Síntesi, caracterització química i estudi de l'activitat biològica de nous complexos de Pt(II) amb lligands de tipus diaminocarboxílic i els respectius ésters i derivats peptídics

El cisplatí, PtCl2(NH3)2, ha estat una de les drogues més utilitzades en la quimioteràpia del càncer des del descobriment de la seva activitat. Però degut a la seva alta toxicitat i greus efectes secundaris, s'han sintetitzat nous compostos amb la finalitat de reduir aquests inconvenients. En aquest sentit, el treball desenvolupat en aquesta tesi doctoral ha estat la síntesi i caracterització de tretze complexos de Pt(II) amb la finalitat d'estudiar llur activitat antitumoral. Aquests complexos presenten unes característiques estructurals comunes: geometria cis, dos lligands làbils de tipus clorur i un lligand diaminoquelatant derivat dels àcids d,l-2,3-diaminopropiònic (Hdap) i d,l-2,4-diaminobutíric (Hdab). S'han dissenyat unes estratègies sintètiques a partir de les quals els lligands han estat funcionalitzats amb diferents grups de tipus éster, aminoàcid i peptídic: Etdap·2HCl, Etdab·2HCl, [(dap-Metala)·2CF3COOH], [(dab-Metala)·2CF3COOH], [(dap-phe)·2CF3COOH], [(dab-phe)·2CF3COOH], [(dap-Mettrp)·2CF3COOH], [(dab-Mettrp)·2CF3COOH], [(dap-ASTTTNYT-NH2)·2CF3COOH], essent Metala= éster metílic de L-alanina, phe= L-fenilalanina, Mettrp= éster metílic del L-triptofà. Aquests lligands diaminoquelatants s'han utilitzat per sintetitzar els corresponents complexos de Pt(II): PtCl2(Hdap), PtCl2(Hdab), PtCl2(Etdap), PtCl2(Etdab), PtCl2(dap-Metala), PtCl2(dab-Metala), PtCl2(dap-ala), PtCl2(dab-ala), PtCl2(dap-phe), PtCl2(dab-phe), PtCl2(dap-Mettrp), PtCl2(dab-Mettrp), PtCl2(dap-ASTTTNYT-NH2). A través de diferents tècniques i assaigs biològics (dicroisme circular, electroforesi en gel d'agarosa, microscopia de forces atòmiques, citometria de flux, assaigs de proliferació cel·lular) s'ha pogut demostrar l'activitat antitumoral d'aquests compostos. A través de la tècnica de dicroisme circular (DC) s'ha pogut demostrar que els lligands lliures no interaccionen covalentment amb el DNA de Calf Thymus i no modifiquen l'estructura secundària de la doble hèlix. En canvi, els respectius complexos han demostrat tenir capacitat per interaccionar amb el DNA i modificar la seva estructura secundària. Els complexos PtCl2(Hdap), PtCl2(Hdab) i PtCl2(dab-phe) mostren un comportament similar al cisplatí, generant adductes cis-bifuncionals que distorcionen la doble hèlix de forma no desnaturalitzant amb obertura de la doble cadena. Els complexos PtCl2(Etdap), PtCl2(Etdab), PtCl2(dap-ala), PtCl2(dab-ala), PtCl2(dap-Metala), PtCl2(dab-Metala), PtCl2(dap-phe), PtCl2(dap-ASTTTNYT-NH2) quan interaccionen amb el DNA generen un canvi en la conformació del DNA de la forma B a la forma C, produint-se un augment de la curvatura de l'hèlix per rotació de les bases nitrogenades. En aquests estudis s'ha comprovat que l'estructura del complex influeix en l'efecte generat sobre l'estructura secundària de l'àcid nucleic. En primer lloc, existeix una diferència en el comportament en funció del tamany del lligand diaminoquelatant, de manera que els complexos amb el lligand (dab) provoquen un efecte més remarcable. També s'observa aquest canvi de comportament al passar dels complexos que tenen el grup funcional esterificat als que el tenen protonat. D'aquesta manera, s'observa un major efecte sobre l'estructura secundària del DNA en aquells complexos que tenen el lligand diaminoquelatant de tres