Cone excitations and color vision.
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Animals↗
Biomedical subjects
R A Mathies
Publications and source records attributed to R A Mathies.
Ultraviolet resonance Raman spectroscopy of bacteriorhodopsin.
Ultraviolet resonance Raman spectra of bacteriorhodopsin have been obtained using 229 nm excitation from a hydrogen-shifted neodymium yttrium aluminum garnet (Nd: YAG) laser. High signal-to-noise spectra are observed exhibiting vibrational bands at 762, 877, 1011, 1175, 1356, 1552 and 1617 cm-1 which are assigned to scattering from tryptophan and tyrosine side chains. This demonstrates the feasibility of using UV resonance Raman spectroscopy to monitor aromatic amino acid structural changes during the bacteriorhodopsin photocycle.
Bacteriorhodopsins↗
Effects of modified chromophores on the spectral sensitivity of salamander, squirrel and macaque cones.
1. Chemically modified retinal chromophores were used to investigate the mechanisms that produce the characteristic spectral absorptions of cone pigments. Spectral sensitivities of single cones from the salamander, squirrel and macaque retina were determined by electrical recording. The chromophore was then replaced by bleaching the pigment and regenerating it with a retinal analogue. 2. Exposing a bleached cone to 9-cis-retinal for a brief period (less than 20 min) caused its flash sensitivity to recover to about 0.2 of the pre-bleach value. Similar exposure to a locked 6-s-cis, 9-cis analogue gave a recovery to about 0.03 of the pre-bleach value. 3. Unlike the flash sensitivity, the saturating photocurrent amplitude often recovered completely after bleaching and regenerating the pigment. 4. When the 3-dehydroretinal chromophore in the salamander long-wavelength-sensitive (red) cone was replaced with 11-cis-retinal, shortening the conjugated chain in the chromophore, the spectral sensitivity underwent a blue shift of 67 nm. 5. Pigments containing the planar-locked 6-s-cis.9-cis-retinal analogue absorbed at substantially longer wavelength than those containing unmodified 9-cis-retinal. The opsin shift, a measure of the protein's ability to modify the chromophore's absorption was larger for the locked analogue than for 9-cis-retinal. This suggests that the native chromophore assumes a twisted 6-s-cis conformation in these pigments. 6. The spectral sensitivities of red and green macaque cones containing 9-cis-retinal or planar-locked 6-s-cis.9-cis-retinal retained the 30 nm separation characteristic of the native pigments. This suggests that the different absorptions of of the 6-7 carbon bond in the retinal chromophore.
Animals↗
Structure of the retinal chromophore in sensory rhodopsin I from resonance Raman spectroscopy.
Sensory rhodopsin I (SR-I) is a retinal-containing pigment which functions as a phototaxis receptor in Halobacterium halobium. We have obtained resonance Raman vibrational spectra of the native membrane-bound form of SR587 and used these data to determine the structure of its retinal prosthetic group. The similar frequencies and intensities of the skeletal fingerprint modes in SR587, bacteriorhodopsin (BR568), and halorhodopsin (HR578) as well as the position of the dideuterio rocking mode when SR-I is regenerated with 12,14-D2 retinal (915 cm-1) demonstrate that the retinal chromophore has an all-trans configuration. The shift of the C = N stretching mode from 1628 cm-1 in H2O to 1620 cm-1 in D2O demonstrates that the chromophore in SR587 is bound to the protein by a protonated Schiff base linkage. The small shift of the 1195 cm-1 C14-C15 stretching mode in D2O establishes that the protonated Schiff base bond has an anti configuration. The low value of the Schiff base stretching frequency together with its small 8 cm-1 shift in D2O indicates that the Schiff base proton is weakly hydrogen bonded to its protein counterion. This suggests that the red shift in the absorption maximum of SR-I (587 nm) compared with HR (578 nm) and BR (568 nm) is due to a reduction of the electrostatic interaction between the protonated Schiff base group and its protein counterion.
Bacteriorhodopsins↗
Bacteriorhodopsin's M412 intermediate contains a 13-cis, 14-s-trans, 15-anti-retinal Schiff base chromophore.
