Resonance Raman spectroscopic study of the tryptic 39-kDa fragment of phytochrome

The 39-kDa fragment of oat phytochrome phyA, obtained by tryptic digestion at the amino acids 65 and 425, was studied by resonance Raman spectroscopy. The parent state P(r) reveals far-reaching similarities with that of the native phytochrome implying that the structures of the tetrapyrrole chromophore and its immediate protein environment are not affected by the proteolysis. However, the resonance Raman spectrum of the final product of the P(r) phototransformation, denoted as P(bl), is more closely related to that of the P(fr) precursor of the native phytochrome, i.e. meta-R(C), rather than to that of P(fr) itself. The resonance Raman spectra indicate a high conformational flexibility of the chromophore in P(bl) so that, unlike in P(fr), the tetrapyrrole rings C and D adopt a largely coplanar conformation. The protein interactions with ring D of the chromophore, which in the native phytochrome stabilize the specific chromophore structure of P(fr), cannot be established in the 39-kDa fragment due to the lack of the major C-terminal part of the protein. These findings, furthermore, support the view that the meta-R(C)-->P(fr) transition is associated with a coupling of chromophore and protein structural changes that represent crucial events for the photoactivation of phytochrome.     

How color visual pigments are tuned.

The absorption maximum of the retinal chromophore in color visual pigments is tuned by interactions with the protein (opsin) to which it is bound. Recent advances in the expression of rhodopsin-like transmembrane receptors and in spectroscopic techniques have allowed us to measure resonance Raman vibrational spectra of the retinal chromophore in recombinant visual pigments to examine the molecular basis of this spectral tuning. The dominant physical mechanism responsible for the opsin shift in color vision is the interaction of dipolar amino acid residues with the ground- and excited-state charge distributions of the chromophore.     

Anthracycline antibiotic arugomycin binds in both grooves of the DNA helix simultaneously: an NMR and molecular modelling study.

Perturbations to the 1H and 31P chemical shifts of DNA resonances together with twenty-four intermolecular nuclear Overhauser effects show that the anthracycline antibiotic arugomycin intercalates between the basepairs of the hexamer duplex d(5'-GCATGC)2 at the 5'-CpA and 5'-TpG binding sites. In the complex two drug molecules are bound per duplex with full retention of the dyad symmetry. Arugomycin adopts a threaded binding orientation with chains of sugars positioned in both the major and minor groove of the helix simultaneously. The complex is stabilized by hydrogen bonding, electrostatic and van der Waals interactions principally in the major groove and involving substituents on the rigidly oriented bicycloamino-glucose sugar of the antibiotic. A specific hydrogen bond is identified between the C2'-hydroxyl and the guanine N7 at the intercalation site. Together, interactions in the major groove appear to account for the intercalation specificity of arugomycin that requires both a guanine and thymine at the intercalation site. We are unable to identify any sequence specific interactions between the minor groove and the arugarose sugar (S1) which binds only weakly, through van der Walls contacts, over the d(GCA).d(TGC) trinucleotide sequence. The data indicate that the sugar chains of arugomycin are flexible and play little part in the interaction of the antibiotic with DNA. The intensity of sequential internucleotide NOEs identifies the intercalation site as being assymmetric. A family of conformers computed using restrained energy minimisation and molecular dynamics indicate that basepair buckling is a feature of the anthracycline intercalation site that may serve to maximise intermolecular van der Waals interactions by wrapping the basepairs around the antibiotic chromophore.     

Ultraviolet resonance Raman study of DNA and of its interaction with actinomycin D.

The DNA-Actinomycin D interaction has been studied by resonance Raman effect using DNA as chromophore. First, the resonance Raman spectra of DNA obtained with a U.V. excitation at wavelengths of 300 nm and 280 nm are presented. The main Raman hands are assigned to the convenient nucleic bases by comparison with the spectra of mononucleotides obtained under the same experimental conditions. In particular, with a 300 nm excitation, the 1582 cm-1 line is provided by adenine, while the 1492 cm-1 one is almost exclusively due to guanine. Then, the DNA-Actinomycin D complex has been studied: the line enhancements and the specificity of the resonance permits the displaying of the DNA spectrum free of any contribution of Actinomycin. The interaction provides a large intensity decrease of the 1492 cm-1 guanine line: this is a direct consequence of the orbital overlapping of the guanine 2-aminogroup with the ring nitrogen of Actinomycin in the DNA-Actinomycin pi complex.     

