Open Access Article
Seung-Hyun
Lee‡
a,
Sechang
Park‡
b,
Ju-Young
Choi
a,
Yun-Je
Choi
a,
Hyung Woo
Ji
a,
Hyeyoung
Joung
a,
Dam-Bi
Kim
a,
Kang-Hoon
Yoon
a,
Gyumin
Ji
b,
Daeho
Choi
b,
Jaekang
Lee
b,
Ki-Jung
Paeng
a,
Jaesung
Yang
a,
Soohaeng
Cho
*b and
Chan-Moon
Chung
*a
aDepartment of Chemistry, Yonsei University, Wonju, Gangwon-do 26493, Republic of Korea. E-mail: cmchung@yonsei.ac.kr
bDepartment of Physics, Yonsei University, Wonju, Gangwon-do 26493, Republic of Korea. E-mail: shcho@yonsei.ac.kr
First published on 13th October 2023
Recently, polyimides (PIs) containing the anthracene moiety have been demonstrated to show a wide range of electrical bistable switching behavior, depending on the chemical structures or electrode materials used in the memory devices. There is a need to develop advanced anthracene-containing PIs having higher memory performance. In this study, a new anthracene-containing diamine, 4-(anthracen-9-ylmethoxy)-1,3-diaminobenzene (AMDA), was synthesized, and polymerized with 4,4′-(hexafluoroisopropylidene)diphthalic anhydride (6FDA) to prepare 6FDA-AMDA PI. For comparison, another PI (6FDA-AnDA PI) was prepared from 6FDA and 2,6-diaminoanthracene (AnDA). 6FDA-AMDA PI and 6FDA-AnDA PI have anthracene moieties in the side and main chains, respectively. 6FDA-AMDA PI showed higher solubility in common organic solvents and less tendency of gelation compared to 6FDA-AnDA PI. The prepared PIs exhibited excellent thermal stability. The Al/6FDA-AMDA PI/indium tin oxide (ITO) device showed write-once-read-many times (WORM) behavior with an on/off ratio up to 106, a threshold voltage of 2.40 V, and a high device yield of 80%. In contrast, the Al/6FDA-AnDA PI/ITO device exhibited WORM behavior with an on/off ratio of up to 104, a threshold voltage at 2.50 V and a 20% device yield. The mechanisms associated with the memory effect are explained using density functional theory (DFT) and time-dependent density functional theory (TD-DFT) calculations. The lower switching voltage and higher device yield of 6FDA-AMDA PI may be attributed to more effective inter-chain charge transfer of the side-chain PI, compared to the main chain PI (6FDA-AnDA PI). This study demonstrates that the 6FDA-AMDA PI is suitable as an active material for solution-processable non-volatile memories.
Various polymer materials have been reported to show electrical resistive switching effects.10–15 Among them polyimides (PIs) have attracted significant attention as an active layer for memory devices due to their many advantages, including outstanding thermal stability, good dimensional stability, excellent processability, and superior electrical properties.16–29 High dimensional thermal stability is required to prevent delamination upon the thermal treatment of the memory devices.30 Regarding processability, the advantage is that devices can be made using simple methods such as spin coating, without using vacuum deposition equipment that is commonly used for memory device research and development. These PIs were designed by introducing electron-donating and electron-accepting groups, which enable device-tailored electronic transitions.5,31 PI structures containing different electron donor and acceptor moieties have been demonstrated to exhibit non-volatile or volatile memory behavior.