metilens (dab) i amb el grup carboxilat terminal protonat. Per tal de modelitzar la interacció d'aquests complexos amb el DNA, s'ha estudiat la interacció d'aquests compostos de Pt(II) amb 5'-GMP a través de RMN-1H, observant la variació dels senyals corresponents al H8 de 5'-GMP. Així s'ha pogut demostrar que aquests compostos interaccionen amb la 5'-GMP a través d'un enllaç covalent Pt-N7, de la mateixa manera a com interacciona el cisplatí. A través d'electroforesi en gel d'agarosa i microscopia de forces atòmiques (AFM) s'ha pogut determinar l'efecte que generen els lligands lliures i els respectius complexos de Pt(II) sobre l'estructura terciària del plasmidi pBR322. Els lligands provoquen un augment de l'agregació de les molècules de DNA i un lleuger augment de la compactació de l'estructura terciària. Aquests resultats s'atribueixen a la capacitat d'aquests compostos a interaccionar per pont d'hidrogen amb el DNA. Els corresponents complexos de Pt(II) provoquen un augment de l'agregació i una important compactació, degut per una banda a la capacitat de l'àtom de Pt a interaccionar covalentment amb el DNA, i per altra banda, a la capacitat del lligand a interaccionar per pont d'hidrogen amb l'àcid nucleic. Finalment s'ha estudiat l'activitat citotòxica d'aquests complexos de Pt(II) en diferents línies cel·lulars: A431 (línia de carcinoma epidermoide), HeLa (línia de carcinoma de coll d'úter) i HL-60 (línia promielocítica de leucèmia). Els complexos moderadament solubles en aigua, PtCl2(Hdap), PtCl2(Hdab), PtCl2(dap-ala), PtCl2(dab-ala), PtCl2(dap-phe) i PtCl2(dab-phe), han demostrat ser actius. L'activitat depèn de la concentració de complex, del temps d'incubació i de la línia cel·lular. Per temps d'incubació alts i concentracions de complex elevades s'observa la màxima activitat. Els complexos de l'alanina, PtCl2(dap-ala) i PtCl2(dab-ala), són els que mostren més activitat, mentre que els compostos de la fenilalanina són els menys actius, degut probablement a la voluminositat del lligand, la qual pot impedir o dificultar el transport del compost a través de la membrana cel·lular. L'activitat citotòxica dels complexos insolubles en aigua, PtCl2(Etdap) i PtCl2(Etdab), queda bloquejada per l'elevada concentració de DMSO (12%) necessària per solubilitzar els compostos. Aquests resultats permeten deduir que la presència d'un 12% de DMSO anul·la l'activitat d'aquests complexos, ja que el DMSO pot coordinar-se amb el Pt ocupant les posicions làbils del complex i evitant que es pugui coordinar amb el DNA. Els assaigs de proliferació cel·lular del complex PtCl2(dap-ASTTTNYT-NH2) i del pèptid lliure ASTTTNYT-NH2 han demostrat que ambdós compostos són actius. Tot i això, l'activitat del complex és superior a la del pèptid lliure, ja que el Pt pot interaccionar covalentment amb el DNA i augmentar l'efecte citotòxic. Per tant, el complex presenta un lligand portador biològicament actiu que pot transportar el metall a través de la membrana cel·lular i facilitar així la seva interacció amb el DNA. A través de la tècnica de citometria de flux s'ha comprovat que en tots els casos la mort cel·lular produïda pels complexos ha estat per apoptosi. Per últim, s'ha sintetitzat i caracteritzat un complex trinuclear de Pt(II), {[Pt(Me2Bpy)2][PtCl2(Me2Bpy)]2}, essent Me2Bpy= 4,4'-dimetil-2,2'-dipiridil. La resolució de la seva estructura per difracció de Raig-X ha permès determinar l'existència d'una interacció intramolecular Pt-Pt de 3.474 Å.

