Science - USA (2020-07-10)

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the electrodes by passive layers has been
used to minimize direct electrode-electrolyte
contact ( 13 ), but at the expense of increased
cell resistance. On a chemistry level, the un-
even electron density of the J-T–active TM
ions has been diluted through ionic-doping
and defect introduction strategies ( 7 ). For ex-
maple, the doping strategy can be executed
by incorporating electrochemically inactive,
J-T free Mn4+ in the LiNi1-x-yCoxMnyO 2 series
cathodes and a consequent reduction of an
equivalent amount of Ni3+ to J-T free Ni2+ ( 4 ).
In parallel to the above cathode-level
remedies, other cell-level measures can
also be invoked to limit the extent of the
acid-base reaction. For example, the elec-
trolyte salt anion can be replaced with
bis(trifluoromethane)sulfonimide [TFSI,
(CF 3 SO 2 ) 2 N–], in which the covalent C–F
bonds are not prone to hydrolysis, unlike
the highly polar P–F bonds as in the PF 6 –
anion. Also, apart from the native moisture
present, the anodic decomposition of elec-
trolyte solvents on the cathode at the high
applied charging potentials serves as
a second source of protic species ( 14 ).
Thus, limiting the charging potential,
introduction of additives that can
scavenge the H+ byproduct, increas-
ing the solvent-system anodic decom-
position potential threshold, or de-
creasing the kinetics of such reactions
may all be pursued to achieve the
promise of long–cycle-life recharge-
able batteries.j

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bital to overlap strongly with the four filled
2 p orbitals of the oxide ligand-group in the
equatorial x-y plane, yielding four s-bond-
ing orbitals that are predominantly oxygen
in character. However, the half-filled dz 21
orbital, oriented along the z axis, overlaps
weakly with the two filled 2p orbitals of the
oxide ligand group along the same axis. This
case leads to the formation of a low-energy
axial s-bonding orbital filled with oxide elec-
trons and a high-energy axial s-antibonding
orbital half-filled with the dz 2 single electron.
The longer axial TM–O bonds with a
weaker overlap are more ionic compared to
the shorter, more covalent equatorial TM–O
bonds, resulting in a higher negative charge
on the axial oxygen atoms with a more basic
character from a Lewis acid-base perspec-
tive. Thus, J-T distortion induces higher
reactivity with acid and increased TM-ion
dissolution in LIBs in two ways: It places
an electron into the dz 21 orbital, and the
electron is delocalized over the TM and
O atoms; and it enhances the Lewis-base
strength of the axial oxygens com-
pared to the equatorial oxygens.
Given this background, we can now
address how the presence of acid leads
to metal-ion dissolution in LIBs from
TMOs with J-T ions. The hydrolysis
of the LiPF 6 salt in the electrolytes
of LIBs by residual moisture gener-
ates the strong Lewis acid HF, whose
H+ ions interact exclusively with the
axial oxygens, which are the stronger
Lewis bases, at the cathode-electrolyte
interface (see the second figure, top).
The acid-base interaction may lead
to the formation of H 2 O, through ox-
ide protonation. However, this cannot
happen independently, as the oxygens
in the TMO have less negative charge
compared to the oxygen in H 2 O be-
cause of the higher covalency of TM–O
bonds compared to the H–O bonds.
The formation of H 2 O by the proton-
ation of the TMO oxides requires a net
electron transfer from the TMO to the
axial oxide orbital. This charge trans-
fer originates from the dz 21 orbital of
the TMO that contains the most reac-
tive electron. Thus, protonation of the
axial oxide ion and formation of H 2 O
are accompanied by a simultaneous
metal-to-ligand electron transfer that
leaves the TM with a higher oxidation
state (see the second figure, bottom).
These as-formed TM cations (Mn4+,
Fe5+, and Ni4+) are strong oxidizers that
reduce back directly to the stable, J-T
free state (Mn2+, Fe3+, and Ni2+) through
a two-electron reduction pathway by
oxidizing electrolyte solvent molecules
into CO 2 and other reactive protic spe-

