Weifeng
Peng
a,
Huanyu
Lei
a,
Luhao
Qiu
a,
Feng
Bao
a and
Mingjun
Huang
*ab
aSouth China Advanced Institute for Soft Matter Science and Technology, School of Emergent Soft Matter, South China University of Technology, Guangzhou 510640, China. E-mail: huangmj25@scut.edu.cn
bGuangdong Provincial Key Laboratory of Functional and Intelligent Hybrid Materials and Devices, South China University of Technology, Guangzhou 510640, China
First published on 21st June 2022
Polymers with low dielectric permittivity and dielectric loss are essential for the microelectrics and wireless communication industries. The perfluorocyclobutyl (PFCB) aryl ether group has been proven to afford polymer materials with a high fluorine content and large free volume, resulting in many attractive properties, e.g., good thermal and chemical stability, high hydrophobicity, transparency and low dielectric permittivity. Herein, a series of PFCB-containing polyimides were designed and synthesized. The conformational isomers of the diamine monomer could be separated, providing an opportunity to explore the effects of the isomer conformations on the polyimide properties. All these PFCB-containing polyimides present relatively loose chain packings due to their strongly distorted chain conformations. The combined loose chain packing and high fluoro content afford these PFCB-containing polyimides excellent optical transparency and dielectric properties. In particular, dielectric permittivity and dielectric loss values as low as 2.50 and 0.0035 at high frequency (10 GHz) were obtained, enabling potential applications in the microelectronics industry.
Dielectric polymers with high thermal stability are strictly required for the production of microprocessor chips, in which metal wire bonding is involved.11 Among the diverse high-performance polymer materials, polyimides are known as a “problem solver” because of their excellent integrative properties including excellent flexibility, thermal stability, solvent resistance and mechanical strength.12–15 Nonetheless, the polar imide group endows the polyimide with a relatively high dielectric constant (around 3.5), which does not meet the requirements of the microelectronics industry.16 From the perspective of molecular structure design, there are two main strategies to lower the dielectric constant in polyimides: one is introducing large pendant groups to decrease the packing density of the polyimide chains;5,17–19 the other is increasing the amount of fluorine atoms on the polyimide backbone to reduce the polarization ability.20–22 These two strategies could also be combined to further decrease the dielectric constant.21
The perfluorocyclobutyl aryl ether (PFCB) group has been proven to afford polymer materials with high fluorine content and large free volume, resulting in many attractive properties, e.g., good thermal and chemical stability, high hydrophobicity, transparency and low dielectric permittivity.23–26 PFCB-containing polymers have demonstrated good performance in photoelectric materials, non-wetting electro-spun surfaces, light-emitting and hole-transporting materials, proton exchange membranes, dielectric materials in ICs and FPCBs, etc.23 The integration of the PFCB group into polyimides was reported by Huang et al.27,28 The PFCB-containing yellow polyimides showed improved dielectric properties and low water absorption.
In this work, a series of transparent polyimides with high PFCB content are designed and synthesized (Scheme 1a). The PFCB-containing dianhydride and diamine monomers 5,5′-((perfluorocyclobutane-1,2-diyl)bis(oxy))bis(isobenzofuran-1,3-dione) (PFODPA) and 4,4′-((perfluorocyclobutane-1,2-diyl)bis(oxy))dianiline (PFODA) were synthesized successfully. It is worth noting that the isomers of PFODA could be separated based on the minor difference in their polarities (Fig. S1†), providing an opportunity to explore the effects of the isomer conformation on the polyimide properties. 4,4′-(Hexafluoroisopropylidene)diphthalic anhydride (6FDA) and bis(trifluoromethyl)-4,4′-diaminobiphenyl (TFMB) were chosen for polymerization with PFODA and PFODPA with the aim of lowering the dielectric constant and dielectric loss. The introduction of the PFCB group with its distorted conformation and high fluorine content endows the polyimides with various advantages, e.g., excellent processability, hydrophobicity, high optical transparency and attractive dielectric properties. All these PFCB-containing polyimides present a low dielectric constant (<2.5) and dielectric loss (<0.01). In particular, the 6FDA-co-PFODPA-PFODA copolymerized film possesses an ultra-low dielectric constant value of 2.36 and dielectric loss of 1.3 × 10−3 at 1 kHz, and a dielectric constant of 2.5 and dielectric loss of 3.5 × 10−3 at 10 GHz. These PFCB-containing polyimide films may have potential applications in the electronics industry, e.g., as the dielectric layer in ULSI and the substrate film in FPCB at high frequency.
