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@ARTICLE{Philipp:888332,
author = {Philipp, Martin and Gadermaier, Bernhard and Posch, Patrick
and Hanzu, Ilie and Ganschow, Steffen and Meven, Martin and
Rettenwander, Daniel and Redhammer, Günther J. and
Wilkening, H. Martin R.},
title = {{T}he {E}lectronic {C}onductivity of {S}ingle {C}rystalline
{G}a‐{S}tabilized {C}ubic
{L}i$_7${L}a$_3${Z}r$_2${O}$_{12}$ : {A} {T}echnologically
{R}elevant {P}arameter for {A}ll‐{S}olid‐{S}tate
{B}atteries},
journal = {Advanced materials interfaces},
volume = {7},
number = {16},
issn = {2196-7350},
address = {Weinheim},
publisher = {Wiley-VCH},
reportid = {FZJ-2020-04851},
pages = {2000450 -},
year = {2020},
abstract = {The next‐generation of all‐solid‐state lithium
batteries need ceramic electrolytes with very high ionic
conductivities. At the same time a negligible electronic
conductivity σeon is required to eliminate self‐discharge
in such systems. A non‐negligible electronic conductivity
may also promote the unintentional formation of Li
dendrites, being currently one of the key issues hindering
the development of long‐lasting all‐solid‐state
batteries. This interplay is suggested recently for
garnet‐type Li7La3Zr2O12 (LLZO). It is, however, well
known that the overall macroscopic electronic conductivity
may be governed by a range of extrinsic factors such as
impurities, chemical inhomogeneities, grain boundaries,
morphology, and size effects. Here, advantage of
Czochralski‐grown single crystals, which offer the unique
opportunity to evaluate intrinsic properties of a chemically
homogeneous matrix, is taken to measure the electronic
conductivity σeon. Via long‐time, high‐precision
potentiostatic polarization experiments an upper limit of
σeon in the order of 5 × 10−10 S cm−1 (293 K) is
estimated. This value is by six orders of magnitude lower
than the corresponding total conductivity σtotal = 10−3 S
cm−1 of Ga‐LZO. Thus, it is concluded that the high
values of σeon recently reported for similar systems do not
necessarily mirror intragrain bulk properties of chemically
homogenous systems but may originate from chemically
inhomogeneous interfacial areas.},
cin = {JCNS-FRM-II / JCNS-2 / MLZ},
ddc = {600},
cid = {I:(DE-Juel1)JCNS-FRM-II-20110218 /
I:(DE-Juel1)JCNS-2-20110106 / I:(DE-588b)4597118-3},
pnm = {6G4 - Jülich Centre for Neutron Research (JCNS) (POF3-623)
/ 6G15 - FRM II / MLZ (POF3-6G15)},
pid = {G:(DE-HGF)POF3-6G4 / G:(DE-HGF)POF3-6G15},
experiment = {EXP:(DE-MLZ)HEIDI-20140101},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000539609000001},
doi = {10.1002/admi.202000450},
url = {https://juser.fz-juelich.de/record/888332},
}