Albert S. Leea,
Sung Yeoun Oha,
Seung-Sock Choia,
He Seung Leea,
Seung Sang Hwangab and
Kyung-Youl Baek*ab
aMaterials Architecturing Research Center, Korea Institute of Science and Technology, Hwarangno 14-gil 5, Seong-Buk Gu, Seoul 136-791, Republic of Korea. E-mail: baek@kist.re.kr
bNanomaterials Science and Engineering, University of Science and Technology, 217 Gajungro, 176 Gajung-dong, Yuseong-Gu, Daejeon 305-333, Republic of Korea
First published on 29th July 2015
A series of organic–inorganic hybrid spin-on-glass polymethylsilsesquioxanes were synthesized utilizing a cyclic siloxane precursor, 1,3,5,7-tetramethyl-1,3,5,7-tetrahydroxyl cyclosiloxane (MT4-OH), copolymerized with methyltriethoxysilane (MTES) at various comonomer ratios. By selectively introducing this 2-D cyclic crosslinker, we were able to obtain spin-on-glass hybrimers with low dielectric constant (2.5–2.7), high nanoindentation modulus (5–10.5 GPa), with high thermal stability (>700 °C) without the use of porogens or additives. The use of the cyclic monomer MT4-OH greatly increased the mechanical properties, which allowed for impeccable reliability of a variety of patterns obtained through etching and chemical mechanical planarization processes, while maintaining optimal gap-filling properties. Due to the superior dielectric, mechanical, and integrated processing of these materials, these hybrids derived from MT4-OH may be utilized as next generation spin-on-glass low-dielectric constant materials.
Low-dielectric constant materials must possess a vast myriad of electrical, thermal, chemical, and mechanical properties, which are just as crucial as the low dielectric permittivity property that classifies them.5 In order for low-dielectric constant materials to be successfully integrated into integrated circuits, the material must be able to withstand 10–15 repeated temperature treatments exceeding 400 °C, have low coefficients of thermal expansion (CTE), excellent adhesion to metal interconnects such as copper, chemical resistant to the solvents and etchants commonly used during chip fabrication, as well as superior mechanical properties to withstand the etching processes known as chemical mechanical polishing (CMP).6 As such, organic polymers such as polynorbornenes, polyimides, and poly(aryl ethers), while possessing low-dielectric properties,7 but lacking in one or more of the other prerequisites for actual applications into integrated circuits, have been more or less passed over nowadays.
Polysilsesquioxanes (PSSQs) are a class of inorganic–organic hybrid materials with a single organic functional group covalently linked to a trifunctional silane.8 PSSQs are synthesized via sol–gel processing consisting of hydrolysis of either alkoxy- or chloro-ligands, followed by polycondensation of the silanol groups to form Si–O–Si bridges.8,9 In addition to the superior thermal and mechanical properties imbued by the inorganic Si–O–Si backbones, the organic groups allow for a myriad of applications which require organic functionalities. Moreover, as polysilsesquioxanes are soluble in organic solvents, spin-on-glass PSSQs have been sought out as one of the materials of choice to supplant expensive and time-consuming deposition processes of hybrid films.10
With regards to low-dielectric constant materials, polymethylsilsesquioxanes (PMSSQs) has been the material most extensively researched, due to the low polarizability of the Si–C methyl group, giving rise to its low dielectric constant (∼2.7), while exhibiting superior thermal stabilities (>500 °C).11,12 Numerous studies have detailed the various structure–property relationships of PMSSQs and the different synthetic variables which govern its molecular weight, thermal stability, structure, and their effect on their electrical properties.13 And while numerous studies have investigated the effect of sacrificial porogens to further decrease the dielectric constant,14 issues arising from metal infiltration into pores,15 as well as decrease in mechanical properties were problems left to address in such cases.
