Linear and non-linear response:phenomenology and calculation with TDDFT

David A. StrubbeDepartment of Physics,

University of California, Merced, USA

Benasque, 21 August 2018

Linear and non-linear optics

Relation to other topics in school:

Background:Gross, fundamentals of TDDFT

Applications (mainly linear, could do nonlinear):Octopus tutorial

More details:Requist, quantum theory of polarizationTancogne-Dejean, Microscopic-macroscopic connectionJornet Somoza, linear response in chemistry

Linear and non-linear optics

Consider only perturbative processes via Taylor expansion of dipole moment. Not high-harmonic generation!

Polarizability (linear optics)

absorption, refraction

Hyperpolarizability: second-harmonic generation (SHG) etc.

Quantized picture

absorption two-photon absorption

second-harmonic generation

refraction

A zoo of nonlinear optical processes

sum-frequency generation (SFG)

difference-frequency generation (DFG)

second-harmonic generation (SHG)

optical rectification

Pockels (electrooptic) effect

third-harmonic generation (THG)

two-photon absorption

four-wave mixing

Energy conservation requires frequency arguments to sum to zero.

Applications of non-linear optics

Characterization in surface science and chemistry (very sensitive)

Optical parametric amplifiers

Pockels cells

Laser pointers

Tunable light sources

Optical logic

coherent anti-Stokes Raman spectroscopy (CARS) (kind of 4-wave mixing)

Two-photon fluorescencent labels in biology

Typically inorganic crystals are used in applications, but organic molecules have the potential to be cheaper and more efficient.

SHG and SFG at the National Ignition FacilityLawrence Livermore National Laboratory, Livermore, California

600 KH2PO4 crystals of 400 kg each, ultrapure to avoid absorption.

192 laser beams for inertial confinement fusion

Total power = 500 TW1053 nm1053 nm1053 nm

527 nm351 nm

The challenges of nonlinear optics: a cautionary tale

The original experimental report of SHG (quartz, 694 nm)

Lesson: check your proofs!

Symmetry properties of nonlinear susceptibility tensorsInversion symmetry: even orders are zero (µ, b, d, etc.).

Apply inversion:

Therefore

surface: breaks symmetry

e.g. Si crystal bulk: no SHG

Symmetry properties of nonlinear susceptibility tensors

Permutation symmetry:

“Kleinman symmetry,” only when off-resonance or

Also Kramers-Kronig relations.

Symmetry properties of susceptibility tensors

Spatial symmetries: e.g. chloroform (CHCl3)

Zincblende structure (e.g. GaAs) has only

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Conventions and units

A. Willetts, J. E. Rice, D. M. Burland, and D. P. Shelton, J. Chem. Phys. 97, 7590 (1992)

Many conventions for pre-factors! Multiple papers on just conventions…

Commonly used units: au, esu

1 au of β= 3.206361×10−53 C3 m3/J2 (SI)= 8.6392×10−33 cm4 statvolt−1 (esu of β)

Nonlinear optics in solidsSusceptibility tensors for solids

Now can have q-dependence as well.

β ~ 10000 au

KTiOPO4 c(2) ~ 10-8 esu

CHCl3 β ~ 1 au, c(2) ~ 10-8 esu

Phase-matching condition for constructive interference:

Adjust angle of incidence to satisfy and get significant conversion.

(NOT momentum conservation; it’s the wavevector in the material)

Molecules vs solids: orders of magnitude.

Other perturbations

Other perturbations: ionic displacement and strain (Raman tensors, Grüneisen parameters, phonon anharmonicity, pyroelectric tensor, piezoelectric tensor, second-order elastic coefficients, …)

S. Baroni, S. de Gironcoli, A. Dal Corso, and P. Gianozzi, Rev. Mod. Phys. 73, 515 (2001)

Representation of electric field in finite and periodic systems:

Quantum theory of polarization

A Dal Corso, F Mauri, and A Rubio, Phys. Rev. B 53, 15638 (1996)

Related to theory of Wannier functions

Solution measurements of hyperpolarizability

(Time-averaged) inversion symmetry of solution makes ordinary measurement give zero.

