V. Focused Fundamental Research - EERE - U.S. Department of ...
V. Focused Fundamental Research - EERE - U.S. Department of ...
V. Focused Fundamental Research - EERE - U.S. Department of ...
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Thackeray – ANL<br />
V.F.1 Energy Frontier <strong>Research</strong> Center at ANL (ANL)<br />
Li 2 MnO 3 precursor, and improving their structural stability<br />
over long-term cycling.<br />
Figure V - 216 shows the first charge/discharge curve<br />
between 4.6 and 2.0 V (15 mA/g) for a LNP-treated<br />
LCMO electrode. The numbered points along the curves<br />
indicate predetermined states <strong>of</strong> charge at which cells were<br />
prepared for the XAS measurements. Point 1 represents the<br />
fresh, uncharged electrode, point 2 (at ~4.3 V) corresponds<br />
to the extraction <strong>of</strong> ~90 mAh/g capacity, and point 3<br />
represents a fully charged electrode at 4.6 V corresponding<br />
to the full ~280 mAh/g practical capacity <strong>of</strong> the electrode.<br />
Point 4 represents a fully discharged electrode at 2.0 V<br />
after one complete cycle.<br />
Cell Voltage (V)<br />
5<br />
4<br />
3<br />
2<br />
1<br />
2<br />
0 30 60 90 120 150 180 210 240 270 300<br />
Capacity (mAh/g)<br />
Figure V - 216: Charge/discharge curve between 4.6 and 2.0 V (15 mA/g)<br />
for LNP-treated LCMO electrodes. Numbered points indicate predetermined<br />
states <strong>of</strong> charge at which cells were prepared for XAS measurements.<br />
In general, the results obtained at all points <strong>of</strong> charge<br />
for the Mn (not shown) and Co K-edges agree well with<br />
those reported elsewhere for manganese and cobalt in<br />
similar systems. Attention was focused on the dilute<br />
element <strong>of</strong> interest, namely nickel, as introduced by way <strong>of</strong><br />
surface treatment on LCMO. However, several<br />
observations are worth noting. For example, from the<br />
XANES data in Figure V - 217a, it can be observed that the<br />
cobalt environment in the parent LNP-treated LCMO<br />
electrode (point 1, Figure V - 216) is identical to the Co<br />
environment in the untreated LCMO sample; both spectra<br />
overlap and are similar to Co 3+ in LiCoO 2 , again revealing<br />
the composite nature <strong>of</strong> the material. This observation<br />
reveals that the LNP treatment has little effect on the Corich<br />
regions <strong>of</strong> the composite material.<br />
However, from the Fourier transformed Mn K-edge<br />
data in Figure V - 217b, in which Li 2 MnO 3 is used as a<br />
reference, it can be seen that the local environment <strong>of</strong><br />
manganese in the LNP-treated LCMO has undergone<br />
slight modifications with respect to that <strong>of</strong> manganese in<br />
the parent LCMO. Both LCMO and LNP-treated LCMO<br />
samples show increased amplitudes in the second-shell<br />
Mn-M correlations at ~2.5 Å with respect to pure<br />
Li 2 MnO 3 . For LCMO, this is attributed to contact between<br />
4<br />
3<br />
the boundaries <strong>of</strong> the LiCoO 2 - and Li 2 MnO 3 -like domains,<br />
in agreement with Bareno et al. For LNP-treated LCMO,<br />
even higher amplitudes for the Mn-M correlation are<br />
observed. This result is attributed to the insertion <strong>of</strong> nickel<br />
into the transition metal layers <strong>of</strong> the Li 2 MnO 3 -like<br />
domains in the 0.5Li 2 MnO 3 •0.5LiCoO 2 composite<br />
structure as described in more detail below.<br />
Normalized Intensity (a.u.)<br />
FT magnitude (a.u.)<br />
1.8<br />
1.6<br />
1.4<br />
1.2<br />
1.0<br />
0.8<br />
point 1<br />
0.6<br />
point 2<br />
0.4<br />
Co K<br />
point 3<br />
point 4<br />
0.2<br />
LCMO<br />
0.0<br />
7705 7710 7715 7720 7725 7730 7735 7740<br />
15<br />
10<br />
5<br />
Normalized Intensity (a.u.)<br />
0.08<br />
0.07<br />
0.06<br />
0.05<br />
0.04<br />
point 1<br />
0.03<br />
point 2<br />
0.02<br />
point 3<br />
point 4<br />
0.01<br />
7704 7706 7708 7710 7712 7714<br />
(b)<br />
Energy (eV)<br />
Mn-O<br />
Energy (eV)<br />
Mn-M<br />
(a)<br />
Mn K<br />
Li 2<br />
MnO 3<br />
LCMO<br />
LCMO/LNP<br />
0<br />
0 1 2 3 4 5 6 7 8<br />
R (Å)<br />
Figure V - 217: (a) Co K-edge XANES showing LNP-treated LCMO at all<br />
points <strong>of</strong> charge in Figure V - 216 and untreated LCMO. The inset in (a)<br />
shows a magnified view <strong>of</strong> the Co K pre-edge region for all points <strong>of</strong> charge.<br />
(b) Magnitude <strong>of</strong> the Fourier transformed Mn K-edge data for LNP-treated<br />
LCMO, untreated LCMO, and a Li2MnO3 reference.<br />
Figure V - 218a shows the Ni K-edge XANES data <strong>of</strong> the<br />
LNP-treated LCMO electrode at points 1 and 4 in the<br />
electrochemical data (Figure V - 216) relative to a Ni 2+<br />
reference, 0.5Li 2 MnO 3 •0.5LiMn 0.5 Ni 0.5 O 2 (alternatively,<br />
Li 1.2 Mn 0.6 Ni 0.2 O 2 ). The excellent overlap <strong>of</strong> all three<br />
spectra indicates that the nickel ions are predominantly<br />
divalent in the uncharged electrode as well as after one<br />
complete cycle. Figure V - 218b shows the Ni K-edge XANES<br />
data <strong>of</strong> the LNP-treated LCMO electrodes at points 1, 2<br />
and 3 <strong>of</strong> Figure V - 216 relative to Ni 3+ (LiNi 0.8 Co 0.2 O 2 ) and<br />
Ni 4+ (LiNi 0.8 Co 0.2 O 2 charged to 5.2 V) references. At a<br />
relatively early stage <strong>of</strong> charge, point 2 (4.3 V), the nickel<br />
ions reach an oxidation state <strong>of</strong> ~3+. This finding is<br />
significant because it would be expected that a lithium-<br />
FY 2011 Annual Progress Report 663 Energy Storage R&D