Sangwook Park‡
a,
Yoona Choi‡b,
Sunwoo Parka,
Hayoon Leea,
Kiho Leea,
Jongwook Park*a and
Woojin Jeon*b
aIntegrated Engineering, Department of Chemical Engineering, Kyung Hee University, Deogyeong-daero, Giheung-gu, Yongin-si, Gyeonggi-do 17104, Republic of Korea. E-mail: jongpark@khu.ac.kr
bDepartment of Advanced Materials Engineering for Information and Electronics, Integrated Education Program for Frontier Science & Technology (BK21 Four), Kyung Hee University, Deogyeong-daero, Giheung-gu, Yongin-si, Gyeonggi-do 17104, Republic of Korea. E-mail: woojin.jeon@khu.ac.kr
First published on 10th September 2024
High dielectric constant (high-k) materials play a crucial role in modern electronics, particularly in semiconductor applications such as transistor gate insulators and dielectrics in metal–insulator–metal (MIM) capacitors. However, achieving optimal crystallinity and suppressing interfacial layer formation during deposition processes remain key challenges. To address these challenges, this study introduces a novel approach using atomic layer deposition (ALD) with a new Hf precursor incorporating an iodo ligand. The synthesized precursor, IHf, demonstrates enhanced thermal stability and reactivity, leading to superior film properties. ALD deposition of HfO2 thin films using IHf yields excellent crystallinity and effectively inhibits interfacial layer formation, resulting in enhanced capacitance density and improved leakage current characteristics in MIM capacitors. Notably, IHf-deposited HfO2 films exhibit a significant reduction in leakage current, achieving an equivalent oxide thickness of 1.73 nm at a leakage current density of 7.02 × 10−8 A cm−2 @ +0.8 V. These findings highlight the potential of IHf as a promising precursor for high-performance electronic device fabrication, paving the way for advancements in semiconductor technology.
In particular, in ALD processes, it is necessary to form crystallization seeds during the deposition stage to achieve the desired crystal structure and crystallinity.8–10 One method to enhance both the crystal structure and crystallinity of high-k thin films is by increasing the deposition temperature.11 However, there is a limitation on raising the deposition temperature due to the thermal decomposition of precursors in ALD processes12–14. To overcome this issue, the Chung research group introduced N-alkoxy carboxamidate ligands into the precursors. The incorporation of these ligands improved the volatility and thermal characteristics of the precursor, resulting in enhanced high-temperature reactivity.15 Particularly, derivatives such as HfCp(edpa)3, composed of a cyclopentadienyl ligand and three carboxamidate ligands, demonstrated high thermal stability and rapid crystallization. However, these compounds suffer from increased viscosity and a melting point range of 62–135 °C, which renders them solid at room temperature, thus posing drawbacks for ALD processes. Therefore, this study proposes new derivatives that can enhance the thermal stability of ALD precursors.
In this study, we present an ALD process for HfO2 using a novel Hf precursor with an iodo ligand. By introducing the iodo ligand, which exhibits relatively low reactivity compared to other halide precursors,16–19 we synthesized a new precursor, IHf, which offers increased thermal stability and higher chemical adsorption density compared to conventional halide precursors. The ALD process using IHf and O3 yielded HfO2 thin films with excellent crystallinity and effectively suppressed the formation of interfacial layers when used with TiN as bottom electrode material. This resulted in an increase in capacitance density in the TiN/HfO2/TiN MIM capacitor due to the increased dielectric constant of HfO2 and simultaneous improvement in leakage current characteristics by inhibiting interfacial layer formation. Particularly noteworthy is the significant improvement in leakage current characteristics, achieving an equivalent oxide thickness of 1.73 nm at a leakage current density of 7.02 × 10−8 A cm−2 @ +0.8 V in the HfO2 single layer.
The newly synthesized compound was obtained through a three-step synthesis process (Scheme 2). The starting material, cyclopentadiene, was synthesized via retro-Diels–Alder reaction and cracking distillation of dicyclopentadiene, achieving a yield of 91% without additional purification. The obtained cyclopentadiene was then subjected to substitution with lithium using n-BuLi reagent. Confirmation of lithium substitution was achieved using 1H-NMR spectroscopy. As the reaction progressed, multiplet peaks at δ 6.61 and δ 6.49, as well as the pentet peak at δ 3.01 representing cyclopentadiene, disappeared, while a new singlet peak emerged at δ 5.32, indicating successful lithium substitution. In the second step, upon introducing iodine, the appearance of a singlet peak at δ 5.04 and doublet peaks at δ 5.96 and δ 6.10 confirmed the formation of the desired product. In the final synthesis step, the resulting product was confirmed through 1H-NMR spectroscopy. The final synthesized compound exhibited a proton singlet peak around δ 2.84 representing dimethylamine and a proton triplet peaks at δ 5.74, 6.04 attributed to iodocyclopentadiene (Fig. S1†). The purity of the IHf precursor is over 98%, and the content of metals has been confirmed to be below 1 ppb for all 12 types of metals. The 12 types of metals are Ag, Au, Cd, Co, Li, Mg, Mn, Ni, Pb, Sn, V, and W atoms. As shown in Scheme 2 and Fig. S2,† the purity of the ligand compound (2) was confirmed to be over 99% through high-performance liquid chromatography (HPLC) experiments. Therefore, it can be confirmed that there is no CpHf content in the final compound, IHf precursor.