Electric-field-induced second-harmonic generation (EFISH) is coherent third-order process, based on field lining up molecules.

Hyper-Rayleigh scattering (HRS) is incoherent second-order process, based on orientational fluctuations.

Measurements are usually in solution for molecules. Solvent effects can be strong and complicate comparison between experiment and theory.(In theory, handle via polarizable continuum models or explicit solvent in small clusters or periodic system.)

What is measured directly and often reported:

Solution measurements of hyperpolarizability

Consider projection along dipole moment.

Vertical-vertical and horizontal-vertical polarizations for experiment.

Vibrational / rotational contributions

Many measurements are at l = 1064 nm. For organic molecules, typically:- above vibrational frequencies, so can neglect vibrations- below electronic resonances so little dispersion

D. Bishop, Rev. Mod. Phys. 62, 343 (1990)

Rotational and vibrational contributions can be estimated from simple harmonic models, for low-frequency response (e.g. THz).

E. Roman, J. R. Yates, M. Veithen, D. Vanderbilt, and I. Souza, Phys. Rev. B 74, 245204 (2006)

Z* = Born effective charge

Local-field factors for solvent

+

+

+

+

+

–––––

–––

–

+++

+

Lorentz:

Clausius-Mossotti relations,relate bulk to molecular susceptibilities.

Also generalizations for ellipsoidal cavity, polar solvents.

Theoretical methods for nonlinear response

1. Finite differences (static)

2. Explicit time-propagation

3. Sternheimer equation (2n+1 Theorem)

4. Sum over states (Casida equation)

5. Dyson equation

Finite differencesApply static fields and calculate dipole moment.No need for special capabilities in code.Probably most common method used.Hope static and IR are similar!

F. Vila, D.A. Strubbe, Y. Takimoto, X. Andrade, A. Rubio, S. G. Louie, and J. J. Rehr, J. Chem. Phys. 133, 034111 (2010)

CHCl3

fit or stencil

Convergence is more demanding for nonlinear response

Response extends far from molecule (> 15 a0)

Compare: only 12 a0 converges ground stateall atoms contained within 3 a0 radius

R

F. Vila, D.A. Strubbe, Y. Takimoto, X. Andrade, A. Rubio, S. G. Louie, and J. J. Rehr, J. Chem. Phys. 133, 034111 (2010)

Comparison of Gaussian-type orbitals, SIESTA numerical basis sets, real-space grid: need five-zeta basis sets with diffuse functions, or very long-range real-space grid.

(SIESTA)

(aug-cc-pV5Z)

(h =0.25, r=22)

Explicit time-propagationCannot use “kick” for all frequencies at once (as for linear optics).Must calculate separately for each frequency combination.Scaling is like one ground-state calculation per time step.Incident laser pulses (duration ~ imaginary broadening).

Takimoto, Vila, and Rehr, J. Chem. Phys. 127, 154114 (2007)

p-nitroaniline

Explicit time-propagation

Takimoto, Vila, and Rehr, J. Chem. Phys. 127, 154114 (2007)

Sternheimer equation

aka density-functional perturbation theory (DFPT)Calculate variation of wavefunctions in linear response.No need for unoccupied states.SCF cycle for one frequency at a time

Need small imaginary broadening ih near resonances for numerical stability.

Sternheimer equation: 2n+1 Theorem

Solving nth-order perturbation theory gives 2n+1 derivative of total energy.

X. Gonze and J.-P. Vigneron, Phys. Rev. B 39, 13120 (1989)

n = 0: Hellman-Feynman Theorem. No wavefunction derivatives at all.n = 1: Linear variation of wavefunctions gives quadratic response.

Quantum ESPRESSO and Octopus use equations on previous slide.ABINIT formulation: find b by minimizing with respect to y(1) (variational).

