Magnetometric Characterization of Intermediates in the Solid-State Electrochemistry of Redox-Active Metal-Organic Frameworks

Our research interest lies in understanding the electronic and spin states of 2D pi-d conjugated meta organic frameworks and their correlation with their electrochemical behavior of the MOFs in solid state energy storage devices. In the last five years, many new 2D conjugating MOF materials have been reported and studied for their use as active materials in electrochemical cells. However, the mechanism of their charge storage processes is still unclear.

Spectroscopic methods, including x-ray diffraction, x-ray photo electron spectroscopy, and the x-ray absorption fine structure are the mostly common use techniques in this field. Those techniques are crucial for categorizing the specific elements, crystal structure, and oxygen states. It is not possible to separate our 2D MOF from the device while analyzing its electrochemical intermediate state.

Measurement must be taken on a mixture that includes conductive additives and binders. However, to accurately determine the MOF’s electrochemical behavior, it is necessary to calibrate the contribution of these additives. Most spectroscopic methods assume well localized electrons in MOFs, but our protocol provides a physical view and reveals strongly correlated phenomena in these materials.

We’ll continue to better understand the electronic, magnetic, and quantum properties of 2D conjugate MOFs, and bridge the gap between coordination, chemistry, and solid state physics through physical insights. To begin, prepare the copper THQ CB PVDF electrode by dissolving 10 milligrams of PVDF in 1.4 milliliters of NMP. Disperse 50 milligrams of pre-synthesized copper THQ MOF, followed by 40 milligrams of carbon black in the solution and leave it to stir vigorously overnight.

Coat the homogenous slurry onto an aluminum disc of 15 millimeter diameter and approximately 9.7 milligrams mass. Next, assemble the lithium copper THQ coin cells from the bottom to the top, starting with a negative shell, a 0.5 millimeter spacer, lithium, a separator, the prepared copper THQ electrode, a spacer, a spring, and a positive shell. Add a drop of 0.04 milliliters of electrolyte before and after placing the separator.

To prepare the electrochemical intermediates, use a homemade device to compress the coin cell by tightening the screw. Then connect the device to the measuring cables in the glove box. Next, connect the instrument outside the glove box to the ports corresponding to the coin cell.

Finally, perform cyclic voltammetry and galvanostatic charge or discharge measurements to obtain the intermediates at various potentials. After electrochemical cycling, carefully disassemble the coin cell to avoid short circuits, rinse the cycled copper THQ electrode with five milliliters of battery grade dimethyl carbonate, and dry it for 30 minutes at room temperature. Using a clean spatula, transfer the sample from the aluminum disc to aluminum foil.

Transfer the sample powder into a sample tube and seal it tightly with a cap and transparent film, or with a vacuum, until further use. Electrochemical performances of the lithium copper THQ batteries demonstrated that the carbon and binder did not affect the electron transfer, and the battery delivered with a specific capacity of 390 milliampere hours per gram in the first discharge process. Differential capacity analysis of copper THQ CB PVDF electrode demonstrated three electronic states, namely copper state, pi-d conjugated state, and delocalized pi-electron state account for the three redox peaks and cyclic voltammetry curves varied from 4.0 to 1.5 volts.

Connect the sample tube to a rubber tube and seal it with a valve. Then flame the seal head of the sample tube under a vacuum. Set up the ESR spectrometer.

Then insert the prepared sample tube into the microwave cavity and center the sample. Then, to register the ESR of the sample, choose the optimal parameters, such as microwave power, magnetic field sweep time, center field sweep width, modulation frequency and width, and channel amplitude, and time constant. Then sweep the magnetic field and record the ESR spectrum.

Adjust the manganese marker insertion amount to 800 and capture the ESR spectrum with the manganese marker as previously demonstrated. Calibrate the magnetic field using six hyperfine lines for manganese divalent ions. The copper THQ MOF exhibited a broad ESR line.

When copper THQ was reduced to 1.5 volts, the copper ion’s signal disappeared and the radical signal remained, indicating that the ions were reduced to copper. Quantitative ESR measurement confirmed that the copper THQ MOF had 96%copper ions in the paramagnetic state. ESR line width of copper iron narrowed with decreasing temperature, while chemical shift remained constant, indicating significant anti-ferromagnetic interaction.

A significant temperature independent paramagnetic term was observed in ESR spin susceptibility compared to SQUID magnetic susceptibility.