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Low-temperature fabrication of an HfO2 passivation layer for amorphous indium–gallium–zinc oxide thin film transistors using a solution process

Scientific Reportsvolume 7, Article number: 16265 (2017) | Download Citation


We report low-temperature solution processing of hafnium oxide (HfO2) passivation layers for amorphous indium–gallium–zinc oxide (a-IGZO) thin-film transistors (TFTs). At 150 °C, the hafnium chloride (HfCl4) precursor readily hydrolyzed in deionized (DI) water and transformed into an HfO2 film. The fabricated HfO2 passivation layer prevented any interaction between the back surface of an a-IGZO TFT and ambient gas. Moreover, diffused Hf4+ in the back-channel layer of the a-IGZO TFT reduced the oxygen vacancy, which is the origin of the electrical instability in a-IGZO TFTs. Consequently, the a-IGZO TFT with the HfO2 passivation layer exhibited improved stability, showing a decrease in the threshold voltage shift from 4.83 to 1.68 V under a positive bias stress test conducted over 10,000 s.


Amorphous oxide semiconductor (AOS)-based thin-film transistors (TFTs) are promising alternatives for conventional amorphous silicon-based TFTs because of their superior electrical characteristics, such as high field-effect mobility (μFET), low off-current, and high transparency in the visible range1,2,3,4. However, AOS TFTs have a significant issue of inferior bias instability due to the adsorption/desorption of oxygen and water molecules in the channel layer5,6. Various passivation layers, such as SiO2, SiNx, and Al2O3, have been adopted to address this issue6,7,8,9. These inorganic materials are generally deposited by vacuum processes including plasma-enhanced chemical vapor deposition (PECVD), pulsed laser deposition (PLD), and sputtering. However, vacuum-based processes have the disadvantages of being complex and costly, and plasma damage on the back surface of a channel can lead to performance degradation of TFTs8,9,10.

Solution-processed passivation layers have been explored to overcome the limitations of vacuum processes. These layers have the advantages of being simple processes, and are inexpensive and do not use potentially damaging plasmas. Organic materials, such as poly(methyl methacrylate) (PMMA)11,12, polydimethylsiloxane (PDMS)5, and polyacrylate (PA)6 are commonly used to fabricate solution-processed passivation layers. These materials have been suggested as passivation layers for flexible electronics because they can be fabricated at low temperatures, i.e., below 150 °C. However, they are more permeable to gases compared with inorganic materials, and hence the instability issue of AOS TFTs caused by the interaction between a channel and the ambient atmosphere cannot be completely eliminated9,10. Solution-processed passivation layers using inorganic materials, such as Y2O3 and Al2O3, have been studied as an alternative to organic passivation layers13,14,15,16. Although they are much better gas barriers than organic passivation layers, they must be fabricated at high temperatures, i.e., above 250 °C, which limits their use with some flexible substrates.

In this study, a solution-processed hafnium oxide (HfO2) passivation layer was fabricated at low temperature (150 °C) using an aqueous solution of hafnium chloride (HfCl4) because strongly hydrated HfCl4 decomposes and transforms into HfO2 at lower temperature than anhydrous HfCl4. The electrical characteristics and stability of the indium–gallium–zinc oxide (a-IGZO) TFT with HfO2 passivation were compared with those of a-IGZO TFTs without passivation, and with the commonly used PMMA and Y2O3 passivation11,12,13,14,15. Thermogravimetric analysis and differential scanning calorimetry (TGA/DSC) and X-ray photoelectron spectroscopy (XPS) analysis of the HfO2 passivation layer verified the formation of the HfO2 passivation layer at 150 °C. The effect of HfO2 passivation was also demonstrated by comparing the XPS depth profile results for a-IGZO TFTs without passivation and with HfO2 passivation.


