Ultrafast exciton dynamics in molecular systems

The theory of subpicosecond Frenkel exciton dynamics in molecular systems is reviewed with emphasis on a stepwise imp loved description of the coupling to intra- and intermolecular vibrations. After introducing the concept of multiexciton states the motion of electronic Frenkel excitons as they appear in light harvesting antennae of photosynthetic organisms is discussed. The description is based on a multiexciton density matrix theory which accounts for the exciton-vibrational coupling in a perturbative manner. Some improvements of this density matrix theory as suggested in literature are shortly mentioned. Afterwards, vibrational Frenkel excitons as found in polypeptides are considered. By utilizing the multiconfiguration time-dependent Hartree method an exact description of the coupling to longitudinal vibrations of the peptide chain becomes possible. The discussion of the computed transient infrared absorption spectra is supported by the introduction of adiabatic single- and two-exciton states. (Less)

[1]  Volkhard May,et al.  Controlling excitonic wavepacket motion in the PS1 core-antenna system , 2004 .

[2]  Thomas Renger,et al.  Ultrafast excitation energy transfer dynamics in photosynthetic pigment–protein complexes , 2001 .

[3]  V. May,et al.  Adiabatic vibrational excitons: Amide I states in α-helices as an example , 2005 .

[4]  C. Hunter,et al.  Emitting excitonic polaron states in core LH1 and peripheral LH2 bacterial light-harvesting complexes , 2004 .

[5]  V. May,et al.  Vibrational excitons in alpha-helical polypeptides: multiexciton self-trapping and related infrared transient absorption. , 2006, The Journal of chemical physics.

[6]  M. Beck,et al.  The multiconfiguration time-dependent Hartree (MCTDH) method: A highly efficient algorithm for propa , 1999 .

[7]  V. May,et al.  Exciton exciton annihilation dynamics in chromophore complexes. II. Intensity dependent transient absorption of the LH2 antenna system. , 2004, The Journal of chemical physics.

[8]  D. L. Dexter A Theory of Sensitized Luminescence in Solids , 1953 .

[9]  S. Mukamel,et al.  Polarons, localization, and excitonic coherence in superradiance of biological antenna complexes , 1997 .

[10]  Volkhard May,et al.  Charge and Energy Transfer Dynamics in Molecular Systems: A Theoretical Introduction , 2000 .

[11]  V. May,et al.  Theory of linear absorption spectra of biological and non-biological chromophore complexes , 2002 .

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

[13]  V. Sundström,et al.  Microscopic Theory of Exciton Annihilation: Application to the LH2 Antenna System , 2001 .

[14]  R. Knox,et al.  Theory of Molecular Excitons , 1964 .

[15]  M. Kasha Molecular Excitons in Small Aggregates , 1976 .

[16]  R. Marcus,et al.  Photophysical Properties of PS-2 Reaction Centers and a Discrepancy in Exciton Relaxation Times† , 2002 .

[17]  S. Mukamel,et al.  Linear and nonlinear infrared signatures of local α- and 310-helical structures in alanine polypeptides , 2003 .

[18]  C. Falvo,et al.  Relaxation channels of two-vibron bound states in alpha-helix proteins. , 2003, Physical review. E, Statistical, nonlinear, and soft matter physics.

[19]  V. May,et al.  Exciton exciton annihilation dynamics in chromophore complexes. I. Multiexciton density matrix formulation , 2003 .

[20]  S. Mukamel Principles of Nonlinear Optical Spectroscopy , 1995 .

[21]  A. A. Maradudin,et al.  Modern Problems in Condensed Matter Sciences , 1991 .

[22]  S. Mukamel,et al.  Two‐exciton spectroscopy of photosynthetic antenna complexes: Collective oscillator analysis , 1996 .

[23]  S. Mukamel,et al.  Multiple Exciton Coherence Sizes in Photosynthetic Antenna Complexes viewed by Pump−Probe Spectroscopy , 1997 .

[24]  V. Pouthier Two-vibron bound states in alpha-helix proteins: the interplay between the intramolecular anharmonicity and the strong vibron-phonon coupling. , 2003, Physical review. E, Statistical, nonlinear, and soft matter physics.

[25]  Alwyn C. Scott,et al.  Davydov’s Soliton , 1992 .

[26]  Shaul Mukamel,et al.  Dielectric friction and the transition from adiabatic to nonadiabatic electron transfer. I. Solvation dynamics in Liouville space , 1988 .

[27]  Leonas Valkunas,et al.  NONLINEAR ANNIHILATION OF EXCITONS.: THEORY , 2000 .

[28]  Th. Förster Zwischenmolekulare Energiewanderung und Fluoreszenz , 1948 .

[29]  Volkhard May,et al.  Ultrafast Laser Pulse Control of Exciton Dynamics: A Computational Study on the FMO Complex† , 2004 .

[30]  S. Mukamel,et al.  Exciton-migration and three-pulse femtosecond optical spectroscopies of photosynthetic antenna complexes , 1998 .

[31]  T. Pullerits,et al.  Potential surfaces and delocalization of excitons in dimers , 2002 .

[32]  P. Hamm,et al.  Direct Observation of Self-Trapped Vibrational States in α-Helices , 2004 .

[33]  R. Grondelle,et al.  Energy-transfer dynamics in the LHCII complex of higher plants: Modified redfield approach , 2004 .

[34]  B. Bartolo,et al.  Spectroscopy of the Excited State , 1976 .

[35]  S. Mukamel,et al.  Tunneling versus sequential long‐range electron transfer: Analogy with pump–probe spectroscopy , 1989 .

[36]  H. Sumi,et al.  Theory of Excitation Transfer in the Intermediate Coupling Case , 1999 .