Fig. 1 (a) Thermal decomposition of CpHf and IHf precursors. Linear growth behavior of HfO2 thin film deposition processes using (b) CpHf + O3 and (c) IHf + O3. |
The surface morphology and crystallinity difference of HfO2 films deposited using CpHf and IHf precursors was analyzed (Fig. 2). O3 was used as the reactant, and deposition temperature was kept constant at 300 °C. HfO2 thin films deposited using CpHf and IHf do not exhibited any significant difference in morphology, as shown in AFM analyses (Fig. S4†). As-deposited films with CpHf showed no distinct crystallization peak up to a thickness of 15 nm, indicating an amorphous state. However, after post-deposition rapid thermal annealing (PDA) at 600 °C for 30 s under a N2 atmosphere, crystallization-induced diffraction peaks were observed, showing a mixture of monoclinic and tetragonal phases. Notably, distinct peaks were only evident at a thickness of 15 nm, diminishing as the film thickness decreased to 10 and 7 nm, resembling the amorphous state. Conversely, films deposited with IHf exhibited broad peaks around 30–35°, indicating a meso-crystalline structure instead of amorphous, even in the as-deposited state.24 This suggests that crystalline seeds were embedded with IHf deposition at 300 °C, leading to significantly higher crystallinity after annealing. XRD results of HfO2 thin films after conducting PDA revealed much stronger and clearer diffraction peaks for IHf-deposited films compared to CpHf, even at 7 nm thickness, indicating more effective induction of crystallization by IHf precursors from the as-deposited state and enhanced crystallinity after annealing.
The chemical state analysis of the deposited HfO2 films was confirmed using XPS (Fig. 3). The oxidation state of Hf was analyzed using Hf 4f spectra, showing no significant difference between films deposited with CpHf and IHf, both confirming Hf4+ oxidation states. However, depth profiling revealed differences between the precursors. In the HfO2 film deposited using CpHf, approximately 3 at% of nitrogen content was shown (Fig. 3(b)). Furthermore, nitrogen content was not detected on the surface of the film, but it was observed after 4 seconds of Ar sputtering. Particularly, on the nitrogen-free surface of the HfO2 film, the Hf:O ratio was 36.4:63.6 at%, indicating a favorable O/Hf ratio of 1.75. However, in the film where nitrogen content was detected, the film exhibited an O/Hf ratio of 40.3:56.5 at%, resulting in an O/Hf ratio of 1.40, indicating a highly oxygen-deficient composition. In contrast, in the HfO2 film deposited with IHf, no nitrogen content was detected, and the Hf:O ratio was 34.5:65.4 at%, indicating an ideal stoichiometry with an O/Hf ratio of 1.89 (Fig. 3(c)). To identify the cause of nitrogen content in HfO2 films deposited with CpHf, N 1s spectra were analyzed. In HfO2 films deposited with CpHf, the oxidation state of nitrogen included in the film was confirmed at etch times of 15 s and 50 s, revealing oxidized TiN (Ti–O–N) states with a binding energy of 398.4 eV at both locations.25,26 Conversely, the oxidation state of nitrogen in HfO2 films deposited with IHf showed Ti–N bonding with a binding energy of 397.7 eV.27,28 This indicates that the TiN bottom electrode undergoes oxidation damage by O3 when deposited with CpHf. This is related to the difference in deposition rates observed in Fig. 1. In ALD, the deposition rate is determined by the chemisorption density of precursors, which is reduced by the steric hindrance effect, where the adsorption sites are blocked by the physical size of the ligands, and the screening effect, where the adsorption sites are blocked by physisorption of precursors.29–31 Surfaces that are not covered by adsorbates due to these effects are subsequently exposed to the reactant during the reactant feeding step. Particularly, on substrates with high reactivity with oxygen such as TiN, surface oxidation occurs, leading to the formation of interfacial layers. Thus, the lower deposition rate with CpHf indicates that more TiN substrate exposure occurs due to these effects compared to IHf, resulting in more severe oxidation damage of the TiN substrate, appearing as Ti–O–N. TEM analyses were conducted to investigate the formation of the interfacial layer based on the precursors (Fig. S5†).32 In the case of CpHf, a relatively significant interfacial layer (IL) formation is observed, which corresponds well with the XPS results. Especially, Ti O–N formed by TiN oxidation damage is in an unstable state, leading to additional oxidation to TiO2 and causing an oxygen scavenging effect, which assumes additional oxygen from the deposited metal oxide film.30 Moreover, this additional oxidation may also induce some N diffusion from the TiN substrate into the HfO2 thin film, as evidenced from the relatively high N-contamination level within the depth of the HfO2 thin film (Fig. 3(b)). Therefore, it can be inferred that the formation of Ti–O–N interfacial layers contributes to the low O/Hf ratio and to N incorporation in HfO2 films deposited with CpHf. This TiON interface formation with CpHf precursor can be further accounted for in Fig. 1(b), with the larger increase in thickness with CpHf as compared to IHf at temperatures larger than 325 °C. Consequently, IHf can be considered a more effective Hf precursor than CpHf for ALD deposition of HfO2 films, as it suppresses TiN substrate oxidation damage, thereby inhibiting interfacial layer formation ensuring improved O/Hf stoichiometry and preventing N contamination in HfO2 thin films. Consequently, IHf can be considered a more effective Hf precursor than CpHf for ALD deposition of HfO2 films, as it suppresses TiN substrate oxidation damage, thereby inhibiting interfacial layer formation and ensuring O/Hf stoichiometry.