Figure 1(a) shows the deionized (DI) water-based solution process used to fabricate the a-IGZO TFTs with HfO2 passivation. The a-IGZO TFTs without passivation and with PMMA and Y2O3 passivation were also prepared for comparison. Figure 1(b) shows the transfer characteristics of the a-IGZO TFTs without passivation and with PMMA, Y2O3, and HfO2 passivation annealed at 150 °C. The 150 °C-annealed a-IGZO TFT with PMMA passivation, which is a commonly-used organic passivation layer, showed proper switching characteristic, as reported previously11,12. However, the a-IGZO TFT with Y2O3 passivation, which is the most widely studied solution-processed passivation among inorganic materials, showed no switching characteristic, while the a-IGZO TFT with HfO2 passivation showed proper switching characteristic13,14,15. This indicated that the thermal energy at the annealing temperature at 150 °C was insufficient for the Y2O3 precursor solution to form a passivation layer, which resulted in an excess carrier concentration in the channel layer13. The passivated a-IGZO TFTs were annealed from 100 to 250 °C to identify the minimum processing temperature for Y2O3 and HfO2 passivation. Figure 2(a) shows the evolution of the transfer characteristics for the a-IGZO TFT with Y2O3 passivation as a function of annealing temperature. It reveals that the annealing temperature of the solution-processed passivation layer made with the Y2O3 precursor solution should be ca. 250 °C to form a passivation layer. On the other hand, the HfO2 precursor solution would form an HfO2 passivation layer after thermal annealing at 150 °C. The transfer characteristic of the a-IGZO TFT with HfO2 passivation exhibited similar performance to that of the a-IGZO TFT without passivation (Fig. 2(b)). The μFET, threshold voltage (Vth), on/off ratio, and subthreshold swing (SS) of the a-IGZO TFT with HfO2 passivation were 9.60 ± 0.98 cm2/Vs, 1.49 ± 0.89 V, (2.54 ± 1.11) × 108, and 0.35 ± 0.4 V/dec, respectively (Table 1).

Figure 1
Figure 1

(a) Schematic structure of the a-IGZO TFT with solution-processed HfO2 passivation and (b) transfer characteristics of the a-IGZO TFTs without passivation and with PMMA, Y2O3, and HfO2 passivation annealed at 150 °C.

Figure 2
Figure 2

Transfer characteristics of the a-IGZO TFTs with (a) Y2O3 and (b) HfO2 passivation as a function of annealing temperature.

Table 1 Extracted parameters of the a-IGZO TFTs without passivation and with PMMA, Y2O3, and HfO2 passivation annealed at 150 °C.

To confirm the effectiveness of the HfO2 passivation layer, the positive bias stress (PBS) test was performed for 10,000 s with VGS = 20 V, and VDS = 10.1 V. Figure 3(a,b) show the evolution of the transfer characteristics for the a-IGZO TFTs without passivation and with HfO2 passivation under PBS. After the test, the Vth shift (ΔVth) of the a-IGZO TFT with HfO2 passivation was 1.68 V, whereas that of the a-IGZO TFT without passivation was 4.83 V. Therefore, although the HfO2 passivation layer was fabricated at the low temperature of 150 °C, it was effective as a passivation layer. The a-IGZO TFT with PMMA passivation annealed at 150 °C was also subjected to the PBS test for comparison. The ΔVth of the a-IGZO TFT with PMMA passivation was 3.54 V after 10,000 s, which was inferior to that of the a-IGZO TFT with HfO2 passivation (Fig. 3(c)). This demonstrated that the barrier property of the HfO2 passivation layer annealed at 150 °C was better than that of the PMMA passivation layer when processed at low temperature.

Figure 3
Figure 3

PBS test results of the a-IGZO TFTs (a) without passivation and with (b) PMMA and (c) HfO2 passivation, and (d) comparison of the PBS test results.


The thermal decomposition characteristics of the HfCl4 precursor for the HfO2 passivation layer depend on its hydration state. The HfCl4 starting material is weakly hydrated with a composition of HfCl4·1/6H2O. When using an anhydrous solvent for the HfO2 precursor solution, the HfCl4·1/6H2O decomposes into anhydrous HfOCl2 via the intermediate Hf(OH)Cl3, as follows:

$${{\rm{HfCl}}}_{4}+\frac{1}{6}{{\rm{H}}}_{2}{\rm{O}}\to \frac{1}{6}{\rm{Hf}}({\rm{OH}}){{\rm{Cl}}}_{3}+\frac{5}{6}{{\rm{HfCl}}}_{4}+\frac{1}{6}{\rm{HCl}}$$
$${\rm{Hf}}({\rm{OH}}){{\rm{Cl}}}_{3}\to {{\rm{HfOCl}}}_{2}+{\rm{HCl}}$$

