To use all functions of this page, please activate cookies in your browser.
my.chemeurope.com
With an accout for my.chemeurope.com you can always see everything at a glance – and you can configure your own website and individual newsletter.
 My watch list
 My saved searches
 My saved topics
 My newsletter
Davydov soliton
Additional recommended knowledgeDavydov soliton is a quantum quasiparticle representing a propagating along the protein αhelix selftrapped amide I excitation that is a solution of the Davydov Hamiltonian. The Davydov model describes the interaction of the amide I vibrations with the hydrogen bonds that stabilize the αhelix of proteins. The elementary excitations within the αhelix are given by the phonons which correspond to the deformational oscillations of the lattice, and the excitons which describe the internal amide I excitations of the peptide groups. Referring to the atomic structure of an αhelix region of protein the mechanism that creates the Davydov soliton (polaron, exciton) can be described as follows: vibrational energy of the C=O stretching (or amide I) oscillators that is localized on the αhelix acts through a phonon coupling effect to distort the structure of the αhelix, while the helical distortion reacts again through phonon coupling to trap the amide I oscillation energy and prevent its dispersion. This effect is called selflocalization or selftrapping. ^{[1]}^{[2]}^{[3]} Solitons in which the energy is distributed in a fashion preserving the helical symmetry are dynamically unstable, and such symmetrical solitons once formed decay rapidly when they propagate. On the other hand, an asymmetric soliton which spontaneously breaks the local translational and helical symmetries possesses the lowest energy and is a robust localized entity. ^{[4]} Davydov's Hamiltonian is formally similar to the FröhlichHolstein Hamiltonian for the interaction of electrons with a polarizable lattice. Thus the Hamiltonian of the energy operator is
where is the quasiparticle (exciton) Hamiltonian, which describes the motion of the amide I excitations between adjacent sites; is the phonon Hamiltonian, which describes the vibrations of the lattice; and is the interaction Hamiltonian, which describes the interaction of the amide I excitation with the lattice. ^{[1]}^{[2]}^{[3]} The quasiparticle (exciton) Hamiltonian is:
where the index counts the peptide groups along the αhelix spine, the index α = 1,2,3 counts each αhelix spine, J is the energy of the amide I vibration (CO stretching), J is the dipoledipole coupling energy between a particular amide I bond and those ahead and behind along the same spine, J is the dipoledipole coupling energy between a particular amide I bond and those on adjacent spines in the same unit cell of the protein αhelix, and are respectively the boson creation and annihilation operator for a quasiparticle at the peptide group. n,α ^{[5]}^{[6]} The phonon Hamiltonian is
Finally, the interaction Hamiltonian is
The mathematical techniques that are used to analyze Davydov's soliton are similar to some that have been developed in polaron theory. In this context the Davydov's soliton corresponds to a polaron that is (i) large so the continuum limit approximation in justified, (ii) acoustic because the selflocalization arises from interactions with acoustic modes of the lattice, and (iii) weakly coupled because the anharmonic energy is small compared with the phonon bandwidth ^{[5]}. The Davydov soliton is a quantum quasiparticle and it obeys Heisenberg's uncertainty principle. Thus any model that does not impose translational invariance is flawed by construction ^{[5]}. Supposing that the Davydov soliton is localized to 5 turns of the αhelix results in significant uncertainty in the velocity of the soliton Δv = 133 m/s, a fact that is obscured if one models the Davydov soliton as a classical object. There are three possible fundamental approaches towards Davydov model: ^{[6]}^{[8]} (i) the quantum theory, in which both the amide I vibration (excitons) and the lattice site motion (phonons) are treated quantum mechanically; (ii) the mixed quantumclassical theory, in which the amide I vibration is treated quantum mechanically but the lattice is classical; and (iii) the classical theory, in which both the amide I and the lattice motions are treated classically. References


This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article "Davydov_soliton". A list of authors is available in Wikipedia. 