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Molecular electronics and

Quantum Mechanical Simulations of Polymers for Molecular Electronics and Photonics... [Pg.146]

The work described in this paper is an illustration of the potential to be derived from the availability of supercomputers for research in chemistry. The domain of application is the area of new materials which are expected to play a critical role in the future development of molecular electronic and optical devices for information storage and communication. Theoretical simulations of the type presented here lead to detailed understanding of the electronic structure and properties of these systems, information which at times is hard to extract from experimental data or from more approximate theoretical methods. It is clear that the methods of quantum chemistry have reached a point where they constitute tools of semi-quantitative accuracy and have predictive value. Further developments for quantitative accuracy are needed. They involve the application of methods describing electron correlation effects to large molecular systems. The need for supercomputer power to achieve this goal is even more acute. [Pg.160]

As the analytical, synthetic, and physical characterization techniques of the chemical sciences have advanced, the scale of material control moves to smaller sizes. Nanoscience is the examination of objects—particles, liquid droplets, crystals, fibers—with sizes that are larger than molecules but smaller than structures commonly prepared by photolithographic microfabrication. The definition of nanomaterials is neither sharp nor easy, nor need it be. Single molecules can be considered components of nanosystems (and are considered as such in fields such as molecular electronics and molecular motors). So can objects that have dimensions of >100 nm, even though such objects can be fabricated—albeit with substantial technical difficulty—by photolithography. We will define (somewhat arbitrarily) nanoscience as the study of the preparation, characterization, and use of substances having dimensions in the range of 1 to 100 nm. Many types of chemical systems, such as self-assembled monolayers (with only one dimension small) or carbon nanotubes (buckytubes) (with two dimensions small), are considered nanosystems. [Pg.136]

Fullerenes have shown particular promise as acceptors in molecular electronics, and numerous interesting TTF/Cgo ensembles have been reported.42 For example, Orduna and co-workers75,76 prepared the TTF/C60 dyad 13 and observed photoinduced electron-transfer from the TTF to the fullerene. Martin et al 1 observed two separate one-electron transfer events in their conjugated dyads 14 (where n = 2). The TTF-porphyrin-fullerene triad 15, prepared by Carbonera et al.7 showed long-lived photoinduced charge separation. [Pg.770]

Another example is provided by the minimum energy coordinates (MECs) of the compliant approach in CSA (Nalewajski, 1995 Nalewajski and Korchowiec, 1997 Nalewajski and Michalak, 1995,1996,1998 Nalewajski etal., 1996), in the spirit of the related treatment of nuclear vibrations (Decius, 1963 Jones and Ryan, 1970 Swanson, 1976 Swanson and Satija, 1977). They all allow one to diagnose the molecular electronic and geometrical responses to hypothetical electronic or nuclear displacements (perturbations). The thermodynamical Legendre-transformed approach (Nalewajski, 1995, 1999, 2000, 2002b, 2006a,b Nalewajski and Korchowiec, 1997 Nalewajski and Sikora, 2000 Nalewajski et al., 1996, 2008) provides a versatile theoretical framework for describing diverse equilibrium states of molecules in different chemical environments. [Pg.454]

The HF results generated for representative polyatomic molecules have used the /V-derivatives estimated by finite differences, while the -derivatives have been calculated analytically, by standard methods of quantum chemistry. We have examined the effects of the electronic and nuclear relaxations on specific charge sensitivities used in the theory of chemical reactivity, e.g., the hardness, softness, and Fukui function descriptors. New concepts of the GFFs and related softnesses, which include the effects of molecular electronic and/or nuclear relaxations, have also been introduced. [Pg.475]

Nalewajski, R. F. 2000. Coupling relations between molecular electronic and geometrical degrees of freedom in density functional theory and charge sensitivity analysis. Computers Chem. 24 243-257. [Pg.477]

Heller, M. J. Utilization of synthetic DNA for molecular electronic and photonic-based device applications, in Lee, S. C. and Savage, L. (eds), Biological Molecules in Nanotechnology the Convergence of Biotechnology, Polymer Chemistry and Materials Science, IBC Press, Southborough, MA, USA, 1998, pp. 59-66. [Pg.555]

Esterification constitutes a valuable alternative to the amidation strategy. As with amidation, the formation of the ester bond is performed following a first reaction step with acyl chloride. The ester bond has been extensively utilized to attach many organic and inorganic moieties. Porphyrins are a classic example of substrates covalently bound via esterification strategies their photoinduced electron transfer to the nanotube has been studied for applications in molecular electronics and photovoltaic devices (Fig. 3.6) [21]. [Pg.49]

In the first decade of the century a number of experiments were described which were interpreted as involving the ejection of molecular electrons and indicated the order of magnitude of the ionization poten-... [Pg.35]

S. Tuchman, S. Sideman, S. Kenig, and N. Lotan, Enzyme based logic gates controlled by outside signals principles and design, in Molecular Electronics and Molecular Electronic Devices, K. Sienicki, Ed., Vol. HI, CRC Press, Boca Raton, FL, 1994, pp. 223-238. [Pg.140]

