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Many-body Green functions theory for electronic and optical
properties of organic systems(are physicists any good at chemistry?)
Claudio AttaccaliteCNRS/CINAM Campus de Luminy, Case
913 13288 Marseille , France
Excited States Bridging Scales, Marseille, November 7-10 (2016)
Outline
● From the Green’s mill to modern computer codes
● From solids to molecules
● The future…..
Outline
● From the Green’s mill to modern computer codes
● From solids to molecules
● The future…..
What do electrons in solids?
Direct and inverse photoemission
Electrons moves in bands that correspond to the
energy to remove or add one electron
How to calculate band-structures?Problems with DFT (and HF)
The KohnSham eigensystems do not represent the real bands of a solid even if we know the exact Vxc
● Band width too large for metals● Band gaps too small● In materials with d or f orbitals, the Density of States is in disagreement with experiments
● Metalinsulator transition not described● The magnetic moments in the transition metal oxides are systematically underestimated
● Etc...
Green functions Let's "watch" the propagation of an added electron
Green’s function
|ψ0N ⟩ ψ+(r , t)| ψ0
N ⟩ ψ(r ' , t ') ψ+ (r , t)| ψ0N ⟩
● Probability amplitude for propagation of additional electron from (r,t) to (r',t') in a many electron system.
● Generalization of the density matrix (r,r’,t) where fields operators have different times.
iG (r ' , t ' ; r , t)=⟨ψ0N| ψ(r ' , t ' )ψ+
(r ,t )| ψ0N ⟩θ( t '−t)
Ref: Quantum Statistics of Nonideal Plasmas, D. Kremp, M. Schlanges and W. D. Kraeft
Which information iscontained in the Green function?
G(r ' ,r ;ω)=∑s
ψN+1(r ´ )[ ψN+1
(r )]∗
ω−ϵsN+1+iη
+∑s
ψN−1(r ´ )[ ψN−1
(r )]∗
ω−ϵsN+1−iη
By Fourier transform and some mathematics….
Poles of Green's function give energies for addition/removing an electron, charged excitations (including ionization energy and electron affinities in molecules)
ρ(r ' , r )=−iG (r ' , r ; t→0 ⁺ )
The t=0 limit is the density matrix!The t=0 limit is the density matrix!
How to calculate Green functions
From the EOM of the annihilation field operator:
Historical note:Green’s functions were originally introduced by the British (miller and) mathematical physicist George Green in the context of the theory of electricity and magnetism. Nowadays, all functions satisfying an inhomogeneous integraldifferential equation with a Dirac delta function as source term are called Green functions.
i∂t ψ(r , t)=[ψ(r ,t ), H ]
We obtain a infinite hierarchy of nparticle Green’s functions similar to the ones of density matrix:
h(1)G(1 ;1' )−i∫ d 2V (1,2)G(1,2 ;1 ' ,2+)=δ(1−1 ' )
G2
G1
G3
Gn
G4
This equations can be closed by introducinga single particle operator
nonlocal in space and time, that includecorrelation effects
G=G0+G0 Σ(G)G
Martin-Schwinger Tower
can be calculated by perturbation theory
Problem with metals and the electron-gas ...
Ref: ManyBody Quantum Theory in Condensed Matter Physics: An Introduction, H. Bruus and K. Flensberg
e
e e
e
e
e
ee
Metal Electron gas
Lets use perturbation theory to improve DFT/HF and calculate the Green functions
Problem with metals and the electron-gas ...
Ref: ManyBody Quantum Theory in Condensed Matter Physics: An Introduction, H. Bruus and K. Flensberg
Lets use perturbation theory to improve DFT/HF and calculate the Green functions
It diverges!!
It diverges!!
e
e e
e
e
e
ee
Metal Electron gas
How to solve the problem of divergences
We solved this problem many years ago
…. condensed matter physicists discussed with their cousins particle physicists ……...