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1. Density functional theory (DFT) calculations were utilized to analyze the differences between the conformations, and revealed that the cis and trans conformations of both the PFODPA and PFODA monomers have almost the same minimized-energy state (Table S1†). Although numerous PFCB-containing polymers have been reported, the influence of PFCB conformational isomers on material properties has rarely been studied. Luckily, the two isomers of PFODA present a minor polarity difference (ΔRf = 0.05) in silica chromatography (Fig. S1†). The optimized geometries of the PFODA isomers are shown in Scheme 1a. PFODA-trans possesses lower polarity and elutes first from the silica column. This polarity difference was also observed in the DFT calculations, with PFODA-cis showing a higher dipole moment (3.11 Debye) than PFODA-trans (1.24 Debye). These two isomers were separated and confirmed by 1H, 13C, and 19F nuclear magnetic resonance (NMR) (Fig. S2–S5†) and mass spectroscopy (Fig. S6†). On the contrary, the conformational isomers of PFODPA and its precursor show no observable polarity differences and are thus unable to be separated.
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1 molar ratio) was copolymerized with PFODA. The molecular weight of 6FDA-co-PFODPA-PFODA polyimide was higher than that of pure PFODPA-PFODA, but still much lower than that of 6FDA-PFODA. The structures of polyimides were characterized using the FT-IR and NMR spectra shown in Fig. S7 and S8.† Typical characteristic peaks of polyimides can easily be found in the FT-IR spectra; the peaks at 1785 cm−1 and 1726 cm−1 correspond to the symmetric and asymmetric –C
O stretching vibrations, those at 1375 cm−1 and 722 cm−1 to the C–N stretching vibration and imide ring deformation,30 and that at 963 cm−1 to the characteristic absorption of perfluorocyclobutyl aryl ether.27,28 Additionally, the characteristic peaks of amide at around 3200 cm−1 and 1500 cm−1 disappeared, indicating the complete imidization of the polyimides. The NMR spectra (Fig. S8†) and elemental analysis (Table S3†) further verified that the fluorine-containing polyimides had been synthesized successfully.
All these PFCB-containing polyimides present broad diffraction peaks in wide-angle X-ray diffraction (WAXD), revealing their amorphous structure caused by the rather asymmetric conformation of the PFCB groups (Fig. S9†). The d-spacings of the main halos, which represent the packing density among the polyimide chains,31,32 decrease sequentially from PFODPA-TFMB (5.94 Å) to 6FDA-PFODA-trans (5.85 Å), 6FDA-PFODA-cis (5.84 Å), PFODPA-PFODA (5.84 Å), and further to 6FDA-PFODA (5.68 Å). The loosest packing of PFODPA-TFMB indicates that it had the most distorted chain conformation resulting from the PFCB-containing dianhydride group. 6FDA-PFODA-trans and 6FDA-PFODA-cis share similar chain packing densities, and the mixture of these isomers could facilitate the loose packing in 6FDA-PFODA.
As shown in Table S4,† the relatively loose chain packing affords these fluorine-containing polyimides excellent solubility. They can dissolve in most polar solvents, e.g., N-methylpyrrolidone (NMP), N,N-dimethylacetamide (DMAc), N,N-dimethylformamide (DMF), dimethyl sulfoxide (DMSO), m-cresol, acetone, tetrahydrofuran (THF), dichloromethane (DCM) and trichloromethane.
