graphene surface act as oxidant, and self-limit react with metal precursors to form HfO2 film onto graphene directly. Raman spectra reveal H2O-based atom layer deposition method will not introduce defects into graphene. The surface root mean square o...

Competitive Si and La effect in HfO2 phase stabilization in multi-layer (La2O3)0.08(HfO2) films

The effect of Si diffusion in HfO2 and the presence of La on phase transformation were investigated. Tetragonal HfO2 structures exhibited high permittivity, and the addition of exotic atoms to HfO2 facilitated tetragonal phase transformation. In multi-layer (La2O3)0.08(HfO2) films, the top HfO2 layer was transformed into a perfect tetragonal structure, and the bottom HfO2 layer near the interfacial layer was of a cubic structure, after annealing at 800 °C. The permittivity reached 50–60. Si diffusion into the HfO2 film stabilized the tetragonal structure, and La incorporation into HfO2 facilitated the transition of the cubic structure.

Direct growth of Sb2Te3 on graphene by atomic layer deposition

The direct growth of Sb2Te3 on graphene is achieved by atomic layer deposition (ALD) with pre-(Me3Si)2Te treatment. The results of atomic force microscopy (AFM) indicate Volmer–Weber island growth is the dominant growth mode for ALD Sb2Te3 growth on graphene. High resolution transmission electron microscopy (HRTEM) analysis reveals perfect crystal structures of Sb2Te3 on graphene and no interface layer generation. The characterization of X-ray photoelectron spectroscopy (XPS) implies the impermeability of graphene can maintain Sb2Te3 intact and isolate the adverse effects of substrates. Our study provides a step forward to grow high quality Sb2Te3 at low temperature and expand the potential applications of graphene in ALD techniques.

Low-temperature plasma-enhanced atomic layer deposition of HfO2/Al2O3 nanolaminate structure on Si

HfO2/Al2O3 nanolaminate was deposited on a Si substrate by plasma-enhanced atomic layer deposition at 150 °C with in situ plasma treatment. Unilayer HfO2 and Al2O3 films were prepared for comparison. Films were treated by rapid thermal annealing at 870 °C in a nitrogen atmosphere for 30 s. Al atoms in the HfO2/Al2O3 nanolaminate diffuse into HfO2 layers during rapid thermal annealing, facilitating the formation of tetragonal HfO2. The HfO2/Al2O3 nanolaminate has an effective dielectric constant of 20.7, a breakdown electric field of 7.4 MV/cm, and leakage current of 2.3 × 10−5 mA/cm2 at a gate bias of Vg = −1 V. The valence band offset, conduction band offset, and the band gap of the film are 2.75, 1.96, and 5.83 eV, respectively.

Al2O3–Gd2O3 double-films grown on graphene directly by H2O-assisted atomic layer deposition

We demonstrate the direct Al2O3–Gd2O3 double-films growth on graphene by H2O-assisted atomic layer deposition (ALD) using a hexamethyl disilazane precursor {Gd[N(SiMe3)2]3}. No defects are brought into graphene as shown by Raman spectra; the surface root-mean-square (RMS) roughness of the Al2O3–Gd2O3 double-films is down to 0.8 nm, comparable with the morphology of pristine graphene; the films are compact and continuous, and the relative permittivity is around 11, which indicate that H2O-assisted ALD can prepare high quality dielectric films on graphene.

Properties of HfO2/La2O3 nanolaminate films grown on an AlGaN/GaN heterostructure by plasma enhanced atomic layer deposition

HfO2/La2O3 nanolaminate (HLOL) films were grown on AlGaN/GaN heterostructure by plasma enhanced atomic layer deposition (PEALD). After high-temperature rapid thermal annealing (RTA), the properties of the films were characterized. Si (coming from the La2O3 metal precursor) and La atoms diffuse into the HfO2 layer, cubic and tetragonal phase HfO2 exist in the HLOL film. The HLOL film has an effective dielectric constant of 35.7 and a breakdown electric field of 5.5 MV cm−1. Moreover, the HLOL film is an effective barrier to suppress the gate leakage current, which is 5 orders of magnitude lower compared to a conventional Schottky diode. The HLOL dielectric film on AlGaN/GaN could also improve the gate voltage swing range.

Total-Dose Radiation Response of HfLaO Films Prepared by Plasma Enhanced Atomic Layer Deposition

HfLaO and HfO₂ films were deposited by plasma enhanced atomic layer deposition (PEALD). PEALD makes in-situ plasma treatment possible, and the film growth temperature can be reduced. The films were characterized. High resolution transmission electron microscopy (HRTEM) indicated both films were amorphous. X-ray photoelectron spectroscopy (XPS) suggested that the interface layer was most likely composed of Hf-Si-O and La-Si-O. MIS capacitors with HfLaO and HfO₂ dielectrics were irradiated by gamma rays with the dose up to 2×10⁶ rad (Si). Electrical measurements indicated that the dielectrics showed relatively stable electrical properties. The equivalent oxide thicknesses (EOT) of HfLaO samples were calculated to be 0.9 nm. At a gate condition of |V_g-V_fb| = 1 V, the leakage current densities were 0.02 mA/cm². With the increasing of the radiation dose, the maximum oxide trap charge density and interface trap charge density for HfLaO samples were calculated to be 2.6×10⁶ cm^-2 and 1.2×10¹² cm^-2, respectively. The analysis of the IV curves suggested that the conduction mechanism in HfLaO samples is the Poole-Frenkel emission.