Micro-scale metallization of high aspect
Transcription
Micro-scale metallization of high aspect
Microelectronic Engineering 77 (2005) 116–124 www.elsevier.com/locate/mee Micro-scale metallization of high aspect-ratio Cu and Au lines on flexible polyimide substrate by electroplating using SU-8 photoresist mask S.H. Cho, S.H. Kim, J.G. Lee, N.-E. Lee * Department of Materials Engineering and Center for Advanced Plasma Surface Technology, Sungkyunkwan University, 300 Chunchun-dong, Suwon, Gyunggi-do 440-746, Republic of Korea Received 10 July 2004; accepted 14 September 2004 Available online 19 October 2004 Abstract In order to fabricate flexible microelectronic devices, fabrication of metallization lines and metal electrodes on the flexible substrate is essential. Cu lines are often used as interconnect lines in electronic devices and Au as microelectrodes in organic transistors and bioelectronics devices due to its good electrochemical stability and biocompatibility. For minimizing the size of device, the realization of metallization lines and microelectrodes with the scale of a few micrometers on the flexible substrate is very important. In this work, micro-scale metallization lines of Cu and Au were fabricated on the flexible polyimide (PI) substrate by electroplating using the patterned mask of a negative-tone SU-8 photoresist. Surface of PI substrate was treated by O2 inductively coupled plasma for improvement of the adhesion strength between Cr layer and PI and in situ sputter-deposition of 100-nm thick Cu seed layers on the sputter-deposited 50-nm thick Cr adhesion layer was followed. Electroplating of high aspect-ratio Cu and Au lines using a sulfuric acid and a noncyanide solution with the patterned SU-8 mask, respectively, removal of SU-8, and selective wet etch of Cr adhesion and Cu seed layers were carried out. Micro-scale Au electrode lines were successfully fabricated on the PI substrate. Micro-scale gap-filled Cu lines with spin-coated polyimide on the PI substrate with the thickness of 6–12 lm and the aspect ratio of 1–3 were successfully fabricated. 2004 Elsevier B.V. All rights reserved. Keywords: Cu metallization; Au electrode; Electroplating; Polyimide; Gap-filling; Flexible electronics 1. Introduction * Corresponding author. Tel.: +823 129 07398; fax: +823 129 07410. E-mail address: nelee@skku.edu (N.-E. Lee). Polymer for microelectronic applications has attracted a great deal of concern in the past few years because polymers can be applied to the man- 0167-9317/$ - see front matter 2004 Elsevier B.V. All rights reserved. doi:10.1016/j.mee.2004.09.007 S.H. Cho et al. / Microelectronic Engineering 77 (2005) 116–124 ufacturing of various flexible and low-cost electronic and display devices [1–20]. There have been extensive research activities on flexible electronics based on polymeric materials [1–21]. Flexible TFT (thin film transistor) [1–11], flexible flat panel displays including organic light emitting diodes (OLED) [12,13] and liquid-crystal displays (LCD) [14], sensors [15–17], microelectromechanical systems (MEMS) [18], photovoltaic devices [19,20] and FPCB (flexible printed circuit board) [21] based on all polymeric materials or partial employment of polymeric materials have been developed due to low-cost and ease of fabrication. It is expected that flexible microelectromechanical (MEMS) and semiconductor devices as well as flexible displays can be fabricated on flexible substrate for many applications in the future. Cu metallization on flexible substrate has been frequently used in FPCB and advanced packaging technology. In this case, a subtractive fabrication method for Cu lines with the scale of several tens of micrometers has usually been used [21]. In this method, wet etching of Cu from the Cu foil or thin films on flexile substrate delineates Cu line patterns. For the fabrication of Cu lines with the width of several micrometers and a high aspect-ratio, however, an additive fabrication or build-up method that utilizes electroplating of Cu on patterned photoresist mask is expected to be required for the precise