Journal
ACS APPLIED NANO MATERIALS
Volume 4, Issue 1, Pages 53-60Publisher
AMER CHEMICAL SOC
DOI: 10.1021/acsanm.0c02073
Keywords
lithium-sulfur batteries; graphene; three-dimensional current collectors; energy storage; lithium-ion batteries
Funding
- SC-GEAR [19-GE01]
- NASA-EPSCoR award [NNH17ZHA002C]
- South Carolina EPSCoR/IDeA Program [18-SR03]
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Graphene foams (GFs) are shown to be an ideal 3D lightweight current collector for lithium-sulfur batteries (LSBs), enabling high sulfur loading and increased capacity. GF-SPAN cathodes demonstrate capacities of up to 200 mAh g(electrode)(-1) at the electrode level, surpassing conventional Al/C electrodes by 3 times.
Extending lithium-sulfur battery (LSB) electrode architecture into three dimensions (3D) has been proposed for more than a decade. A 3D lightweight and porous current collector that is capable of holding high amounts of sulfur (S) without any significant decrease in performance has been elusive. Although many material solutions (such as sulfurized polyacrylonitrile or SPAN) have been identified for alleviating polysulfide formation and the so-called shuttle effect, their incorporation into 3D current collectors with high capacity at the electrode level has not yet been realized. Here, we show that graphene foams (GFs) are ideally suited as 3D lightweight current collectors for LSBs and outperform the conventional carbon-coated Al (Al/C) foils at the electrode level. Specifically, we demonstrate that the open framework of GFs facilitates high mass loading of SPAN without any deterioration in capacity at the active material level even at high S loading. At the electrode level, GF-SPAN cathodes exhibited capacities of similar to 200 mAh g(electrode)(-1) at 0.1C even with low S loadings (similar to 1.1 mg cm(-2)), which is at least 3 times higher than conventional Al/C electrodes. More importantly, we fabricated cells with a high mass loading of 26.5 mg cm(-2) S by stacking multiple GFs to achieve an areal capacity as high as similar to 20 mAh cm(-2) (at a current density of 3.0 mA cm(-2) up to 50 cycles), which is at least 3 times higher than LSB areal capacity (6 mAh cm(-2)) needed to displace LIBs.
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