Further reaction of the HfOCl2 leads to HfO2 and HfCl4, which sublimes at ca. 300 °C at atmospheric pressure17,18.

$$2{{\rm{HfOCl}}}_{2}\to {{\rm{HfO}}}_{2}+{{\rm{HfCl}}}_{4}$$

However, the hydrolysis reaction readily occurs when water is used as the solvent to form Hf(OH) x Cl4−x , as follows:

$${{\rm{HfCl}}}_{4}+x{{\rm{H}}}_{2}{\rm{O}}\,\to {\rm{Hf}}{({\rm{OH}})}_{x}{{\rm{Cl}}}_{4-x}+x\text{HCl}\,(x=1\,or\,2)$$

The Hf(OH) x Cl4−x is unstable and transforms into HfOCl2, which leads to formation of the oxychloride octahydrate (HfOCl2·8H2O), as follows:

$${\rm{Hf}}({\rm{OH}}){{\rm{Cl}}}_{3}\to {{\rm{HfOCl}}}_{2}+{\rm{HCl}}$$
$${\rm{Hf}}{({\rm{OH}})}_{2}{{\rm{Cl}}}_{2}\to {{\rm{HfOCl}}}_{2}+{{\rm{H}}}_{2}{\rm{O}}$$

This strongly hydrated HfOCl2·8H2O has a tetrameric structure that has only doubly-bridging OH bonds. The HfOCl2 decomposes and transforms into HfO2 at ca. 150 °C according to the following reaction17:

$${{\rm{HfOCl}}}_{2}+n{{\rm{H}}}_{2}{\rm{O}}\,\to {{\rm{HfO}}}_{2}+2{\rm{HCl}}+(n-1){{\rm{H}}}_{2}{\rm{O}}$$

Figure 4 shows the TGA/DSC analysis result of the HfO2 precursor solution, where the HfCl4 is dissolved in DI water. There is an abrupt weight loss around 100 °C, but it is hard to distinguish the HfOCl2 decomposition from water solvent evaporation. This is due to the decomposition characteristic of strongly hydrated HfOCl2·8H2O. This result shows a distinguishable trend in decomposition temperature from the previously reported TGA result of anhydrous HfCl4 reported previously, where a large weight loss occurs between 200 and 300 °C17. Thus, the hydration state is the most significant parameter for the passivation temperature of solution-processed HfO2. Using water as the solvent is the best way to maximize the extent of hydration, which enables formation of the solution-processed inorganic passivation layer at low temperature.

Figure 4
Figure 4

The TGA/DSC curves of the HfO2 precursor solution.

XPS was used to examine the solution-processed Y2O3 and HfO2 passivation layers that were annealed at 150 and 250 °C (Fig. 5). The Y 3d spectra of Y2O3 and Hf 4 f spectra of HfO2 showed doublet features (Fig. 5(a,b)). At the higher annealing temperature, the Y 3d5/2 and Y 3d3/2 peaks shifted from 157.8 to 157.5 eV, and from 159.7 to 159.5 eV, respectively, and the Hf 4f7/2 and Hf 4f5/2 peaks from 17.3 to 17.1 eV and 18.8 to 18.6 eV, respectively. This indicated that there was an increase in Y–O and Hf–O bonding, and a decrease in the number of hydroxyl groups at the higher annealing temperature19,20,21,22,23. Specific analyses for oxide and hydroxide were done by deconvoluting the O 1s spectra of the Y2O3 and HfO2 passivation layers, which had been annealed at 150 and 250 °C. The O 1s peak was deconvoluted into two peaks centered at 529.5 and 531.3 eV for Y2O3, and at 530.4 and 531.8 eV for HfO2 (Fig. 5(c–f)). The first peak corresponded to the binding energy of the oxide, and the second peak to the hydroxyl groups18,19,24,25. The O 1s spectrum of Y2O3 annealed at 150 °C was similar to that of the as-deposited film, indicating a large number (59.6%) of hydroxyl groups (Fig. 5(c) 20. This amount decreased to 42.5% as the annealing temperature increased to 250 °C (Fig. 5(e)), when the spectrum resembled that of a conventional Y2O3 film20,21. However, the O 1s spectrum of HfO2 was already similar to that of a standard HfO2 film when annealed at only 150 °C18,19. It had a small number of hydroxyl groups (21.4%), and there was a slight decrease for the 250 °C-annealed film. Therefore, the solution processed HfO2 passivation layer is sufficiently oxidized when annealed at 150 °C, and a small number of hydroxyl groups can ensure TFT reliability because dissociated hydrogen from hydroxide bonds can diffuse into a channel and affect the characteristic of TFT26,27.