Recently, PIs containing an anthracene moiety have been demonstrated to show electrically on and off state bistable switching behavior.32–37 Anthracene-based moieties have been introduced into PIs as a hole-trapping site, forming an efficient electron-donating structure. It is possible to tune the highest occupied molecular orbital (HOMO) energy level and the lowest unoccupied molecular orbital (LUMO) energy level, as well as the charge transfer ability of PIs. In our previous report,36 resistive switching memory devices were fabricated from 4,4′-(hexafluoroisopropylidene)diphthalic anhydride (6FDA)-2,6-diaminoanthracene (AnDA) PI, with an anthracene moiety in the main chain. 6FDA-AnDA poly(amic acid) (PAA) was first prepared by the reaction of 6FDA and AnDA, and then the PAA intermediate was imidized to 6FDA-AnDA PI. However, the 6FDA-AnDA PAA sample had a tendency to undergo gelation even at very low concentration of the PAA, so there was some difficulty to synthesize 6FDA-AnDA PI. In addition, the memory device yield of 6FDA-AnDA was very low (around 20%). In this context, it is necessary to develop an anthracene-containing PI having higher solubility in common solvents and a higher device yield. If an anthracene-containing PI is soluble in common solvents, its processability can be greatly improved because one can have much choice of selection of solvents that are the most suitable for the device fabrication process. It should be noted that, except for our previous literature,36 there have been no reports on the device yields in the research literature on other conventional anthracene-containing PI memory systems without any dielectric additive such as graphene oxide.
In this paper, we report the synthesis and electronic properties of a new PI containing anthracene moiety. A novel diamine, 4-(anthracen-9-ylmethoxy)-1,3-diaminobenzene (AMDA), was prepared and polymerized with 6FDA. A comparison PI (6FDA-AnDA PI) was also prepared from 6FDA and AnDA. 6FDA-AMDA PI and 6FDA-AnDA PI had anthracene moieties in the side and main chains, respectively. The memory behaviors of the PIs were studied by using a sandwich device configuration of a PI film between Al and ITO electrodes. The results of this study provide a new strategy to design efficient non-volatile resistive memory devices.
n = 1.58 × 104 g mol−1, with a molecular weight of
w = 2.60 × 104 g mol−1, PDI = 1.67 (established by GPC). 6FDA-AnDA PI was synthesized through a similar procedure except for the use of a different diamine monomer (AnDA) (Scheme 2(b)). The 6FDA-AnDA PI IR (KBr, cm−1): absorption peaks were 3061, 1784, 1729, and 1364 cm−1.
n was 1.57 × 104 g mol−1,
w = 3.75 × 104 g mol−1 and PDI = 2.38 (GPC).
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| Fig. 2 (a) A schematic illustration of the fabrication process of the memory devices, with cross-section SEM images of (b) 6FDA-AMDA PI and (c) 6FDA-AnDA PI coated on ITO glass. | ||
O asymmetrical stretching), 1719 cm−1 (imide C
O symmetrical stretching), and 1376 cm−1 (imide C–N stretching). The 1H and 13C NMR spectra of Amidol-DP are shown in Fig. S1 and S2 (ESI†), respectively. The signal around 7.8–8.0 ppm in Fig. S1 (ESI†) was assigned to the phthalimido protons of Amidol-DP.
The anthracene group was incorporated into Amidol-DP using AM via the Mitsunobu reaction.40,41 For the reaction product, the Amidol-DP-AM IR absorption was found at 1247 cm−1 (C–O–C stretching) (Fig. 1(b)). The results of the elemental analysis of Amidol-DP-AM agreed with the calculated values. To obtain AMDA, two phthalic groups in Amidol-DP-AM were removed by hydrolysis with hydrazine monohydrate. The crude product was purified by silica gel chromatography. The 1H NMR spectrum of AMDA is shown in Fig. 1(a): two peaks around 4.2–4.5 ppm were assigned to the amino group protons of AMDA.26 The 13C NMR spectrum of AMDA is shown in Fig. S3 (ESI†). As shown in Fig. 1(b), AMDA showed characteristic bands at 3359 cm−1 and 3405 cm−1 due to N–H stretching.36 In addition, the results of the elemental analysis of AMDA agreed with its calculated values. These results indicate the successful synthesis of AMDA.