Binding of actinomycin D to [d(ATCGAT)]2: NMR evidence of multiple complexes

Actinomycin D (actD) binds to the oligonucleotide [d(ATCGAT)]2 with a hypochromatic and red-shifted visible absorbance band compared to free drug and a CD spectrum with double negative bands at 460 and 385 nm. These spectral features are similar to those of the actD-[d(ATGCAT)]2 complex, while actD-[d(AT)5]2 gives spectra similar to those of free drug. Upon dilution or raising the temperature, the spectral characteristics accompanying complex formation disappear in the actD-[(ATCGAT)]2 sample but remain in the actD-[d(ATGCAT)]2 complex under the same experimental conditions. These results suggest that (a) sequence-specific binding of actD occurs with [d(ATCGAT)]2 but not with [d(AT)5]2, (b) the binding is not as strong as with [d(ATGCAT)]2, and (c) actD binds [d(ATCGAT)]2 with the same mechanism as it binds [d(ATGCAT)]2, i.e., by intercalation. From NMR spectra of the actD-[d(ATCGAT)]2 complex, three types of signals can be detected below 20 degrees C, one major and two minor ones. At higher temperatures, exchange between the two minor ones becomes fast enough that only one type of minor signal was seen. Partial resonance assignments were made by using 2D nuclear Overhauser effect (NOE) and 2D homonuclear Hartmann-Hahn (HOHAHA) experiments. Proton chemical shift changes of the major complex are consistent with actD chromophore ring intercalation between hexamer base pairs. Data from NOE-detected dipolar interactions between actD and [d(ATCGAT)]2 protons were interpreted in terms of a major complex with the actD chromophore ring system intercalated at the CG position and minor complexes with the drug intercalated off center at the GA positions.(ABSTRACT TRUNCATED AT 250 WORDS)     

Mode of reversible binding of neocarzinostatin chromophore to DNA: base sequence dependency of binding.

The reversible binding of neocarzinostatin chromophore to polynucleotides was studied in order to understand the molecular basis of its base sequence-specificity in DNA damage production. Studies of the spectroscopic and thermodynamic properties of chromophore-polynucleotide interactions reveal that the binding of the chromophore to poly(dA-dT) is qualitatively and quantitatively different from that to poly(dG-dC) (and poly(dI-dC]. From these and other experiments using double-stranded mixtures of homopolynucleotides, it is proposed that the observed A T specific intercalation might result from differential recognition of minor variations in the B-DNA type structure by the chromophore.     

Resonance Raman spectroscopy of octopus rhodopsin and its photoproducts

We report here the resonance Raman spectra of octopus rhodopsin and its photoproducts, bathorhodopsin and acid metarhodopsin. These studies were undertaken in order to make comparisons with the well-studied bovine pigments, so as to understand the similarities and the differences in pigment structure and photochemical processes between vertebrates and invertebrates. The flow method was used to obtain the Raman spectrum of rhodopsin at 13 degrees C. The bathorhodopsin spectrum was obtained by computer subtraction of the spectra containing different photostationary mixtures of rhodopsin, isorhodopsin, hypsorhodopsin, and bathorhodopsin, obtained at 12 K using the pump-probe technique and from measurements at 80 K. Like their bovine counterparts, the Schiff base vibrational mode appears at approximately 1660 cm-1 in octopus rhodopsin and the photoproducts, bathorhodopsin and acid metarhodopsin, suggesting a protonated Schiff base linkage between the chromophore and the protein. Differences between the Raman spectra of octopus rhodopsin and bathorhodopsin indicate that the formation of bathorhodopsin is associated with chromophore isomerization. This inference is substantiated by the chromophore chemical extraction data which show that, like the bovine system, octopus rhodopsin is an 11-cis pigment, while the photoproducts contain an all-trans pigment, in agreement with previous work. The octopus rhodopsin and bathorhodopsin spectra show marked differences from their bovine counterparts in other respects, however. The differences are most dramatic in the structure-sensitive fingerprint and the HOOP regions. Thus, it appears that although the two species differ in the specific nature of the chromophore-protein interactions, the general process of visual transduction is the same.     