Sternheimer equation: examples from Octopus code

CO SHG

X Andrade, S Botti, MAL Marques, and A Rubio, J. Chem. Phys. 126, 184106 (2007)

H2O optical rectification

CO linear spectrum

Sternheimer equation: examples from Octopus codeEfficient scaling with system size: same as ground state.e.g. comparison of TDLDA vs. CIS with Gaussian basis for vibrating N@C60

G. P. Zhang, D.A. Strubbe, S. G. Louie, and T. F. George, Phys. Rev. A 84, 023837 (2011)

Applicable to any method giving excited-state energies and matrix elements, in particular Casida equation for TDDFT.

(Also other theories such as configuration interaction, coupled cluster, Bethe-Salpeter equation, etc.)

Most commonly used as RPA though: just use Kohn-Sham energies and matrix elements.

Sum over states

Sum over states

Arbitrary (or physical but unknown) imaginary broadenings G.

Convergence in two sums on states is difficult!

Applied occasionally to two-photon absorption in TDDFT.

Y-R Shen, The Principles of Nonlinear Optics

Dyson-like equation

Efficient scheme for solids (for linear and non-linear optics): k-points.Need q->0 limit, equivalent to k.p perturbation theory.

G. Senatore and K. R. Subbaswamy, Phys. Rev. A 35, 2440 (1987)E. Luppi, H. Hübener, and V. Véniard, J. Chem. Phys.132, 241104 (2010)

Complicated macroscopic/microscopic relations…

GaAs SHG

Dyson-like equation

Must converge with respect to unoccupied states in a triple sum.

E. Luppi, H. Hübener, and V. Véniard, Phys. Rev. B 82, 235201 (2010)

Magnetic perturbations

Term in Hamiltonian:

Daniele Varsano, Leonardo A. Espinosa-Leal, Xavier Andrade, Miguel A. L. Marques, Rosa di Felice and Angel Rubio, Phys. Chem. Chem. Phys. 11, 4481 (2009)

