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FIRESIDE CHATS FOR LOCKDOWN TIMES The frontiers and the challenges (Part 3) Nicola Marzari, EPFL OUTLINE What is density-functional theory? (Part I) What does it take to perform these calculations? (Part II) Why is it relevant for


  1. FIRESIDE CHATS FOR LOCKDOWN TIMES The frontiers and the challenges (Part 3) Nicola Marzari, EPFL

  2. OUTLINE • What is density-functional theory? (Part I) • What does it take to perform these calculations? (Part II) • Why is it relevant for science and technology? (Part III) • What can it do? and cannot do? (Part III) (to keep in touch, info in the Learn section of the Materials Cloud website, and https://bit.ly/3eqighg) April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  3. WHAT CAN I DO WITH IT? • Which properties are “ ground state ” properties ? • How accurate are we? • What is the microscopic origin of the observed behavior ? • How can we be realistic? (introduce the effects of temperature, pressure, composition; study non- periodic systems such as liquids; go from a few atoms to many) April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  4. EXAMPLES • From total energy to thermodynamics – temperature, pressure, chemical potentials and partial pressures, electrochemical potential, pH • From DFT to real electrons – many-body perturbation theory – quantum Monte Carlo – DMFT, cluster DMFT, DCA April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  5. Examples • Length, time, phase and composition sampling – linear scaling, multiscale, – metadynamics, sketch-map – minima hopping, random-structure searches • Complex properties – phase diagrams – spectroscopies and microscopies: IR, Raman, XPS, XANES, NMR, EPR, ARPES, STM, TEM… – transport: ballistic, Keldysh, Boltzmann April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  6. Easy: equilibrium volume Eric B. Isaacs and Chris Wolverton, Phys. Rev. Materials 2, 06380 (2018) April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  7. Difficult: formation energies Eric B. Isaacs and Chris Wolverton, Phys. Rev. Materials 2, 06380 (2018) April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  8. Out-of-bounds: (transport) band gaps Eric B. Isaacs and Chris Wolverton, Phys. Rev. Materials 2, 06380 (2018) April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  9. Think beyond the energy Hellmann-Feynman Theorem dE d l April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  10. Helmann-Feynman theorem April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  11. Linear-response theory dE d l S. Baroni et al. , Phys. Rev. Lett. (’87), Rev. Mod. Phys (‘01) April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  12. Linear-response theory S. Baroni et al. , Phys. Rev. Lett. (’87), Rev. Mod. Phys (‘01) April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  13. Phonons and temperature • A harmonic crystal is exactly equivalent to a Bose- Einstein gas of independent, harmonic oscillators. April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL) • .

  14. Vibrational spectroscopies: IR, Raman April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  15. Magnetic spectroscopies: NMR Chemical Shifts Mauri 2001 April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  16. Sampling excitations Electronic Ψ Ψ Occupation Magnetic (electron spin) Vibrational Configurational In polymers and bio-molecules, vibrational and Conformational configurational can not always be distinguished

  17. Statistical mechanics on relevant degrees of freedom Collection of microscopic states consistent with thermodynamic Ensemble boundary conditions [ ] exp − β E i Probability to be in a given state i i = P Q [ ] ∑ Q = exp − β E i Partition Function i F = − β ln[ Q ] Free energy (Helmholtz) ∑ S = − k B P i ln( P i ) Entropy i April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  18. For the vibrational free energy, analytically! April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  19. Thermomechanics (bulk modulus of diamond) April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  20. Otherwise, thermodynamical averages Under hypothesis of ergodicity, we can assume that the temporal average along a trajectory is equal to the ensemble-average over the phase space ! ! ò - b A exp( E ) d r d p = A ! ! ò - b exp( E ) d r d p T 1 ò = A A ( t ) dt T 0 April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  21. Molecular dynamics ! m d 2  r ( t )   r F (  ∇ V (  dt 2 = r ) = − r ) ! v ( t ) April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  22. A drop to drink Bingqing Cheng, Edgar A. Engel, Jörg Behler, Christoph Dellago, Michele Ceriotti, PNAS 116 1110 (2019) April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  23. April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  24. We’ll always have Monte Carlo ! ! ò - b A exp( E ) d r d p = A ! ! ò - b exp( E ) d r d p Metropolis algorithm (by Arianna and Marshall Rosenbluth) i → j = 1 when E j < E i P i → j = exp( − β ( E j − E i )) when E j > E i P redrawn from the book by D. Frenkel and B. Smith, Understanding Molecular Simulation Academic Press Downhill moves always accepted, uphill moves with some “ thermal-like ” probability April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  25. Thermodynamics of substitutional alloys April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  26. Free energy from thermodynamic integration of the dependence of the chemical potential Nicola Marzari, Stefano de Gironcoli, and Stefano Baroni, Phys. Rev. Lett. 72, 4001 April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  27. Multi-scale, multi physics: semiclassical transport 1. Vibrational properties from density-functional theory, electrons from many-body perturbation theory 2. Carriers’ scattering rates from density-functional perturbation theory 3. Wannier interpolations for electrons 4. Transport properties from Boltzmann’s equation April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  28. Resistivity in doped graphene FIRST-PRINCIPLES EXPTS (Efetov and Kim) C.-H. Park et al., Nano Letters (2014) T. Y. Kim, C.-H. Park, and N. Marzari, Nano Letters (2016)

  29. Anharmonicity = finite lifetimes April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  30. Thermal conductivity (SMRTA) ∑ ! 2 _ _ 2 ( q ) ω 2 ( qs ) n qs K = + 1) τ qs c s ( n qs 3 N 0 Ω k B T 2 qs Transverse modes Transverse modes Acoustic Acoustic Optical Optical April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  31. Composition dependence in SiGe alloys J. Garg, N. Bonini, B. Kozinsky and N. Marzari, Phys. Rev. Lett. (2011) April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  32. Generalized Wigner Boltzmann Simoncelli, Marzari, Mauri, Nature Physics (2019) Total K = Peierls + coherences

  33. April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  34. A FUN EXAMPLE G. Prandini, G.M. Rignanese, and N. Marzari, npj Computational Materials 5, 129 (2019) April 2020 - Fireside chats for lockdown times: The frontiers and the challenges (Part 3 of 3) - Nicola Marzari (EPFL)

  35. Multi-scale/physics: electrochemistry permittivity isosurfaces (b) di ff use ion distribution E 0 V λ H = 3–5 ˚ A Dabo, Bonnet, Li and Marzari, "Ab-initio Electrochemical Properties of Electrode Surfaces" , in Fuel Cell Science: Theory, Fundamentals and Bio-Catalysis, A. Wiecowski and J. Norskov (2011). O. Andreussi, I. Dabo and N. Marzari, “Revised self-consistent continuum solvation in electronic structure calculations”, J. Chem. Phys. 136, 064102 (2012). www.quantum-environment.org

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