DNA-nogalamycin interactions

The anthracycline antibiotic nogalamycin differs from the more common daunomycin-type anthracyclines by substitution on both ends of the intercalating chromophore, giving nogalamycin the approximate shape of a dumbbell. The chromophore of daunomycin is substituted on only one end. In nogalamycin, the positively charged amino sugar substituent of daunomycin is replaced by an uncharged nogalose sugar and a methyl ester group. The other end of nogalamycin, where daunomycin is unsubstituted, is fused to a bicyclo amino sugar with a positively charged dimethylamino group. Much larger DNA fluctuations are required for intercalative entry of nogalamycin than for entry of daunomycin. This report describes the X-ray crystal structure of the complex between nogalamycin and the self-complementary DNA hexamer d(me5CGTsAme5CG). The DNA contains cytosines methylated at the 5-positions and a phosphorothioate linkage at the TpA step. Nogalamycin intercalates at the terminal CpG steps and interacts with both strands in both grooves of the DNA. Large conformational adjustments in both nogalamycin and the DNA are necessary to form a stable, intercalative complex. The interactions of the bases with the nogalamycin substituents lead to sliding of bases relative to each other along the normal to Watson-Crick hydrogen bonds. The planarities of base pairs surrounding the intercalation site are distorted. The backbones of the two strands are distorted asymmetrically by nogalamycin with large deviations from standard B-DNA geometry. The complex between nogalamycin and DNA illustrates the conformational flexibility of DNA. The hydrogen-bonding interactions between nogalamycin and DNA do not suggest a sequence-specific binding of the drug, although additional secondary effects might lead to differences between various intercalation sites.     

Dependence of Mode of DNA Binding to Benzocrown Derivatives of Actinocin on the Size and Distance from the Chromophore of Crown Fragments

Complexes of DNA with benzocrown derivatives of actinocin were studied by viscometry and dynamic birefringence. Changes in the macromolecular structure of DNA caused by complex formation were determined. Models of DNA binding to the studied compounds were suggested on the basis of data obtained. The intercalation of actinocin chromophore of benzocrown derivatives of actinocin was shown to occur only when benzocrown groups were bound to the chromophore via the glycine spacer. A change of the distance between the crown group and the chromophore prevented ligand intercalation. Increase of the ionic strength resulted in appearance of a new, nonintercalative binding mode for crown-containing compounds determined by interaction of the crown groups with DNA.     

Resonance Raman studies of bovine metarhodopsin I and metarhodopsin II

The resonance Raman spectra of bovine metarhodopsin I and metarhodopsin II have been measured. The spectra are compared with model chromophore resonance Raman data. It was found that metarhodopsin I is linked to opsin via a protonated Schiff base linkage, whereas metarhodopsin II is linked by an unprotonated Schiff base. A recent suggestion that the chromophore of metarhodopsin II is retinal is explicitly disproved. The chromophores of both metarhodopsins are found to have an essentially all-trans conformation. The basic mechanism for color regulation in both forms appears to be electron delocalization. The data tend to support the model of cis-trans isomerization as the primary mechanism for vision. Also, the conclusions and inferences of this work on energy uses and storage by rhodopsin in neural generation are discussed.     

Dependence of mode of DNA binding to benzo crown derivatives of actinocin on the size and distance from the chromophore of crown fragments

Complexes of DNA with benzocrown derivatives of actinocin were studied by viscometry and dynamic birefringence. Changes in the macromolecular structure of DNA caused by complex formation were determined. Models of DNA binding to the studied compounds were suggested on the basis of data obtained. The intercalation of actinocin chromophore of benzocrown derivatives of actinocin was shown to occur only when benzocrown groups were bound to the chromophore via glycine fragment. A change in the distance between the crown group and the chromophore prevents ligand intercalation. Increase in medium ionic strength results in appearance of new nonintercalational binding mode for crown-containing compounds with DNA caused by interaction of the crown groups with DNA.     