~µ⇥ ~B<latexit sha1_base64="UXwNkqFwwcW6O3BpAqw+3i/d2LI=">AAACAXicjVBNS8NAEJ3Ur1q/ol4EL4tF8FQSEfRY6sVjBdsKTSib7aZdursJu5tCCfXiX/HiQRGv/gtv/hu3aQ8qCj4YeLw3w8y8KOVMG8/7cEpLyyura+X1ysbm1vaOu7vX1kmmCG2RhCfqNsKaciZpyzDD6W2qKBYRp51odDnzO2OqNEvkjZmkNBR4IFnMCDZW6rkHwZiSPBDZFAWGCapRITSmPbfq17wC6G9ShQWaPfc96CckE1QawrHWXd9LTZhjZRjhdFoJMk1TTEZ4QLuWSmyXhXnxwRQdW6WP4kTZkgYV6teJHAutJyKynQKbof7pzcTfvG5m4oswZzLNDJVkvijOODIJmsWB+kxRYvjEEkwUs7ciMsQKE2NDq/wvhPZpzfdq/vVZtd5YxFGGQziCE/DhHOpwBU1oAYE7eIAneHbunUfnxXmdt5acxcw+fIPz9gmmjZcA</latexit><latexit sha1_base64="UXwNkqFwwcW6O3BpAqw+3i/d2LI=">AAACAXicjVBNS8NAEJ3Ur1q/ol4EL4tF8FQSEfRY6sVjBdsKTSib7aZdursJu5tCCfXiX/HiQRGv/gtv/hu3aQ8qCj4YeLw3w8y8KOVMG8/7cEpLyyura+X1ysbm1vaOu7vX1kmmCG2RhCfqNsKaciZpyzDD6W2qKBYRp51odDnzO2OqNEvkjZmkNBR4IFnMCDZW6rkHwZiSPBDZFAWGCapRITSmPbfq17wC6G9ShQWaPfc96CckE1QawrHWXd9LTZhjZRjhdFoJMk1TTEZ4QLuWSmyXhXnxwRQdW6WP4kTZkgYV6teJHAutJyKynQKbof7pzcTfvG5m4oswZzLNDJVkvijOODIJmsWB+kxRYvjEEkwUs7ciMsQKE2NDq/wvhPZpzfdq/vVZtd5YxFGGQziCE/DhHOpwBU1oAYE7eIAneHbunUfnxXmdt5acxcw+fIPz9gmmjZcA</latexit><latexit sha1_base64="GASambTtqNrE+veB5VCwy2OmqjU=">AAACAXicdVDLSsNAFJ34rPUVdSO4GSyCq5KIoMtSNy4r2Ac0oUymk3boZBJmbgolxI2/4saFIm79C3f+jdO0BZ8HLhzOuZd77wkSwTU4zoe1tLyyurZe2ihvbm3v7Np7+y0dp4qyJo1FrDoB0UxwyZrAQbBOohiJAsHawehq6rfHTGkey1uYJMyPyEDykFMCRurZh96Y0cyL0hx7wCOmcSHU855dcatOAfw/qaA5Gj373evHNI2YBCqI1l3XScDPiAJOBcvLXqpZQuiIDFjXUEnMMj8rPsjxiVH6OIyVKQm4UL9OZCTSehIFpjMiMNQ/van4l9dNIbz0My6TFJiks0VhKjDEeBoH7nPFKIiJIYQqbm7FdEgUoWBCK5sQnMXLv8kihNZZ1XWq7s15pVafx1FCR+gYnSIXXaAaukYN1EQU3aEH9ISerXvr0XqxXmetS9Z85gB9g/X2CaU3lv0=</latexit><latexit sha1_base64="GASambTtqNrE+veB5VCwy2OmqjU=">AAACAXicdVDLSsNAFJ34rPUVdSO4GSyCq5KIoMtSNy4r2Ac0oUymk3boZBJmbgolxI2/4saFIm79C3f+jdO0BZ8HLhzOuZd77wkSwTU4zoe1tLyyurZe2ihvbm3v7Np7+y0dp4qyJo1FrDoB0UxwyZrAQbBOohiJAsHawehq6rfHTGkey1uYJMyPyEDykFMCRurZh96Y0cyL0hx7wCOmcSHU855dcatOAfw/qaA5Gj373evHNI2YBCqI1l3XScDPiAJOBcvLXqpZQuiIDFjXUEnMMj8rPsjxiVH6OIyVKQm4UL9OZCTSehIFpjMiMNQ/van4l9dNIbz0My6TFJiks0VhKjDEeBoH7nPFKIiJIYQqbm7FdEgUoWBCK5sQnMXLv8kihNZZ1XWq7s15pVafx1FCR+gYnSIXXaAaukYN1EQU3aEH9ISerXvr0XqxXmetS9Z85gB9g/X2CaU3lv0=</latexit><latexit sha1_base64="GASambTtqNrE+veB5VCwy2OmqjU=">AAACAXicdVDLSsNAFJ34rPUVdSO4GSyCq5KIoMtSNy4r2Ac0oUymk3boZBJmbgolxI2/4saFIm79C3f+jdO0BZ8HLhzOuZd77wkSwTU4zoe1tLyyurZe2ihvbm3v7Np7+y0dp4qyJo1FrDoB0UxwyZrAQbBOohiJAsHawehq6rfHTGkey1uYJMyPyEDykFMCRurZh96Y0cyL0hx7wCOmcSHU855dcatOAfw/qaA5Gj373evHNI2YBCqI1l3XScDPiAJOBcvLXqpZQuiIDFjXUEnMMj8rPsjxiVH6OIyVKQm4UL9OZCTSehIFpjMiMNQ/van4l9dNIbz0My6TFJiks0VhKjDEeBoH7nPFKIiJIYQqbm7FdEgUoWBCK5sQnMXLv8kihNZZ1XWq7s15pVafx1FCR+gYnSIXXaAaukYN1EQU3aEH9ISerXvr0XqxXmetS9Z85gB9g/X2CaU3lv0=</latexit><latexit sha1_base64="GASambTtqNrE+veB5VCwy2OmqjU=">AAACAXicdVDLSsNAFJ34rPUVdSO4GSyCq5KIoMtSNy4r2Ac0oUymk3boZBJmbgolxI2/4saFIm79C3f+jdO0BZ8HLhzOuZd77wkSwTU4zoe1tLyyurZe2ihvbm3v7Np7+y0dp4qyJo1FrDoB0UxwyZrAQbBOohiJAsHawehq6rfHTGkey1uYJMyPyEDykFMCRurZh96Y0cyL0hx7wCOmcSHU855dcatOAfw/qaA5Gj373evHNI2YBCqI1l3XScDPiAJOBcvLXqpZQuiIDFjXUEnMMj8rPsjxiVH6OIyVKQm4UL9OZCTSehIFpjMiMNQ/van4l9dNIbz0My6TFJiks0VhKjDEeBoH7nPFKIiJIYQqbm7FdEgUoWBCK5sQnMXLv8kihNZZ1XWq7s15pVafx1FCR+gYnSIXXaAaukYN1EQU3aEH9ISerXvr0XqxXmetS9Z85gB9g/X2CaU3lv0=</latexit>

