Wenrui Lei†
,
Kelsey Harrison†
,
Si Tong Bao,
Kyunam Lee
,
Michael L. Steigerwald
,
Qian Cheng*,
Nicholas M. Orchanian
*,
Colin Nuckolls
* and
Qifeng Jiang
*
Department of Chemistry, Columbia University, New York, NY 10027, USA. E-mail: cn37@columbia.edu; qj2175@columbia.edu
First published on 29th August 2025
Here, we explore a conjugated, contorted polymer framework tailored for ultrafast-rate charging/discharging, leveraging a tunable synthetic strategy to control its molecular length. We systematically explore the helical perylene diimide (hPDI) ladder polymers across three length regimes, short, medium, and long, to determine the optimal electrochemical stability and performance. The intermediate-length polymer strikes a critical balance between electrode integrity, solubility, and rate capability. Its reversible redox activity and structural robustness make it well-suited for both Li+ and Mg2+ ions. The hPDI-medium cathode delivers a remarkable specific power of 22.4 kW kg−1 after 10000 cycles in Li batteries and 1.7 kW kg−1 after 3000 cycles in Mg batteries, and we extend this to practically relevant mass loadings. This study highlights the critical role of molecular engineering in the rational design of high-performance organic cathode materials for sustainable energy storage.
We focused previously on atomically defined helical perylene diimide (hPDI) oligomers up to six PDI subunits in length as OEMs. The oligomer with six PDI subunits in length is named hPDI-short.18 Several design elements emerged from these studies, enabling fast-charging and long-lifetime cathodes with Li-metal anodes and liquid electrolyte: (1) molecular contortion provided by the ladder backbone facilitates rapid ion transport. (2) The longer, conjugated structures have higher electronic conductivity, further boosting performance. This initial study highlighted improvements in cathode performance as a function of increasing ladder length, but the iterative synthetic procedure precluded extension of these oligomers to high-molecular weight systems, which could provide deeper insight into structure–property relationships and a higher-performing OEM.
Our new high-yielding synthesis allows us to test, for the first time, longer versions of the hPDI series. We synthesize two polymers: hPDI-medium (∼15 PDI subunits) and hPDI-long (∼90 PDI subunits). These new polymers exhibit ultrafast-charging capability as cathodes in both Li-metal batteries and Mg-metal batteries (Fig. 1). Controlling the degree of polymerization allows us to assess how ladder length influences battery performance. We identify a “sweet spot” in ladder length, exhibiting optimal ultrafast-charging and improved long-term stability in Li and Mg electrolyte systems (Fig. S1–S3). hPDI-medium demonstrates minimal capacity decay at rates up to 50 C in Li cells and delivers an impressive specific power of 22.4 kW kg−1 after 10000 cycles, with an energy density of 235 Wh kg−1. hPDI-medium overcomes the typical sluggish kinetics and electrode instability associated with Mg ions, having excellent capacity retention at rates up to 20 C, and delivers a specific power of 1.7 kW kg−1 and energy density of 65 Wh kg−1 after 3000 cycles.
Next, we assemble Li and Mg cells with the hPDI-n cathode series to evaluate their battery performance. Cyclic voltammetry shows the highly reversible redox activity expected for PDI subunits in the voltage range of 1.5–3.3 V vs. Li/Li+ and 0.7–2.3 V vs. Mg/Mg2+ (Fig. S7–S9).20–22 The resulting b-values indicate charge/discharge is a capacitive-controlled (b = 1) process for all hPDI-n polymers in the Li system, while stronger coulombic interactions of the divalent Mg ion give rise to mixed diffusion and capacitive-controlled (0.5 < b < 1) processes for hPDI-short and hPDI-medium in the Mg system. Interestingly, higher b-values (0.9 < b < 1) for hPDI-long in the Mg system indicate a predominantly capacitive-controlled process.23,24
Galvanostatic cycling tests demonstrate excellent rate capability for both Li and Mg-metal batteries (Fig. 3 and Table 1). In Li cells with a 1,3-dioxolane/1,2-dimethoxyethane (DME)-based electrolyte, hPDI-medium delivers the highest initial capacity of 110 mA h g−1 at 1 C (1 C = 0.13 A g−1), when compared to the other ladder lengths, and retains remarkably high capacity retention (91%) under ultrafast-charging, up to 50 C (Fig. 3a and b). hPDI-short shows similar performance to hPDI-medium, delivering an initial capacity of 107 mA h g−1 and retaining 86% of its capacity up to 50 C. The longest ladder of the series, hPDI-long, maintains the best capacity retention (94%) at 50 C, but only delivers an initial capacity of 93 mA h g−1 at 1 C. We speculate that the longer ladder length polymer packs to occlude access to its redox active sites, lowering the capacity. There is a trade-off between ladder length and cathode performance, where hPDI-medium achieves high capacity at fast-charging rates even without additives commonly employed in OEMs.25–27 Compared to other polyimide-based cathodes reported for fast-charging Li-metal batteries, hPDI-medium demonstrates best-in-class rate performance (Fig. 3c).28–31 With >99.0% coulombic efficiency across all rate tests, as well as complete recovery of its initial capacity in the final 1 C cycles, hPDI-medium demonstrates excellent redox reversibility for high power applications.
