Hyunjung
Jin‡
ab,
Kyeongmin
Kim‡
ab,
Kyuyeon
Kim‡
ac,
Sungmin
Park
d,
Eul-Yong
Shin
a,
Jae Won
Heo
efg,
Hyunjoo
Lee
hi,
Se-Woong
Baek
c,
In Soo
Kim
efg,
Hyungju
Ahn
*j and
Hae Jung
Son
*ab
aAdvanced Photovoltaics Research Center, Korea Institute of Science and Technology (KIST), Seoul 02792, Republic of Korea. E-mail: hjson@kist.re.kr
bGraduate School of Energy and Environment (KU-KIST Green School), Korea University, Seoul 02841, Republic of Korea
cDepartment of Chemical and Biological Engineering, Korea University, Seoul, 02841, Republic of Korea
dPhotonics Convergence Display Research Center, ICT Convergence Research Division, Gumi Electronics and Information Technology Research Institute (GERI), Gumi, Gyeongbuk 39253, Republic of Korea
eNanophotonics Research Center, Korea Institute of Science and Technology (KIST), Seoul, 02792, Republic of Korea
fSchool of Advanced Materials Science and Engineering, Sungkyunkwan University (SKKU), Suwon 16419, Republic of Korea
gKIST-SKKU Carbon-Neutral Research Center, Sungkyunkwan University (SKKU), Suwon 16419, Republic of Korea
hClean Energy Research Center, Korea Institute of Science and Technology (KIST), 02792, Seoul, Republic of Korea
iDivision of Energy & Environment Technology, KIST School, Korea University of Science and Technology, Seoul 02792, Republic of Korea
jPohang Accelerator Laboratory, POSTEHC, Pohang, Gyungbuk 37673, Republic of Korea. E-mail: hyungju@postech.ac.kr
First published on 1st May 2024
As a promising solution to address the growing concern of electronic waste, transient electronics, such as biomedical implants, environmental sensors, and hardware-secured devices, have garnered considerable attention. These devices can be engineered to exhibit partial solubility, degradability, or physical dissolution. For the development of degradable transient organic electronics, it is important to develop degradable polymeric organic semiconductors. However, few studies have focused on controlling the degradation rates of polymers in films. In this study, we designed and synthesized three different degradable polymers, namely, PY-m-TIPO, PY-p-TIPO, and PY-t-TIPO, through in situ polymerization in the film state. Notably, PY-t-TIPO exhibited a significantly higher charge mobility of 1.67 × 10−3 cm2 V−1 s−1 in organic thin-film transistors (OTFTs) than PY-m-TIPO and PY-p-TIPO although all the degradable polymer films exhibited similar amorphous properties. We demonstrated that the number of bonding arms affects not only the degradation rate of the polymer films but also the charge mobility of the corresponding OTFTs. Our study provides design guidelines for developing degradable polymers with controllable degradation rates for high charge mobility in transient OTFTs.
The early prototypes of transient electronics were reported to be silicon-based devices.2,19–22 However, inorganic semiconductors, such as silicon, have drawbacks such as mechanical brittleness, toxicity, and high manufacturing costs. Furthermore, elements such as gallium and indium have limited global reserves. Organic semiconductors have attracted significant attention as an alternative to silicon-based devices. These materials are known for their ease of fabrication, mechanical flexibility,23 and tunable properties. Organic semiconductors can be applied in various systems such as organic light-emitting diodes,24–28 organic photovoltaics,29–33 and organic sensors.34–36 Compared to inorganic active materials, polymers are a promising class of materials that exhibit the desired combination of good electrical properties and degradability, owing to the vast chemical design space enabled by synthetic methodologies. To facilitate their application in transient electronics, developing organic semiconductors that simultaneously exhibit excellent electrical properties and degradability to promote their application in transient electronics is a challenging research task. In particular, it is important to develop organic semiconductors that can control the degradation rate of thin films,37 which may depend on the chemical structure of the organic semiconductor38 and the morphology of the thin film.39
In this study, we developed various degradable polymers through the reaction between an aldehyde-attached small molecule, Y5-TA-Cl, and the geometrical isomers of m-PO-N, p-PO-N, and t-PO-N, which yielded PY-m-TIPO, PY-p-TIPO, and PY-t-TIPO, respectively, as shown in Fig. 1a. We elucidated the effects of the number of bonding arms in the network core and the geometrical-isomeric structures of the degradable polymers on the charge mobilities of the polymer-film-based organic thin-film transistors (OTFTs) and degradation behavior under acidic conditions. Furthermore, the synthesized degradable polymers were used in OTFTs to investigate their electronic properties and applicability in the development of degradation-controllable transient electronics.