dimensional control of fine patterns [22]. For the fabrication of smaller devices or systems on flexible substrates in the near future, therefore, micro-scale metallization on flexible substrates should be developed. Evaporated Au on organic materials using a shadow mask has usually used as electrodes in organic TFT for ohmic contact formation [1–11] and in bioelectronic devices [23] because of its good biocompatibility and electrochemical stability. In this case, adhesion of Au layers on the polymer substrate is not enough for required flexibility due to the poor bonding of Au to the polymeric materials [24]. Adhesion improvement between Au and polymer substrate is required for the micro-scale Au metallization. Also, fabrication of the high aspect-ratio patterns is difficult in case of using a shadow mask for pattern formation. 117 In this paper, micro-scale Cu and Au metallization processes on flexible polyimide (PI) substrate were investigated. Fabrication in this experiment is based on a LIGA-like process [25] utilizing UV (ultra-violet) lithography and electroplating of Cu and Au lines. For electroplating of Cu and Au, Cr adhesion and Cu seed layers were deposited in sequence after O2 inductively coupled plasma treatment of the PI substrate for the improvement in the adhesion strength of the Cr adhesion layer to the polyimide substrate. Electroplating of Cu and Au on patterned SU-8 mask was carried out on patterned SU-8 mask for the formation of Cu and Au lines with the scale of a few micrometers. Also, gap-filling process of the patterned Cu lines was performed by spin coating of a polyimide solution. The results obtained in this experiment can be applied to the fabrication of flexible microelectronic devices. 2. Experiment Surface of polyimide film was treated by O2 inductively coupled plasma (ICP) before the sputter deposition of Cr/Cu layers for the improvement of adhesion of Cr layer to the PI substrate. Hightemperature PMDA-ODA polyimide (PI) films (Du Pont; Kapton) with the thickness of 125 lm and squared shape of 2 cm · 2 cm were used as substrate and processed without the carrier. For plasma surface treatment of the polyimide films, a modified commercial 8-in. inductively coupled plasma (ICP) etcher having a 3.5-turn spiral copper coil on the top of chamber separated by a 1-cm thick quartz window and a turbo pump backed by a rotary pump was used in this experiment. A top RF power of 13.56 MHz was applied to the top electrode coil to induce ICP. Bottom electrode power of 13.56 MHz was applied to the substrate holder to induce self-bias voltage (Vdc) to the sample and in turn ion-bombardment. Surface treatments were carried out at the O2 flow of 300 sccm and the fixed top RF power of 40 W and bottom powers of 0, 60 and 125 W with the DC self-bias voltage of 0, 130 and 280 V for 35 s. The surface roughness and contact angle of the PI film surface treated by O2 ICP were 118 S.H. Cho et al. / Microelectronic Engineering 77 (2005) 116–124 measured by atomic force microscopy (AFM) and contact angle measurement for the surface property measurement. Next, 50-nm thick Cr adhesion and 100-nm thick Cu seed layers were deposited in sequence by in situ sputter deposition at the Ar flow of 20 sccm, the chamber pressure of 2 mTorr, and the RF (13.56 MHz) power of 100 W (0.3 W/ cm2). Resistivity of electroplated copper film with no pattern was calculated from the sheet resistance values obtained from a 4-point probe measurement. The thickness of electroplated Cu and Au was measured by an a-step profile meter. A contact anglemeter (SEO 300X by Surface & Electro-Optics Corporation) was used for contact angle measurements. Deionized (DI) water was used as a liquid probe for contact angle measurements. After water was dropped onto the surface of the plasma-treated PI films, the contact angle of water on the substrates was immediately measured by means of the advanced angle method. All experiments were carried out at 25 ± 0.1 C. For the evaluation of adhesion strengths of the Cr layer on the plasma-treated PI surfaces, Cu electroplating with the