M. Buck reviews in great depth the literature on self-assembled monolayers (SAMs) of thiols on gold, a classic means of surface modification. The wide variety of functional groups that is provided by synthetic chemists makes thiol-SAMs an exciting playground for applications where the gap between two worlds, the inorganic and the organic, needs to be closed. Examples are molecular electronics and biochemistry. [Pg.278]

Since 2004 [183], graphene research has evolved from a heavily theoretical and fundamental field into a variety of research areas [301]. Its electrical, magnetic, physical-mechanical, and chemical properties position it as the most promising material for molecular electronic and optoelectronic applications, possibly replacing the currently used silicon and metal oxide based devices. Nonetheless, further research is essential in order to control easily such properties and construct devices with specific and novel architectures to explore in depth all of these exciting properties, as well as to achieve the synthesis of large-scale, size- and layer-count controlled graphene. [Pg.162]

Kim WY, Kim KS (2010) Tuning molecular orbitals in molecular electronics and spintro-nics. Acc Chem Res 43 111-120... [Pg.172]

Although, from a purely chemical point of view, learning how to create these complicated supramolecular structures has its own value, there are plenty of more practical reasons to investigate this chemistry. In the short term, these include catalysis and sensor applications, and in the long term, molecular electronics and molecular machines. With perhaps the exception of catalysis, all these applications will require some sort of signal transduction to allow for communication with the supramolecular device. This, of course, is one of the main reasons that electrochemistry is useful for supramolecular chemistry. Electron transfer provides a well-understood and very sensitive method to both communicate with supramolecular assemblies and control their structure.8... [Pg.1]

Thus suppose we had included the interaction of the radiation s magnetic field B with the atomic or molecular electrons and nuclei. The Hamiltonian for this interaction is [Equation (1.268)] -B , where p is the magnetic dipole-moment operator for the system. This gives additional terms in cm that are proportional to... [Pg.316]

We have seen that the molecular electronic and vibrational wave functions el and vib each transform according to the irreducible representations of the molecular point group. We now consider the rotational wave function ptot. [Pg.474]

In the past fifty years, the NMR Chemical Shielding have evolved from corrections to the measurement of nuclear magnetic moments as quoted from Ramsey s 1950 original papers (Phys. Rev. 77, 567 and 78, 699), to one of the most important tools for structural elucidation in many branches of chemistry. There are no simple relationships between molecular structure and chemical shifts. Their dependence on the molecular electronic and geometrical structure can be derived via complex quantum mechanical equations. [Pg.381]

One of the most promising bottom-up approaches in nanoelectronics is to assemble 7i-conjugated molecules to build nano-sized electronic and opto-electronic devices in the 5-100 nm length scale. This field of research, called supramolecular electronics, bridges the gap between molecular electronics and bulk plastic electronics. In this contest, the design and preparation of nanowires are of considerable interest for the development of nano-electronic devices such as nanosized transistors, sensors, logic gates, LEDs, and photovoltaic devices. [Pg.250]

The LB deposition is one of the best methods to prepare highly organized molecular systems, in which various molecular parameters such as distance, orientation, extent of chromophore interaction, or redox potential can be controlled in each monolayer. We have been studying photophysical and photochemical properties of LB films in order to construct molecular electronic and photonic devices. The molecular orientation and interactions of redox chromophores are very important in controlling photoresponses at the molecular level. Absorption and fluorescence spectra give important information on them. We have studied photoresponses, specific interactions, and in-plane and out-of-plane orientation of various chromophores in LB films [3-11], In addition to the change of absorp-... [Pg.391]


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A Summary of Electronic and Molecular Geometries

Calculation of molecular electronic wave functions and energies

Centre Molecular Orbitals and Pauling 3-Electron Bonds

Classifying molecular orbitals and electronic states

Combining the Localized Electron and Molecular Orbital Models

Correlation of molecular and atomic electronic states

DNA and Molecular Electronics

Electron Density Distributions and Molecular Orbitals

Electron Transfer Along Bridging Molecules, Molecular Wires and Semiconductor Particles Embedded in Membranes

Electron Transport in Two- and Three-terminal Molecular Devices

Electron-Group Arrangements and Molecular Shapes

Electronic Spectra and Molecular Structure

Electrons molecular orbitals and

Experimental and Theoretical Electronic Charge Densities in Molecular

Formalisms for the Explicit Inclusion of Electronic Polarizability in Molecular Modeling and Dynamics Studies

General Atomic and Molecular Electronic

General Atomic and Molecular Electronic Structure System

Molecular Geometry and the Number of Electrons

Molecular One-and Two-Electron Integrals

Molecular and Biomolecular Electronics

Molecular and Supramolecular Electronic Devices

Molecular and electronic structure

Molecular electronic and photonic device

Molecular electronics and photonics

Molecular geometry and the valence-shell electron pair repulsion model

Molecular orbitals and electronic

Molecular orbitals and electronic states

Molecular orbitals and electronic transitions

Molecular shapes and electronic

Perturbation Theory and Its Application to the Molecular Electronic Structure Problem

Relationship Between Electronic Configuration and Molecular Behaviour

Skill 1.3c-Predict molecular geometries using Lewis dot structures and hybridized atomic orbitals, e.g., valence shell electron pair repulsion model (VSEPR)

The Correlation of Molecular and Atomic Electronic States

Valence shell electron pair repulsion and molecular geometry

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