Enhancement of moisture resistance of spin-on low-k HSQ films by hot wire generated atomic hydrogen treatment Alka A. Kumbhar, Sunil Kumar Singh, R.O. Dusane * Department of Metallurgical Engineering and Materials Science, Indian Institute of Technology, Bombay, Mumbai-400 076, India Abstract Spin on hydrogen silsesquioxane (HSQ) is a material with low dielectric constant (k) and shows potential as intermetal dielectric (IMD) layers for future VLSI circuits. One major challenge in the integration of these films is the moisture uptake with time, which degrades the electrical performance and hence limits their application. In the present work, we show (under accelerated conditions) that the as deposited films absorb moisture significantly which is reflected in the related signatures in the infrared (IR) spectroscopic data. Subsequently there is an increase in the leakage current with a concurrent decrease in the electrical breakdown field. Upon treatment with atomic hydrogen generated by a hot filament (T F = 1900 -C), drastic reduction in the moisture absorption is observed. Also there is almost a 2 orders of magnitude reduction in the leakage current and no indication of any electrical breakdown within the range of applied field. Keywords: Hot wire generated atomic hydrogen treatment; Surface passivation; Intermetal dielectric (IMD); Moisture absorption 1. Introduction Continuous reduction in chip size and increase in chip complexity have given rise to the need for multilevel metallization. However, the RC delay contributed from multilevel interconnects limits the performance of the chip. Therefore, it is necessary to use a low-k material as dielectric and high conductivity metal for interconnects, to reduce this delay and increase the signal propagation speed [1]. Among the various low-k dielectric materials [2], hydrogen silsesquioxane (HSQ) shows a lot of promise for implementation at the < 0.13 Am technology. The low-k property can be achieved if the density of Si –H bonds are maintained at a high level and the formation of – OH bond due to the absorption of water in the film is minimized. The Si –H bond in the as cured HSQ is sensitive to temperature and moisture absorption since it tends to break forming Si –OH. The electric and dielectric properties of low-k IMD layers depend on their resistance moisture uptake [3]. Moisture resistance is thus a reliability concern for the long-term stability of the IMD layers even after packaging. In order to inhibit moisture absorption and the subsequent degradation of the properties we have carried out hot wire generated atomic hydrogen treatment of the HSQ films. To study the moisture resistance of these treated HSQ films, the effect of moisture penetration was evaluated by accelerated water treatment tests and subsequent determination of the I – V characteristics. 2. Experimental details HSQ films were spin-coated on to p-type silicon wafers and baked on a hot plate at 100 -C, 250 -C and 350 -C for 1 min each followed by furnace curing 1 h in nitrogen ambient at 400 -C and 500 -C [4]. The HSQ films were exposed to atomic hydrogen generated by hot wire (referred to as hot wire generated atomic hydrogen (HWGAH) treatment) in our hot wire CVD (HWCVD) chamber [5]. The treatment parameters are given in Table 1. For the moisture reliability test, the as cured as well as the 330 Parameter Value Gas used Gas flow Pressure Substrate temperature (T S) Filament temperature (T F) Time H2 10 sccm 1 Torr 250 -C 1900 -C 30 min HWGAH treated HSQ films were immersed in water at 80 -C for 3 h in a closed beaker (container). These conditions were chosen for accelerated testing and are similar to the pressure cooker test (PCT) in an earlier study [6]. The chemical structure of the cured HSQ films before and after the hot wire and water treatment was investigated by Fourier transform infrared (FTIR) spectroscopy. The thickness of HSQ films was measured by Dektak II profilometer. The