Disentangling Peptide Configurations via Two-Dimensional Electronic Spectroscopy: Ab Initio Simulations Beyond the Frenkel Exciton Hamiltonian

Two-dimensional (2D) optical spectroscopy techniques based on ultrashort laser pulses have been recently extended to the optical domain in the ultraviolet (UV) spectral region. UV-active aromatic side chains can thus be used as local highly specific markers for tracking dynamics and structural rearrangements of proteins. Here we demonstrate that 2D electronic spectra of a model proteic system, a tetrapeptide with two aromatic side chains, contain enough structural information to distinguish between two different configurations with distant and vicinal side chains. For accurate simulations of the 2DUV spectra in solution, we combine a quantum mechanics/molecular mechanics approach based on wave function methods, accounting for interchromophores coupling and environmental effects, with nonlinear response theory. The proposed methodology reveals effects, such as charge transfer between vicinal aromatic residues that remain concealed in conventional exciton Hamiltonian approaches. Possible experimental setups are discussed, including multicolor experiments and signal manipulation techniques for limiting undesired background contributions and enhancing 2DUV signatures of specific electronic couplings.

[1]  A. Tortschanoff,et al.  Photon echo peak shift experiments in the UV: p-terphenyl in different solvents , 2008 .

[2]  S. Mukamel,et al.  Multidimensional femtosecond correlation spectroscopies of electronic and vibrational excitations. , 2000, Annual review of physical chemistry.

[3]  J. M. Womick,et al.  Probing ultrafast dynamics in adenine with mid-UV four-wave mixing spectroscopies. , 2011, The journal of physical chemistry. A.

[4]  K. Yoshihara,et al.  Nanosecond laser photolysis of the benzene monomer and eximer , 1980 .

[5]  Monitoring the folding of Trp-cage peptide by two-dimensional infrared (2DIR) spectroscopy. , 2013, The journal of physical chemistry. B.

[6]  Andrew M. Moran,et al.  Two-Dimensional Electronic Spectroscopy in the Ultraviolet Wavelength Range. , 2012, The journal of physical chemistry letters.

[7]  Yu Zhang,et al.  Multidimensional attosecond resonant X-ray spectroscopy of molecules: lessons from the optical regime. , 2013, Annual review of physical chemistry.

[8]  Manuela Merchán,et al.  Density matrix averaged atomic natural orbital (ANO) basis sets for correlated molecular wave functions , 1995 .

[9]  Marco Garavelli,et al.  A tunable QM/MM approach to chemical reactivity, structure and physico-chemical properties prediction , 2007 .

[10]  K. P. Lawley,et al.  Ab initio methods in quantum chemistry , 1987 .

[11]  S. Mukamel,et al.  Simulation protocols for coherent femtosecond vibrational spectra of peptides. , 2006, The journal of physical chemistry. B.

[12]  Benjamin M. Bulheller,et al.  Ultraviolet spectroscopy of protein backbone transitions in aqueous solution: combined QM and MM simulations. , 2010, The journal of physical chemistry. B.

[13]  FRANCESCO AQUILANTE,et al.  MOLCAS 7: The Next Generation , 2010, J. Comput. Chem..

[14]  Marcus Beutler,et al.  Generation of high-energy sub-20 fs pulses tunable in the 250-310 nm region by frequency doubling of a high-power noncollinear optical parametric amplifier. , 2009, Optics letters.

[15]  Darius Abramavicius,et al.  Coherent Multidimensional Optical Spectroscopy of Excitons in Molecular Aggregates; Quasiparticle versus Supermolecule Perspectives , 2009 .

[16]  Katia Manova-Todorova,et al.  Picosecond dynamics of a membrane protein revealed by 2 D IR , 2006 .

[17]  P. Hamm,et al.  Watching hydrogen-bond dynamics in a β-turn by transient two-dimensional infrared spectroscopy , 2006, Nature.

[18]  Prabuddha Mukherjee,et al.  Picosecond dynamics of a membrane protein revealed by 2D IR. , 2006, Proceedings of the National Academy of Sciences of the United States of America.

[19]  Per-Olof Widmark,et al.  Density matrix averaged atomic natural orbital (ANO) basis sets for correlated molecular wave functions , 1990 .

[20]  George C. Schatz,et al.  The journal of physical chemistry letters , 2009 .

[21]  G A Petsko,et al.  Aromatic-aromatic interaction: a mechanism of protein structure stabilization. , 1985, Science.

[22]  R. Hochstrasser,et al.  STRUCTURE OF THE AMIDE I BAND OF PEPTIDES MEASURED BY FEMTOSECOND NONLINEAR-INFRARED SPECTROSCOPY , 1998 .

[23]  S. Mukamel,et al.  The coupled electronic oscillators vs the sum‐over‐states pictures for the optical response of octatetraene , 1996 .

[24]  S. Mukamel,et al.  Probing amyloid fibril growth by two-dimensional near-ultraviolet spectroscopy. , 2011, The journal of physical chemistry. B.

[25]  S. Matsika,et al.  Two-dimensional ultrafast fourier transform spectroscopy in the deep ultraviolet. , 2009, Optics express.

[26]  Kerstin Andersson,et al.  Second-order perturbation theory with a CASSCF reference function , 1990 .

[27]  P. Weber,et al.  Ultrafast Dynamics in Superexcited States of Phenol , 2001 .

[28]  S. Mukamel,et al.  Two-dimensional near-ultraviolet spectroscopy of aromatic residues in amyloid fibrils: a first principles study. , 2011, Physical chemistry chemical physics : PCCP.

[29]  Giulio Cerullo,et al.  Ab Initio Simulations of Two-Dimensional Electronic Spectra: The SOS//QM/MM Approach , 2014 .

[30]  Martin T. Zanni,et al.  Concepts and Methods of 2D Infrared Spectroscopy , 2011 .