3.1 Microstructure analysis
Figure 2 shows the XRD of La2O3 and LaAlOx thin films deposited on Si substrate at 700°C. Based on some references, the La2O3 film is amorphous at 500°C. Its weak diffraction peaks will appear at 600°C at 2θ equal to 29.96° and 39.53° [14]. According to reports, high-k gate dielectrics featuring an amorphous structure are considered more appropriate for CMOS device applications due to the fact that polycrystalline materials with grain gaps tend to create current pathways leading to increased leakage currents and reduced device reliability [26]. A comparison of La2O3 and LaAlOx films annealed at 700°C reveals that the LaAlOx films do not show any obvious diffraction peaks, which indicates that aluminum doping does increase the crystallization temperature of La2O3, which is conducive to enhancing the dielectric properties of Al/LaAlOx/Si/Al MOS capacitors at high-temperature states [27, 28].
The morphology of the thin film samples was examined using a scanning electron microscope (SEM) to analyze both their surface and cross-section. Figure 3 illustrates the SEM images of the cross-sectional views of LaAlOx thin films following exposure to various heat treatment temperatures. The film thickness reduces from 40 nm initially to 35 nm as the annealing temperature increases. This could be attributed to the transformation of hydroxyl groups into oxides in the films fabricated using the sol-gel technique and the evaporation of organic solvents involved in the films [14]. As seen from the Mapping diagram of the LaAlOx film, the La, Al, and O elements are consistent throughout the film.
The surface morphology of LaAlOx thin films was analyzed using AFM. The images in Fig. 4 (a) and (b) depict the 2D and 3D AFM representations of the thin film samples, respectively. The RMS of the LaAlOx film after annealing at 500°C is measured to be 0.919 nm, and it decreases to a minimum of 0.320 nm when annealed at 700°C. Subsequently, the RMS increases to 0.539 nm when the annealing temperature reaches 800°C. This investigation replicates previous research, demonstrating that the annealing temperature significantly impacts surface roughness and grain size. A smoother gate dielectric layer resulting from a lower annealing temperature can effectively reduce interface trap density and enhance device performance The decrease in the RMS of LaAlOx films from 500°C to 700°C may be because the films are initially disordered, and as the temperature increases, the films tend to be ordered, and the roughness decreases. The rise in the RMS of the films between 700°C and 800°C may be due to the tendency of the films to crystallize [19].
The chemistry at the interface is crucial for high-k/Si gate stacks, and precise identification of interfacial details will establish guidelines for choosing appropriate high-k gate dielectric materials for CMOS devices. The variation patterns of Si 2p, O 1s, La 3d, and Al 2p spectra of LaAlOx/Si gate stacks with annealing temperature were determined by XPS measurements. Figure 5 shows the XPS measurement spectra of LaAlOx thin films. XPS experiments were conducted on the film specimens under varying annealing temperatures. C 1s (284.8 eV) in amorphous carbon was selected for the core calibration, and it can be observed in the figure that five elements, namely, La, Al, O, C, and Si, were detected in the full XPS spectrum of the LaAlOx film. It can be found that no peaks of other elements are detected except those of La, Si, Al, C, and O elements, indicating that Al has been doped into La2O3.
Figure 6 depicts the O1s core energy level spectra of LaAlOx gate-dielectric thin films with Si gate stacks, illustrating variations in response to annealing temperature. At 530.15 and 531.31 eV, all O1s peaks are deconvoluted into two subpeaks. In the film the first one comes from the bond between M and O in the film, while the second one comes from the bond between M and OH [29]. The existence of M-OH in gate dielectric films typically results in the generation of trap and defect states within the film's band gap, which can cause a rise in leakage current and a reduction in breakdown voltage for electrical devices. Meanwhile, forming a higher percentage of M-O bonds can lead to better dielectric properties for the device. Based on the data in Fig. 6(e), it is evident that the concentration of M-O bonds rises as the annealing temperature increases. The presence of M-OH bonds diminishes as the annealing temperature rises, as indicated in Table 1. This phenomenon can be attributed to the increase in temperature leading to thermal condensation within the La-OH and Al-OH bond films, gradually transforming them into La -O and Al-O bonds. Consequently, this results in an increased coordination number of metal ions, thereby facilitating the bonding of metal ions with oxygen ions. It can also be seen that as the annealing temperature increases to 800°C, the fitted O1s peak shifts to the direction of high binding energy, indicating that LaAlOx is fully oxidized and more silicate layers are formed, which will adversely affect the dielectric properties of Al/LaAlOx/Si/Al MOS capacitors.
Figure 6(f) illustrates the La 3d spectra of LaAlOx thin films at various annealing temperatures. The spectra display a central peak (La 3d5/2) and a spin-splitting peak (La 3d3/2), with energy differences of approximately 16.80, 16.80, 16.90, and 17.00 eV from 500 to 800°C. Based on the available literature, it has been observed that the splitting energies of La3d3/2 and La3d5/2 are approximately 16.80 eV, indicating the presence of the La + state. [30]. At 700°C, the movement of the peaks towards lower binding energies suggests the existence of O-La-O bonds within the LaAlOx films. However, with an increase in temperature to 800°C, there is a shift in binding energy towards higher values due to the close proximity of the La silicate layer to the interface with the Si substrate [14].
