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Theoretical characterization of the interactions between organic ligands and metallic clusters

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Theoretical characterization of the interactions

between organic ligands and metallic clusters

Barbara Fresch, Francoise Remacle

Laboratoire de Chimie Physique Théorique,

Université de Liège, Belgique

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Motivations:

 Understanding the impact of protecting organic ligand shells on the structure-property relation of metallic clusters and nanoparticles.

 Exploiting ligands-metal core interactions to tune the properties of metal clusters according to specific applications (catalysis, nano-electronics, bio-labelling…).

Examples:

Pd13(PH3)6(SCH3)6 Pd55(SCH3)20 [Au13(PH3)10Cl2]3+

Insights from quantum chemistry calculations at the level of density functional theory

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Pd13(PH3)12 Pd13(SCH3)12  studying the characteristic of the ligand-metal interaction in terms of

binding mode, adsorption energy, charge transfer

ε=-1.89eV ε=-1.74eV

ε=-0.62eV ε=-0.66eV

-0.02|e|

 From a single ligand to a

ligand shell

ε=-0.51eV ε=-1.61eV +0.2|e|

3

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Pd13(PH3)6(SCH3)6 P:+1.58|e| (0.26)

S: -0.64 |e| (-0.11)

 What if we mix different

ligands: cooperative effects?

Engineering the composition of the ligand shell to tailor the properties of the system

4

Integrating theoretical results and experimental expertise-1

 Structures: we can determine true minima of the PES but a search of the absolute minimum is prohibitive

Ex: Au13Cl2(PH3)103+

Y. Shichibu et al., Nanoscale 4, 4125 (2012)

 Stoichiometry: how many ligands/ surface reconstruction

To what extent it is actually possible to control the composition of the ligand shell?  Size selective and specific synthetic routes

4

Structural informations ideally in different environment (crystal/solution)

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Integrating theoretical results and experimental expertise-2 Which properties?

ΔG=-0.34eV

Structure dependent optical adsorption

5

B. Fresch et al. Eur. Phys. J. D 2012, 66 (12), 1-9.

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Vibrational Frequencies-IR spectra

Ionisation potential, Electron Affinity, Charging Energy

 S-C stretching

frequencies: 712cm-1

versus 654cm-1

(weakening of the bond)

HOMO Vertical ionization [Pd13(PH3)6(SCH3)6]+ Pd13(PH3)6(SCH3)6 Geometry relaxation Spin Density AIP=5.85eV

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Directions of Research-1

Mechanism of Reactions ΔG 0eV -0.1eV -1.0eV Transition State Kinetics

Barngrover, B. M.; J. Phys. Chem. A 2013, 117, 5377– 5384. Askerka, M.; J. Phys. Chem. A 2012, 116, 7686– 7693 7

 Formation of molecular H2?  Sulfidation of the surface?

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Solvent

How it affects Properties?

Spatial segregation of ligands

Directions of Research-2

Pd13(SCH3)12(H2O)14 Spin Density P:+1.58|e| (0.26) S: -0.64 |e| (-0.11) Pd: -0.94 |e| P:+1.31|e| (0.22) S: -0.09|e| (-0.016) Pd: -1.21 |e| Is there a driving force allowing the synthesis of “Janus” clusters? 8

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Truly nano-sized system?

Pd

55

(PH

3

)

20

Pd

55

(SCH

3

)

20

Pd

55

(PH

3

)

10

(SCH

3

)

10

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Two modified base pairs (tio-uracil) Interaction with Silver cations

Hybrid QM/MM approach

Metals (or Metallic clusters) in supra-molecular aggregates

(Ph. Thesis, Dr. Renuka Ganesan)

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11

Exploring conformational space and Dynamics of molecular aggregates

 Classical Force Field

 Application of external forces

(nano-manipulation experiments)

F(pN)

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 rather “big” systems, explicit solvation

 well developed for “all-organic” system (metals and surfaces can be modelled)  transitions between different minima of the potential energy surface

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Laboratoire de Chimie Physique Théorique:

Prof. Francoise Remacle

Dr. Fabien Dufour Dr. Mike Klymenko Dr. Renuka Ganesan Dr. Tian Min Yan Benoit Mignolet

Gustavo Lugo

ARC-NANOFORCE project MULTI

TOLOP

Prof. Francesca Ottaviani and all the organisation

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