The structure of the retinal chromophore about the C = N and C14-C15 bonds in bacteriorhodopsin's M412 intermediate has been determined by analyzing resonance Raman spectra of 2H and 13C isotopic derivatives. Normal mode calculations on 13-cis-retinal Schiff bases demonstrate that the C15-D rock and N-CLys stretch are strongly coupled for C = N-syn chromophores and weakly coupled for C = N-anti chromophores. When the Schiff base geometry is anti, the C15-D rock appears as a localized resonance Raman active mode at approximately 980 cm-1, which is moderately sensitive to 13C substitution at positions 14 and 15 (approximately 7 cm-1) and insensitive to 13C substitution at the epsilon position of lysine. When the Schiff base geometry is syn, in-phase and out-of-phase combinations of the C15-D rock and N-CLys stretch are predicted at approximately 1060 and approximately 910 cm-1, respectively. The in-phase mode is more sensitive to 13C substitution at positions 14 and 15 (approximately 15 cm-1) and at the epsilon position of lysine (approximately 4 cm-1). Calculations and comparison with experimental data on dark-adapted bacteriorhodopsin indicate that the in-phase mode at approximately 1060 cm-1 carries the majority of the resonance Raman intensity. M412 exhibits a C15-D rock at 968 cm-1 that shifts 8 cm-1 when 13C is added at positions 14 and 15 and is insensitive to 13C substitution at the epsilon-position of lysine. This demonstrates that M412 contains a C = N-anti Schiff base.(ABSTRACT TRUNCATED AT 250 WORDS)
Bacteriorhodopsins↗
Complete assignment of the hydrogen out-of-plane wagging vibrations of bathorhodopsin: chromophore structure and energy storage in the primary photoproduct of vision.
Resonance Raman vibrational spectra of the retinal chromophore in bathorhodopsin have been obtained after regenerating bovine visual pigments with an extensive series of 13C- and deuterium-labeled retinals. A low-temperature spinning cell technique was used to produce high-quality bathorhodopsin spectra exhibiting resolved hydrogen out-of-plane wagging vibrations at 838, 850, 858, 875, and 921 cm-1. The isotopic shifts and a normal coordinate analysis permit the assignment of these lines to the HC7 = C8H Bg, C14H, C12H, C10H, and C11H hydrogen out-of-plane wagging modes, respectively. The coupling constant between the C11H and C12H wags as well as the C12H wag force constant are unusually low compared to those of retinal model compounds. This quantitatively confirms the lack of coupling between the C11H and C12H wags and the low C12H wag vibrational frequency noted earlier by Eyring et al. [(1982) Biochemistry 21, 384]. The force constants for the C10H and C14H wags are also significantly below the values observed in model compounds. We suggest that the perturbed hydrogen out-of-plane wagging and C-C stretching force constants for the C10-C11 = C12-C13 region of the chromophore in bathorhodopsin result from electrostatic interactions with a charged protein residue. This interaction may also contribute to the 33 kcal/mol energy storage in bathorhodopsin.
Animals↗
Orientation of the protonated retinal Schiff base group in bacteriorhodopsin from absorption linear dichroism.
Linear dichroism experiments are performed on light-adapted bacteriorhodopsin (BR568) films containing native retinal (A1) and its 3,4-dehydroretinal (A2) analogue to measure the angle between the chromophore transition dipole moment and the membrane normal. QCFF/pi calculations show that the angle between the transition moment and the long axis of the polyene is changed by 3.4 degrees when the C3-C4 bond is unsaturated. The difference vector between the two transition moments points in the same direction as the Schiff base (N----H) bond for the all-trans BR568 chromophore. Because the plane of the chromophore is perpendicular to the membrane plane, a comparison of the transition moment orientations in the A1- and A2-pigments enables us to determine the orientation of the N----H bond with respect to the absolute chromophore (N----C5 vector) orientation. The angles of the transition moments are 70.3 degrees +/- 0.4 degrees and 67.8 degrees +/- 0.4 degrees for the A1- and A2-pigments, respectively. The fact that the change in the transition moment angle (2.5 degrees) is close to the predicted 3.4 degrees supports the idea that the chromophore plane is nearly perpendicular to the membrane plane. The decreased transition moment angle in the A2-analogue requires that the N----H bond and the N----C5 vector point toward the same membrane surface. Available results indicate that the N----C5 vector points toward the exterior in BR568. With this assignment, we conclude that the N----H bond points toward the exterior surface and its most likely counterion Asp-212. This information makes possible the construction of a computer graphics model for the active site in BR568.
Bacteriorhodopsins↗
Halorhodopsin and sensory rhodopsin contain a C6-C7 s-trans retinal chromophore.
Halorhodopsin (HR) and sensory rhodopsin (SR) have been regenerated with retinal analogues that are covalently locked in the 6-s-cis or 6-s-trans conformations. Both pigments regenerate more completely with the locked 6-s-trans retinal and produce analogue pigments with absorption maxima (577 nm for HR and 592 nm for SR) nearly identical to those of the native pigments (577 and 587 nm). This indicates that HR and SR bind retinal in the 6-s-trans conformation. The opsin shift for the locked 6-s-trans analogue in HR is 1,200 cm-1 less than that for the native chromophore (5,400 cm-1). The opsin shift for the 6-s-trans analogue in SR is 1,100 cm-1 less than that for the native retinal (5,700 cm-1). This demonstrates that approximately 20% of the opsin shift in these pigments arises from a protein-induced change in the chromophore conformation from twisted 6-s-cis in solution to planar 6-s-trans in the protein. The reduced opsin shift observed for the locked 6-s-cis analogue pigments compared with the locked 6-s-trans pigments may be due to a positive electrostatic perturbation near C7.