thickness of 20 lm was performed on the 150-nm thick Cu/Cr seed/adhesion layers deposited on the strip of PI with the width of 0.5 cm and the length of 3 cm. Adhesion strength of the Cr/Cu films on the flexible substrates (Cu/Cr/PI systems) was measured using Micro-tester system by LLOYD Instruments (AMETEK) and the method to deduce peel strength values from the T-peel tests [26] was used following the procedure described in the previous literature [27]. For the formation of mask used in the electroplating of Cu and Au, a negative photoresist, SU-8 2010 [28], with the thickness of about 10– 12 lm was coated on the surface of the Cu/Cr/PI substrate by a spin coater. The coated substrate was placed for about 1 h on the flat board in the clean room for the exclusion of bubbles. Electroplating of Cu line was carried out in the sulfuric acid bath with the electric current density of the 12 mA/cm2 and at the bath temperature of 25 C. Electroplating of the Au lines was carried out in the noncyanide solution [29] with the electric current density of 5 mA/cm2 and at the temperature of 60 C. Removal of SU-8 was carried out in acetone and then by chemical dry etching using a remote microwave plasma source with CF4/O2/Ar process gases [30]. The layers of Cr and Cu were selectively etched using a wet etching solution. PI 2560 gap-filler supplied by HD MicroSystems was spin-coated for the gap-filling of Cu lines with the line and spacing of @4–12 lm. After spin coating of the gap-filler, the samples were slowly cured at 250 C on the hot plate and the polyimide layer with the thickness of @20 lm was formed. Fabricated Cu and Au patterns were observed using a scanning electron microscope (SEM) operating at the acceleration voltage of 7.5 kV. 3. Results and discussion Fig. 1 shows 4.0 · 4.0 lm2 AFM image of the surface of O2 plasma-treated PI films as a function of the bottom power. The root-mean-squared (RMS) roughness of the untreated PI film was 0.9 nm. However, the RMS roughness values of the plasma-treated PI films at the bottom power of 0, 60, and 125 W were increased to 3.6, 11.1, and 23.9 nm, respectively. In this experiment, the bottom power in the ICP system controls the bombardment energy of oxygen ions in the plasma and as a result reactive etching of the polyimide surface leads to the increased morphological surface roughening. As seen in Fig. 1, increased bias power roughens the surface more due to a faster etch rate under increased bombarding energy of oxygen ions. The reason for using the range of low substrate bias power density is that excessive treatments under high-energy ion-bombardment can cause more chain scission leading to a weak boundary layer that is detrimental to metal/polymer adhesion. Fig. 2 shows the contact angle values of the plasma-treated PI films obtained together with the RMS roughness values obtained from the AFM images in Fig. 1. While the contact angle of untreated PI films was 73.8, contact angles of the O2 plasma-treated PI films by the bottom power of 0, 60, and 125 W were reduced to 0. The complete wetting of DI water is caused by a very large increase in surface roughness induced S.H. Cho et al. / Microelectronic Engineering 77 (2005) 116–124 119 Fig. 1. A 4.0 · 4.0-lm2 AFM image of the surface by O2 plasma-treated PI films as a function of the bottom power. (a) untreated (b) top: 40 W (c) top: 40 W, bottom: 60 W (d) top: 40 W, bottom: 125 W [RMS roughness: (a) 0.861 nm; (b) 3.567 nm; (c) 11.06 nm; (d) 23.92 nm]. by an oxygen ion bombardment together with modified chemical bonding states. The combined results indicate that the obtained RMS roughness is inversely proportional to the contact angle, as observed in Fig. 2. The decrease of the contact angle is attributed possibly to the increase in the total No treatment 70 25 60 20 50 40 15 30 10 20 10 5 0 0 120 RMS roughness(nm) Contact angle(deg.) 130 -10 No treatment Top: 40 W Top: 40 W bottom: 60 W Top: 40 W bottom: 125 W Fig. 2. Contact angle and RMS roughness values as a function of the bottom power. Peel strength (gf/mm) O2: 300 sccm Time: 35 sec 80 surface