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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

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