hPDI | Li | Mg | ||
---|---|---|---|---|
Capacity at 50 C (mA h g−1) | Retention of 1 C capacity | Capacity at 20 C (mA h g−1) | Retention of 1C capacity | |
Short | 93 | 86% | 49 | 61% |
Medium | 100 | 91% | 65 | 80% |
Long | 87 | 94% | 33 | 78% |
Fast-charging in divalent ion systems is typically more challenging, but the hPDI series shows strong performance in Mg cells under high-rate operations (Fig. 3d and e). With a chloride-free, DME-based electrolyte, hPDI-medium delivers an initial capacity of 81 mA h g−1 at 1 C with 80% retention up to 20 C and >99.0% coulombic efficiency. hPDI-short delivers 80 mA h g−1 capacity at 1 C with 61% capacity retention at 20 C, while hPDI-long delivers a significantly lower initial capacity of 42 mA h g−1 at 1 C. Despite lower capacity, hPDI-long shows substantially improved capacity retention (78%) at 20 C compared to hPDI-short. Fig. 3f displays the capacity retention of hPDI-medium and hPDI-long at 20 C, where they outperform hPDI-short as well as organic polymers reported for Mg batteries.32–37 While fast-charging capacity retention is significantly improved, the large difference in overall capacity between hPDI-medium and hPDI-long in the Mg system further points to unfavorable packing in the longest polymer, where stronger coulombic interactions inhibit access to all redox sites. The synthetic precision in OEMs is critical for Mg batteries. Beyond organic systems, the capacity retention of hPDI-medium under fast-charging conditions exceeds that of well-established inorganic cathodes for Li and Mg batteries (Fig. S10).38–44
We use SEM and HR-STEM to better understand the enhanced battery performance of hPDI-medium (Fig. S11 and S12). SEM images of hPDI-short, hPDI-medium and hPDI-long morphology. hPDI-short has a film-like network evenly distributed across fibers of the carbon paper electrode. hPDI-medium and hPDI-long both show large, agglomerated particles dispersed on the carbon paper fibers. HR-STEM images of the cathode slurries on mesh grids provides some distinction between hPDI-medium and hPDI-long morphologies where extension into the long polymer regime gives rise to more densely agglomerated particles. The lower overall capacity of hPDI-long, particularly in the Mg system, can therefore be explained by its dense morphology inhibiting the diffusion of divalent Mg ions which is further supported by b-values indicating that charge storage is predominantly a capacitive-controlled process. Thus, we attribute enhanced performance of hPDI-medium to a morphology that allows access to redox sites while maintaining stability in the electrolyte.
We better understand the structure–property relationship from additional electrochemical characterization. Electrochemical impedance spectroscopy (EIS) measurements of Li batteries are shown in Fig. 4a, highlighting critical changes with increasing polymer length. The charge transfer resistance (Fig. S13) of 9.7 Ω is measured for hPDI-medium, lower than both hPDI-short (95 Ω) and hPDI-long (42 Ω). This lower resistance for hPDI-medium suggests enhanced kinetics for charge transfer, explaining its high capacity during fast-charging.45,46 hPDI-medium strikes an optimal balance between insolubility and electrochemical performance (Fig. 4b). We tested an additional polymer length (40-subunit) in between hPDI-medium and hPDI-long which confirms the 15-subunit polymer as the best performing material in this series (Fig. S14).
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Fig. 4 (a) EIS of hPDI-short, hPDI-medium, and hPDI-long in Li cells. (b) The hPDI ladder length “sweet spot” for dissolution and charge transfer resistance. |
With hPDI-medium identified as the sweet spot for cathode performance, we used this material for ultrahigh-rate, long-term cycling studies in Li and Mg batteries (Fig. 5). At a 77 C rate (10 A g−1) in a Li battery, hPDI-medium exhibits remarkable electrochemical reversibility, maintaining a coulombic efficiency >99.5% every cycle and preserving 99% of its initial 106 mA h g−1 capacity after 5000 cycles. There is a minuscule capacity fade of 0.0002% per cycle, underscoring its resilience to repetitive high-rate processes. Extended cycling data (Fig. S15 and S16) highlights this material's stability, demonstrating no additional capacity loss up to 10000 total cycles. Fig. 5b presents a Ragone plot of hPDI-medium and other polyimide-based polymers in Li batteries (excluding OEMs with carbon nanotube additives) based on the delivered cell voltages and active electrode components.28–31 hPDI-medium achieves the highest specific power (22.4 kW kg−1), while maintaining a high specific energy (235 Wh kg−1) after 10
000 cycles. The feasibility of hPDI-medium for practical applications is further demonstrated in Li cells assembled with >700% higher mass loading (2.5 mg cm−2) delivering a similar capacity of 105 mA h g−1 at 1 C (Fig. S17).
We also observe the excellent long-term cycling stability of hPDI-medium in a Mg battery (Fig. 5c and S18). After 3000 cycles at 10 C (1.3 A g−1), the material retains 67% of its initial 75 mA h g−1 capacity and maintains >99.5% coulombic efficiency. Fig. 5d is a Ragone plot comparing the long-term cycling stability and energy density of organic polymers in Mg batteries, highlighting the excellent performance of hPDI-medium.32–37 hPDI-medium demonstrates a specific energy of 65 Wh kg−1 and specific power of 1.7 kW kg−1, making it one of the highest power Mg batteries reported. The stability of hPDI-medium is also verified by ex situ Raman spectroscopy, confirming preserved integrity of the molecular structure after prolonged cycling (Fig. S19). The excellent performance of hPDI-medium with monovalent and divalent ions is promising for applications.
Synthesis details, materials characterization, and electrochemical data can be found in the SI. See DOI: https://doi.org/10.1039/d5sc04900h.
Footnote |
† Both authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2025 |