~µ = ~r ⇥ i~~r<latexit sha1_base64="PfEffYIpKXOE1qCz+zraxC3DXPg=">AAACGHicjVBNS8NAEN34WetX1KOXxSJ4qokIehGKXjxWsB/QhDLZbtulu5uwuymUkJ/hxb/ixYMiXnvz37hNe1BR8MHA470ZZuZFCWfaeN6Hs7S8srq2Xtoob25t7+y6e/tNHaeK0AaJeazaEWjKmaQNwwyn7URREBGnrWh0M/NbY6o0i+W9mSQ0FDCQrM8IGCt13dNgTEkWiDTHV7jgKseBYYJqzHAwjEDN5UBCxCHvuhW/6hXAf5MKWqDedadBLyapoNIQDlp3fC8xYQbKMMJpXg5STRMgIxjQjqUS7OYwKx7L8bFVergfK1vS4EL9OpGB0HoiItspwAz1T28m/uZ1UtO/DDMmk9RQSeaL+inHJsazlHCPKUoMn1gCRDF7KyZDUECMzbL8vxCaZ1Xfq/p355Xa9SKOEjpER+gE+egC1dAtqqMGIugBPaEX9Oo8Os/Om/M+b11yFjMH6Buc6Sefo6Ah</latexit><latexit sha1_base64="PfEffYIpKXOE1qCz+zraxC3DXPg=">AAACGHicjVBNS8NAEN34WetX1KOXxSJ4qokIehGKXjxWsB/QhDLZbtulu5uwuymUkJ/hxb/ixYMiXnvz37hNe1BR8MHA470ZZuZFCWfaeN6Hs7S8srq2Xtoob25t7+y6e/tNHaeK0AaJeazaEWjKmaQNwwyn7URREBGnrWh0M/NbY6o0i+W9mSQ0FDCQrM8IGCt13dNgTEkWiDTHV7jgKseBYYJqzHAwjEDN5UBCxCHvuhW/6hXAf5MKWqDedadBLyapoNIQDlp3fC8xYQbKMMJpXg5STRMgIxjQjqUS7OYwKx7L8bFVergfK1vS4EL9OpGB0HoiItspwAz1T28m/uZ1UtO/DDMmk9RQSeaL+inHJsazlHCPKUoMn1gCRDF7KyZDUECMzbL8vxCaZ1Xfq/p355Xa9SKOEjpER+gE+egC1dAtqqMGIugBPaEX9Oo8Os/Om/M+b11yFjMH6Buc6Sefo6Ah</latexit><latexit sha1_base64="SAAYVGuvLpDpCYnNOeGWP7pzCrk=">AAACGHicdVDLSsNAFJ34rPUVdelmsAiuaiKCboSiG5cV7AOaUG6mk3boZBJmJoUS8hlu/BU3LhRx251/4zRtweeBC4dz7uXee4KEM6Ud58NaWl5ZXVsvbZQ3t7Z3du29/aaKU0log8Q8lu0AFOVM0IZmmtN2IilEAaetYHgz9VsjKhWLxb0eJ9SPoC9YyAhoI3XtU29ESeZFaY6vcMFljj3NIqoww94gADmTPQEBh7xrV9yqUwD/TypojnrXnni9mKQRFZpwUKrjOon2M5CaEU7zspcqmgAZQp92DBVgNvtZ8ViOj43Sw2EsTQmNC/XrRAaRUuMoMJ0R6IH66U3Fv7xOqsNLP2MiSTUVZLYoTDnWMZ6mhHtMUqL52BAgkplbMRmABKJNlmUTgrN4+TdZhNA8q7pO1b07r9Su53GU0CE6QifIRReohm5RHTUQQQ/oCb2gV+vRerberPdZ65I1nzlA32BNPgGeTaAe</latexit><latexit