Biomedical subjects

Jukka-Pekka Jalkanen

Publications and source records attributed to Jukka-Pekka Jalkanen.

5 recordsLinked to original sources

PubMed2006

Surface enhanced second harmonic generation from macrocycle, catenane, and rotaxane thin films: experiments and theory.

Surface enhanced second harmonic generation (SE SHG) experiments on molecular structures, macrocycles, catenanes, and rotaxanes, deposited as monolayers and multilayers by vacuum sublimation on silver, are reported. The measurements show that the molecules form ordered thin films, where the highest degree of order is observed in the case of macrocycle monolayers and the lowest in the case of rotaxane multilayers. The second harmonic generation activity is interpreted in terms of electric field induced second harmonic (EFISH) generation where the electric field is created by the substrate silver atoms. The measured second order nonlinear optical susceptibility for a rotaxane thin film is compared with that obtained by considering only EFISH contribution to SHG intensity. The electric field on the surface of a silver layer is calculated by using the Delphi4 program for structures obtained with TINKER molecular mechanics/dynamics simulations. An excellent agreement is observed between the calculated and the measured SHG susceptibilities.

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PubMed2006

Interaction model for the adsorption of organic molecules on the silver surface.

Adsorption of organics on a silver surface is simulated. An Embedded Atom Model is used for the metal, a standard force field for the organics, and a combination of the charge equilibration model and the Morse potential for their electrostatic and nonbonding interactions. The only adjustable parameters of this approach appear in the Morse potential. They are tuned to reproduce experimental and high level quantum chemical data. The adsorption energies of 13 molecules on the Ag(111) surface are obtained with an average error of less than 1 kcal mol(-1). The model should be transferable to molecules with the same chemical groups used in regressing the potential parameters when physisorption or weak chemisorption, i.e., no bond breaking, occur, and also to other Ag surfaces. When used to simulate perylene tetracarboxylic acid dianhydride (PTCDA) on Ag(111), correct geometry of mono- and multilayers are observed in molecular dynamics simulations at room temperature.

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PubMed2005

Experimental and theoretical study of the adsorption of fumaramide [2]rotaxane on Au(111) and Ag(111) surfaces.

Thin films of fumaramide [2]rotaxane, a mechanically interlocked molecule composed of a macrocycle and a thread in a "bead and thread" configuration, were prepared by vapor deposition on both Ag(111) and Au(111) substrates. X-ray photoelectron spectroscopy (XPS) and high-resolution electron-energy-loss spectroscopy were used to characterize monolayer and bulklike multilayer films. XPS determination of the relative amounts of carbon, nitrogen, and oxygen indicates that the molecule adsorbs intact. On both metal surfaces, molecules in the first adsorbed layer show an additional component in the C 1s XPS line attributed to chemisorption via amide groups. Molecular-dynamics simulation indicates that the molecule orients two of its eight phenyl rings, one from the macrocycle and one from the thread, in a parallel bonding geometry with respect to the metal surfaces, leaving three amide groups very close to the substrate. In the case of fumaramide [2]rotaxane adsorption on Au(111), the presence of certain out-of-plane phenyl ring and Au-O vibrational modes points to such bonding and a preferential molecular orientation. The theoretical and experimental results imply that the three-dimensional intermolecular configuration permits chemisorption at low coverage to be driven by interactions between the three amide functions of fumaramide [2]rotaxane and the Ag(111) or Au(111) surface.

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PubMed2005

Quantum chemical interaction energy surfaces of ethylene and propene dimers.

Ab initio studies of nonbonding interactions for ethylene and propene dimers were conducted at the MP2/6-311+G(2df,2pd) level. The dimers were attractive in all of the orientations studied; however, the attraction was <0.1 kcal/mol for ethylene D2h and C2h dimers, for which the pi-electron clouds or H atoms interact closely. A previously introduced transferable potential model, NIPE [Jalkanen, J.-P.; Pakkanen, T. A.; Yang, Y.; Rowley, R. L. J. Chem. Phys. 2003, 118, 5474], which is based on quantum chemical calculations of small alkane molecules, was tested against the propene and ethylene dimer data. Comparisons of results showed that interaction energies for orientations dominated by interactions between the propene methyl groups or two hydrogens were accurately predicted with the NIPE model. Interactions involving the double bond were not predicted as well, because the original NIPE regression data set did not contain any information about pi-electron systems. An extension of the NIPE model to include pi-electron interactions is proposed. Additional interaction sites are used with the same energy function as atomic interactions. This addition provides a more accurate description of the interaction energies of both ethylene and propene and extends the transferability of the NIPE model to alkenes.

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PubMed2004

Mapping the interaction energy surfaces of cyclic alkanes: evaluating the transferability of an ab initio based potential model.

Detailed interaction energy maps are computed for symmetric cyclopropane and tetrahedrane dimer systems using ab initio methods. Interaction energies of cubane and cyclohexane dimers are also reported. The global minimum energy structures of cyclopropane and tetrahedrane systems are both D(3d) structures with energies of -1.850 and -2.171 kcal mol(-1). The ability of NIPE potential model, based on ab initio nonbonding data of neopentane (N), isobutane (I), propane (P), ethane (E) and all their combinations to predict the pair interaction energies of these strained cyclic hydrocarbons is also investigated. The difference between the energies predicted by NIPE and those obtained from the ab initio calculations increases with ring strain In general, NIPE values are in close agreement with the ab initio results for alkane ring structures having low ring strain.

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