k Research Interests

Vibrational Excitons in Polypeptides

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The ongoing progress in the field of ultrafast infrared spectroscopy has brought new interest to the studies of ultrafast vibrational dynamics in biologically relevant molecular systems also initiating various accompanying theoretical simulations. In particular, the long--standing debate on the existence of self--trapped vibrational states in alpha-helical polypeptides has been reanimated. Following the idea of the so-called Davydov soliton proposed some three decades ago exciton self-trapping in these systems has been extensively studied theoretically. However, an experimental proof for the existence of self-trapped states in alpha-helices has been lacking until recently. Using infrared femtosecond spectroscopy the observation of self-trapped N-H first overtone stretching vibrations in dissolved poly-gamma-benzyl-L-glutamate helices has been reported. The interpretation of the transient absorption spectra (TAS) was mainly based on recent theoretical work. Within a linear chain model as well as a three-dimensional model of an alpha-helical polypeptide vibrational single and two-exciton self-trapped states have been obtained assuming a coupling to low-frequency longitudinal helix vibrations. The two energetically lowest two-exciton self-trapped levels could be assigned to the observed peaks in the excited state absorption part of the TAS.
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While these approaches directly aim at a calculation of the spectrum of the high-frequency amide group vibrations dressed by low-frequency longitudinal helix vibrations we suggested an alternative computational scheme. Instead of carrying out different approximate canonical transformations of the original Hamiltonian we, first, computed the adiabatic single and two-exciton states of the system. They follow as overall eigenstates but with the longitudinal helix coordinates treated as parameters. These types of calculations resulted in an approximate picture of the spectrum with the focus on single and double amide I-excitation. In a second step, the results have been improved by a numerically exact solution of the complete time-dependent Schroedinger equation. To study a sufficiently long chain we did not perform calculations for the 3D helix structure but considered a model for one of the three linear chains of hydrogen bonded amide groups. Then, up to nine low-frequency coordinates of the longitudinal amide group displacements could be considered. A numerical solution of the respective Schroedinger equation became possible by using the multiconfiguration time-dependent Hartree (MCTDH) method. Within this method the total wavefunction is represented as a time-dependent superposition of products of time-dependent single coordinate wave functions (time-dependent Hartree products). Based on the Dirac--Frenkel variational principle, equations of motion are formulated for the expansion coefficients as well as for the single coordinate wave functions. Since the latter depend on time, they may be adapted to the full wavefunction, thus drastically reducing the numerical effort compared to a standard basis set expansion with time independent functions. The energetically lowest single and two--exciton state could be determined via imaginary time propagation done within the MCTDH method. Real time propagation of the complete wavefunction enabled us to obtain the linear absorption spectrum and the TAS. This has been achieved in using the time-dependent formulation of the absorption spectra. It offers the complete set of single and two-exciton states coupled to the longitudinal helix vibrations together with the oscillator strengths of linear and excited state absorption. Therefore, our treatment also improves other studies. Besides the description of transitions into the different exciton levels our calculations also account for the multitude of satellites related to the longitudinal chain vibrations. Thus, a more realistic description of what has been observed in the experiment could be achieved.
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Literature:

  1. D. Tsivlin and V. May:
    Multidimensional Wave Packet Dynamics in Polypeptides.
    Coupled Amide--Exciton Chain--Vibrational Motion in an alpha-Helix.
    Chem. Phys. (2007), available online.
  2. D. V. Tsivlin and V. May:
    Self-Trapping of the N-H Vibrational Mode in alpha-Helical Polypeptides
    J. Chem. Phys. 125, 224902 (2006).
  3. D. V. Tsivlin, H.-D. Meyer, and V. May:
    Vibrational Excitons in alpha-Helical Polypeptides:
    Multiexciton Self-Trapping and Related Infrared Transient Absorption
    J. Chem. Phys. 124, 134907 (2006).