Figure 5
Figure 5

XPS results for (a) the Y 3d spectra of the Y2O3 and (b) the Hf 4 f spectra of the HfO2 passivation layer annealed at 150 °C and 250 °C, and the O 1s spectra of the (c) Y2O3 and (b) HfO2 passivation layer annealed at 150 °C, and the (e) Y2O3 and (f) HfO2 passivation layer annealed at 250 °C.

In the PBS test, the principal origin of instability is the interaction between the ambient gas and the back surface of the TFT6,8,28. When a positive bias is applied to a gate, accumulated free electrons are captured by the adsorbed oxygen molecules on the back surface of a TFT. This can be mitigated with a passivating layer. Our results demonstrated that an effective HfO2 passivation layer could be formed at an annealing temperature of 150 °C, and this effectively reduced the interaction between ambient gases and the back-channel layer.

The oxygen vacancy (Vo) in the channel layer can act as a trap site and lead to PBS instability15,29. Hence, XPS depth analyses for the channel layers of the a-IGZO TFTs without passivation and with the HfO2 passivation layer were also made, to confirm additional benefits of the solution-processed HfO2 passivation. Figure 6(a,c) show the O 1s spectra for the back-channel region of the a-IGZO film without passivation and with HfO2 passivation, respectively, and Fig. 6(b,d) show the same for their bulk-channel regions. We used 25% of the total channel etching time of the a-IGZO film without passivation and with HfO2 passivation in the back-channel region that was adjacent to the back surface or HfO2 layer, and 75% of the total channel etching time in the bulk-channel region that is far from the back surface or HfO2 layer. The O 1s peak was deconvoluted into three peaks centered at 530.1 ± 0.2, 531.0 ± 0.2, and 532.0 ± 0.2 eV29. These features corresponded to In, Ga, and Zn metal oxide bonds (M–O), Vo, and metal hydroxide species (–OH), respectively. For the a-IGZO film without passivation, there was little difference between the Vo ratios of the back- and bulk-channel regions; the Vo ratios for the back- and bulk-channel regions were 31.9 and 32.9% respectively (Fig. 6(a,b)). However, in the case of the a-IGZO film with HfO2 passivation, the Vo ratio in the back-channel was 23.7% and that in the bulk-channel was 32.7%, i.e., there was a decreased Vo and increased M–O in the back-channel region compared with the bulk-channel region (Fig. 6(c,d)). Figure 6(e) shows the Hf 4d spectra for the back- and bulk-channel regions of the a-IGZO film with HfO2 passivation. The Hf 4d spectra of these films were also studied because the core level binding energy of Ga 3d at 20.6 eV is near that of Hf 4 f (18.9 eV)22,23,30.

Figure 6
Figure 6

XPS depth analyses for the O 1s spectra of the (a) back- and (b) bulk-channel of the a-IGZO TFT without passivation, and the (c) back- and (d) bulk channel of the a-IGZO TFT with HfO2 passivation, and (e) the Hf 4d spectra of the a-IGZO TFT with HfO2 passivation.

It has been reported that Hf4+ can act as an oxygen binder and reduce Vo in AOS films28,31,32,33,34. This could be due to the low standard electrode potential (SEP) of Hf (−1.70 V), which could strengthen M–O more effectively than Ga (SEP: −0.52 V) in the a-IGZO film35. The Hf4+ diffused into the back-channel region of the a-IGZO film and reduced the Vo concentration in the back-channel layer. The resulting reduced instability of the a-IGZO TFT with HfO2 passivation was attributed to the barrier effect of the back surface and a reduction in the number of Vo-related trap sites (Fig. 7).

