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LC <str<strong>on</strong>g>effects</str<strong>on</strong>g> <strong>on</strong> <strong>the</strong> evaluati<strong>on</strong> <strong>of</strong> β<br />

<strong>of</strong> high intrinsic<br />

hyperpolarizability molecules.<br />

Cláudia Cardoso, Universidade de Coimbra


F, external<br />

Study <strong>the</strong> n<strong>on</strong>linear<br />

optical resp<strong>on</strong>se <strong>of</strong><br />

<strong>org</strong>anic molecules<br />

Study <strong>of</strong> <strong>the</strong> molecules<br />

with high intrinsic<br />

hyperpolarizability<br />

applied field<br />

Technological Applicati<strong>on</strong>s:<br />

signal processing,<br />

optical data storage,<br />

etc.<br />

, <strong>first</strong><br />

hyperpolarizability


How to compare different<br />

molecules?<br />

●<br />

two molecules with <strong>the</strong> same β but different<br />

number <strong>of</strong> π electr<strong>on</strong>s are not intrinsically<br />

equivalent.<br />

●<br />

quantum sum rules impose limits <strong>on</strong> <strong>the</strong> <strong>first</strong><br />

and sec<strong>on</strong>d hyperpolarizabilities.


fundamental limit:<br />

N: effective<br />

number <strong>of</strong><br />

polarizable<br />

electr<strong>on</strong>s<br />

M. G. Kuzyk, Phys. Rev. Lett. 85, 1218 (2000)<br />

Intrinsic<br />

Hyperpolarizability:


e- acceptor<br />

group<br />

e- d<strong>on</strong>or<br />

group<br />

<str<strong>on</strong>g>L<strong>on</strong>g</str<strong>on</strong>g> pi bridge<br />

Optimizati<strong>on</strong> <strong>of</strong>...<br />

●<br />

●<br />

<strong>the</strong> electr<strong>on</strong>-d<strong>on</strong>ating/withdrawing strengths <strong>of</strong><br />

<strong>the</strong> terminal d<strong>on</strong>or and acceptor groups<br />

c<strong>on</strong>jugati<strong>on</strong> path


1<br />

4<br />

2<br />

5<br />

3<br />

6<br />

7


Experimental Results<br />

The best molecules are <strong>on</strong>es that<br />

are l<strong>on</strong>g with many undulati<strong>on</strong>s in<br />

<strong>the</strong> potential energy functi<strong>on</strong>,<br />

which allows <strong>the</strong> electr<strong>on</strong> densities<br />

<strong>of</strong> <strong>the</strong> eigenstates to be well<br />

separated.<br />

OPTICS LETTERS Vol. 32, 59 2007<br />

Recipe<br />

● increased length<br />

● linear chain<br />

● mimic <strong>the</strong> optimal undulati<strong>on</strong><br />

● make use <strong>of</strong> aromatic moieties with a<br />

wide <str<strong>on</strong>g>range</str<strong>on</strong>g> <strong>of</strong> stabilizati<strong>on</strong> energies


Calculati<strong>on</strong><br />

Method<br />

●<br />

Geometries optimizati<strong>on</strong><br />

●<br />

β : Finite field calculati<strong>on</strong><br />

● Semi-empirical calculati<strong>on</strong>s :<br />

●<br />

<strong>TDDFT</strong> absorpti<strong>on</strong> spectra<br />

●<br />

PM6 Hamilt<strong>on</strong>ian (COSMO)<br />

DFT / <strong>TDDFT</strong>:<br />

B3LYP / 6-311G(d,p)+<br />

LC-BLYP/ 6-311G(d,p)+<br />

Solvent <str<strong>on</strong>g>effects</str<strong>on</strong>g>: PCM<br />

●<br />

●<br />

Aim:<br />

Reproduce <strong>the</strong> exp. values<br />

Understand <strong>the</strong> role <strong>of</strong> <strong>the</strong><br />

different c<strong>on</strong>jugati<strong>on</strong> paths


Gas-phase calculati<strong>on</strong>s underestimate β<br />

Calculati<strong>on</strong>s do<br />

not reproduce<br />

increase for<br />

MOL6 and MOL7<br />

(au)<br />

1.2E+5<br />

9.0E+4<br />

6.0E+4<br />

exp<br />

PM6<br />

DFT<br />

DFT:<br />

1,2,4 OK!<br />

3.0E+4<br />

0.0E+0<br />

0 1 2 3 4 5 6 7 8<br />

molecules


Solvent <str<strong>on</strong>g>effects</str<strong>on</strong>g> improve (some) results<br />

