mWe measured the Y~~-~,~ Raman band of horse heart deoxymyoglobin and human deoxyhemoglobin as a function of temperature between 10 and 300 K. A self-consistent spectral analysis of the deoxymyoglobin Raman band reveals that it is underlied by three different sublines with frequencies at f l , = 209 cm-', i12 = 217 cm-', and R, = 225 cm-' and an identical half-width of 13 cm-l. All these parameters were found to be independent of temperature. These sublines were attributed to different conformational substates of the Fe2+-His F8 linkage, which comprise different out-off-plane displacements of the heme iron and tilt angles of the Fe2+-N,(His F8) bond. The intensity ratio 1J12 exhibits a van't Hoff behavior between 150 and 300 K, bends over in a region between 150 and 80 K, and remains constant at lower temperature. In contrast, I2/I1 shows a maximum at 170 K and approaches a constant value at 80 K. These data can be fitted by a modified van't Hoff expression, which accounts for the freezing into nonequilibrium distributions of substrates in a temperature interval AT around a distinct temperature TI and also for the linear temperature dependence of the protein's specific heat. The fits to the above intensity ratios yield a freezing temperature of TI = 117 K and a transition region of AT = 55 K. The v~~-~~~ Raman band of human deoxyhemoglobin was decomposed into seven sublines with frequencies at 195,202,211,218,226,234, and 240 cm-', with half-widths of 12 cm-'. While the low-frequency sublines are strong at
GILCH ET AL.300 K, the high-frequency sublines dominate the band at cryogenic temperatures. In comparison, we also investigated the temperature dependence of the near-infrared band I11 at 760 nm. Band I11 of deoxymyoglobin can be decomposed into two subbands which are 165 cm-l apart. The ratio of their absorption cross sections shows a temperature dependence which parallels that of the ratio I 3 / ( I 2 + I,) of the corresponding Raman sublines. Band I11 of deoxyhemoglobin was decomposed into three subbands, the absorption cross sections of which also depend on temperature , similar to what has been observed for the v~~-~~~ subbands. These observations provide strong evidence that the frequency positions of the subbands of band I11 and the v~~-~~~ sublines are governed by the same coordinates. For both proteins investigated, the frequency positions and the half-widths of the band I11 subbands depend significantly on temperature. This is rationalized in terms of an earlier proposed model (Cupane et al., Eur. Biophys. J. 21; 385 1993) which assumes that the corresponding electronic transition is coupled to a bath of low-frequency modes. Our data indicate that these modes are harmonic below 130 K but become anharmonic above this temperature. This onset of anharmonic motions is interpreted as resulting from conformational transitions within the protein which affect the prostethic group via heme-protein coupling.