O asymmetric stretching), 1726 cm−1 (imide C
O symmetric stretching) and 1363 cm−1 (imide C–N stretching).36 In addition, the broad absorption band at 2400–3400 cm−1 due to the –COOH groups of the precursor (6FDA-AMDA PAA) disappeared. The 6FDA-AnDA PI showed a similar spectroscopic trend.
The PIs showed
n values up to 15
800 g mol−1 (Table 1) and were soluble in common organic solvents, including NMP, DMF, DMSO, DMAc, and THF (as shown in Table S1 and Fig. S4, ESI†). It was demonstrated that 6FDA-AMDA PI exhibited better solubility and less tendency of gelation compared to 6FDA-AnDA PI. This is probably attributed to the less rigid main chain structure and the presence of a side chain in 6FDA-AMDA PI.42,43
| Polymer |
n
(×104) |
w
(×104) |
PDIa ( w/ n) |
T g (°C) | T 5 (°C) | T 10 (°C) |
|---|---|---|---|---|---|---|
| a Determined through GPC in DMF using polystyrenes as standard. b Measured by DSC from a second heating scan with a heating rate of 10 °C min−1 under N2 atmosphere. c 5% weight loss temperature under N2 atmosphere. d 10% weight loss temperature under N2 atmosphere. | ||||||
| 6FDA-AMDA PI | 1.58 | 2.60 | 1.67 | 374 | 398 | 457 |
| 6FDA-AnDA PI | 1.57 | 3.75 | 2.38 | 358 | 517 | 532 |
It should be noted that the performance of the PI memory devices can be affected by the surface morphology of PIs. The root mean square (RMS) surface roughness values of the 6FDA-AMDA PI and 6FDA-AnDA PI films were 1.10 and 1.08 nm, respectively (Fig. S5, ESI†). These very smooth morphologies are advantageous for memory device performance.44
The thermal stabilities of the prepared PIs were investigated by thermogravimetric analysis (TGA) and differential scanning calorimetry (DSC) under a nitrogen atmosphere (Fig. 4 and Table 1). The 5% weight loss temperatures (T5) of 6FDA-AMDA PI and 6FDA-AnDA PI were 398 °C and 517 °C, respectively, and the 10% weight loss temperatures (T10) of the PIs were 457 °C and 532 °C, respectively. The 6FDA-AMDA PI underwent thermal degradation in a two-step manner. The first weight loss is probably attributed to the degradation of anthracene side groups of the 6FDA-AMDA PI.45 The second degradation process is the degradation of the PI backbones. The DSC curves are displayed in Fig. 4(b). The glass transition temperatures (Tg) of 6FDA-AMDA PI and 6FDA-AnDA PI were 374 °C and 358 °C, respectively. These results indicate that 6FDA-AMDA PI and 6FDA-AnDA PI have very good thermal and dimensional stability up to 350 °C.
UV-vis absorption spectra and cyclic voltammetry (CV) diagrams of the PIs were employed to estimate the highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) energy levels of the PIs (Fig. 5).24,32 The optical and electrochemical properties are summarized in Table 2. The absorption edges (λonset) of 6FDA-AMDA PI and 6FDA-AnDA PI were 400 nm and 417 nm, respectively (Fig. 5(a)).