PM6:<br />

Solvent improves<br />

trend<br />

Mols 6, 7 not<br />

well reproduced<br />

(au)<br />

2.0E+5<br />

1.5E+5<br />

1.0E+5<br />

exp<br />

PM6<br />

DFT<br />

DFT/B3LYP:<br />

1,2,4 KO!<br />

5.0E+4<br />

0.0E+0<br />

0 1 2 3 4 5 6 7 8<br />

molecules


Molecules under study<br />

1<br />

4<br />

2


DFT B3LYP<br />

2.0E+5<br />

1.5E+5<br />

exp<br />

vac<br />

dmso<br />

(au)<br />

1.0E+5<br />

5.0E+4<br />

0.0E+0<br />

0 31 52 63 47 5 16 27 48 9<br />

molecules


Wr<strong>on</strong>g geometry?<br />

mol2<br />

Increasing <strong>the</strong><br />

torsi<strong>on</strong> angle:<br />

Fast energy<br />

increase<br />

Low decrease<br />

9E+4<br />

6E+4<br />

B3LYP+solv.<br />

exp<br />

Azobenzene:<br />

“(...) <strong>the</strong> energetic difference<br />

between <strong>the</strong> planar and twisted<br />

forms is ei<strong>the</strong>r zero or totally<br />

negligible at room temperature.”<br />

L. Briquet et al, Chem. Phys. Lett.,<br />

417, 2006, 190<br />

(au)<br />

3E+4<br />

0E+0<br />

0 10 20 30 40 50 60 70 80<br />

Torsi<strong>on</strong> angle (º)


Orbitals:<br />

HOMO<br />

mol4<br />

mol7


Orbitals:<br />

LUMO<br />

mol4<br />

mol7


<str<strong>on</strong>g>L<strong>on</strong>g</str<strong>on</strong>g> Range<br />

<str<strong>on</strong>g>correcti<strong>on</strong></str<strong>on</strong>g>s<br />

<str<strong>on</strong>g>L<strong>on</strong>g</str<strong>on</strong>g> molecules<br />

– Sekino et al. J. Chem.<br />

Phys. 126, 014107 2007<br />

Str<strong>on</strong>g e-<br />

d<strong>on</strong>ors/acceptors<br />

The β ratio <strong>of</strong> BLYP and<br />

HF increases<br />

m<strong>on</strong>ot<strong>on</strong>ically<br />

– J. Phys. Chem. A, Vol.<br />

113, No. 6, 2009 Loboda<br />

et al.


<str<strong>on</strong>g>L<strong>on</strong>g</str<strong>on</strong>g> <str<strong>on</strong>g>range</str<strong>on</strong>g> <str<strong>on</strong>g>correcti<strong>on</strong></str<strong>on</strong>g>s<br />

●<br />

DFT and HF exchange c<strong>on</strong>tributi<strong>on</strong>s are<br />

partiti<strong>on</strong>ed at <strong>the</strong> operator level.<br />

●<br />

The electr<strong>on</strong> repulsi<strong>on</strong> operator, 1/ r12, is<br />

partiti<strong>on</strong>ed using <strong>the</strong> error functi<strong>on</strong><br />

●<br />

n<strong>on</strong>local HF part becomes larger for greater<br />

distances.<br />

GAMESS | Y.Tawada et al J.Chem.Phys. 120, 8425 (2004)