dielectric constant (k) was extracted from the capacitance – voltage (C – V) characteristics measured at 100 kHz frequency. The C –V characteristics and the current – voltage (I – V) measurements were performed on MIS structures fabricated as Aluminum/HSQ/c-Si. 3. Results and discussion The HSQ film consists of a mixed cage/network structure before thermal curing. Part of the cage structure in the film is transformed to a network structure after thermal curing. This structural transformation results in significant lowering of the dielectric constant (k) down to 2.9. The associated vibrations of the network/cage structure in the HSQ films can be seen at 1070 (Si –O –Si network) and 1130 cm 1 (Si –O – Si cage) in its FTIR spectra (curve 1 as shown in Fig. 1). Their respective bending bands appear at 830 and 880 cm 1 respectively while the band at 2250 cm 1 corresponds to the Si –H stretching mode [7]. Infrared Absorbance (a. u.) Table 1 Parameters of hot wire hydrogen treatment of the HSQ films Si-OH 0.6 (4) Water treated HWGAH HSQ 0.4 0.0 (3) HWGAH 0.2 (2) Si-O (Network) Si-O (cage) Water treated HSQ (1) as cured HSQ 4000 3500 3000 Si-H 2500 2000 1500 1000 -1 Wavenumber (cm ) Fig. 2. FTIR spectra of the HSQ film and the HWGAH treated HSQ films after water treatment. Fig. 1 presents two major observations on the curing of HSQ films. First, the peak at 1130 cm 1 (assigned to cage like structure) decreases with increase in curing temperature while the peak at 1070 cm 1 (assigned to the network structure) increases with the curing temperature. Initially at lower curing temperatures (100 – 350 -C), the peak at 1130 cm 1 is stronger than that at 1070 cm 1. At higher temperatures > 350 -C, this trend changes, i.e. the intensity of the 1130 cm 1 peak decreases while that of 1070 cm 1 increases. Thus at higher temperature, the bonding structure of the HSQ film changes from cage like to a network structure. Another important observation is that the intensity of the Si – H peak (at 2250 cm 1), which appears to be the same for low curing temperature, starts to decrease at 400 -C. At high curing temperatures > 400 -C, the Si – H bonds are easily broken which causes generation of dangling bonds and hence absorption of moisture in the films. Thus, 1.0 Infrared Absorbance (a. u.) Si-O (cage) (4) 0.6 Annealed at 400°C for 1h Water and HWGAH HSQ (3) 0.4 Baked at 350°C for 1min Absorbance Si-O (Network) 0.8 Annealed at 500°C for 1h Baked at 250°C for 1min HWGAH 0.2 Baked at hot plate 100°C for 1min Si-O (cage) 0.0 Si-O (Network) (2) Water treated HSQ (1) -0.2 Si-H as cured HSQ As deposited -0.4 1600 2400 2000 1600 1200 800 Wavenumber (cm-1) Fig. 1. FTIR spectra of the HSQ films cured at different temperatures. 1400 1200 1000 800 600 Wavenumber (cm-1) Fig. 3. FTIR spectra in the range 1600 – 600 cm 1 of as cured and hot wire hydrogen treated HSQ film after 3 h of water treatment. Leakage Current density (A/cm2) 331 (2) 1.25x10-6 HSQ water treated 1.25x10-7 HSQ HWGAH HSQ/water treated 1.25x10-8 (1) (4) HWGAH HSQ (3) 1.25x10-9 1.25x10-10 0.0 0.2 0.4 0.6 0.8 1.0 Electric Field (MV/cm) Fig. 4. Leakage current density as a function of electric field of the as deposited (curve 1), as deposited but after water treatment (curve 2), HWGAH treated (curve 3) and HWGAH treated but after water treatment (curve 4). increasing the curing temperature for the HSQ films causes reduction in the Si –H (2250 cm 1) bond density and in turn increases the Si –O – Si (1070 cm 1) bond densities (see Fig. 1 annealed at 400 -C for 1 h). The appearance of the Si – H stretching mode at 2250 cm 1 is characteristic of the HSQ supplied by Dow Corning Inc. This material is a derivative of SiO2 in which one of the four oxygen atoms bonded to every Si atom is replaced by hydrogen. The higher electronegativity of oxygen atom is responsible in shifting the Si– H stretching mode from 2000 to 2250 cm 1. When this film is subjected to boiling water treatment, the film not