Solid
electrolytes based on LiBH
4
receive much attention
because of their high ionic conductivity, electrochemical robustness,
and low interfacial resistance against Li metal. The highly conductive
hexagonal modification of LiBH
4
can be stabilized via the
incorporation of LiI. If the resulting LiBH
4
-LiI is confined
to the nanopores of an oxide, such as Al
2
O
3
,
interface-engineered LiBH
4
-LiI/Al
2
O
3
is obtained that revealed promising properties as a solid electrolyte.
The underlying principles of Li
+
conduction in such a nanocomposite
are, however, far from being understood completely. Here, we used
broadband conductivity spectroscopy and
1
H,
6
Li,
7
Li,
11
B, and
27
Al nuclear magnetic
resonance (NMR) to study structural and dynamic features of nanoconfined
LiBH
4
-LiI/Al
2
O
3
. In particular, diffusion-induced
1
H,
7
Li, and
11
B NMR spin–lattice
relaxation measurements and
7
Li-pulsed field gradient (PFG)
NMR experiments were used to extract activation energies and diffusion
coefficients.
27
Al magic angle spinning NMR revealed surface
interactions of LiBH
4
-LiI with pentacoordinated Al sites,
and two-component
1
H NMR line shapes clearly revealed heterogeneous
dynamic processes. These results show that interfacial regions have
a determining influence on overall ionic transport (0.1 mS cm
–1
at 293 K). Importantly, electrical relaxation in
the LiBH
4
-LiI regions turned out to be fully homogenous.
This view is supported by
7
Li NMR results, which can be
interpreted with an overall (averaged) spin ensemble subjected to
uniform dipolar magnetic and quadrupolar electric interactions. Finally,
broadband conductivity spectroscopy gives strong evidence for 2D ionic
transport in the LiBH
4
-LiI bulk regions which we observed
over a dynamic range of 8 orders of magnitude. Macroscopic diffusion
coefficients from PFG NMR agree with those estimated from measurements
of ionic conductivity and nuclear spin relaxation. The resulting 3D
ionic transport in nanoconfined LiBH
4
-LiI/Al
2
O
3
is characterized by an activation energy of 0.43 eV.