Computational Attempts to Approach Magnetism in Metal Organic Frameworks (MOFs)
The approach to magnetic materials with DFT is a challenging task that is often overlooked.
This slides are about our journey to try to model some properties.
linkers: - Tunability - Incorporation of Mt properties - Porousity They are suitable for different applications: - Catalysis - Gas storage/chromatography - drug delivery |
lattice with Cu and Co as metal center, linker: tetrazole-5-carboxylate ethyl ester Structure hexagonal lattice Very stable (Solvent, pH, T) Magnetic properties |
hysteresis suggests FM fraction. Kagome lattice generates frustration but long range order. Co2+, 3 d7 Small hysteresis low T = FM fraction Good fit with Curie-weiss law χmol = C/(T − Θ) AFM ordering Θ = −94K f = Θ/TN = 14.1 |
frustration Cu2+, 3 d9 Small hysteresis low T = FM fraction Good fit with Curie-weiss law χmol = C/(T − Θ) Stronger interaction Θ = −531K f = Θ/TN = 10.2 |
should be trivial, but it is delicate. Goal is MODEL not reality. Issues overlooked: Light elements not detected Different possibilities for oxidation states, H2 O vs OH– Disorder Thermal effects |
it is pretty reasonble: 1. DFT simply works! This is a source of abuse of DFT usage 2. Plenty of cases where DFT is not ideal 3. Our case is about magnetic properties! Issue of Magnetic material: electron are over-delocalized(wrong description of the exchange-kinetic energy component) DFT master recipe to improve results: 1. GGA $ * 2. GGA + U $ *** 3. HYBRIDS $$$ *** |
correction The idea: effective Hubbard parameter system dependent! Performed at a linear response regime UI = ∂EGGA ∂(nIf )2 − ∂EGGA 0 ∂(nIf )2 = χ−1 0 − χ−1 (1) Specific for your system! Physical Review B 71 (3), 035105 |
They d9 configuration results in a different configuration. Even large U parameters can not converge (PhysRevB.84.115108: Ud = 9.79eV , Up = 8.47eV ). Cu-MOF GGA Cu-MOF GGA+U |
to thanks: - Prof. Nachtigall and the whole research group - CUCAM project - EU - European structural and investing funds and the MSMT This Presentation is powered by L A TEX- Beamer Class |