More recently, various chemical modifications to the Si–O based hybrids have been reported as new methodologies for new interlayer low-dielectric constant materials. Several groups have reported on the low-dielectric properties of benzoxazine-functionalized polysilsesquioxanes,16,17 cyanate ester composites,18 as well as the functionalization of benzocyclobutene19 to the Si–O–Si backbone to utilize the high free-volume of the crosslinked organic components to substantially lower the dielectric constants. However, despite the improvements in thermal, mechanical, and electrical properties, none of these studies have shown that integration was possible with these new materials.
In this study, we investigated the effect of incorporating Si–C methyl groups via a cyclic siloxane precursor, tetrahydroxyl tetramethyl cyclosiloxane (MT4-OH), copolymerized with methyltriethoxysilane (MTES) at various comonomer ratios. By chemically incorporating this 2D cyclic monomer into the poly(methyl)silsesquioxane matrix, we sought to increase the internal free volume to further decrease the dielectric constant, while examining the thermal, mechanical, electrical, and most importantly, integration reliability of these robust hybrid materials as low-dielectric constant spin-on-glass resins without the use of additives or porogens which may depreciate mechanical properties.
The synthesis of MT4-MSSQs was straightforward, as we utilized a modified literature procedure for which MTES-based sol–gel conditions were well-known.13 Moreover, this acid-catalyzed sol–gel reaction allowed for fast and complete hydrolysis of the ethoxy groups of MTES. The MT4-MSSQs were named according to the monomer mol ratio of MTES:
MT4-OH followed the MT4-MSSQ code as such: for MTES
:
MT4-OH mol ratio of 3
:
7, the MT4-MSSQs were named MT4-MSSQ37. In this study, we studied the various spin-on-glass PMSSQs with MTES
:
MT4-OH mol ratio of 0.5
:
9.5, 1
:
9, 2
:
8, 3
:
7, and 5
:
5. Increasing the MT4-OH ratio over 50% resulted in a precipitous loss in solubility and were excluded for further study.
The obtained MT4-MSSQ spin-on-glass resins were first characterized by 1H NMR and FTIR. As shown in Fig. 1a, the ethoxy groups of MTES for the obtained MT4-MSSQs were completely hydrolysed as indicated by the lack of ethoxy groups at around 3.8 ppm. This complete hydrolysis of alkoxy groups has been reported as a critical point for spin-on-glass low dielectric constant materials, as unhydrolyzed alkoxy groups around contribute to substantial film shrinkage, compared to their hydrolyzed Si–OH silanol groups when thermally cured under high temperatures.13,22 While small amounts of silanol groups were found at 7.3 ppm, the relative amounts were difficult to quantify due to the weak and broad signals. In addition, the FTIR spectrum for the various MT4-MSSQs (Fig. 1b) revealed that all the PMSSQ resins were of high molecular weight and random-branched structure, as indicated by the sharp and doubly split Si–O–Si peaks ranging from 1000–1200 cm−1 characterized as a and b.8,13 Moreover, the peaks centered at 960 cm−1 and 3500 cm−1 were assigned to the uncondensed Si–OH silanol groups, c. Interestingly, the relative amounts of uncondensed Si–OH silanol groups slightly increased as MTES content increased, which was surprising considering the amorphous networking of the Si–O–Si bonds during the hydrolysis–polycondensation reaction leading to similar degrees of condensation under acidic conditions.13 However, as shown, as MTES content increased, uncondensed silanol content increased slightly, indicating that the MT4-OH monomer functioned to increase the degree of condensation due the tetrasiloxane core only required polycondensation reaction between silanols to obtain highly condensed rigid Si–O–Si networks.
