Abstract:Amorphous tantalum oxide thin films were deposited by reactive rf magnetron sputtering onto [001] silicon substrates. Growth temperature, oxygen partial pressure, and total gas pressure have been varied to obtain thin films with different densities. The thin films were analyzed by glancing angle-of-incidence x-ray diffraction, atomic force microscopy, and variable angle-of-incidence spectroscopic ellipsometry in the near infrared to vacuum ultraviolet spectral region for photon energies from E=1 to 8.5 eV, and… Show more
“…These results are consistent with the results reported in literature. 16,17 In the past, the refractive index of tantalum oxide films had been shown to be dependent on the O/Ta ratio. 16,18 Tantalum sub- 20 Since the films were deposited under the same conditions, it is likely that the lower refractive index of the 10 nm Ta 2 O 5 was due to an increased number of voids or pores in the film.…”
Films of tantalum pentoxide ͑Ta 2 O 5 ͒ with thickness of 10-100 nm were deposited on Si wafers and have been compared using spectroscopic ellipsometry ͑SE͒ and x-ray reflectivity ͑XRR͒. ͑Ta 2 O 5 ͒ was chosen for comparison work based on various criterions for material selection outlined in this article. Measurements were performed at six positions across the sample area to take into consideration thickness and composition inhomogeneity. SE and XRR fitted curves required the incorporation of a linearly graded interface layer. SE systematically measured higher values of film thickness as compared to XRR. A linear equation was established between the thickness measurements using SE and XRR. The slope of the linear equation established was found to be 1.02± 0.01. However, the intercepts were found to be 1.7± 0.2 and 2.6± 0.3 when the interface was excluded and included, respectively. These differences in the values of intercepts were attributed to the uncertainties in the determination of the interface layer.
“…These results are consistent with the results reported in literature. 16,17 In the past, the refractive index of tantalum oxide films had been shown to be dependent on the O/Ta ratio. 16,18 Tantalum sub- 20 Since the films were deposited under the same conditions, it is likely that the lower refractive index of the 10 nm Ta 2 O 5 was due to an increased number of voids or pores in the film.…”
Films of tantalum pentoxide ͑Ta 2 O 5 ͒ with thickness of 10-100 nm were deposited on Si wafers and have been compared using spectroscopic ellipsometry ͑SE͒ and x-ray reflectivity ͑XRR͒. ͑Ta 2 O 5 ͒ was chosen for comparison work based on various criterions for material selection outlined in this article. Measurements were performed at six positions across the sample area to take into consideration thickness and composition inhomogeneity. SE and XRR fitted curves required the incorporation of a linearly graded interface layer. SE systematically measured higher values of film thickness as compared to XRR. A linear equation was established between the thickness measurements using SE and XRR. The slope of the linear equation established was found to be 1.02± 0.01. However, the intercepts were found to be 1.7± 0.2 and 2.6± 0.3 when the interface was excluded and included, respectively. These differences in the values of intercepts were attributed to the uncertainties in the determination of the interface layer.
“…In Figure 2, we also show, by a magenta dash-dotted line, the optical ELF of Ta 2 O 5 built from eq 4, where the outer (leastbound) electron excitation contribution is obtained from eq 2, with the parameters resulting from the REELS measurements, which are given in Table 1, and where the inner-shell contribution is also included. The measurements by Franke et al 23 at very low transferred energies are depicted by orange dots.…”
Section: Improving the Elf Through The Melf-gosmentioning
confidence: 99%
“…20−22 From experimental ellipsometry data, Franke et al 23 got the dielectric function of Ta 2 O 5 thin films in the spectral region 0.03−8.5 eV. Reflection electron energy loss measurements are an established way of determining the energy loss function of a material, 1,24 and the spectrum of amorphous Ta 2 O 5 for 200 eV electrons has been measured up to 60 eV energy losses, but being expressed in arbitrary units it is not an immediate task to obtain the energy loss function.…”
We present a study where the energy loss function of Ta 2 O 5 , initially derived in the optical limit for a limited region of excitation energies from reflection electron energy loss spectroscopy (REELS) measurements, was improved and extended to the whole momentum and energy excitation region through a suitable theoretical analysis using the Mermin dielectric function and requiring the fulfillment of physically motivated restrictions, such as the f-and KK-sum rules. The material stopping cross section (SCS) and energy-loss straggling measured for 300−2000 keV proton and 200− 6000 keV helium ion beams by means of Rutherford backscattering spectrometry (RBS) were compared to the same quantities calculated in the dielectric framework, showing an excellent agreement, which is used to judge the reliability of the Ta 2 O 5 energy loss function. Based on this assessment, we have also predicted the inelastic mean free path and the SCS of energetic electrons in Ta 2 O 5 .
“…47,48 The Fresnel equations are evaluated for normal incidence, taking into account the bulk dielectric properties of the oxide layers [49][50][51][52] and of the metals. 53 Deviations from the bulk dielectric properties of the oxide and metal layers are not taken into account in the present work.…”
Heterosystems of metal/insulator/gold type with titanium oxide and tantalum oxide as internal barriers are studied using internal photoemission (IPE), field induced current transport (current transients after voltage steps) and chemical reaction induced current transport (chemicurrent). IPE investigations over a broad energy range from 0.8 to 4.5 eV allow a determination of the interstitial layers band gap and the maximum height of the internal tunnel barrier. The built-in field of the heterosystem is derived by the evaluation of the slope in the photoyield versus photon energy plot. Current transients recorded after voltage steps allow the determination of the heterosystems time constants which generally have a value of some milli seconds. In titanium oxide systems additional time constants with values of several 100 s appear for bias voltages >0.5 V. These time constants are assigned to slow processes altering the height of the titanium oxide barriers. and electron sources in spin polarized tunneling. 5 In the present work we present a comparative investigation of charge transport induced by different methods through thin oxide films. Charges are driven through the oxide by: i) application of a device voltage ii) illumination of the samples with monochromatic light at variable photon energies, leading to spectra of internal photoemission, iii) non adiabatic chemical surface reactions. All three methods are combined since it is possible to derive the nature of excited carriers transport through heterosystems.6 For aluminum and tantalum oxide heterosystems it was found, that they form a high pass filter for excited electrons and holes (defect electrons). 4,6 Since the height of the internal barriers for electrons and holes can be modified by an applied bias voltage, it became possible to characterize the spectra of excited charge carriers with energies below the vacuum barrier. Bias voltages of up to 1 V could be applied to the system which had an internal barrier height of 3 eV.To increase the detection efficiency for excited electrons travelling from the surface of a metal towards the bulk, one can either decrease the thickness of the top metal film of a heterosystem or one can reduce the height of the internal barrier. But with a decrease of the internal barrier the method of applying a bias voltage for tuning this barrier might become problematic, since tunnel currents become larger with lower barrier heights. Additionally, the influence of midgap states, impurities and remanent changes of the internal barrier might become more relevant for lower barriers.8,9 These problems are adressed in the present work.A comparison of metal/insulator/metal heterojunctions is presented with potentiostatically formed titanium and tantalum oxide as interjacent insulating layer. Titanium and tantalum oxide were chosen since both have bandgaps smaller than 4.5 eV.10 For amorphous tantalum oxide values of 4.2 eV are typical 11,12 whereas crystalline samples show values of 3.9-4.5 eV.12,13 Bulk titanium oxide values are for rut...
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