Figure 7
Figure 7

Schematic mechanism for the stability enhancement by solution-processed HfO2 passivation layer of a-IGZO TFT.

In conclusion, a DI water-based solution-processed HfO2 passivation layer was successfully prepared at the low temperature of 150 °C. This prevented any interaction between ambient gases and the back surface of an a-IGZO TFT, and the diffusion of Hf4+ into the channel layer suppressed oxygen deficiencies. PBS testing for 10,000 s revealed that the bias instability ΔVth improved from 4.83 V for the a-IGZO TFT without passivation to 1.68 V with HfO2 passivation. Moreover, the stability enhancement by HfO2 passivation was superior to that by PMMA passivation. The DI water-based solution-processed HfO2 passivation is competitive with organic passivation from the perspective of a low-temperature process for flexible electronics.


Fabrication of the a-IGZO TFTs

The a-IGZO TFTs were fabricated with an inverted staggered structure. The a-IGZO film (40-nm-thick) was deposited using radio-frequency (RF) magnetron sputtering on a heavily doped p-type Si wafer having a thermally oxidized SiO2 coating 1,200 Å thick. The IGZO target was three inches in diameter and consisted of In2O3:Ga2O3:ZnO at a ratio of 1:1:1 (mol%). After channel deposition, the samples were annealed in ambient air at 300 °C for 1 h. Aluminum layers (200-nm-thick) were deposited for source/drain electrodes by thermal evaporation using a shadow mask. The width and length of the channel were 1,000 and 150 μm, respectively.

Fabrication of the passivation layer

To fabricate the HfO2 passivation layer, the HfO2 precursor solution (0.1 M) was prepared by dissolving hafnium (IV) chloride (HfCl4; Aldrich, 98%) in DI water. For the Y2O3 passivation layer, the Y2O3 precursor solution was made using yttrium (III) chloride hexahydrate (YCl3·6H2O; Aldrich, 99.9%) using the same molar ratio and solvent as the HfO2 precursor solution. For the PMMA passivation layer, the PMMA precursor solution was synthesized by dissolving 40 mg/mL of PMMA ([CH2C(CH3)(CO2CH3)]n; Aldrich; Mw ca.15,000) in butyl acetate (CH3COO(CH2)3CH3; Sigma–Aldrich, 99%). All solutions were stirred for 1 h at room temperature and aged for 24 h. The precursor solutions were then spin-coated onto the fabricated a-IGZO TFTs at 3,000 rpm for 30 s, and annealed at 100 to 250 °C in air for 1 h.

Electrical characteristics and chemical properties measurement

The electrical characteristics of the a-IGZO TFTs without passivation and with PMMA, Y2O3, and HfO2 passivation were measured using a semiconductor parameter analyzer (model HP 4156 C; Agilent Technologies). To analyze the stability, PBS tests were conducted for 10,000 s with VGS = 20 V and VDS = 10.1 V in air. The thermal decomposition characteristic of the precursor solution was measured using TGA/DSC (model SDT Q600; TA Instruments). The chemical properties of the channel and passivation layer of samples were measured using XPS (model K-Alpha; Thermo Fisher Scientific).

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This work was supported by the National Research Foundation of Korea (NRF) grant funded by the Korea government (MSIT) (No. 2017R1A2B3008719).

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  1. School of Electrical and Electronic Engineering, Yonsei University, 50 Yonsei-ro, Seodaemun-gu, Seoul, 03722, Republic of Korea

    • Seonghwan Hong
    • , Sung Pyo Park
    • , Yeong-gyu Kim
    • , Byung Ha Kang
    • , Jae Won Na
    •  & Hyun Jae Kim


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S.H., S.P.P., Y.-G.K., B.H.K., and J.W.N. designed the research. S.H. and S.P.P. conducted experiments. S.H. analyzed the results and wrote the manuscript. H.J.K. guided the project. All authors reviewed the manuscript.

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The authors declare that they have no competing interests.

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Correspondence to Hyun Jae Kim.

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