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| Fig. 5 The (a) UV-vis absorption spectra of PIs coated on a quartz substrate and (b) CV diagrams of PIs on an ITO-coated glass substrate. | ||
| Polymer | λ onset (nm) | E g (eV) | E ox (eV) | HOMOd (eV) | LUMOe (eV) |
|---|---|---|---|---|---|
| a Onset wavelength. b Energy gap values estimated using the equation Eg = 1240/λonset (eV). c Oxidation potential. d Estimated using the equation HOMO = −[(Eox(onset) − E(ferrocene) + 4.8)] (eV). e Estimated using the equation LUMO = HOMO + Eg (eV). | |||||
| 6FDA-AMDA PI | 400 | 3.10 | 0.57 | −4.96 | −1.86 |
| 6FDA-AnDA PI | 417 | 2.97 | 0.59 | −4.98 | −2.01 |
The electrochemical analysis of PIs was conducted by cyclic voltammetry using PI thin films spin coated on ITO glass as a working electrode. From the CV diagrams (Fig. 5(b)), the oxidation onset potentials (Eox) of 6FDA-AMDA PI and 6FDA-AnDA PI were determined to be 0.57 V and 0.59 V vs. the Ag/AgCl electrode, respectively. The external ferrocene/ferrocenium (Fc/Fc+) redox standard potential (E1/2) was determined to be 0.41 eV vs. the Ag/AgCl electrode in acetonitrile. The absolute energy level of ferrocene (4.8 eV) below the zero vacuum level was used as the calibration ref. 46. Therefore, the HOMO levels of the 6FDA-AMDA PI and 6FDA-AnDA PI were calculated to be −4.96 eV and −4.98 eV. From the HOMO level and band gaps, the LUMO level was estimated to be −1.86 eV for 6FDA-AMDA PI and −2.01 eV for 6FDA-AnDA PI. The differences between the HOMO/LUMO levels and the band gaps of the 6FDA-AMDA PI and 6FDA-AnDA PI can be attributed to the differences in the polymer structure.
The electrical properties of the memory devices were investigated by carrying out I–V measurements (Fig. 6). Fig. 6(a) and (b) show representative I–V characteristic curves of the memory devices with a compliance current of 0.01 A. The devices of Al/6FDA-AMDA PI/ITO first stayed in the high resistance state (HRS) (i.e., in the off state at a smaller bias). During the first sweep, the current increases abruptly at 2.40 V, indicating transition from an off to on state. After the devices have reached the low resistance state (LRS), i.e., the on state, the conduction state could remain even during the forward and reverse voltage sweep (sweep 500) with a compliance current, 0.01 A or power off. The 6FDA-AMDA PI memory device had a high yield of 80%, with successful outcomes in 20 out of 25 point cells. The yield of the 6FDA-AMDA PI device was much higher than that of the 6FDA-AnDA PI device (with a yield of 20%).
All devices exhibited WORM memory behavior with an on/off current ratio of about 106 for 6FDA-AMDA PI and about 104 for 6FDA-AnDA PI at a 0.2 V read voltage. In Fig. 6(c) and (d), the retention times and stress tests of both the on and off states of all devices are shown. The 6FDA-AMDA PI device maintained both an on state and off state without degradation for at least 104 s under a constant stress of −0.2 V. Also, the 6FDA-AnDA PI device maintained the on state without degradation for at least 104 s under a constant stress of −0.2 V (Fig. 6(d)). Then, the off state is kept for around 104 s without obvious degradation. All devices demonstrate outstanding irreversible WORM performance.