sha1_base64="SAAYVGuvLpDpCYnNOeGWP7pzCrk=">AAACGHicdVDLSsNAFJ34rPUVdelmsAiuaiKCboSiG5cV7AOaUG6mk3boZBJmJoUS8hlu/BU3LhRx251/4zRtweeBC4dz7uXee4KEM6Ud58NaWl5ZXVsvbZQ3t7Z3du29/aaKU0log8Q8lu0AFOVM0IZmmtN2IilEAaetYHgz9VsjKhWLxb0eJ9SPoC9YyAhoI3XtU29ESeZFaY6vcMFljj3NIqoww94gADmTPQEBh7xrV9yqUwD/TypojnrXnni9mKQRFZpwUKrjOon2M5CaEU7zspcqmgAZQp92DBVgNvtZ8ViOj43Sw2EsTQmNC/XrRAaRUuMoMJ0R6IH66U3Fv7xOqsNLP2MiSTUVZLYoTDnWMZ6mhHtMUqL52BAgkplbMRmABKJNlmUTgrN4+TdZhNA8q7pO1b07r9Su53GU0CE6QifIRReohm5RHTUQQQ/oCb2gV+vRerberPdZ65I1nzlA32BNPgGeTaAe</latexit><latexit sha1_base64="SAAYVGuvLpDpCYnNOeGWP7pzCrk=">AAACGHicdVDLSsNAFJ34rPUVdelmsAiuaiKCboSiG5cV7AOaUG6mk3boZBJmJoUS8hlu/BU3LhRx251/4zRtweeBC4dz7uXee4KEM6Ud58NaWl5ZXVsvbZQ3t7Z3du29/aaKU0log8Q8lu0AFOVM0IZmmtN2IilEAaetYHgz9VsjKhWLxb0eJ9SPoC9YyAhoI3XtU29ESeZFaY6vcMFljj3NIqoww94gADmTPQEBh7xrV9yqUwD/TypojnrXnni9mKQRFZpwUKrjOon2M5CaEU7zspcqmgAZQp92DBVgNvtZ8ViOj43Sw2EsTQmNC/XrRAaRUuMoMJ0R6IH66U3Fv7xOqsNLP2MiSTUVZLYoTDnWMZ6mhHtMUqL52BAgkplbMRmABKJNlmUTgrN4+TdZhNA8q7pO1b07r9Su53GU0CE6QifIRReohm5RHTUQQQ/oCb2gV+vRerberPdZ65I1nzlA32BNPgGeTaAe</latexit><latexit sha1_base64="SAAYVGuvLpDpCYnNOeGWP7pzCrk=">AAACGHicdVDLSsNAFJ34rPUVdelmsAiuaiKCboSiG5cV7AOaUG6mk3boZBJmJoUS8hlu/BU3LhRx251/4zRtweeBC4dz7uXee4KEM6Ud58NaWl5ZXVsvbZQ3t7Z3du29/aaKU0log8Q8lu0AFOVM0IZmmtN2IilEAaetYHgz9VsjKhWLxb0eJ9SPoC9YyAhoI3XtU29ESeZFaY6vcMFljj3NIqoww94gADmTPQEBh7xrV9yqUwD/TypojnrXnni9mKQRFZpwUKrjOon2M5CaEU7zspcqmgAZQp92DBVgNvtZ8ViOj43Sw2EsTQmNC/XrRAaRUuMoMJ0R6IH66U3Fv7xOqsNLP2MiSTUVZLYoTDnWMZ6mhHtMUqL52BAgkplbMRmABKJNlmUTgrN4+TdZhNA8q7pO1b07r9Su53GU0CE6QifIRReohm5RHTUQQQ/oCb2gV+vRerberPdZ65I1nzlA32BNPgGeTaAe</latexit>

