Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/9081
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dc.contributor.authorGODBOLE, RHUSHIKESHen_US
dc.contributor.authorHIWASE, SHWETAen_US
dc.contributor.authorHossain, Mujaffaren_US
dc.contributor.authorKADAM, SUPRIYAen_US
dc.contributor.authorWABLE, MINALen_US
dc.contributor.authorRane, Suniten_US
dc.contributor.authorMondal, Sukantaen_US
dc.contributor.authorDas, Bidisaen_US
dc.contributor.authorBanerjee, Abhiken_US
dc.contributor.authorOGALE, SATISHCHANDRAen_US
dc.date.accessioned2024-09-20T04:03:36Z
dc.date.available2024-09-20T04:03:36Z
dc.date.issued2024-09en_US
dc.identifier.citationApplied Physics Reviews, 11(03), 031416.en_US
dc.identifier.issn1931-9401en_US
dc.identifier.urihttps://doi.org/10.1063/5.0208785en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/9081
dc.description.abstractWe have examined the case of light atom (B, N) doped and co-doped graphitic films grown on copper for the anode-free Li Metal Battery (AFLMB) application. For nitrogen doping, the depositions were carried out by laser ablating pure graphite (Gr) in the presence of Nitrogen (N2) or Ammonia (NH3). In another interesting case, 5 wt. % Boron nitride (BN) was added into the graphite target itself to obtain BN-doped graphite films. It was found that the growth condition mediated film constitution and properties significantly influence the Coulombic efficiency and cycling stability of the cells when tested for AFLMB. The cycle life demonstrated by the cells of pure graphitic film (Gr) was only about 110 cycles, while the N-doped graphite films obtained using N2 gas (N2–Gr) exhibited stability up to about 300 cycles. Interestingly the N-doped films obtained using NH3 gas (NH3–Gr) exhibited a stability of 715 cycles and B, N co-doped graphite (BN–Gr) film resulted in an even longer cycle life of 795 cycles. Density functional theory calculations were also performed to deeply understand the interaction and binding energy of Lithium within the undoped and doped graphene sheets modeled through the addition of light elements. It was found that the binding of Li is stronger in the (B, N) co-doped graphene as compared to the N-doped graphene and undoped graphene but much weaker than the B-doped graphene. Therefore, an improved lateral Li diffusion in the (B, N) co-doped graphene is observed where the Li binding strength is optimum resulting in better cycling stability.en_US
dc.language.isoenen_US
dc.publisherAIP Publishingen_US
dc.subjectSolid-Electrolyte Interphaseen_US
dc.subjectBoron-Nitride Nanosheetsen_US
dc.subjectIon Batteryen_US
dc.subjectLithium Diffusionen_US
dc.subjectHigh-Energyen_US
dc.subjectGrapheneen_US
dc.subjectPerformanceen_US
dc.subjectIntercalationen_US
dc.subjectSpectroscopyen_US
dc.subjectAdsorptionen_US
dc.subject2024en_US
dc.subject2024-SEP-WEEK3en_US
dc.subjectTOC-SEP-2024en_US
dc.titleLight element (B, N) co-doped graphitic films on copper as highly robust current collectors for anode-free Li metal battery applicationsen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleApplied Physics Reviewsen_US
dc.publication.originofpublisherForeignen_US
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