I–log
V curves of the Al/6FDA-AMDA PI/ITO device for the off state. In the region of positive HRS below 0.77 V, the conduction state was characterized by Ohmic conduction (slope = 1.02). This phenomenon occurred due to the thermal carriers at the interface between the 6FDA-AMDA PI and Al.36 In the range of 0.77 V to 2.40 V, the I–V slope of the fitting line was 3.72 in the positive HRS. This indicates that the SCLC mechanism is dominant in the off state. When the applied voltage exceeds 2.40 V, the device exhibited a transition from the off state to on state. The carriers were injected from the electrode to the active layer, overcoming the energy barrier and flowing through the device following the Ohmic conduction.47 With increases in the applied voltage, the generated charge carriers near the electrode lead to an accumulation of space charges. The individual charge carriers undergo electrostatic repulsion, and can inhibit further charge injection to the active layer, which led to an SCLC. Then, an abrupt increase of the current value emerged when the threshold voltage was reached. The anthracene moieties, trifluoromethyl groups, and imide rings might act as the trapping sites in the PI structure.45
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| Fig. 7 The experimental and fitted I–V curves of the Al/6FDA-AMDA PI/ITO memory device in the on and off states. | ||
Fig. 8 shows the HOMO and LUMO levels of the PIs and the work functions of electrodes determined from UV-vis spectra and CV diagrams. For all the PIs, the energy barrier for the hole injection from ITO to HOMO (0.16 and 0.18 eV) was lower than the electron injection from Al to LUMO (2.42 and 2.27 eV). Therefore, the hole injection from the ITO electrode was much easier than the electron injection from the Al electrode. The results show that the PIs are p-type materials, which means the hole transfer process is dominant.27,44
To gain insight into the field-induced switching behavior of the memory devices based on the PI active layer, the electronic properties were studied by DFT calculation. Calculations of the optimized geometry and molecular orbitals of the basic unit were carried out using the B3LYP/6-31G(d) level with the Gaussian09 program package. The electronic transition mechanism of PIs can be explained as field-induced charge transfer between the diamine (AMDA or AnDA) and 6FDA monomer units.27,45 In Fig. 9, the HOMO level is located on the donor (diamine units), and the LUMOs are located on the acceptor (dianhydride units). In the PIs, AMDA and AnDA act as electron donors, while 6FDA acts as an electron acceptor to promote the charge transfer complex formation.48 At the threshold voltages of 6FDA-AMDA PI and 6FDA-AnDA PI, the holes of the HOMO level were excited to the LUMO+4 (3.15 eV) and LUMO+2 (3.11 eV) levels, respectively. The excited states of the PIs promote the inter-/intra-molecular charge transfer processes. The charge transfer can occur to form a conductive complex, including from the LUMO+4 and LUMO+2 levels of the donor to the LUMOs of the acceptor.27 Each device may show switching at 3.15 V or 3.11 V, but the devices actually showed switching at 2.40 V (6FDA-AMDA PI) and 2.50 V (6FDA-AnDA PI). The decrease in the switching voltage to the on state may be due to the intermolecular charge transfer between the PI chains. It may be predicted that 6FDA-AMDA PI has more efficient intermolecular charge transfer due to flexible anthracene side chains, compared to 6FDA-AnDA PI having the rigid anthracene main chains. Furthermore, the much higher device yield of 6FDA-AMDA PI (80%) than 6FDA-AnDA PI (20%) might partly be due to the increased intermolecular charge transfer. The stability of the charge transfer complex is related to the recombination abilities of holes and electrons.49 The –CF3 group of 6FDA has the strongest electron-withdrawing ability and the anthracene moiety has higher electron donor power. The 6FDA and diamines containing the anthracene moiety form a stable charge transfer complex through the imide ring. Thus, the stable charge transfer state of PIs can exhibit non-volatile WORM behavior.
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| Fig. 9 The calculated frontier molecular orbitals of the basic units of (a) 6FDA-AMDA PI (6FDA-AMDA-6FDA) and (b) 6FDA-AnDA PI (AnDA-6FDA). | ||
In the DFT-optimized structure of the 6FDA-AMDA-6FDA, the spacing between the AMDA moiety and the two 6FDA moieties was 14.4 and 8.6 Å. Given these distances between the electron donor and acceptor, a charge transfer process is shown to occur from the AMDA (donor) to one of the two 6FDA (acceptor) in the same PI chain, as is evident from Fig. 9. In a thin film in which a vast number of PI chains are closely packed, the degree of structural heterogeneity in terms of the distance and relative orientation between neighboring AMDA and 6FDA moieties irrespective of whether they belong to a single chain or not is excessively high. Hence it is difficult to model an appropriate system to perform DFT calculations, preventing us from validating if charge transfer between different chains happens. Nevertheless, as we can assume a high degree of chain packing in a thin film state, we conjecture that charge transfer across chains may also occur in addition to that along a single chain although we are unable to say which processes occur preferentially.
Footnotes |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3ma00453h |
| ‡ These authors contributed equally. |
| This journal is © The Royal Society of Chemistry 2023 |