Perturbation:

↵⌫µ,� =@↵⌫µ

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Quantity of interest (circular dichroism):

Gauge issue with A and non-local pseudopotentials.

Can use Sternheimer or real-time

Magnetic perturbations in solids

Vector potential can be expressed in different gauges.

Separate wavefunction into gauge-dependent and gauge-independent parts.E and B fields as in quantum theory of polarization.Sternheimer equation for response.Carefully combine parts into gauge-independent quantity.

IV Lebedeva, DA Strubbe, IV Tokatly, and A Rubio, arxiV:1806.09886 (2018)

~B = ~r⇥ ~A<latexit sha1_base64="n0ObZVpWdIyf77TqGjd6bT3yiW4=">AAACDnicjVBNS8NAEN34WetX1KOXxVLwVBIR9CLUevFYwX5AE8pku2mXbjZhd1MoIb/Ai3/FiwdFvHr25r9xm/agouCDgcd7M8zMCxLOlHacD2tpeWV1bb20Ud7c2t7Ztff22ypOJaEtEvNYdgNQlDNBW5ppTruJpBAFnHaC8dXM70yoVCwWt3qaUD+CoWAhI6CN1Ler3oSSrJHjC1wwT0DAIceeZhFVc+0y79sVt+YUwH+TClqg2bffvUFM0ogKTTgo1XOdRPsZSM0Ip3nZSxVNgIxhSHuGCjDL/Kx4J8dVowxwGEtTQuNC/TqRQaTUNApMZwR6pH56M/E3r5fq8NzPmEhSTQWZLwpTjnWMZ9ngAZOUaD41BIhk5lZMRiCBaJNg+X8htE9qrlNzb04r9cYijhI6REfoGLnoDNXRNWqiFiLoDj2gJ/Rs3VuP1ov1Om9dshYzB+gbrLdPxnyb7g==</latexit><latexit 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~E = �1

c

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Ramanspectroscopy

34

phononcreation

Lightcreates(ordestroys)vibrationsthroughexcitedstates

Ramantensorfrompolarizabilityderivativewithrespecttoatomicpositions

staticlinear-responsecalculationofRamantensorsM.Lazzeri andF.Mauri,Phys.Rev.Lett. 90,036401(2003)

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resonant Raman: need optical method, e.g. TDDFT or Bethe-Salpeter eqn.non-resonant: can make static approximation

Some references on linear and nonlinear response

DA Strubbe, L Lehtovaara, A Rubio, MAL Marques, and SG Louie, “Response functions in TDDFT: concepts and implementation,” in Fundamentals of Time-dependent density-functional theory (ch. 7) and references therein.

Yuen-Ron Shen, The Principles of Nonlinear Optics (Wiley 1984 / 2002).

P. N. Butcher and D. Cotter, The Elements of Nonlinear Optics (Cambridge University Press, 1990).