Fig. 1 (a) Chemical structures and (b) synthetic route of the degradable polymers PY-m-TIPO, PY-p-TIPO, and PY-t-TIPO. |
The key strategy for controlling the degradation rate of degradable polymers is to vary the number and positions of amines in the crosslinker, which may also affect the molecular packing structures and morphology of the thin films. In this study, degradable polymers were synthesized in the film state through in situ one-shot preparations using the Schiff reaction.41–43 To confirm the occurrence of in situ one-shot polymerization in the film state, we conducted a washing test by spin-coating the films with dichloromethane. The films with added PO-N retained their absorption peaks even after washing. Additionally, the films with added t-PO-N, which had the highest amine content, exhibited the highest amount of residual films.
We performed Fourier transform infrared (FT-IR) and ultraviolet-visible (UV-Vis) spectroscopy measurements to investigate the reaction between Y5-TA-Cl and the amine-functionalized crosslinkers in the film. The changes in the FT-IR peaks at 1640–1720 cm−1, which include the peaks assigned to ketone (1694 cm−1) and aldehyde (1679 cm−1) groups, were monitored via deconvolution and curve-fitting for diverse stoichiometric ratios of PO-N (Y5-TA-Cl:PO-N = 1:0, 1:0.25, 1:0.5, 1:0.75, 1:1). Fig. 2 and Fig. S7 (ESI†) present the summary of the results. Irrespective of the PO-N types, the intensities of the aldehyde peak at 1679 cm−1 and the imine peak at 1630 cm−1 simultaneously decreased and increased, respectively, with increasing PO-N concentration. We estimated the polymerization yield by comparing the decreased peak area for the aldehyde group with that for the ketone group at 1694 cm−1, as shown in Table 1. After the reaction, some aldehyde monomers were retained in the p-PO-N film even when the Y5-TA-Cl:p-PO-N stoichiometric ratio was 1:1. This resulted in a lower polymerization yield of 89% than the 95% yield of the m-PO-N film. This is probably because the linear polymers prepared using p-PO-N had a relatively low degree of molecular movement in the film, which decreased the reactivity of the Schiff reaction. The polymerization yield of the resulting polymer films was confirmed again at around 88% by performing the gel-permission chromatography (GPC) measurements and the GPC data are shown in Fig. S8 (ESI†).
Crosslinker | Stoichiometric ratio of Y5-TA-Cl:PO-N | Normalized value of integrated area | Integration area ratio | Polymerization yield [%] |
---|---|---|---|---|
m-PO-N | 1:0 | 1.134 | 1 | — |
1:0.25 | 0.953 | 0.84 | 16.0 | |
1:1.5 | 0.675 | 0.59 | 40.5 | |
1:0.75 | 0.496 | 0.34 | 56.3 | |
1:1 | 0.091 | 0.08 | 92.0 | |
p-PO-N | 1:0 | 1.170 | 1 | — |
1:0.25 | 1.030 | 0.88 | 12.0 | |
1:1.5 | 0.826 | 0.71 | 29.4 | |
1:0.75 | 0.421 | 0.36 | 64.1 | |
1:1 | 0.124 | 0.11 | 89.4 | |
t-PO-N | 1:0 | 1.112 | 1 | — |
1:0.25 | 0.841 | 0.76 | 24.4 | |
1:1.5 | 0.693 | 0.62 | 37.7 | |
1:0.75 | 0.389 | 0.35 | 65.0 | |
1:1 | 0.056 | 0.05 | 95.0 |
The UV-Vis absorption spectra of the PY-m-TIPO, PY-p-TIPO, and PY-t-TIPO degradable polymers and Y5-TA-Cl films are shown in Fig. 3a and summarized in Table S1 (ESI†). After polymerization, the absorption spectra of all the films were blue-shifted compared with the Y5-TA-Cl spectrum. Therefore, the maximum absorption peaks of PY-m-TIPO, PY-p-TIPO, and PY-t-TIPO were observed at 788, 790, and 792 nm, respectively. Additionally, the 0–0 peaks of the polymers were less intense than those of Y5-TA-Cl, and the absorption onsets of the polymers were blue-shifted. These results are because polymerization disturbed the packing structure of Y5-TA-Cl in the film, increasing the amorphous properties of the polymers. The absorption spectra of PY-m-TIPO, PY-p-TIPO, and PY-t-TIPO exhibited similar features to each other.