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Fig. 1 Thermal properties of polyimides: (a) DSC curves of the polyimides (exo up); (b) TMA curves of the polyimides; (c) tan δ curves obtained from DMA; (d) TGA curves of the polyimides. | ||
| Polyimides |
T
g
(°C) |
T
g
(°C) |
T
g
(°C) |
T
5
(°C) |
T
10
(°C) |
R
w
(%) |
CTEf (ppm K−1) |
σ
max
(MPa) |
E (GPa) | ε (%) |
|---|---|---|---|---|---|---|---|---|---|---|
| a T g measured using DSC at a heating rate of 10 °C min−1. b T g recorded using TMA at a heating rate of 5 °C min−1. c T g measured using DMA at a heating rate of 5 °C min−1 at 1 Hz. d Temperatures of 5 wt% and 10 wt% weight loss. e Residual weight retention at 800 °C under a nitrogen atmosphere. f Thermal expansion coefficient recorded using TMA from 50–150 °C. g Tensile strength. h Young's modulus. i Elongation at break. | ||||||||||
| 6FDA-PFODA-trans | 251.5 | 237.4 | 238.2 | 501.1 | 518.4 | 40.1 | 63.9 | 87.4 | 2.5 | 5.9 |
| 6FDA-PFODA-cis | 248.9 | 238.1 | 243.7 | 504.1 | 519.4 | 45.4 | 63.5 | 96.2 | 3.1 | 5.8 |
| 6FDA-PFODA | 250.1 | 247.6 | 261.2 | 503.9 | 518.0 | 45.3 | 58.7 | 88.3 | 2.7 | 5.1 |
| PFODPA-TFMB | 223.3 | 217.3 | 234.5 | 503.4 | 519.6 | 41.2 | 64.1 | 83.6 | 2.2 | 6.9 |
| 6FDA-co-PFODPA-PFODA | 208.4 | 220.4 | 233.9 | 502.2 | 515.2 | 43.7 | 70.1 | 73.2 | 2.5 | 4.5 |
| PFODPA-PFODA | 174.4 | — | — | 494.9 | 508.6 | 41.1 | — | — | — | — |
The C–F bond is one of the strongest chemical bonds (484.9 kJ mol−1) in organic chemistry,35 which endows the fluorine-containing polyimide films with excellent thermal stability (Fig. 1d). These polyimides exhibit similar initial decomposition temperatures of around 450 °C, which is attributed to the decomposition of the PFCB group.26–28 The 5% weight loss temperatures of these films exceed 500 °C (Fig. 1d and Table 1), which is comparable to most aromatic polyimides.36,37
These polyimide films show high tensile strength values of 83.6–96.2 MPa, tensile modulus values of 2.2–3.1 GPa, and elongation at break values of 5.1–6.9% (Table 1). The 6FDA-co-PFODPA-PFODA film has the weakest mechanical properties, with a low tensile strength of 73.2 MPa and an elongation at break value of 3.5%. The relatively low molecular weight of the film is the main cause, due to the polymerization difficulties caused by the too-high content of PFCB groups.
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| Fig. 3 (a) Dielectric constants of the polyimide films at low frequency. (b) Dielectric loss of the polyimide films at low frequency. | ||
| 6FDA-PFODA-trans | 6FDA-PFODA-cis | 6FDA-PFODA | PFODPA-TFMB | 6FDA-co-PFODPA-PFODA | 6FDA-TFMB | |
|---|---|---|---|---|---|---|
| D k at 1 kHz | 2.42 | 2.44 | 2.43 | 2.46 | 2.37 | 2.78 |
| D f at 1 kHz | 0.0020 | 0.0035 | 0.0029 | 0.0094 | 0.0013 | 0.0044 |
| D k at 10 GHz | 2.59 | 2.62 | 2.60 | 2.53 | 2.50 | 2.91 |
| D f at 10 GHz | 0.0067 | 0.0049 | 0.0053 | 0.0071 | 0.0035 | 0.0048 |
| W A (%) | 0.18 | 0.16 | 0.12 | 0.21 | 0.10 | 0.23 |
As the cis/trans-isomers were successfully separated and the corresponding polyimide films were prepared, the conformation effect on the dielectric performance can be compared quantitatively. The optimized geometries of the 6FDA-PFODA-trans and 6FDA-PFODA-cis units are shown in Fig. S10.† The dihedral angle between the phenyl and imide rings changes slightly (φ2 = 40.2°) compared with that of 6FDA-TFMB (φ2 = 38.3°). The dipole moment (μ) and polarizability (α) of each unit were calculated via the DFT (CAM-B3LYP/6-311++G(d,p)) method that we previously used42 and are summarized in Table 3. The introduction of PFCB groups breaks the electronic conjugation of the diamine and increases the length of the repeat unit, resulting in a low dipole moment. A lower dipole moment was achieved in all the PFCB-containing polyimides compared with that of 6FDA-TFMB. Because of the more symmetric conformation, a much lower μ (2.21 Debye) is obtained for 6FDA-PFODA-trans than for 6FDA-PFODA-cis (3.71 Debye). The polarizability (α) increases to 450 a.u. for 6FDA-PFODA-cis/trans.