In order to elucidate the optimal curing temperature for the MT4-MSSQ resins, thermal curing was carried out 100 °C, 200 °C, and 400 °C for 2 h for the MT4-MSSQ37 spin-on-glass resin. As shown, the silanol peaks c, completely disappeared after thermal curing, indicating that the thermal curing process was complete, even at 100 °C. However, for conventional low-dielectric constant materials, incomplete thermal curing is a critical issue, as uncondensed silanol groups contribute to both diffusion of metal, compromising the metal–dielectric interface, and in some cases failing to insulate the metal inconnects.5 As such, high temperature curing at 200 °C and 400 °C were investigated. As expected, uncured silanol groups were not detected, but interestingly, the relative intensity of the Si–O–Si bonding peaks around 1000–1200 cm−1 changed. This was attributed to the change in Si–O–Si networking after thermal curing providing a highly crosslinked internal Si–O–Si network when cured at 400 °C.
Additionally, the SEC derived weight averaged molecular weights (Mw) for all of the MT4-MSSQ spin-on-glass resins were tabulated in Table 1. As shown, the Mw values for all MT4-MSSQ resins were in the range of 10–14k, with Mw increasing as MT4-OH mol ratio increased. The increase in Mw was attributed to the innate characteristic of the four silanol groups of MT4-OH, acting as branching points for intramolecular and intermolecular condensations between MT4-OH and MTES. Also, the polydispersity indices (PDI) for all of the MT4-OH resins were between 2.2 and 2.5, indicating the stabilization of network structure as obtained sols.
Sample name | Mn | Mw | PDI |
---|---|---|---|
MT4-MSSQ595 | 4700 | 10![]() |
2.2 |
MT4-MSSQ19 | 4600 | 10![]() |
2.3 |
MT4-MSSQ28 | 4500 | 11![]() |
2.5 |
MT4-MSSQ37 | 5000 | 12![]() |
2.4 |
MT4-MSSQ55 | 5900 | 13![]() |
2.3 |
The degree of condensation (DoC) of the Si–O–Si bonds was investigated by 29Si NMR. As shown in Fig. 3, two characteristic peaks were observed and characterized to the T3 alkyl-Si(OSi–)3 and T2 alkyl-Si(OSi–)2OH peaks centered at −68 ppm and −58 ppm, respectively.20,23 The degree of condensation as described by Bae,24,25 is the degree in which all of the Si–O silicons are condensed, respective to the uncondensed silicons. Thus, for purely T resins, the degree of condensation (DoC) can be simply expressed by the integrated ratio of T3 to T2 characteristic peaks. In the MT4-MSSQ spin-on-glass resins obtained in this study, all of the degree of condensation values were about 75–92%, indicating that the Si–O–Si frameworks were mostly condensed. This is an important feature, as excess uncondensed Si–OH groups contribute to shrinkage of the coating layer induced by the thermal treatments required for curing,13,22 which invariably leads to both a decrease in mechanical properties and interface reliability. As the MT4-OH contents increased, a slight increase in degree of condensation was observed, most likely due to the MTES monomers acting as branching points and probably source of uncondensed silanol groups.
![]() | ||
Fig. 3 29Si NMR spectra for MT4-MSSQ spin-on-glass resins with calculated degrees of condensation (DoC) values. |
Next, the dielectric properties for the MT4-MSSQ spin-on-glass resins were examined. In Fig. 5, the dielectric constant and breakdown strength values for various MT4-MSSQ spin-on-glass resins after curing were shown. The breakdown voltage values for all of the MT4-MSSQ spin-on-glass resins all exceeded 2.0 MV cm−1 and remained relatively the same regardless of comonomer composition. However, the dielectric constant values increased from 2.2 to 2.75 with increase in MT4-OH contents. While this was contrary to what we hypothesized, the increase in dielectric constant was attributed to the relatively denser internal Si–O–Si structure formed through the polycondensations between MT4-OH monomers within the MT4-MSSQ network. Moreover, the MTES monomer most likely acted as branching and or curing point as uncondensed silanol groups were primarily derived from MTES, as indicated by the lower degree of condensations for MT4-MSSQ resins containing higher MTES content. We were also able to discern that once the MT4-OH contents increased over 30%, the dielectric constant values reached a plateau around 2.75, which is more or less the theoretical value for poly(methyl)silsesquioxanes (PMSSQs),1 and also very close to the dielectric constant of the MT4-OH monomer itself (k = 3.0). Moreover, when the dielectric constant values were compared to the non-cured, as-cast thin films shown in ESI, Fig S1,† the dielectric constants were approximately 0.2 lower, indicative of the full curing of silanol groups, also supported by FTIR results in Fig. 2.