DNA-drug interactions. The crystal structure of d(CGATCG) complexed with daunomycin

The structure of a d(CGATCG)-daunomycin complex has been determined by single crystal X-ray diffraction techniques. Refinement, with the location of 40 solvent molecules, using data up to 1.5 A, converged with a final crystallographic residual, R = 0.25 (RW = 0.22). The tetragonal crystals are in space group P4(1)2(1)2, with cell dimensions of a = 27.98 A and c = 52.87 A. The self-complementary d(CGATCG) forms a distorted right-handed helix with a daunomycin molecule intercalated at each d(CpG) step. The daunomycin aglycon chromophore is oriented at right-angles to the long axis of the DNA base-pairs. This head-on intercalation is stabilized by direct hydrogen bonds and indirectly via solvent-mediated, hydrogen-bonding interactions between the chromophore and its intercalation site base-pairs. The cyclohexene ring and amino sugar substituent lie in the minor groove. The amino sugar N-3' forms a hydrogen bond with O-2 of the next neighbouring thymine. This electrostatic interaction helps position the sugar in a way that results in extensive van der Waals contacts between the drug and the DNA. There is no interaction between daunosamine and the DNA sugar-phosphate backbone. We present full experimental details and all relevant conformational parameters, and use the comparison with a d(CGTACG)-daunomycin complex to rationalize some neighbouring sequence effects involved in daunomycin binding.     

Interaction of the C14-OH group of adriamycin with DNA phosphate as spectroscopically evidenced

Monitoring the band of the antisymmetric stretching vibration of the backbone PO-2 group in DNA-anthracycline complexes demonstrates an extraordinary wavenumber shift for the adriamycin complex compared to that of daunomycin. The structures of both anthracyclines, however, are very closely related and differ only by a surplus hydroxyl group of adriamycin in the C14 position. The wavenumber shift observed for the DNA-adriamycin complex is unequivocally attributed to an additional linkage of the C14-OH of adriamycin to the phosphate group of DNA. Thus, several of the hypothetical structural models for the DNA-adriamycin complex for which a hydrogen bond between the C14 hydroxyl of the drug and DNA phosphate was postulated (S. Neidle, Cancer Treatment Rep. 61, 928 (1977); G. J. Quigley et. al., Proc. Natl. Acad. Sci. USA 77, 7204 (1980)) get the first clear-cut experimental evidence.     

Electronic and vibrational spectroscopy of the cytochrome c:cytochrome c oxidase complexes from bovine and Paracoccus denitrificans.

The 1:1 complex between horse heart cytochrome c and bovine cytochrome c oxidase, and between yeast cytochrome c and Paracoccus denitrificans cytochrome c oxidase have been studied by a combination of second derivative absorption, circular dichroism (CD), and resonance Raman spectroscopy. The second derivative absorption and CD spectra reveal changes in the electronic transitions of cytochrome a upon complex formation. These results could reflect changes in ground state heme structure or changes in the protein environment surrounding the chromophore that affect either the ground or excited electronic states. The resonance Raman spectrum, on the other hand, reflects the heme structure in the ground electronic state only and shows no significant difference between cytochrome a vibrations in the complex or free enzyme. The only major difference between the Raman spectra of the free enzyme and complex is a broadening of the cytochrome a3 formyl band of the complex that is relieved upon complex dissociation at high ionic strength. These data suggest that the differences observed in the second derivative and CD spectra are the result of changes in the protein environment around cytochrome a that affect the electronic excited state. By analogy to other protein-chromophore systems, we suggest that the energy of the Soret pi* state of cytochrome a may be affected by (1) changes in the local dielectric, possibly brought about by movement of a charged amino acid side chain in proximity to the heme group, or (2) pi-pi interactions between the heme and aromatic amino acid residues.     