| Polyimide | ρ (g cm−3) | M (g mol−1) | μ (Debye) | α (a.u.) | V vdw (cm3 mol−1) | α/Vvdw | K p |
|---|---|---|---|---|---|---|---|
| ρ: experimental density; M: molecular weight of repeat unit; μ: dipole moment; α: polarizability; Vvdw: van der Waals volume; Kp: packing coefficient of the polyimides. μ, α, Vvdw were calculated using DFT (CAM-B3LYP/6-311++G(d,p)), a.u. for α is Bohr3 per atom and 1 Bohr = 0.52917 Å.a The density value was measured from the isomer mixtures in PFODPA-TFMB. | |||||||
| 6FDA-PFODA-trans | 1.246 | 786.5 | 2.21 | 452.16 | 446.66 | 1.012 | 0.708 |
| 6FDA-PFODA-cis | 1.249 | 786.5 | 3.71 | 450.66 | 437.43 | 1.030 | 0.695 |
| PFODPA-trans-TFMB | 1.241a | 772.5 | 2.46 | 443.47 | 439.66 | 1.009 | 0.706 |
| PFODPA-cis-TFMB | 1.241a | 772.5 | 3.91 | 439.57 | 427.95 | 1.027 | 0.688 |
| 6FDA-TFMB | 1.283 | 728.5 | 4.55 | 416.79 | 410.54 | 1.015 | 0.723 |
Additionally, the polyimide chain packings as quantified by the packing coefficients (Kp) were explored to evaluate the density of dipoles.43 Low Kp values correspond to loose PI chain packing with a large free volume. The incorporation of PFCB groups decreases the Kp values of 6FDA-PFODA-cis/trans. Hence, 6FDA-PFODA-cis/trans with relatively loose chain packing exhibit low dielectric permittivity (Dk,10 GHz = 2.59 and 2.62, respectively). 6FDA-PFODA-trans has a higher Kp value (0.708) than 6FDA-PFODA-cis (0.695) due to its more symmetric nature. Nevertheless, a higher dielectric permittivity value was obtained in 6FDA-PFODA-cis, which was mainly attributed to its large polarizability per unit volume (α/Vvdw = 1.030).40,44 The rigid 6FDA-TFMB was found to have highly dense chain packing using WAXD (Fig. S9†) and exhibits the largest Kp (0.723), affording the largest dielectric permittivity (Dk,10 GHz = 2.91).
Furthermore, an even lower dielectric permittivity (Dk, 10 GHz = 2.53) was found for PFODPA-TFMB, as well as for the multicomponent co-PI 6FDA-co-PFODPA-PFODA sample constructed from the dianhydride-containing PFCB monomer. Apparently, PFODPA-TFMB with either the trans or cis conformation exhibits a lower chain packing density, as validated by both the WAXD (Fig. S9†) and packing coefficient calculation (Table 3). The best dielectric performance was realized in the multicomponent 6FDA-co-PFODPA-PFODA, i.e., Dk,1 kHz = 2.37, Df,1 kHz = 0.0013, Dk,10 GHz = 2.5, and Df,10 GHz = 0.0035. This could be rationalized by that fact that 6FDA-co-PFODPA-PFODA has the highest content of PFCB groups among all the tested samples in Table 2. These PFCB groups would result in lower α/Vvdw and Kp values to decrease Dk, as well as a lower dipole moment density to reduce the dielectric loss. Currently, there are few well-established theories to explain the dielectric loss. In general, these PFCB-containing polyimides have relatively low dielectric loss values comparable to that of 6FDA-TFMB.
Moisture can significantly impact the dielectric constant due to the large polarity of water molecule, which is a key issue in application. The water absorption of the materials was measured after immersion in deionized water for 72 h at room temperature (Table 2). The PFCB-containing polyimides have extremely low water absorption values ranging from 0.1–0.21%. The contact angles of the PFCB-containing polyimides were also found to all be above 90° (Fig. S11†). These results indicate that the polyimides are rather hydrophobic, and the values of the water contact angles were consistent with the trends in the water absorption experiments.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d2py00550f |
| This journal is © The Royal Society of Chemistry 2022 |