Abstract
An electrochemical cell based on the reversible oxygen reduction reaction (ORR), 2Li+ + 2e− + O2 ↔ Li2O2, provides among the most energy dense platform for portable electrical energy storage. Such lithium-oxygen (Li-O2) cells offer theoretical specific energies competitive with fossil fuels and have long been considered an important storage technology for enabling electrified transportation. Multiple, fundamental challenges with the cathode, anode, and electrolyte have limited practical interest in Li-O2 cells because these fundamental problems lead to practical shortcomings, including poor rechargeability, high overpotentials, and specific energies well below theoretical expectations. We create and study in situ formation of solid electrolyte interphases (SEIs) based on bromide ionomers tethered to the Li anode that take advantage of three powerful, fundamental processes for overcoming the most stubborn of these challenges. Formed in situ, the ionomer SEIs are specifically shown to exhibit three attributes required for stable Li-O2 cell operation. First, they protect the Li anode against parasitic reactions and also stabilize Li electrodeposition during cell recharge. Second, bromine species liberated during the anchoring reaction function as a redox mediator for the recharge reaction at the cathode, reducing the charge overpotential. Finally, the ionomer SEI form an exceptionally stable interphase with Li, which is shown to protect the metal in high Gutmann donor number liquid electrolytes. Such electrolytes have been reported to exhibit rare stability against nucleophilic attack by Li2O2 and other cathode reaction intermediates but are known for their reactivity with Li metal anodes. We conclude that rationally designed SEIs able to regulate transport of matter and ions at the electrolyte/anode interface provide a highly promising materials platform for addressing the major barriers to practical Li-O2 storage technology.
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Appendix: Supplementary Information
Appendix: Supplementary Information
8.1.1 Experimental
8.1.1.1 Li-O2 Battery Methods and Materials
8.1.1.1.1 Cathode Preparation
A cathode slurry was prepared by mixing 180 mg of Super P carbon (TIMCAL), 20 mg of polyvinylidene fluoride (PVDF; Aldrich), and 2000 mg of N-Methyl-2-pyrrolidone (NMP; Aldrich) in a ball mill at 50 Hz for 1 h. Toray TGP-H-030 carbon paper was coated with an 80 μm thick layer of carbon slurry using a doctor blade. The resulting coated carbon paper was dried at 100 °C overnight under vacuum and transferred into an argon-filled glovebox (O2 < 0.2 ppm, H2O < 1.0 ppm; Innovative Technology) without exposure to air. 5/8-inch diameter disks were punched and weighed from the carbon paper to yield individual carbon cathodes. The weight of the active carbon layer (not including the carbon paper) averaged 1.0 mg ± 0.1 mg.
8.1.1.1.2 Electrolyte Preparation
LiNO3 and LiTFSI were heated under vacuum overnight at 100 °C to remove all traces of water and transferred directly into the glovebox. N,N-dimethylacetamide (DMA; Aldrich) and bis(2-methoxyethyl) ether (diglyme; Aldrich) solvents were dried over 3 Å molecular sieves (Aldrich). Lithium 2-bromoethanesulfonate was obtained through ion exchange with sodium 2-bromoethanesulfonate (Aldrich).
8.1.1.1.3 Coin Cell Assembly
First, a 1/2-inch (12.7 mm) diameter hole was punched in the top (cathode) side of each CR2032 case. Then, a stainless steel wire cloth disk, 3/4-inch (19 mm) disk diameter, and 0.0055-inch (0.140 mm) wire diameter from McMaster-Carr were added, followed by a cathode disk, ¾-inch diameter separator (either Whatman GF/D glass fiber or Celgard 3501), 100 μL of desired electrolyte, ½-inch diameter lithium metal, 15.5 mm diameter stainless steel spacer disk, stainless steel wave spring (MTI Corporation), and anode cap of the CR2032 case. The assembly was crimped to a pressure of 14 MPa with a hydraulic coin cell crimple (BT Innovations).