energy of PI films due to the increase in surface area induced by roughening as well as due to the creation of new binding states by O2 plasma treatment [31,32]. The adhesion strength measurement was performed using T-peel test. Fig. 3 shows a relation Top: 40 W 110 Top: 40 w, bottom: 60 W 100 Top: 40 W, bottom: 125 W 90 80 70 60 50 40 0 5 10 15 20 25 RMS roughness (nm) Fig. 3. Peel strength measured as a function of RMS roughness. S.H. Cho et al. / Microelectronic Engineering 77 (2005) 116–124 between RMS roughness and peel strength. The values of peel strength were averaged at least over five samples for the sample plasma treatment conditions. The error bars in Fig. 3 indicate the range of the measured values for the same plasma-treatment condition. If surface roughening is a major contributor to the improvement of adhesion, O2 plasma-treated PI films at the bottom power of 125 W will produce the largest improvement in peel strength. As we were expecting, O2 plasmatreated PI film at the bottom power of 125 W was found to have the highest peel strength, 126 gf/nm. Based on this observation, it is concluded that increase in surface roughness plays a big role in the enhancement of adhesion at the range of large surface roughness. The effect of roughened surface on the adhesion strength of metals on the PI surface has been already investigated although correlated quantitative measurements of roughness, contact angle, and peel strength have not been given in detail [33–36]. Important observation from those previous works is that a grass-like surface textures with a large surface area, as observed in Fig. 1, possibly provide the bonding sites out of the horizontal because the PI chains oriented intrinsically parallel to the substrate surface are disturbed [35,36]. Interestingly, surface roughness effect was not effective in the range of small surface roughness even though the roughness values were not quantified [34]. The results in this study also confirm the effec- tiveness of surface roughening on the significant adhesion improvement at the surface roughness value as large as @24 nm. Fig. 4 shows the resistivity of electroplated Cu with the thickness of 0.8–3.7 lm in our experimental conditions as a function of the Cu thickness. For the purpose of resistivity measurement, the Cu/Cr/PI substrate without patterning was used. Electrical resistivity was determined from the measured sheet resistance and the film thickness values of the electroplated copper film. For the very thin layers with the thickness less than 1.5 lm, the effect of the layer thickness on measured sheet resistance was corrected. The effect of 50nm thick Cr layer on measured sheet resistance value was neglected due to the small thickness and higher resistivity. The sheet resistance was usually measured at three different points and the averaged value was used to estimate the resistivity. The thickness of the electroplated copper film was increased linearly with increasing the electroplating time. With the increase of the electroplated Cu thickness, resistivity was decreased. But at the thickness larger than 1.5 lm, resistivity became saturated at @1.8 · 10 6 X Æ cm that is close to the resistivity of bulk copper @1.7 · 10 6 X Æ cm. Other measurements showed that resistivity values of Cu by chemical vapor deposition and sputtering are @2 · 10 6 X/cm [37] and @ 3 · 10 6 X Æ cm [38], respectively. Other reported resistivity values obtained by electroplating are in the range of 4.0 40 Resistivity Thickness 3.5 -7 Resistivity(10 Ω . cm) 30 3.0 2.5 20 2.0 10 1.5 Thickness (µm) 120 1.0 0 0.5 5 10 15 20 Electroplating time (min) Fig. 4. Resistivity of unpatterned electroplated Cu films as a function of electroplating time. S.H. Cho et al. / Microelectronic Engineering 77 (2005) 116–124 Fig. 5. SEM image of patterned SU-8 mask. 1.8–1.9 · 10 6 X Æ cm [39], similarly to the value obtained in this experiment. Mask pattern with the scale of a few micrometers for Cu and Au electroplating was fabricated using SU-8 negative-tone photoresist. SU-8 is known to be stable in electroplating