Control of Two Solid Electrolyte Interphases at the Negative Electrode of an Anode‐Free All Solid‐State Battery based on Argyrodite Electrolyte

Y Yixian Wang (School of Chemical Engineering & Technology, Key Laboratory for Green Chemical Technology of Ministry of Education) V Vikalp Raj (Materials Science and Engineering Program & Texas Materials Institute (TMI) The University of Texas at Austin Austin TX 78712 USA) K Kaustubh G. Naik (School of Mechanical Engineering Purdue University West Lafayette IN 47907 USA) B Bairav S. Vishnugopi (School of Mechanical Engineering Purdue University West Lafayette, IN 47907 USA) J Jaeyoung Cho M Mai Nguyen E Elizabeth A. Recker (McKetta Department of Chemical Engineering) Y Yufeng Su H Hugo Celio (Materials Science and Engineering Program Walker Department of Mechanical Engineering and Texas Materials Institute The University of Texas at Austin Austin TX 78712 USA) A Andrei Dolocan (Materials Science and Engineering Program and Walker Department of Mechanical Engineering) Z Zachariah A. Page (McKetta Department of Chemical Engineering) J John Watt (Center for Integrated Nanotechnologies Los Alamos National Laboratory Los Alamos NM 87545 USA) G Graeme Henkelman Q Qingsong Howard Tu (Department of Mechanical Engineering Rochester Institute of Technology Rochester New York USA) P Partha P. Mukherjee (School of Mechanical Engineering Purdue University West Lafayette, IN 47907 USA) D David Mitlin (Materials Science and Engineering Program Walker Department of Mechanical Engineering and Texas Materials Institute The University of Texas at Austin Austin TX 78712 USA)

Abstract

AbstractAnode‐free all solid‐state batteries (AF‐ASSBs) employ “empty” current collector with three active interfaces that determine electrochemical stability; lithium metal – Solid electrolyte (SE) interphase (SEI‐1), lithium – current collector interface, and collector – SE interphase (SEI‐2). Argyrodite Li6PS5Cl (LPSCl) solid electrolyte (SE) displays SEI‐2 containing copper sulfides, formed even at open circuit. Bilayer of 140 nm magnesium/30 nm tungsten (Mg/W‐Cu) controls the three interfaces and allows for state‐of‐the‐art electrochemical performance in half‐cells and fullcells. AF‐ASSB with NMC811 cathode achieves 150 cycles with Coulombic efficiency (CE) above 99.8%. With high mass‐loading cathode (8.6 mAh cm−2), AF‐ASSB retains 86.5% capacity after 45 cycles at 0.2C. During electrodeposition of Li, gradient Li‐Mg solid solution is formed, which reverses upon electrodissolution. This promotes conformal wetting/dewetting by Li and stabilizes SEI‐1 by lowering thermodynamic driving force for SE reduction. Inert refractory W underlayer is required to prevent ongoing formation of SEI‐2 that also drives electrochemical degradation. Inert Mo and Nb layers likewise protect Cu from corroding, while Li‐alloying layers (Mg, Sn) are less effective due to ongoing volume changes and associated pulverization. Mechanistic explanation for observed Li segregation within alloying LixMg layer is provided through mesoscale modelling, considering opposing roles of diffusivity differences and interfacial stresses.

Article Details

Volume / Issue Vol. 37, Issue 11
Published March 01, 2025
ISSN 0935-9648
Publisher Unknown Publisher

Journal Info

Advanced Materials

Unknown Publisher

ISSN: 0935-9648 Physical Sciences

Authors (16)

Y

Yixian Wang

School of Chemical Engineering & Technology, Key Laboratory for Green Chemical Technology of Ministry of Education

V

Vikalp Raj

Materials Science and Engineering Program & Texas Materials Institute (TMI) The University of Texas at Austin Austin TX 78712 USA

K

Kaustubh G. Naik

School of Mechanical Engineering Purdue University West Lafayette IN 47907 USA

B

Bairav S. Vishnugopi

School of Mechanical Engineering Purdue University West Lafayette, IN 47907 USA

J

Jaeyoung Cho

M

Mai Nguyen

E

Elizabeth A. Recker

McKetta Department of Chemical Engineering

Y

Yufeng Su

H

Hugo Celio

Materials Science and Engineering Program Walker Department of Mechanical Engineering and Texas Materials Institute The University of Texas at Austin Austin TX 78712 USA

A

Andrei Dolocan

Materials Science and Engineering Program and Walker Department of Mechanical Engineering

Z

Zachariah A. Page

McKetta Department of Chemical Engineering

J

John Watt

Center for Integrated Nanotechnologies Los Alamos National Laboratory Los Alamos NM 87545 USA

G

Graeme Henkelman

Q

Qingsong Howard Tu

Department of Mechanical Engineering Rochester Institute of Technology Rochester New York USA

P

Partha P. Mukherjee

School of Mechanical Engineering Purdue University West Lafayette, IN 47907 USA

D

David Mitlin

Materials Science and Engineering Program Walker Department of Mechanical Engineering and Texas Materials Institute The University of Texas at Austin Austin TX 78712 USA