cies ( 8 , 9 ). These stable, lower-valence TM
oxides and fluorides tend to readily dissolve
into the electrolyte. In turn, the as-formed
water molecule can further react with the
LiPF 6 salt to generate more HF, creating a
closed-loop cycle whose net effect is the de-
struction of the electrolyte salt and solvent,
the cathode and the anode.
The problem of proton-induced oxidation
of TMOs extends to various degrees to other
TMOs beyond Mn3+ that contain J-T–active
ions. For example, the oxidation of TM to
higher states under protic environments has
been observed in LiMn3+Mn4+O 2 , LiNi3+O 2 ,
and Na 4 Fe4+O 4 (10–12), where Mn3+, Ni3+,
and Fe4+ are J-T–active ions. Despite the
fundamental reactivity of J-T–active ions,
oxides containing Ni, Fe, and Mn offer the
advantage of abundance and low cost com-
pared to Co, which is beneficial to the mass
production of batteries.
To reduce metal-ion dissolution, current
research efforts are focused on two fronts.
On an engineering level, surface coating of

Acid generation
The hydrolysis of the LiPF 6 salt and generation of HF with the electrolyte
solvent releases Mn2+ ions into the electrolyte.

Nucleophilic attack by the axial oxide on two protons (H+) in the electrolyte
transfers electrons from the dz 21 orbital of the manganese to oxygen. This
process forms water and causes oxidation of the Mn3+ to Mn4+.

Ion dissolution
The partial structure of a J-T–active Mn3+ oxide at the solid surface,
with the highest occupied molecular orbital with appreciable dz 2
character, is shown for one of the TMO 6 units superimposed.

Solvent
oxidation

Solvated
Mn2+

+ + +
PF 6 – H 2 O Li+ H+F– PF 5 LiOH

+2e–

H+

REFERENCES AND NOTES


  1. A. Manthiram, Nat. Commun. 11 , 1550 (2020).

  2. D. Sperling, A. Brown, Long Live
    Batteries (2018); http://www.forbes.com/
    sites/danielsper-ling/2018/08/30/
    long-live-batter-ies/#488060e4e98a.

  3. Advanced Batteries 2016 Annual Progress
    Report (2017); http://www.energy.gov/sites/prod/
    files/2018/03/f49/FY2016_APRAdvanced
    Batteries_R%26D_Part-1of5-opt.pdf.

  4. J. Li, A. Manthiram, Adv. Energy Mater. 9 ,
    1902731 (2019).

  5. C. Zhan et al., Nat. Commun. 4 , 2437 (2013).

  6. D. H. Jang, J. Electrochem. Soc. 143 , 2204
    (1996).

  7. W. Choi, A. Manthiram, J. Electrochem. Soc. 153 ,
    A1760 (2006).

  8. L. Xing, O. Borodin, Phys. Chem. Chem. Phys. 14 ,
    12838 (2012).

  9. A. Wuersig, W. Scheifele, P. Novák, J.
    Electrochem. Soc. 154 , A449 (2007).

  10. J. C. Hunter, J. Solid State Chem. 39 , 142 (1981).

  11. H. Arai, Y. Sakurai, J. Power Sources81–82, 401
    (1999).
    1 2. P. N o v a k et al., Phys. Chem. Chem. Phys. 20 ,
    30247 (2018).

  12. K. T. Lee, S. Jeong, J. Cho, Acc. Chem. Res. 46 ,
    1161 (2013).

  13. N. P. W. Pieczonka et al., J. Phys. Chem. C 117 ,
    15947 (2013).


ACKNOWLEDGMENTS
This work was supported by the Welch Foundation
(grant F-1254).

10.1126/science.abc5454

10 JULY 2020 • VOL 369 ISSUE 6500 141

How electrolytes affect cathodes
The J-T distortion of Mn3+ cations makes it susceptible to dissolution
from acid formed from the electrolyte attacking basic axial oxygens.
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