LC improves calculated β<br />

2.0E+5<br />

1.5E+5<br />

exp<br />

LC-BLYP<br />

B3LYP<br />

Large<br />

difference<br />

for molecules<br />

1, 2, 4<br />

(au)<br />

1.0E+5<br />

5.0E+4<br />

Still problems<br />

with mol 2...<br />

and 7<br />

0.0E+0<br />

0 31 52 63 47 5 61 72 84<br />

9<br />

molecules


Different<br />

c<strong>on</strong>formers<br />

ΔE = 0.16 eV<br />

2E+5<br />

mol2<br />

(au)<br />

1E+5<br />

5E+4<br />

exp<br />

LC<br />

0E+0<br />

0 1 2 3 4 5 6 7 8<br />

ΔE = 0.09 eV


Mols 6 and 7 are isoelectr<strong>on</strong>ic but<br />

<strong>the</strong> additi<strong>on</strong>al Cl atom in molecule<br />

6, induces a twist in <strong>the</strong> c<strong>on</strong>jugati<strong>on</strong><br />

path, resulting in a decreased<br />

hyperpolarizability.<br />

x<br />

mol7<br />

mol6


B3LYP + solvent:<br />

Huge effect <strong>on</strong><br />

mols 1, 2, 4<br />

2.0E+5<br />

1.5E+5<br />

1.0E+5<br />

exp<br />

B3LYP –<br />

vac<br />

B3LYP –<br />

dmso<br />

LC/BLYP –<br />

dmso<br />

2E+5<br />

2E+5<br />

1E+5<br />

5E+4<br />

mol4<br />

mol7<br />

0E+0<br />

5.0E+4<br />

-5E+4<br />

0.0E+0<br />

0 1 2 3 4<br />

-1E+5<br />

PM6 B3LYP LC PM6 B3LYP LC<br />

Gas phase<br />

DMSO


Solvent and LC:<br />

Same effect <strong>on</strong><br />

mol 4 and 7<br />

0<br />

LC:<br />

B3LYP LC-BLYP<br />

B3LYP+solv LC-BLYP+solv<br />

opens <strong>the</strong> gap<br />

B3LYP LC-BLYP<br />

B3Lyp+solv LC-BLYP+solv<br />

-0.1<br />

Solvent:<br />

closes <strong>the</strong><br />

gap<br />

E (Hartree)<br />

-0.2<br />

-0.3<br />

HOMO-1<br />

HOMO<br />

LUMO<br />

LUMO+1<br />

mol4<br />

mol7<br />

-0.4


LC solvent<br />

Have opposite<br />

<str<strong>on</strong>g>effects</str<strong>on</strong>g><br />

LC effect<br />

larger for mol4<br />

LC+solvent<br />

Coincides with<br />

B3LYP-vac


3<br />

8<br />

6<br />

E01 (eV)<br />

2<br />

1<br />

B3LYP<br />

LC-BLYP<br />

Transiti<strong>on</strong> dipole<br />

4<br />

2<br />

B3LYP<br />

LC-BLYP<br />

0<br />

0 1 2 3 4 5 6 7 8<br />

molecules<br />

Two level model:<br />

2.0E+5<br />

1.5E+5<br />

1.0E+5<br />

0<br />

0 1 2 3 4 5 6 7 8<br />

B3LYP<br />

LC-BLYP<br />

exp<br />

molecules<br />

5.0E+4<br />

0.0E+0<br />

0 1 2 3 4 5 6 7 8<br />

molecules


C<strong>on</strong>clusi<strong>on</strong>s<br />

●<br />

●<br />

LC BLYP + solvent reproduce exp.<br />

Two sets <strong>of</strong> molecules<br />

1. Mols 1,2,4: Azo-benzene<br />

2. Mols 3, 5, 6, 7<br />

● LC important for group 1<br />

●<br />

●<br />

Solvent and LC have opposite <str<strong>on</strong>g>effects</str<strong>on</strong>g><br />

transiti<strong>on</strong>s dipoles and excitati<strong>on</strong> energies<br />

follow hyperpolarizability trends

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