8.1.1.1.4 Testing Environment
Cells were tested at a regulated pure O2 environment of 1.3 atm and allowed to equilibrate for 6 h prior to electrochemical testing. Galvanostatic measurements were conducted using a Neware CT-3008 battery tester.
8.1.1.1.5 Cyclic Voltammetry
The cyclic voltammetry test was done in a two-electrode setup of Li||air cathode. The batteries were cycled between 1.9 V and 4.5 V at a scan rate of 1 mV/sec several times.
8.1.1.2 Anode Stability Methods and Materials
8.1.1.2.1 Impedance Spectroscopy
Cells in the symmetric configuration were assembled in an Ar glovebox. Measurements were done using a Solatron frequency analyzer at a frequency range of 10−3 to 107 Hz. The data was fitted into Nyquist-type plots using the equivalent circuit shown in Supplementary Fig. 10.2 with the software zsimpwin. Impedance was conducted at room temperature at various time intervals.
8.1.1.2.2 Linear Scan Voltammetry
Linear scan voltammetry was done in a Li||SS cell. The batteries were first swept to −0.2 V vs. Li/Li+; then they were swept in reverse direction until the voltage diverges.
8.1.1.2.3 Lithium Versus Stainless Steel Cycling
For cycling tests, lithium vs. stainless steel cells were prepared and were cycled at 0.01 mA/cm2 between 0 and 0.5 V ten times in order to form a stable SEI layer. Then different tests were done as given in the manuscript.
8.1.1.3 Characterization Techniques
8.1.1.3.1 Scanning Electron Microscopy and EDAX
Discharged cells were disassembled inside the glovebox, and the cathodes were removed and transported to the scanning electron microscope (Zeiss LEO 1550 Field Emission SEM) within an airtight container. The cathodes were loaded onto the stage in the presence of a nitrogen stream. Images were taken with a single pass after focusing on a nearby region. EDAX measurements were done by taking multiple counts on a small section of sample.
8.1.1.3.2 X-Ray Diffraction
Cathodes were mounted on a glass microscope slide inside an argon-filled glovebox and coated with paraffin oil to protect them from air during the X-ray diffraction (XRD) measurements. Measurements were done on a Scintag Theta-Theta X-ray diffractometer using Cu K-α radiation at λ = 1.5406 Å and fitted with a 2-dimensional detector. Frames were captured with an exposure time of 10 min, after which they were integrated along χ (the polar angle orthogonal to 2θ to yield an intensity) vs. 2θ plot.
8.1.1.3.3 X-Ray Photoelectron Spectroscopy
XPS was conducted surface science instruments SSX-100 with operating pressure of ~ 2 × 10−9 torr. Monochromatic Al K-α X-rays (1486.6 eV) with beam diameter of 1 mm were used. Photoelectrons were collected at an emission angle of 55°. A hemispherical analyzer determined electron kinetic energy, using a pass energy of 150 V for wide survey scans and 50 V for high-resolution scans. Samples were ion-etched using 4 kV Ar ions, which were rastered over an area of 2.25 × 4 mm with total ion beam current of 2 mA, to remove adventitious carbon. Spectra were referenced to adventitious C 1s at 284.5 eV. CasaXPS software was used for XPS data analysis with Shelby backgrounds. Li 1s and O 1s were assigned to single peaks for each bond, whereas Br 3d was assigned to double peaks (3d5/2 and 3d3/2) for each bond with 1.05 eV separation. Residual SD was maintained close to 1.0 for the calculated fits. Samples were exposed to air only during the short transfer time to the XPS chamber (less than 5 s).
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Choudhury, S. (2019). Designer Interphases for the Lithium-Oxygen Electrochemical Cell. In: Rational Design of Nanostructured Polymer Electrolytes and Solid–Liquid Interphases for Lithium Batteries. Springer Theses. Springer, Cham. https://doi.org/10.1007/978-3-030-28943-0_8
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