The human cofactor complexes ARC (activator-recruited cofactor) and CRSP (cofactor required for Sp1 activation) mediate activator-dependent transcription in vitro. Although these complexes share several common subunits, their structural and functional relationships remain unknown. Here, we report that affinity-purified ARC consists of two distinct multisubunit complexes: a larger complex, denoted ARC-L, and a smaller coactivator, CRSP. Reconstituted in vitro transcription with biochemically separated ARC-L and CRSP reveals differential cofactor functions. The ARC-L complex is transcriptionally inactive, whereas the CRSP complex is highly active. Structural determination by electron microscopy (EM) and three-dimensional reconstruction indicate substantial differences in size and shape between ARC-L and CRSP. Moreover, EM analysis of independently derived CRSP complexes reveals distinct conformations induced by different activators. These results suggest that CRSP may potentiate transcription via specific activator-induced conformational changes.
Resonance Raman vibrational spectra of the Pr, lumi-R, and Pfr forms of phytochrome have been obtained using low-temperature trapping and room temperature flow techniques in conjunction with shifted-excitation Raman difference spectroscopy (SERDS). The Pr to lumi-R photoconversion exhibits a thermal barrier and is completely blocked at 30 K, indicating that thermally assisted protein relaxation is necessary for the primary photochemistry. When Pr is converted to lumi-R, new bands appear in the C = C and C = N stretching regions at 1651, 1636, 1590, and 1569 cm-1, indicating that a significant structural change of the chromophore has occurred. The photoconversion also results in an 18 cm-1 decrease in the N-H rocking band in lumi-R. Normal mode calculations correlate this frequency drop with a change in the geometry of the C15 methine bridge of the phytochromobilin chromophore. Additionally, a C = N stretching mode marker band shifts from 1576 cm-1 in Pr to 1569 cm-1 in lumi-R and to 1552 cm-1 in Pfr. Normal mode calculations show that the frequency drop of this band in the lumi-R-->Pfr interconversion is an indication of a C14-C15 syn-->anti conformational change. Moderately intense hydrogen out-of-plane modes that occur at 805 cm-1 in Pr shift to 829 and 847 cm-1 upon photoconversion to lumi-R and are replaced by a very intense mode at 814 cm-1 in Pfr. These observations indicate that the C and D rings of the chromophore in Pr and lumi-R are moderately planar but that they become highly distorted in Pfr. This information suggests that the primary photochemistry in phytochrome is a Z-->E isomerization of the C15 = C16 bond of Pr giving lumi-R. This is followed by a thermal syn-->anti C14-C15 conformational relaxation to form Pfr. A four-state model is presented to explain the chromophore structural changes in Pr, lumi-R, and Pfr that uses hydrogen bonding to the surrounding protein to stabilize the high-energy Pfr C15 = C16, C14-C15, E,anti chromophore structure. This implicates an anchor and release mechanism between the chromophore and protein that might lead to altered biological signaling in the plant.
Resonance Raman spectra of native and recombinant analogues of oat phytochrome have been obtained and analyzed in conjunction with normal mode calculations. On the basis of frequency shifts observed upon methine bridge deuteration and vinyl and C(15)-methine bridge saturation of the chromophore, intense Raman lines at 805 and 814 cm(-)(1) in P(r) and P(fr), respectively, are assigned as C(15)-hydrogen out-of-plane (HOOP) wags, lines at 665 cm(-)(1) in P(r) and at 672 and 654 cm(-)(1) in P(fr) are assigned as coupled C=C and C-C torsions and in-plane ring twisting modes, and modes at approximately 1300 cm(-)(1) in P(r) are coupled N-H and C-H rocking modes. The empirical assignments and normal mode calculations support proposals that the chromophore structures in P(r) and P(fr) are C(15)-Z,syn and C(15)-E,anti, respectively. The intensities of the C(15)-hydrogen out-of-plane, C=C and C-C torsional, and in-plane ring modes in both P(r) and P(fr) suggest that the initial photochemistry involves simultaneous bond rotations at the C(15)-methine bridge coupled to C(15)-H wagging and D-ring rotation. The strong nonbonded interactions of the C- and D-ring methyl groups in the C(15)-E,anti P(fr) chromophore structure indicated by the intense 814 cm(-1) C(15) HOOP mode suggest that the excited state of P(fr) and its photoproduct states are strongly coupled.
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