Protonation state and structural changes of the tetrapyrrole chromophore during the Pr --> Pfr phototransformation of phytochrome: a resonance Raman spectroscopic study

The photoconversion of phytochrome (phytochrome A from Avena satina) from the inactive (Pr) to the physiologically active form (Pfr) was studied by near-infrared Fourier transform resonance Raman spectroscopy at cryogenic temperatures, which allow us to trap the intermediate states. Nondeuterated and deuterated buffer solutions were used to determine the effect of H/D exchange on the resonance Raman spectra. For the first time, reliable spectra of the "bleached" intermediates meta-R(A) and meta-R(C) were obtained. The vibrational bands in the region 1300-1700 cm(-)(1), which is particularly indicative of structural changes in tetrapyrroles, were assigned on the basis of recent calculations of the Raman spectra of the chromophore in C-phycocyanin and model compounds [Kneip, C., Hildebrandt, P., Németh, K., Mark, F., Schaffner, K. (1999) Chem. Phys. Lett. 311, 479-485]. The experimental resonance Raman spectra Pr are compatible with the Raman spectra calculated for the protonated ZZZasa configuration, which hence is suggested to be the chromophore structure in this parent state of phytochrome. Furthermore, marker bands could be identified that are of high diagnostic value for monitoring structural changes in individual parts of the chromophore. Specifically, it could be shown that not only in the parent states Pr and Pfr but also in all intermediates the chromophore is protonated at the pyrroleninic nitrogen. The spectral changes observed for lumi-R confirm the view that the photoreaction of Pr is a Z --> E isomerization of the CD methine bridge. The subsequent thermal decay reaction to meta-R(A) includes relaxations of the CD methine bridge double bond, whereas the formation of meta-R(C) is accompanied by structural adaptations of the pyrrole rings B and C in the protein pocket. The far-reaching similarities between the chromophores of meta-R(A) and Pfr suggest that in the step meta-R(A) --> Pfr the ultimate structural changes of the protein matrix occur.     

Ultraviolet resonance Raman spectroscopy of distamycin complexes with poly(dA)-poly(dT) and poly(dA-dT): role of H-bonding

Raman spectra are reported for distamycin, excited at 320 nm, in resonance with the first strong absorption band of the chromophore. Qualitative band assignments to pyrrole ring and amide modes are made on the basis of frequency shifts observed in D2O. When distamycin is dissolved in dimethyl sulfoxide or dimethylformamide, large (30 cm-1) upshifts are seen for the band assigned to amide I, while amides II and III shift down appreciably. Similar but smaller shifts are seen when distamycin is bound to poly(dA-dT) and poly(dA)-poly(dT). Examination of literature data for N-methylacetamide in various solvents shows that the amide I frequencies correlate well with solvent acceptor number but poorly with solvent donor number. This behavior implies that acceptor interactions with the C = O group are more important than donor interactions with the N-H group in polarizing the amide bond and stabilizing the zwitterionic resonance form. The resonance Raman spectra therefore imply that the distamycin C = O groups, despite being exposed to solvent, are less strongly H-bonded in the polynucleotide complexes than in aqueous distamycin, perhaps because of orienting influences of the nearby backbone phosphate groups. In this respect, the poly(dA-dT) and poly(dA)-poly(dT) complexes are the same, showing the same RR frequencies. Resonance Raman spectra were also obtained at 200-nm excitation, where modes of the DNA residues are enhanced. The spectra were essentially the same with and without distamycin, except for a perceptable narrowing of the adenine modes of poly(dA-dT), suggesting a reduction in conformational flexibility of the polymer upon drug binding.     

Light-induced proton release of phytochrome is coupled to the transient deprotonation of the tetrapyrrole chromophore

The Pr --> Pfr phototransformation of the bacteriophytochrome Agp1 from Agrobacterium tumefaciens and the structures of the biliverdin chromophore in the parent states and the cryogenically trapped intermediate Meta-R(C) were investigated with resonance Raman spectroscopy and flash photolysis. Strong similarities with the resonance Raman spectra of plant phytochrome A indicate that in Agp1 the methine bridge isomerization state of the chromophore is ZZZasa in Pr and ZZEssa in Pfr, with all pyrrole nitrogens being protonated. Photoexcitation of Pr is followed by (at least) three thermal relaxation components in the formation of Pfr with time constants of 230 micros and 3.1 and 260 ms. H2O/D2O exchange reveals kinetic isotope effects of 1.9, 2.6, and 1.3 for the respective transitions that are accompanied by changes of the amplitudes. The second and the third relaxation correspond to the formation and decay of Meta-R(C), respectively. Resonance Raman measurements of Meta-R(C) indicate that the chromophore adopts a deprotonated ZZE configuration. Measurements with a pH indicator dye show that formation and decay of Meta-R(C) are associated with proton release and uptake, respectively. The stoichiometry of the proton release corresponds to one proton per photoconverted molecule. The coupling of transient chromophore deprotonation and proton release, which is likely to be an essential element in the Pr --> Pfr photocon-version mechanism of phytochromes in general, may play a crucial role for the structural changes in the final step of the Pfr formation that switch between the active and the inactive state of the photoreceptor.     