![]() | ||
Fig. 5 Dielectric constant and breakdown voltage values for MT4-MSSQ spin-on-glass resins after curing. |
Mechanical properties of the MT4-MSSQ spin-on-glass resins were evaluated using nanoindentation method.26,27 As shown in Fig. 6 and detailed in Table 2, the elastic moduli and hardness values increased as MT4-OH contents increased, with MT4-MSSQ55 giving an elastic modulus of 10.5 GPa and hardness of 1.5 GPa. In contrast to the non-cured, as-cast MT4-MSSQ resins, the elastic modulus values were approximately 2–3 GPa greater, and the hardness values 0.5–1 GPa greater as shown in ESI, Fig S2.† This was in line with our previous discussion of the MT4-OH providing internally dense and mechanically robust inorganic backbones. This point was further supplanted by observation of the brittleness index,27 commonly defined by the hardness divided by the elastic modulus. As tabulated in Table 2, the brittleness index for MT4-MSSQ resins after thermal curing decreased with increasing MT4-OH contents, suggesting that the MTES monomers giving rise to uncondensed silanols, as indicated by the relatively lower degree of condensations in Fig. 2 and 3, provided a greater degree of crosslinking between sol–gel matrices.
Sample name | Elastic modulus, E (GPa) | Hardness, H (GPa) | Brittleness index (H/E) | Plasticity index (E/H) |
---|---|---|---|---|
MT4-MSSQ595 | 4.8 | 0.75 | 0.156 | 6.40 |
MT4-MSSQ19 | 5.0 | 0.77 | 0.154 | 6.49 |
MT4-MSSQ28 | 6.1 | 0.89 | 0.146 | 6.85 |
MT4-MSSQ37 | 9.0 | 1.29 | 0.144 | 6.98 |
MT4-MSSQ55 | 10.5 | 1.5 | 0.143 | 7.00 |
In addition to testing the reliability of the MT4-MSSQ37 resins against CMP processes, metal–insulator and metal–insulator–metal (MIM) structures were fabricated as shown in Fig. 8. As shown, the MT4-MSSQ37 resin possesses excellent adhesion to aluminum and the patterned Si wafer, as shown in Fig. 8a, without noticeable delamination, cracks, pinholes, or defects. In addition, Fig. 8b revealed the MIM structure with MT4-MSSQ37 sandwiched between aluminum and tin electrodes. As shown, the interface between both aluminum and tin electrodes were impeccable, with the diffusion barrier thickness around 100 nm and MT4-MSSQ37 resins both having unblemished surface interfaces, due to the excellent processability of MT4-MSSQ37, as well as the thermal and mechanical stability to withstand the metal deposition processes.
Finally, the gap-filling properties of MT4-MSSQ37 coated on patterned Si wafers was investigated. In Fig. 9, the SEM images of MT4-MSSQ37 coated surfaces with various aspect ratios showed that the MT4-MSSQ37 fully filled the etched trenches of the patterned Si wafers while providing a smooth coated interface on top of the Si wafer, again showing the utility of the excellent processability and coating properties of MT4-MSSQ37 spin-on-glass resins.
![]() | ||
Fig. 9 SEM image of MT4-MSSQ coated on pattered Si wafers with (a) aspect ratio of 3![]() ![]() ![]() ![]() |
Footnote |
† Electronic supplementary information (ESI) available: Dielectric constant values and mechanical properties of as-cast MT4-OH resins. See DOI: 10.1039/c5ra11110b |
This journal is © The Royal Society of Chemistry 2015 |