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 ...
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
V.C.2 Interfacial Processes – Diagnostics (LBNL)<br />
Kostecki – LBNL<br />
provide a real-time probe <strong>of</strong> the formation <strong>of</strong> a surface<br />
electrolyte interphase (SEI) on the particle surface during<br />
cycling <strong>of</strong> the electrode.<br />
During the first potential sweep to 5.0 V, a sharp rise<br />
in fluorescence intensity occurred (Figure V - 80) at the<br />
beginning <strong>of</strong> the Ni 2+ oxidation reaction and continued<br />
until the reverse scan caused Ni 4+ reduction. The<br />
fluorescence signal declined after this point until Ni 2+<br />
oxidation during the potential sweep on the second cycle<br />
occurred again. This pattern, repeated for all three cycles<br />
strongly suggests that electrolyte decomposition is<br />
catalyzed by the changes that occur upon Ni oxidation<br />
during the delithiation process. In addition, the loss <strong>of</strong><br />
fluorescence intensity indicates that most <strong>of</strong> these<br />
fluorescent decomposition products either dissolve into the<br />
electrolyte, or decompose to other products right after<br />
formation. However, the rising fluorescence background<br />
intensity demonstrates that some fluorescent species<br />
remained at the particle surface. A similar increase in<br />
fluorescence has also been observed from 1 M LiClO 4 in<br />
EC:DEC electrolyte solutions. Therefore, the fluorescent<br />
species likely originate primarily from decomposition <strong>of</strong><br />
the carbonate-based electrolytes, as opposed to LiPF 6 .<br />
250 Fluorescence Intensity (a.u.)<br />
3e-6<br />
I (A)<br />
2e-6<br />
1e-6<br />
0<br />
-1e-6<br />
-2e-6<br />
-3e-6<br />
200<br />
150<br />
100<br />
50<br />
-4e-6 0<br />
0 10 20 30 40 50<br />
Time (hr)<br />
Figure V - 80: Current (left axis) and fluorescence intensity (right axis) vs. time during three CVs between 3.5 and 5.0 V at 0.05 mV/s.<br />
Transmission FTIR and Raman spectroscopy were<br />
used to probe the structural changes <strong>of</strong> the LMNO spinel<br />
powder (synthesized and provided by Jordi Cabana) after<br />
aging in 1 M LiPF 6 in EC:DEC (1:2 w/w) electrolyte.<br />
Noticeable changes in FTIR spectra after 6 weeks at 55°C<br />
indicate changes in the local structure <strong>of</strong> the crystal. The<br />
Raman spectra <strong>of</strong> the aged LMNO powder suggest the<br />
surface Mn enrichment and possible Ni dissolution<br />
The FTIR spectrum <strong>of</strong> delithiated MNO after one<br />
week at 60°C (Figure V - 79d) appears almost identical to the<br />
fully lithiated sample. Spontaneous relithiation <strong>of</strong> MNO<br />
(and corresponding reduction <strong>of</strong> the active metal) must be<br />
accompanied by electrolyte oxidation at the particle<br />
surface. The increased reactivity <strong>of</strong> LNMO in the charged<br />
state toward the electrolyte and its inability to retain charge<br />
during storage at elevated temperatures, are both critical<br />
issues that must be addressed for this material to be used in<br />
commercial Li-ion batteries.<br />
Our second goal was to investigate the SEI layer<br />
composition on model Sn electrodes to gain insights into<br />
the different electrolyte degradation mechanisms at the<br />
highly reactive Sn (100) surface and the more stable Sn<br />
(001) surface. Preliminary s<strong>of</strong>t X-ray XAS measurements<br />
were performed in the ALS (beam line 8.0.1) on Sn single<br />
crystals with the (100) and (001) orientations after cycling<br />
in EC/DEC 1M LiPF 6 electrolyte. Carbon, oxygen, and<br />
fluorine K-edges were probed with both florescent X-ray<br />
and Auger electron signals, which are proportional to the<br />
X-ray absorption. The surface sensitive Auger electron<br />
signal (escape depth <strong>of</strong> 50Å) indicates different<br />
compositions <strong>of</strong> the surface layers. Observation <strong>of</strong> C π*<br />
and O π* near-edge features at 290 eV and 534 eV<br />
respectively, on Sn (100), are identical to NEXAFS spectra<br />
<strong>of</strong> Li 2 CO 3 . The F K-edge pattern on Sn (001) suggests that<br />
F is in the form <strong>of</strong> LiF within the SEI layer.<br />
Our third objective was to explore the feasibility and<br />
benefits <strong>of</strong> near-field microscopy and spectroscopy<br />
techniques to study interfaces and interphases in Li-ion<br />
systems at subwavelength resolution. Preliminary nearfield<br />
measurements on HOPG model electrodes, Sn anodes<br />
and Li x FePO 4 single particles were carried out using a<br />
near-field spectroscopy instrumentation at JASCO (Japan)<br />
and Neaspec (Germany). The initial results proved to be<br />
extremely encouraging revealing new surface features at<br />
subwavelength resolution, which is unavailable by any<br />
other existing techniques. A similar instrumental setup<br />
from Neaspec will be purchased in October 2011 with<br />
capital equipment funding recently received and will<br />
enable future in-house spectroscopic measurements at the<br />
nanoscale (nanoRaman, i.e. TERS and nano-FTIR) to<br />
characterize cathode and anode structure interfacial<br />
behavior.<br />
Energy Storage R &D 542 FY 2011 Annual Progress Report