solutions. Fig. 5 shows SEM micrograph of a patterned SU-8 electroplating mask on the silicon substrate 121 with the various trench widths, 4–12 lm, optimized by varying the process parameters such as spinning time, spinning speed, soft bake time, exposure time, and development time [28]. Here, Si substrate was used for the process optimization and easy observation of fabricated patterns. The same SU-8 patterning condition described above was applied to the fabrication of SU-8 mask on the plasma-treated PI substrates. Cu metallization lines on the patterned SU-8 mask with the thickness of approximately 12 lm were electroplated by varying the electroplating time in the copper sulfuric acid bath. Platinum (Pt) mesh was used as an anode during electroplating. Au electrodes on the patterned SU-8 mask were electroplated in the non-cyanide bath. Also, the Pt mesh was used as the anode electrode for Au electroplating. After electroplating, SU-8 was successfully removed by a combined method of wet and dry processes. For the complete dissolution of the SU-8, a considerable number of solvents and conditions have been tried [30]. Acetone is very effective in cracking and crazing the cross-linked Fig. 6. (a) SEM image after removal of the SU-8 photoresist, (b) quantitative chemical analysis results by EDS, (c) SEM image of the Cu metallization lines after removal of the Cu/Cr layers, and (d) quantitative chemical analysis results by EDS after removal of seed and adhesion layers. 122 S.H. Cho et al. / Microelectronic Engineering 77 (2005) 116–124 SU-8 [30]. In this work, wet removal using acetone was used first and then ashing of SU-8 using CF4/ O2/Ar microwave remote plasma was followed. The SU-8 mask in the acetone was heated at 200 C on the hot plate for 10 min. SU-8 ashing in a chemical dry etcher utilizes reactive oxygen radicals generated by a remote microwave plasma source transported into the chamber and highly energetic ions that can damage metallization lines are minimized in the remote plasma. Fig. 6(a) shows the SEM micrograph of electroplated Cu lines after removal of SU-8. The chemical analysis data in Fig. 6(b) obtained from the Cr/Cu layers by energy dispersive spectroscopy (EDS) indicate that carbon and nitrogen that are main components of the SU-8 photoresist were not found. This result indicates a successful removal of the SU-8 photoresist. The oxygen on the surface of Cu seed layer, as seen in Fig. 6(b), is possibly due to the oxidation of Cu during the remote CF4/O2/Ar plasma ashing of SU-8 photoresist. Following removal of SU-8 photoresist, a selective wet etching of the Cr adhesion and Cu seed layers was carried out. During the etching of the Cu seed layer, minimal etching of Cu lines cannot be avoided. Cu seed layer was etched by nitric acid (50%) mixed with water. The Cr adhesion layer was dip-etched at 60 C with a solution containing 60 g/l of potassium permanganate and 200 g/l of tri-basic sodium phosphate [8]. During Cr etching, it was found that etching of Cu was negligible from the SEM observation of Cu before and after Cr etching. Fig. 6(c) shows Cu metallization lines on the flexible PI substrate after the removal of the Cu seed and the Cr adhesion layers. After the removal of the Cu/Cr layers, roughness of Cu lines was increased. Traces of Cu and Cr were minimal, judged form the EDS analysis data as shown in Fig. 6(d). Observed manganese trace on the etched surface is due to the use of potassium permanganate during Cr wet etching process and oxygen is from the PMDA-ODA polyimide (PI) film (Du Pont; Kapton) in which 17.2 at.