Embedding biostructures in saccharide glasses protects them against extreme dehydration and/or exposure to very high temperature. Among the saccharides, trehalose appears to be the most effective bioprotectant. In this paper we report on the low-frequency dynamics of carbon monoxy myoglobin in an extremely dry trehalose glass measured by neutron spectroscopy. Under these conditions, the mean square displacements and the density of state function are those of a harmonic solid, up to room temperature, in contrast to D2O-hydrated myoglobin, in which a dynamical transition to a nonharmonic regime has been observed at approximately 180 K (Doster et al., 1989. Nature. 337:754-756). The protective effect of trehalose is correlated, therefore, with a trapping of the protein in a harmonic potential, even at relatively high temperature.

In this work we study the temperature dependence of the Soret band lineshape of the carbonmonoxy derivatives of sperm whale myoglobin, human hemoglobin, and its isolated alpha and beta subunits. To fit the observed spectral profile we use an analytic expression derived for a system whereby a single electronic transition is coupled to Franck-Condon active vibrational modes, within the adiabatic and harmonic approximation. The vibronic structure of the spectra arises from the coupling with high frequency modes; these modes contribute to the total line shape through a series of Lorentzians with peak positions at vibrational overtones and half width related to the time constant of the population decay of the excited electronic state (homogeneous broadening); moreover, the coupling with low frequency modes broadens each Lorentzian to a Voigtian. Inhomogeneous broadening is modeled as a gaussian distribution of the 0-0 transition frequencies and is therefore added as a constant term to the previous gaussian width. This spectral deconvolution enables us to investigate the different contributions to line broadening and the parameters that characterize the vibrational coupling, as well as their dependence upon protein and solvent composition. The investigation is carried out as a function of temperature in the range 20-300 K; relevant information is obtained by comparing experimental results with theoretical predictions. This work supports a description of the investigated proteins as heterogeneous systems, whose heterogeneity depends on the particular protein and on the composition of the external matrix. The delocalized pi electron cloud of the porphyrin ring is coupled not only to the high frequency vibrational modes of the active site but also to a "bath" of lower frequency modes that involve the entire protein; moreover at suitable temperatures (approximately 200 K), anharmonic motions, which are an obvious prerequisite for the jumping among different conformational substates, become evident.

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In this short review we show how suitable analysis of the temperature dependence of the optical absorption spectra of metalloproteins can give insight into their stereodynamic properties in the region of the chromophore. To this end, the theory of coupling between an intense allowed electronic transition of a chromophore and Franck-Condon active vibrations of the nearby atoms is applied to the Soret band of hemeproteins to obtain an analytical expression suitable for fitting the spectral profile at various temperatures. The reported approach enables one to separate the various contributions to the overall bandwidth together with the parameters that characterize the vibrational coupling. The thermal behavior of these quantities gives information on the dynamic properties of the active site and on their dependence upon protein structure and ligation state. The Soret band of hemeproteins appears to be coupled to high frequency vibrational modes of the heme group (as already shown by resonance Raman spectroscopy) and to a "bath" of low frequency modes most likely deriving from the bulk of the protein. For the deoxy derivatives inhomogeneous broadening arising from conformational heterogeneity appears to contribute substantially to the linewidth. The data indicate the onset, at temperatures near 180 K, of large scale anharmonic motions that can be attributed to jumping among different conformational substates of the protein.