Daunomycin intercalation stabilizes distinct backbone conformations of DNA

Daunomycin is a widely used antibiotic of the anthracycline family. In the present study we reveal the structural properties and important intercalator-DNA interactions by means of molecular dynamics. As most of the X-ray structures of DNA-daunomycin intercalated complexes are short hexamers or octamers of DNA with two drug molecules per doublehelix we calculated a self complementary 14-mer oligodeoxyribonucleotide duplex d(CGCGCGATCGCGCG)2 in the B-form with two putative intercalation sites at the 5'-CGA-3' step on both strands. Consequently we are able to look at the structure of a 1:1 complex and exclude crystal packing effects normally encountered in most of the X-ray crystallographic studies conducted so far. We performed different 10 to 20 ns long molecular dynamics simulations of the uncomplexed DNA structure, the DNA-daunomycin complex and a 1:2 complex of DNA-daunomycin where the two intercalator molecules are stacked into the two opposing 5'-CGA-3' steps. Thereby--in contrast to X-ray structures--a comparison of a complex of only one with a complex of two intercalators per doublehelix is possible. The chromophore of daunomycin is intercalated between the 5'-CG-3' bases while the daunosamine sugar moiety is placed in the minor groove. We observe a flexibility of the dihedral angle at the glycosidic bond, leading to three different positions of the ammonium group responsible for important contacts in the minor groove. Furthermore a distinct pattern of BI and BII around the intercalation site is induced and stabilized. This indicates a transfer of changes in the DNA geometry caused by intercalation to the DNA backbone.     

Chromophore structure in lumirhodopsin and metarhodopsin I by time-resolved resonance Raman microchip spectroscopy.

Time-resolved resonance Raman microchip flow experiments have been performed on the lumirhodopsin (Lumi) and metarhodopsin I (Meta I) photointermediates of rhodopsin at room temperature to elucidate the structure of the chromophore in each species as well as changes in protein-chromophore interactions. Transient Raman spectra of Lumi and Meta I with delay times of 16 micros and 1 ms, respectively, are obtained by using a microprobe system to focus displaced pump and probe laser beams in a microfabricated flow channel and to detect the scattering. The fingerprint modes of both species are very similar and characteristic of an all-trans chromophore. Lumi exhibits a relatively normal hydrogen-out-of-plane (HOOP) doublet at 951/959 cm(-1), while Meta I has a single HOOP band at 957 cm(-1). These results suggest that the transitions from bathorhodopsin to Lumi and Meta I involve a relaxation of the chromophore to a more planar all-trans conformation and the elimination of the structural perturbation that uncouples the 11H and 12H wags in bathorhodopsin. Surprisingly, the protonated Schiff base C=N stretching mode in Lumi (1638 cm(-1)) is unusually low compared to those in rhodopsin and bathorhodopsin, and the C=ND stretching mode shifts down by only 7 cm(-1) in D2O buffer. This indicates that the Schiff base hydrogen bonding is dramatically weakened in the bathorhodopsin to Lumi transition. However, the C=N stretching mode in Meta I is found at 1654 cm(-1) and exhibits a normal deuteration-induced downshift of 24 cm(-1), identical to that of the all-trans protonated Schiff base. The structural relaxation of the chromophore-protein complex in the bathorhodopsin to Lumi transition thus appears to drive the Schiff base group out of its hydrogen-bonded environment near Glu113, and the hydrogen bonding recovers to a normal solvated PSB value but presumably a different hydrogen bond acceptor with the formation of Meta I.