% of oxygen exists [40]. This result indicates the Cu seed and Cr adhesion layers were successfully etched on the flexible substrate with the minimal attack on the Cu lines. For electroplating of Au lines, the same procedure of Cu/Cr layer deposition and SU-8 mask patterning was performed. Fig. 7(a) shows the SEM micrographs of the Au lines electroplated in a noncyanide solution with the current density of 5 mA/cm2 at the solution temperature of 60 C. The EDS analysis data in Fig. 7(b) obtained from the substrate surface after removal of the Cu/Cr (seed/adhesion) layers shows no residual Cu and Cr on the PI substrate. This indicates the complete removal of the Cu/Cr layers. Gap-filling process for filling of the trenches between Cu lines was followed after formation of Cu metallization lines. For this process, PI 2560 supplied by HD MicroSystems was used. For the Fig. 7. (a) SEM image of the Au electrode lines after removal of Cu/Cr layers and (b) quantitative chemical analysis results by EDS on the polyimide surface after removal seed and adhesion layers. S.H. Cho et al. / Microelectronic Engineering 77 (2005) 116–124 removal of solvents and hardening of PI, curing of coated layers was performed at the relatively low curing temperature of 250 C since out-gassing from the PI during curing at elevated temperature, for example, at 400 C can occur. For the optimization of gap-filling process by the polyimide gapfiller, spinning speed of spin coater was found to be the most critical parameter. For gap-filling of the trench with the width of @4 lm and the aspect ratio of @3, a two-step process during spin coating was required. In our experimental conditions, spinning with the speed of 500 rpm at the first step and then with the speed of 2000–4000 rpm at the second step was used to control the final thickness of the PI. As seen in Fig. 8(a), at the condition of a single-step process with the spinning speed of 2000–4000 rpm, trenches with the width of @4 lm and the aspect ratio of @1.5 were not filled 123 completely. As seen in Fig. 8(b), an optimized gap-filling of the Cu lines with the trench width of @4 lm and aspect ratio of @3 was successfully obtained using a two-step spin coating. As shown in Fig. 8(b), a globally planarized polyimide surface was obtained. For the device applications, a multilevel metallization scheme can be possibly applied using a combination of polyimide patterning and electroless plating of Cu vias. 4. Conclusion Micro-scale Cu and Au metal lines on the flexible polyimide substrate were successfully fabricated by electroplating of Cu and Au using a negative SU-8 photoresist mask. Cr adhesion and Cu seed layers were deposited on O2 inductively coupled plasma-treated polyimide substrate. The results of the adhesion strength measurements showed that the O2 plasma-treated PI film at the bottom electrode power of 125 W has the highest adhesion strength of 126 gf/nm. Photolithography process of the SU-8 mask with the thickness of 8– 12 lm for Cu and Au electroplating was successfully developed. Electroplating of Cu and Au, removal of SU-8 photo-resist and selective removal process of the Cr/Cu adhesion/seed layers were developed for the fabrication of micro-scale Cu and Au lines with the width as small as 4 lm. Gap-filling process of Cu metallization for filling the trenches with the width of @4 lm and the aspect-ratio of @3 was also successfully applied. Au electrodes with various pattern sizes applicable to organic TFT and sensors were successfully fabricated using a non-cyanide electroplating. Cu metallization process with the scale of a few micrometers on the flexible polyimide substrate can be used for the flexible electronic device fabrication as well as advanced flexible printed circuit board technology. Acknowledgements Fig. 8. (a) SEM image after gap-filling process using a singlestep and (b) SEM image after gap-filling using a two-step process. This work was supported through the Center of Excellency program by the Korea Science and 124 S.H. Cho et al. / Microelectronic Engineering 77 (2005) 116–124 Engineering Foundation and Ministry and Science and Technology (Grant No. R-11-2000-086-00000) and SAIT (Samsung Advanced Institute of Technology). References [1] B. Crone, A. Dodabalapur, Y.-Y. Lin, R.W. Filas, Z. Bao, A. LaDuca, R. Sarpeshkar, H.E. Katz, W. Li, Nature 403 (2000) 521. [2] C.J. Drury, C.M.J. Mutsaers, C.M. Hart, M. Matters, D.M. de Leeuw, Appl. Phys. Lett. 73 (1998) 108. [3] W. Fix, A. Ullmann, J. Ficker, W. Clemens, Appl. Phys. Lett. 81 (2002) 1735. 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