The role of metal contact configuration in the mechanical properties of molecular nanojunctions: Comparative ab-initio study for Au/1,8-octanidithiol and Au/4,4’-bipyridine

P. VÉLEZ, S. A. DASSIE, E.P.M. LEIVA

PHYSICAL REVIEW B

AMER PHYSICAL SOC

Año: 2010 vol. 81 p. 2354351 - 23543512

1098-0121

A comparative study of the mechanical properties of Au/4,4
-bipyridine
4,4
BPD and Au/1,8- octanedithiol
1,8 ODT molecular nanojunctions is developed using different metal wires and small clusters to represent the metal contact. Rupture of the junction at different bonds is analyzed. While in the case of 1,8 ODT, rupture at Au-Au bonds is always found; in the case of 4,4
BPD, rupture of a N-Au bond also appears as possible. Comparison of rupture forces, maximum elongations and force constants with the experimental values lead to the conclusion that the most common geometrical arrangement in scanning tunneling microscopy break junctions should be that where the number of Au atoms is of the order of 4. Activation energies for the rupture of these structures are calculated at sample elongations. as possible. Comparison of rupture forces, maximum elongations and force constants with the experimental values lead to the conclusion that the most common geometrical arrangement in scanning tunneling microscopy break junctions should be that where the number of Au atoms is of the order of 4. Activation energies for the rupture of these structures are calculated at sample elongations. represent the metal contact. Rupture of the junction at different bonds is analyzed. While in the case of 1,8 ODT, rupture at Au-Au bonds is always found; in the case of 4,4
BPD, rupture of a N-Au bond also appears as possible. Comparison of rupture forces, maximum elongations and force constants with the experimental values lead to the conclusion that the most common geometrical arrangement in scanning tunneling microscopy break junctions should be that where the number of Au atoms is of the order of 4. Activation energies for the rupture of these structures are calculated at sample elongations. as possible. Comparison of rupture forces, maximum elongations and force constants with the experimental values lead to the conclusion that the most common geometrical arrangement in scanning tunneling microscopy break junctions should be that where the number of Au atoms is of the order of 4. Activation energies for the rupture of these structures are calculated at sample elongations. octanedithiol
1,8 ODT molecular nanojunctions is developed using different metal wires and small clusters to represent the metal contact. Rupture of the junction at different bonds is analyzed. While in the case of 1,8 ODT, rupture at Au-Au bonds is always found; in the case of 4,4
BPD, rupture of a N-Au bond also appears as possible. Comparison of rupture forces, maximum elongations and force constants with the experimental values lead to the conclusion that the most common geometrical arrangement in scanning tunneling microscopy break junctions should be that where the number of Au atoms is of the order of 4. Activation energies for the rupture of these structures are calculated at sample elongations. as possible. Comparison of rupture forces, maximum elongations and force constants with the experimental values lead to the conclusion that the most common geometrical arrangement in scanning tunneling microscopy break junctions should be that where the number of Au atoms is of the order of 4. Activation energies for the rupture of these structures are calculated at sample elongations. represent the metal contact. Rupture of the junction at different bonds is analyzed. While in the case of 1,8 ODT, rupture at Au-Au bonds is always found; in the case of 4,4
BPD, rupture of a N-Au bond also appears as possible. Comparison of rupture forces, maximum elongations and force constants with the experimental values lead to the conclusion that the most common geometrical arrangement in scanning tunneling microscopy break junctions should be that where the number of Au atoms is of the order of 4. Activation energies for the rupture of these structures are calculated at sample elongations. as possible. Comparison of rupture forces, maximum elongations and force constants with the experimental values lead to the conclusion that the most common geometrical arrangement in scanning tunneling microscopy break junctions should be that where the number of Au atoms is of the order of 4. Activation energies for the rupture of these structures are calculated at sample elongations. /4,4
-bipyridine
4,4
BPD and Au/1,8- octanedithiol
1,8 ODT molecular nanojunctions is developed using different metal wires and small clusters to represent the metal contact. Rupture of the junction at different bonds is analyzed. While in the case of 1,8 ODT, rupture at Au-Au bonds is always found; in the case of 4,4
BPD, rupture of a N-Au bond also appears as possible. Comparison of rupture forces, maximum elongations and force constants with the experimental values lead to the conclusion that the most common geometrical arrangement in scanning tunneling microscopy break junctions should be that where the number of Au atoms is of the order of 4. Activation energies for the rupture of these structures are calculated at sample elongations. as possible. Comparison of rupture forces, maximum elongations and force constants with the experimental values lead to the conclusion that the most common geometrical arrangement in scanning tunneling microscopy break junctions should be that where the number of Au atoms is of the order of 4. Activation energies for the rupture of these structures are calculated at sample elongations. represent the metal contact. Rupture of the junction at different bonds is analyzed. While in the case of 1,8 ODT, rupture at Au-Au bonds is always found; in the case of 4,4
BPD, rupture of a N-Au bond also appears as possible. Comparison of rupture forces, maximum elongations and force constants with the experimental values lead to the conclusion that the most common geometrical arrangement in scanning tunneling microscopy break junctions should be that where the number of Au atoms is of the order of 4. Activation energies for the rupture of these structures are calculated at sample elongations. as possible. Comparison of rupture forces, maximum elongations and force constants with the experimental values lead to the conclusion that the most common geometrical arrangement in scanning tunneling microscopy break junctions should be that where the number of Au atoms is of the order of 4. Activation energies for the rupture of these structures are calculated at sample elongations.
1,8 ODT molecular nanojunctions is developed using different metal wires and small clusters to represent the metal contact. Rupture of the junction at different bonds is analyzed. While in the case of 1,8 ODT, rupture at Au-Au bonds is always found; in the case of 4,4
BPD, rupture of a N-Au bond also appears as possible. Comparison of rupture forces, maximum elongations and force constants with the experimental values lead to the conclusion that the most common geometrical arrangement in scanning tunneling microscopy break junctions should be that where the number of Au atoms is of the order of 4. Activation energies for the rupture of these structures are calculated at sample elongations. as possible. Comparison of rupture forces, maximum elongations and force constants with the experimental values lead to the conclusion that the most common geometrical arrangement in scanning tunneling microscopy break junctions should be that where the number of Au atoms is of the order of 4. Activation energies for the rupture of these structures are calculated at sample elongations.
BPD, rupture of a N-Au bond also appears as possible. Comparison of rupture forces, maximum elongations and force constants with the experimental values lead to the conclusion that the most common geometrical arrangement in scanning tunneling microscopy break junctions should be that where the number of Au atoms is of the order of 4. Activation energies for the rupture of these structures are calculated at sample elongations.