only absorbs water vapor but also undergoes significant changes in its chemical bonding. Fig. 2 shows the FTIR spectra of the as-deposited HSQ film and the HWGAH treated HSQ films after water treatment. Curve 2 of Fig. 2 depicts these changes very clearly. We see that a broad band at 3350 cm 1 appears which is characteristic of water absorption. The integrated area of this band gives the relative amount of moisture absorbed by the HSQ film which is 7.5 for the as cured HSQ films as against 5.8 for the HWGAH treated HSQ films (curve 4). Interestingly the FTIR spectrum of the HWGAH treated HSQ film is similar to that of the untreated HSQ film (curve 3). This indicates that the HWGAH treatment does not affect the cage to network ratio in the HSQ film and that the dielectric property remains essentially unaffected. Fig. 3 shows the same results in an expanded IR range (1600 – 600 cm 1). It should be noticed that a small but significant change occurs in the region 800– 900 cm 1 which reflects the bending mode characteristics of Si – O –Si, after water treatment of the as cured HSQ films (curves 1 and 2). This can be explained on the basis of the following reaction Si H þ HOH ¼ Si OH þ H2 : The significant increase in both the k value and the leakage current could be attributed to these differences. However when the HWGAH treated film is water treated these changes in the bending modes are not seen (curves 3 and 4). The formation of Si – OH after moisture pickup seems to be responsible for the deterioration of the dielectric properties. Fig. 4 shows the leakage current density of HSQ films and HWGAH films before and after boiling water treatment. The leakage current density reduces by more than one order of magnitude by the hot wire hydrogen treatment of the as deposited films (curve 3). This may be due to the passivation of the surface dangling bonds by the active hydrogen radical provided by the hot wire. Even after moisture absorption the HWGAH treated HSQ film show a reduced (one order) leakage current density as compared to the as cured HSQ film. Also the as cured HSQ films without HWGAH treatment undergo an electrical breakdown at 0.75 MV/cm when they absorb moisture. On the other hand we do not observe any such breakdown up to a field of 1 MV/cm in the case of HWGAH treated films even after hot water treatment. 4. Conclusion As cured HSQ films tend to absorb moisture, which eventually leads to the degradation of their dielectric property. Exposure of these films to the hot wire generated hydrogen enhances their resistance to moisture absorption and helps to reduce their leakage current by more than one order of magnitude without affecting the dielectric property. The atomic hydrogen treated films do not reveal any discernible change in the IR spectrum, which clearly indicates that the atomic hydrogen generated by hot wire modifies the HSQ only on the surface and hence is not detectable in FTIR measurement. However the enhancement in the performance is significant enough to make this process applicable in the ULSI backend technology. Acknowledgements This work was carried out under the project supported by DST, Govt. of India (SR/FTP/PS-41/2000). References [1] The National Technology Roadmap for Semiconductors, Semiconductor Industry Association, San Jose, CA, 1997. [2] L. Peters, Semicond. Int. (1998) 64. [3] A.M. Ionescu, F. Mondon, D. Blachier, Y. Morand, G. Reimbond, MRS Symp. Proc. 565 (1999) 101. [4] A.A. Kumbhar, S.K. Singh, A. Srivastav, R.O. Dusane, Proceeding of the Twelfth International Workshop on the Physics of Semiconductor Device, Chennai, India, vol. 1, 2003, p. 268. [5] A.A. Kumbhar, R.O. Dusane, S. Bauer, B. Schroder, J. Non-Cryst. Solids 227 – 230 (1998) 452. [6] T. Furusawa, D. Ryuzaki, R. Yoneyama, Y. Homma, K. Hinode, J. Electrochem. Soc. 148 (2001) F175. [7] M.J. Loboda, C.M. Grover, R.F. Schneider, J. Electrochem. Soc. 145 (1998) 2861.
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