Abstract:Strontium titanate (SrTiO3, STO) films were deposited by plasma-assisted ALD using cyclopentadienyl-based Sr- and Ti-precursors with O2 plasma as the oxidizing agent. Spectroscopic ellipsometry (SE) was employed to determine the thickness and the optical properties of the layers. As determined from Rutherford backscattering spectrometry (RBS), [Sr]/([Sr]+[Ti]) ratios ranging from 0.42 to 0.68 were achieved for 30–40 nm thick films by tuning the [SrO]/[TiO2] ALD cycle ratio. Films deposited at 250°C were amorph… Show more
“…The elemental composition was extracted from the ellipsometry data by means of an optical constant library which was calibrated by means of Rutherford backscattering experiments. 21 The Table I. RTA in flowing N 2 was performed in an AST SHS100 system at temperatures ranging from 550…”
The crystallization behavior of thin strontium titanate (SrTiO3, STO) films with ∼15 nm thickness was studied by Transmission Electron Microscopy (TEM). Amorphous STO films with [Sr]/([Sr]+[Ti]) ratio ranging from 0.50 to 0.63 were deposited at 350°C by plasma-assisted ALD and subsequently treated by rapid thermal annealing in flowing N2 for crystallization. Different temperatures and annealing durations were employed to fully characterize the crystallization process. TEM analysis showed that transrotational crystals were formed and evidenced the influence of the STO composition and of the thermal budget applied on the grain size, crack and void formation. In particular, Sr-rich layers ([Sr]/([Sr]+[Ti] ≥ 0.59) showed a finer crystalline structure which was imputed to a higher nucleation probability at the onset of the crystallization process. Crystallization into the perovskite structure was confirmed for all the film compositions studied. By tuning the STO composition and the thermal budget of the annealing step it was demonstrated that it is possible to control the microstructure of the crystallized film as a further step in optimizing the STO film properties.
“…The elemental composition was extracted from the ellipsometry data by means of an optical constant library which was calibrated by means of Rutherford backscattering experiments. 21 The Table I. RTA in flowing N 2 was performed in an AST SHS100 system at temperatures ranging from 550…”
The crystallization behavior of thin strontium titanate (SrTiO3, STO) films with ∼15 nm thickness was studied by Transmission Electron Microscopy (TEM). Amorphous STO films with [Sr]/([Sr]+[Ti]) ratio ranging from 0.50 to 0.63 were deposited at 350°C by plasma-assisted ALD and subsequently treated by rapid thermal annealing in flowing N2 for crystallization. Different temperatures and annealing durations were employed to fully characterize the crystallization process. TEM analysis showed that transrotational crystals were formed and evidenced the influence of the STO composition and of the thermal budget applied on the grain size, crack and void formation. In particular, Sr-rich layers ([Sr]/([Sr]+[Ti] ≥ 0.59) showed a finer crystalline structure which was imputed to a higher nucleation probability at the onset of the crystallization process. Crystallization into the perovskite structure was confirmed for all the film compositions studied. By tuning the STO composition and the thermal budget of the annealing step it was demonstrated that it is possible to control the microstructure of the crystallized film as a further step in optimizing the STO film properties.
“…In their work, Niinist€ o et al showed a similar temperature dependence of the HfO 2 film crystallinity with a clear transition from amorphous to crystalline films at a deposition temperature of 300 C. The difference in temperature between this work and the one reported by Niinist€ o et al at which this transition could be observed is imputed to a $20%-25% difference between the set stage temperature value and the actual substrate temperature for the reactor employed in this work. 32 It can be concluded that the crystallization temperature of HfO 2 films is rather independent of the oxygen source used in combination with HfCp(NMe 2 ) 3 during the ALD process. However, the usage of a plasma-assisted ALD process may open the possibility for tuning of the crystalline phase by ion bombardment by employing substrate biasing during processing, 33 which is the object of further investigation.…”
Section: B Optoelectronic Properties and Crystallinitymentioning
HfO2 thin films were prepared by plasma-enhanced atomic layer deposition using a cyclopentadienyl-alkylamido precursor [HfCp(NMe2)3, HyALD™] and an O2 plasma over a temperature range of 150–400 °C at a growth per cycle around 1.1 Å/cycle. The high purity of the films was demonstrated by x-ray photoelectron spectroscopy and elastic recoil detection analyses which revealed that by increasing the deposition temperature from 200 to 400 °C, the atomic concentrations of residual carbon and hydrogen reduced from 1.0 to <0.5 at. % and 3.4 to 0.8 at. %, respectively. Moreover, Rutherford backscattering spectroscopy studies showed an improvement in stoichiometry of HfO2 thin films with the increase in deposition temperature, resulting in Hf/O ratio close to ∼0.5 at 400 °C. Furthermore, grazing incidence x-ray diffraction measurements detected a transition from amorphous at the deposition temperature of 300 °C to fully polycrystalline films at 400 °C, consisting of a mixture of monoclinic, tetragonal, and cubic phases. Finally, the surface morphology and conformality of HfO2 thin films studied by atomic force microscopy and transmission electron microscopy are also reported.
“…Further details on the growth process can be found in recent publications. 23,27 For the use as bottom electrode, the Pt film is structured into 100 nm wide bars by means of nanoimprint lithography and reactive ion beam etching (RIBE). The resistive switching cell is completed by a 30 nm TiN film, deposited by sputtering, and capped with a Pt layer.…”
Vertical power MOS transistor as a thermoelectric quasi-nanowire device J. Appl. Phys. 120, 244903244903 (2016) . The STO films, deposited by atomic layer deposition, were integrated in Pt/STO/TiN nanocrossbars with a feature size of 100 nm. By analysis of the transient currents, the switching kinetics are investigated between 10 ns and 10 4 s for the SET and 10 ns and 100 s for the RESET. A clear influence of the composition on the degree of nonlinearity of the switching kinetics was observed. Applying an analytical model for the oxygen vacancy migration, we were able to explain the differences in the SET kinetics by composition-dependent changes in the thermal conductivity and by a lower activation energy for the Ti-rich sample. This might be utilized in design rules of future ReRAM devices. Published by AIP Publishing. [http://dx
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.