The UV-Vis spectroscopy was performed to analyze the absorption profiles of the polymer films during their degradation process (Fig. S9, ESI†). Prior to degradation, the polymer films exhibited two primary absorption peaks, denoted as 0–0 and 0–1 transition peaks at 792 and 723 nm, respectively. The 0–0 peak-normalized data revealed that the intensity of the 0–1 peak gradually increased as the degradation time proceeded and that the peak was slightly redshifted. This shift is attributed to the depolymerization of the imine-based polymers to aldehyde monomers.44 Notably, under acidic conditions, PY-t-TIPO, which features three bonding arms, exhibited higher stability than PY-m-TIPO and PY-p-TIPO, each with two bonding arms. This observation suggests that the polymer degradation accelerates with decreasing number of bonding arms. The structural differences in the positions of the bonding arms also influence the degradation rate of the polymers.
To quantitatively analyze the degradation behavior, we systematically monitored and compared the degradable polymers in the films through FT-IR spectroscopy. The spectra were normalized in relation to the peak ascribed to the unaltered cyanide (–CN) stretching vibration45,46 at 2216 cm−1, as shown in Fig. 4a–c. Gaussian fitting was applied to deconvolute the peaks, as shown in Fig. S10–S12 (ESI†). The intensity of the aldehyde vibration peak47 at 1678 cm−1 progressively increased, while that of the imine stretching vibration peak48 at 1630 cm−1 decreased during the polymer degradation process. A comparison between the polymer films revealed that the degradation rate of the polymer films decreased in the order of PY-p-TIPO, PY-m-TIPO, and PY-t-TIPO, as shown in Fig. 4d and Tables S2–S4 (ESI†). Although the slowest degradation rate of PY-t-TIPO is due to three bonding arms, the slightly different degradation between PY-p-TIPO and PY-m-TIPO may be affected by different molecular conformations of the polymers; the linear shape of PY-p-TIPO would be more favorable for exposure to acid vapors. These findings highlighted the significance of the number of bonding arms and their positions as design parameters for controlling the degradation rate of organic transient electronic devices.
We investigated the effect of degradable polymers with different geometrical crosslinkers on the electrical properties of the OTFTs. For all of the OTFT devices with degradable polymers, the electron mobility (μ) and threshold voltage (Vth) were calculated using the conventional gradual channel approximation equations at VD = 80 V. The detailed electrical parameters of the OTFT devices are summarized in Table 2. PY-t-TIPO showed an electron mobility of 1.67 × 10−3 cm2 V−1 s−1. This is a decreased value compared to 6.87 × 10−3 cm2 V−1 s−1 of Y5-TA-Cl. Nevertheless, it is a remarkable result because the GIWAXS results revealed that the PY-t-TIPO film showed unfavorable amorphous properties. This demonstrates that the degradable polymer is favorable for formation of an interconnected pathway for charge transport in OTFTs. Although the PY-m-TIPO and PY-p-TIPO films exhibited amorphous properties similar to those of PY-t-TIPO, the electron mobilities of the OTFTs prepared using PY-m-TIPO and PY-p-TIPO decreased to 0.18 and 0.24 × 10−3 cm2 V−1 s−1, respectively. It is expected that the chemical structure of the three bonding arms is important to form the networked structure of the polymer for it promotes efficient charge transport. Additionally, geometrical isomerism of m-PO-N and p-PO-N is not significantly important for determining the charge carrier mobility of the polymer.
Material | Acid vapor exposure time | Electron mobility [cm2 V−1 s−1] | V th [V] | I on/Ioff |
---|---|---|---|---|
Y5-TA-Cl | 0 h | 6.87 × 10−3 | 10.0 | 4.2 × 102 |
PY-m-TIPO | 0 h | 0.18 × 10−3 | 6.41 | 1.9 × 102 |
24 h | 0.31 × 10−3 | 22.9 | 0.9 × 102 | |
PY-p-TIPO | 0 h | 0.24 × 10−3 | 4.58 | 1.2 × 102 |
24 h | 0.45 × 10−3 | 18.2 | 0.5 × 102 | |
PY-t-TIPO | 0 h | 1.67 × 10−3 | 13.8 | 3.8 × 102 |
24 h | 0.53 × 10−3 | 23.5 | 1.4 × 102 |
Footnotes |
† Electronic supplementary information (ESI) available: Additional synthesis of monomers and polymers, additional FT-IR results, and NMR results. See DOI: https://doi.org/10.1039/d4tc01377h |
‡ These authors contributed to this work equally. |
This journal is © The Royal Society of Chemistry 2024 |