This improved suppression of interfacial layer formation also affects the enhanced crystallinity observed in Fig. 2. Unlike CpHf, which is hindered in crystallization by nitrogen content and oxygen deficiency, IHf forms crystalline seeds from the as-deposited state due to fewer impurities and ideal O/Hf stoichiometry. Additionally, crystallization due to the template effect of cubic TiN likely contributes to the high crystallinity of HfO2 films deposited with IHf.
These results enable potential improvements in the characteristics of HfO2 films deposited by ALD using IHf precursors. The thermal stability of each precursor is influenced by the cyclopentadienyl ligand binding to the central metal during chemical adsorption. Hence, the enhanced thermal stability of IHf is attributed to the incorporation of the halide group iodine in the cyclopentadienyl ligand. This can be explained by the molecular weight effect due to the introduction of iodine. The molecular weight of IHf is 501.71 g mol−1, which is increased by 125.91 g mol−1 compared to CpHf. As a result of this increase in molecular weight, organometallic compounds achieve relatively higher thermal stability while maintaining their liquid form and electronic state.33,34 Despite these results, IHf demonstrates superior reactivity compared to traditional precursors, where increased thermal stability often leads to decreased reactivity. These results suggest that the addition of the iodine halide group induces an electron-withdrawing effect through the cyclopentadienyl group, relatively reducing the electron density around the hafnium central metal. Consequently, the bond dissociation energy between the dimethylamine group and the hafnium central metal increases. As a result, due to the strong bond energy, IHf material gains the advantage of being capable of deposition even at relatively higher temperatures.
These improvements in crystallinity and suppression of interfacial layer formation led to enhanced electrical properties in metal–insulator–metal (MIM) capacitors of TiN/HfO2/TiN structure (Fig. 4). Firstly, the bulk dielectric constants were determined via a physical thickness versus equivalent oxide thickness (tphy–tox) plot (Fig. 4(a)). The inverse of the slope of (tphy–tox) plot can be used to determine the bulk dielectric constant. The bulk dielectric constants of the HfO2 films deposited with CpHf and IHf were measured to be 12.8 and 16.9, respectively. Dielectric constants below 20 are attributed to crystallization into the monoclinic phase. And, relatively higher crystallinity of HfO2 thin film deposited using IHf attributed to relatively higher dielectric constant than that of CpHf.7 Next, the leakage current characteristics of the MIM capacitors were examined through leakage current density versus applied voltage (J–V) curves. The J value of HfO2 films deposited with IHf was 2–3 orders of magnitude lower than that of the films deposited with CpHf in all examined thicknesses. This improvement can be attributed to enhancements in the intrinsic properties of HfO2 and improvements in the interfacial layer with TiN. Firstly, degradation in leakage current characteristics due to intrinsic aspects related to nitrogen content within the HfO2 films deposited with CpHf is identified. Additionally, relatively oxygen deficient composition in the CpHf-deposited films would cause severe leakage current. The main carrier conduction in HfO2 occurs through Poole–Frenkel (P–F) emission, which involves the detrap of electrons trapped at defect sites within the HfO2 film.35,36 The defects contributing to P–F emission are primarily associated with oxygen vacancies. This indicates that the suppression of interfacial layer formation when using IHf as a precursor effectively inhibits the formation of oxygen vacancies within the HfO2 films, contributing to significant improvements in leakage current. These enhancements in the dielectric constant and leakage current characteristics of HfO2 films deposited with IHf are clearly evident in the leakage current versus equivalent oxide thickness (J–tox) plot (Fig. 4(c)). HfO2 films deposited with CpHf exhibit high leakage currents of over 10−7 A cm−2 at an applied voltage of +0.8 V. In particular, at a thickness of 7 nm, which is the practical utilization thickness of the dielectric layer in DRAM capacitors, a very high leakage current of 10−2 A cm−2 was observed. Conversely, HfO2 films deposited with IHf demonstrate leakage currents of 10−7 A cm−2 even at a thickness of 7 nm, achieving leakage currents at levels suitable for the practical utilization in DRAM at a tox of 1.75 nm.
Fig. 4 (a) tphy–tox plot, (b) J–V curves, and (c) J–tox plot of HfO2 thin films varied thicknesses using CpHf and IHf precursors. |
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4ra05848h |
‡ Sangwook Park and Yoona Choi contributed equally to this work as first authors. |
This journal is © The Royal Society of Chemistry 2024 |