Table 1
Corresponding peak positions, half-height widths, and content percentages of each component of LaAlOx gate dielectric films O 1s
Temperature | | M-O | | | | Vo | | |
Peak position (eV) | FWHM (eV) | Content percentage | | Peak position (eV) | FWHM (eV) | Content percentage | |
500℃ | 529.97 | 2.29 | 74.6% | | 531.32 | 1.77 | 25.4% | |
600℃ | 530.03 | 2.18 | 78.7% | | 531.46 | 1.68 | 21.3% | |
700℃ | 529.47 | 2.51 | 83.3% | | 531.04 | 2.02 | 16.7% | |
800℃ | 529.89 | 2.5 | 87.7% | | 531.57 | 2.24 | 12.3% | |
MOS capacitors were fabricated using Al/LaAlOx/Si/Al structure, where Al top electrodes with an area of 7.068×10− 4 cm2 were deposited on the LaAlOx gate dielectric film via magnetron sputtering under shadowing, and Al back electrodes with the same thickness were applied to the backside of the silicon substrate. Figure 7 shows the variation curves of high-frequency (1 MHz) capacitance-voltage (C-V) with annealing temperature for the LaAlOx gate-dielectric MOS capacitor with double-sweeping in the range of ± 8 V gate voltage. It is evident that the accumulated capacitance \(\:{\text{C}}_{\text{o}\text{x}}\) exhibits a clear pattern of change as the annealing temperature increases. Initially, it rises with the annealing temperature, peaks at 700°C, and subsequently declines. The accumulated capacitances of LaAlOx are 245.01, 332.31, 365.82, and 353.27 pF, respectively. By Eq. [31]:
$$\:\text{k}=\frac{{\text{C}}_{\text{o}\text{x}}\text{d}}{{{\epsilon\:}}_{0}\text{A}}$$
Where \(\:{\text{C}}_{\text{o}\text{x}}\) is the accumulated capacitance, d is the film thickness, \(\:{{\epsilon\:}}_{0}\) is the vacuum dielectric constant (\(\:{{\epsilon\:}}_{0}\)=8.854×10− 12 F/m). The dielectric constants (k) of the samples annealed at 500°C, 600°C, 700°C, and 800°C were determined to be 15.73, 21.35, 20.91, and 20.79 respectively based on the area of the Al top electrode (A). The findings indicate that the effective dielectric constant (k) of the LaAlOx gate dielectric shifts from 15.73 for the annealed sample at 500°C to 20.79 for the annealed sample at 800°C, potentially attributed to the rise in annealing temperature. According to the XPS analysis, it is apparent that elevating the annealing temperature improves the interface quality and suppresses the expansion of low-k SiOx interlayer [32].
Furthermore, the flat-band capacitance (\(\:{\text{C}}_{\text{f}\text{b}}\)) of the sample was used to calculate the \(\:{\text{V}}_{\text{f}\text{b}}\), the EOT, the \(\:{\text{Q}}_{\text{o}\text{x}}\)and the electrical parameters such as the\(\:\varDelta\:{\text{V}}_{\text{f}\text{b}}\), and the \(\:{\text{N}}_{\text{b}\text{t}}\) in Table 2. The \(\:{\text{V}}_{\text{f}\text{b}}\) is associated with the oxide charge density, while the hysteresis is linked to the boundary-trap oxide charge density.
Table 2
Electrical properties derived from C-V and I-V characteristics
Annealing Temperature | k | \(\:EOT\left(nm\right)\) | \(\:{C}_{ox}\left(pF\right)\) | \(\:{C}_{fb}\left(pF\right)\) | \(\:{V}_{fb}\) | \(\:\varDelta\:{V}_{fb}\) | \(\:{Q}_{ox}\left({cm}^{-2}\right)\) | \(\:{N}_{bt}\left({cm}^{-2}\right)\) | \(\:{J}_{g}\left({A/cm}^{2}\right)\) |
500℃ | 15.74 | 9.96 | 245.01 | 61.09 | -0.32 | 1.28 | 1.04×1012 | 2.77×1012 | 1.39×10− 1 |
600℃ | 21.35 | 7.34 | 332.31 | 49.23 | -0.72 | 0.32 | 2.35×1011 | 9.40×1011 | 2.17×10− 2 |
700℃ | 20.91 | 6.67 | 365.82 | 44.88 | -0.24 | 0.16 | 1.81×1012 | 5.17×1011 | 3.54×10−3 |
800℃ | 20.79 | 6.91 | 353.27 | 40.84 | -0.08 | 0.16 | 2.29×1012 | 4.99×1011 | 8.84×10− 3 |
The absolute value of \(\:{\text{V}}_{\text{f}\text{b}}\) decreases as the annealing temperature increases. Films annealed at high temperatures exhibit reduced defects and traps, resulting in improved interface quality compared to films annealed at low temperatures. It is clear from Fig. 7 and Table 2 that the LaAlOx films annealed at 700°C have less hysteresis. It can be inferred that the hysteresis phenomenon is connected to the trapping of oxygen charges at the boundary, which indicates that the interface properties of the doped lanthanum alumina thin film have been enhanced with the increase of annealing temperature. At a gate voltage of 1 V the I-V characteristics depicted in Fig. 8 indicate that the LaAlOx films annealed at 700°C exhibit a minimum leakage current density of 3.54 × 10− 3 A/cm2. Raising the annealing temperature results in a higher surface density of the samples and improved adhesion of the film surface, leading to effectively reduced interfacial density of states and traps. The increase in \(\:{\text{Q}}_{\text{o}\text{x}}\) values with rising annealing temperature may be attributed to the generation of oxygen vacancies in the film caused by higher annealing temperatures. The \(\:{\text{N}}_{\text{b}\text{t}}\) values of samples annealed at higher temperatures appear to be relatively smaller compared to those annealed at 500°C. This could be attributed to the enhanced formation of denser gate dielectric films and higher-quality interfaces facilitated by the elevated annealing temperatures [20].
Nevertheless, as the annealing temperature was raised to 800°C, there was a noticeable rise in the leakage current density of the films. The findings suggest the electrical performances of LaAlOx films are optimal when annealed at 700°C.