Sums an infinite series of perturbation terms in such a way to create a screened interaction W, and then start again perturbation theory in W
Self-energy in terms of a screened interaction
Ref: The GW method F. Aryasetiawan, and O. Gunnarsson, Reports on Progress in Physics, 61(3), 237. (1998)
Where G is the single particle electronic Green's function and W is the screened electronelectron interaction
All correlation effects are included in the selfenergy operator the we approximate as:
Putting together Green’s function and perturbation theory in terms of a screened Coulomb interaction we get the quasiparticle formalism. Namely the mapping of the
true manybody problem onto a single effective singleparticle framework:
Many-body perturbation theory(GW approximation)
Mean-field approaches(DFT, Hartree-Fock, etc.)
Response functionsFrom the derivatives of the Green’s function respect to an external field U
it is possible to calculate the response functions:
Li , j , k ,l=∂ρi , j
∂U k ,l
=−i∂Gi , j
∂U k , l
L=L0+L0[ v+∂Σ/∂G L]L
The BetheSalpeter Equation (BSE)
Similar to TDDFT Cassida equation
χ=χ0+χ0[ v+f xc ] χ
But does not depend from any functional and naturally include exchange effects
h ν
+
-
Ref: G. Strinati, Rivista del Nuovo Cimento 1, 11, (1988)
A sleeping beautyManyBody Perturbation Theory within the GW approximation
for the electron gas was presented by Hedin in
New method for calculating the oneparticle Green's function with application to the electrongas problem. L. Hedin, Physical Review, 139, A796 (1965)
(from the abstract: … there is not much new in principle in this paper. ….)
However, we had to wait until 1980 for the first application to semiconductors
by Hanke, Sham, Strinati and Mattausch
Modern implementation of GW by Hybertsen and Louie (1986)
Modern implementation of BSE by Onida et al. (1995)
Some results
Band gaps Optical excitations
G. Onida, L. Reining, and A. Rubio, RMP 74 (2002).
Outline
● From the Green’s mill to modern computer codes
● From solids to molecules
● The future…..
FIESTA and friends
Other implementations using localized orbitals:1) MOLGW (free): http://www.molgw.org/ 2) TurboMole: http://www.turbomole.com/ 3) FHI: https://aimsclub.fhiberlin.mpg.de/ 4) SIESTA: https://arxiv.org/abs/1105.3360
French Initiative for Electronic Simulations with Thousands of Atoms
[http://perso.neel.cnrs.fr/xavier.blase/fiesta/]
Implementation of GW equations and response functions (BetheSalpeter equation) using a gaussian basis set
The ab-initio zoo: from mean-field to many-body perturbation theory
Ab-initio formalisms are not all equivalent and there is still “some work” towards reliable and cheap enough approaches able to tackle complex systems.X. Blase, V. Olevano and C. Attaccalite PRB 83, 115105 (2011)
Mean-field approaches(DFT, Hartree-Fock, etc.)
The « exact » many-body problem(QMC, CI, coupled-cluster, etc.)
Many-body perturbation theory(GW, Bethe-Salpeter, etc.)
HOMO-LUMO gap of molecules of interest for organic electronics or photovoltaics
Beyond the scissor operator: level ordering and spacing below the gap
HOMO to (HOMO-3) in cytosine
LDA GW CASPT2 EOM-IP-CCSD
σO + π
ππ
HOMO 6.167 (σO) 8.73 (π) 8.73/8.76 (π) 8.78 (π) 8.8-9.0
HOMO-1 6.172 (π) 9.52 (π’) 9.42/ - (σO) 9.55 (π’) 9.45-9.55
HOMO-2 6.81 (σ) 9.89 (σO) 9.49/ - (π’) 9.65 (σO) 9.89
LDA evGW CASPT2/CCSD(T) EOMIPCCSD Exp.
π
σO
σO
σO
σ
π’π’
π’-3.72 eV
(Faber, Attaccalite, Olevano, Runge, Blase, PRB 2011)
(DNA nucleobases)
Bethe-Salpeter equations (BSE) for excitonic interactions: comparison to experiment !