Additional compact formulas for vibrational dynamic dipole polarizabilities and hyperpolarizabilities

Compact expressions, complete through second order in electrical and/or mechanical anharmonicity, are given for the dynamic dipole vibrational polarizability and dynamic first and second vibrational hyperpolarizabilities. Certain contributions not previously formulated are now included

Anharmonicity contributions to the vibrational second hyperpolarizability of conjugated oligomers

Restricted Hartree-Fock 6-31G calculations of electrical and mechanical anharmonicity contributions to the longitudinal vibrational second hyperpolarizability have been carried out for eight homologous series of conjugated oligomers - polyacetylene, polyyne, polydiacetylene, polybutatriene, polycumulene, polysilane, polymethineimine, and polypyrrole. To draw conclusions about the limiting infinite polymer behavior, chains containing up to 12 heavy atoms along the conjugated backbone were considered. In general, the vibrational hyperpolarizabilities are substantial in comparison with their static electronic counterparts for the dc-Kerr and degenerate four-wave mixing processes (as well as for static fields) but not for electric field-induced second harmonic generation or third harmonic generation. Anharmonicity terms due to nuclear relaxation are important for the dc-Kerr effect (and for the static hyperpolarizability) in the σ-conjugated polymer, polysilane, as well as the nonplanar π systems polymethineimine and polypyrrole. Restricting polypyrrole to be planar, as it is in the crystal phase, causes these anharmonic terms to become negligible. When the same restriction is applied to polymethineimine the effect is reduced but remains quantitatively significant due to the first-order contribution. We conclude that anharmonicity associated with nuclear relaxation can be ignored, for semiquantitative purposes, in planar π-conjugated polymers. The role of zero-point vibrational averaging remains to be evaluated

Linear response functions for a vibrational configuration interaction state

Linear response functions are implemented for a vibrational configuration interaction state allowing accurate analytical calculations of pure vibrational contributions to dynamical polarizabilities. Sample calculations are presented for the pure vibrational contributions to the polarizabilities of water and formaldehyde. We discuss the convergence of the results with respect to various details of the vibrational wave function description as well as the potential and property surfaces. We also analyze the frequency dependence of the linear response function and the effect of accounting phenomenologically for the finite lifetime of the excited vibrational states. Finally, we compare the analytical response approach to a sum-over-states approach

Simple finite field nuclear relaxation method for calculating vibrational contribution to degenerate four-wave mixing

A simple extended finite field nuclear relaxation procedure for calculating vibrational contributions to degenerate four-wave mixing (also known as the intensity-dependent refractive index) is presented. As a by-product one also obtains the static vibrationally averaged linear polarizability, as well as the first and second hyperpolarizability. The methodology is validated by illustrative calculations on the water molecule. Further possible extensions are suggested

Simple finite field method for calculation of static and dynamic vibrational hyperpolarizabilities: curvature contributions

In the static field limit, the vibrational hyperpolarizability consists of two contributions due to: (1) the shift in the equilibrium geometry (known as nuclear relaxation), and (2) the change in the shape of the potential energy surface (known as curvature). Simple finite field methods have previously been developed for evaluating these static field contributions and also for determining the effect of nuclear relaxation on dynamic vibrational hyperpolarizabilities in the infinite frequency approximation. In this paper the finite field approach is extended to include, within the infinite frequency approximation, the effect of curvature on the major dynamic nonlinear optical processes

Finite field treatment of vibrational polarizabilities and hyperpolarizabilities: on the role of the Eckart conditions, their implementation, and their use in characterizing key vibrations

In the finite field (FF) treatment of vibrational polarizabilities and hyperpolarizabilities, the field-free Eckart conditions must be enforced in order to prevent molecular reorientation during geometry optimization. These conditions are implemented for the first time. Our procedure facilities identification of field-induced internal coordinates that make the major contribution to the vibrational properties. Using only two of these coordinates, quantitative accuracy for nuclear relaxation polarizabilities and hyperpolarizabilities is achieved in π-conjugated systems. From these two coordinates a single most efficient natural conjugation coordinate (NCC) can be extracted. The limitations of this one coordinate approach are discussed. It is shown that the Eckart conditions can lead to an isotope effect that is comparable to the isotope effect on zero-point vibrational averaging, but with a different mass-dependence

Determination of vibrational polarizabilities and hyperpolarizabilities using field-induced coordinates