BNL = Range-separated hybrid functional
(Stein, Kronik, Baer, JACS 2009)
TDDFT hybrid
Acceptor = TCNE (tetracyanoethylene)Donor = benzene, toluene, o-xylene and naphtalene
(Blase, Attaccalite, APL, 2011)
See also our competitors: Garcia-Lastra and Thygesen, PRL (2011); Baumeier, Andrienko, Rohlfing, JCTC (2012);
F. Bruneval et al. Comp. Phys. Comm. (2016)
A very simple example: dipeptide intramolecular charge-transfer states
(Faber, Boulanger, Duchemin, Attaccalite, Blase, JCP 2013)
TD-DFT versus GW/BSE for charge-transfer excitations
Charge-transfer excitations requiring long-range electron-hole interaction is a well known failure of TD-DFT with local kernels.
Similar situation in solids with extended Wannier excitons.
Excitonic States: (similar to Felix Plasser): from the Electron-Transition Density Matrix electrons are green, holes are gray ϕe (r e)=∫rh
ψ(rh , re)d rh
The future….
Beyond standard approximations
Vibronic coupling(forces?)
Real-time dynamics
Multi-referenceproblems
Multi-referenceproblems
Environment
When a charge arrives onto a molecule, the structural relaxation of the molecule traps the charge and strongly limits the mobility of the carriers (polaronic coupling).
t1u (3-fold)
The relaxation energy is closely related to the electronphonon coupling strength.
LUMO
GW
DFT (LDA)
(courtesy, A. Troisi, Warwick)
Electron-phonon potential
LDA 63 meV GW 109 meVExp. 107 meV
Exps: Wang et al., JCP 2005 ; Hands et al., PRB 2008Theory: Faber et al. J. of Mat. Science 47 (21), 7472 (2012)
Electron-phonon or vibronic coupling in molecular systems
(Implications in superconductivity, inelastic scattering, resonant Raman, etc. ?)
EPC ~ |slope|2
Many-Body Green’s functions and Classical Polarizable Models
I. Duchemin et al., JCP 144, 164106 (2016) and J. Li et al. JPCL, 7, 2814 (2016)
Hybrid QM/MM scheme merging the manybody Green’s function GW formalism with classical discrete polarizable models and its
application to molecular crystals and molecules in solution.
Hybrid QM/MM capture polarization effects not present in standard a deltaSCF DFT scheme.
Beyond standard approximations: self-consistency, higer orders...
C. Faber et al. JCP 139, 194308(2013) and X. Ren et al. PRB 92, 081102(2015)F. Kaplan et al. JCTC 12, 2528(2016)
Improvements are difficult….
Tetracyanoethylene (TCNE)
Real-time dynamicsManybody Green’s function theory can be extended to nonequilibrium situations,
and to study realtime dynamics
Nonlinear response Pumpprobe experiments
Kadanoff, L. P., & Baym, G. A. Quantum statistical mechanics (1962).
Second Harmonic Generation in MoS2 Transient absorption in silicon
M. Grüning, C. Attaccalite PRB 89, 081102 (2014) D. Sangalli & A. Marini EPL, 110, 47004. (2015)
Multi-references problems: DMFT + DFT
C. Weber et al. PRL Phys. 110, 106402 (2013) and PNAS 111, 5790 (2014)
Inclusion of manybody effects results in the correct prediction of similar binding energies
for oxy and carbonmonoxymyoglobin.
The computed electronic structure of the myoglobin complexes and the nature of the Fe–O2 bonding are validated against experimental spectroscopic observables.
A long-standing problem related to the quantum-mechanical description of the respiration process, namely that DFT calculations predict a strong imbalance between O2
and CO binding, favoring the latter to an unphysically large extent.
Dynimical mean field theory+
DFT
Conclusions
The Green’s mill is still used to do science
Green’s function theory is a powerful tool to study excitations in finite and infinite systems.
The field is rapidly evolving and many application in chemistry are on going, stay tuned!!
This presentation is available on: http://attaccalite.com
Ivan Duchemin
CarinaFaber
Acknoledgements
Xavier Blase
Paul Boulanger
Thanks to Martin Spenke for comments on this
presentation
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