An analytical set of field-induced coordinates is defined and is used to show that the vibrational degrees of freedom required to completely describe nuclear relaxation polarizabilities and hyperpolarizabilities is reduced from 3N-6 to a relatively small number. As this number does not depend upon the size of the molecule, the process provides computational advantages. A method is provided to separate anharmonic contributions from harmonic contributions as well as effective mechanical from electrical anharmonicity. The procedures are illustrated by Hartree-Fock calculations, indicating that anharmonicity can be very important

Field-induced coordinates for the determination of dynamic vibrational nonlinear optical properties

Three conjugated organic molecules that span a range of polarity and valence-bond/charge transfer characteristics were studied. It was found that dispersion can be insignificant, and that adequate treatment can be achieved with frequency-dependent field-induced vibrational coordinates (FD-FICs)

Treatment of nonlinear optical properties due to large amplitude anharmonic vibrational motions: umbrella motion in NH3

A general reduced dimensionality finite field nuclear relaxation method for calculating vibrational nonlinear optical properties of molecules with large contributions due to anharmonic motions is introduced. In an initial application to the umbrella (inversion) motion of NH3 it is found that difficulties associated with a conventional single well treatment are overcome and that the particular definition of the inversion coordinate is not important. Future applications are described

Variational calculation of static and dynamic vibrational nonlinear optical properties

The vibrational configuration interaction method used to obtain static vibrational (hyper)polarizabilities is extended to dynamic nonlinear optical properties in the infinite optical frequency approximation. Illustrative calculations are carried out on H2 O and N H3. The former molecule is weakly anharmonic while the latter contains a strongly anharmonic umbrella mode. The effect on vibrational (hyper)polarizabilities due to various truncations of the potential energy and property surfaces involved in the calculation are examined

Variational calculation of vibrational linear and nonlinear optical properties

A variational approach for reliably calculating vibrational linear and nonlinear optical properties of molecules with large electrical and/or mechanical anharmonicity is introduced. This approach utilizes a self-consistent solution of the vibrational Schrödinger equation for the complete field-dependent potential-energy surface and, then, adds higher-level vibrational correlation corrections as desired. An initial application is made to static properties for three molecules of widely varying anharmonicity using the lowest-level vibrational correlation treatment (i.e., vibrational Møller-Plesset perturbation theory). Our results indicate when the conventional Bishop-Kirtman perturbation method can be expected to break down and when high-level vibrational correlation methods are likely to be required. Future improvements and extensions are discussed

Basis set and electron correlation effects on initial convergence for vibrational nonlinear optical properties of conjugated organic molecules

The level of ab initio theory which is necessary to compute reliable values for the static and dynamic (hyper)polarizabilities of three medium size π-conjugated organic nonlinear optical (NLO) molecules is investigated. With the employment of field-induced coordinates in combination with a finite field procedure, the calculations were made possible. It is stated that to obtain reasonable values for the various individual contributions to the (hyper)polarizability, it is necessary to include electron correlation. Based on the results, the convergence of the usual perturbation treatment for vibrational anharmonicity was examined

Initial convergence of the perturbation series expansion for vibrational nonlinear optical properties

Initial convergence of the perturbation series expansion for vibrational nonlinear optical (NLO) properties was analyzed. The zero-point vibrational average (ZPVA) was obtained through first-order in mechanical plus electrical anharmonicity. Results indicated that higher-order terms in electrical and mechanical anharmonicity can make substantial contributions to the pure vibrational polarizibility of typical NLO molecules

Electronic and vibrational contributions to first hyperpolarizability of donor-acceptor-substituted azobenzene

In this study we report on the electronic and vibrational (hyper)polarizabilities of donor–acceptorsubstituted azobenzene. It is observed that both electronic and vibrational contributions to the electric dipole first hyperpolarizability of investigated photoactive molecule substantially depend on the conformation. The contributions to the nuclear relaxation first hyperpolarizability are found to be quite important in the case of two considered isomers (cis and trans). Although the double-harmonic term is found to be the largest in terms of magnitude, it is shown that the total value of the nuclear relaxation contribution to vibrational first hyperpolarizability is a result of subtle interplay of higher-order contributions. As a part of the study, we also assess the performance of long-range-corrected density functional theory in determining vibrational contributions to electric dipole (hyper)polarizabilities. In most cases, the applied long-range-corrected exchange correlation potentials amend the drawbacks of their conventional counterparts