Bacteriorhodopsins↗
Single-molecule fluorescence detection: autocorrelation criterion and experimental realization with phycoerythrin.
A theory for single-molecule fluorescence detection is developed and then used to analyze data from subpicomolar solutions of B-phycoerythrin (PE). The distribution of detected counts is the convolution of a Poissonian continuous background with bursts arising from the passage of individual fluorophores through the focused laser beam. The autocorrelation function reveals single-molecule events and provides a criterion for optimizing experimental parameters. The transit time of fluorescent molecules through the 120-fl imaged volume was 800 microseconds. The optimal laser power (32 mW at 514.5 nm) gave an incident intensity of 1.8 x 10(23) photons.cm-2.s-1, corresponding to a mean time of 1.1 ns between absorptions. The mean incremental count rate was 1.5 per 100 microseconds for PE monomers and 3.0 for PE dimers above a background count rate of 1.0. The distribution of counts and the autocorrelation function for 200 fM monomer and 100 fM dimer demonstrate that single-molecule detection was achieved. At this concentration, the mean occupancy was 0.014 monomer molecules in the probed volume. A hard-wired version of this detection system was used to measure the concentration of PE down to 1 fM. This single-molecule counter is 3 orders of magnitude more sensitive than conventional fluorescence detection systems.
Lasers↗
Why are blue visual pigments blue? A resonance Raman microprobe study.
A resonance Raman microscope has been developed to study the structure of the retinal prosthetic group in the visual pigments of individual photoreceptor cells. Raman vibrational spectra are obtained by focusing the probe laser on intact photoreceptors frozen on a 77 K cold stage. To elucidate the mechanism of wavelength regulation in blue visual pigments, we have used this apparatus to study the structure of the chromophore in the 440-nm absorbing pigment found in "green rods" of the toad (Bufo marinus). The 9-cis isorhodopsin form of the green rod pigment exhibits a 1662-cm-1 C = NH+ Schiff base stretching mode that shifts to 1636 cm-1 in deuterium-substituted H2O. This demonstrates that the Schiff base linkage to the protein is protonated. Protonation of the Schiff base is sufficient to explain the 440-nm absorption maximum of this pigment without invoking any additional protein-chromophore interactions. The absence of additional perturbations is supported by the observation that the ethylenic band and the perturbation-sensitive C-10-C-11 and C-14-C-15 stretching modes have the same frequency as those of the 9-cis protonated retinal Schiff base in solution. Our demonstration that a blue visual pigment contains an unperturbed protonated Schiff base provides experimental evidence that the protein charge perturbation responsible for the opsin shift in the 500-nm absorbing pigments is removed in the opsins of blue pigments, as suggested by the sequence data.
Animals↗
Chromophore structure in bacteriorhodopsin's N intermediate: implications for the proton-pumping mechanism.
By elevating the pH to 9.5 in 3 M KCl, the concentration of the N intermediate in the bacteriorhodopsin photocycle has been enhanced, and time-resolved resonance Raman spectra of this intermediate have been obtained. Kinetic Raman measurements show that N appears with a half-time of 4 +/- 2 ms, which agrees satisfactorily with our measured decay time of the M412 intermediate (2 +/- 1 ms). This argues that M412 decays directly to N in the light-adapted photocycle. The configuration of the chromophore about the C13 = C14 bond was examined by regenerating the protein with [12,14-2H]retinal. The coupled C12-2H + C14-2H rock at 946 cm-1 demonstrates that the chromophore in N is 13-cis. The shift of the 1642-cm-1 Schiff base stretching mode to 1618 cm-1 in D2O indicates that the Schiff base linkage to the protein is protonated. The insensitivity of the 1168-cm-1 C14-C15 stretching mode to N-deuteriation establishes a C = N anti (trans) Schiff base configuration. The high frequency of the C14-C15 stretching mode as well as the frequency of the 966-cm-1 C14-2H-C15-2H rocking mode shows that the chromophore is 14-s-trans. Thus, N contains a 13-cis, 14-s-trans, 15-anti protonated retinal Schiff base.(ABSTRACT TRUNCATED AT 250 WORDS)
Bacteriorhodopsins↗
Direct observation of the femtosecond excited-state cis-trans isomerization in bacteriorhodopsin.
Femtosecond optical measurement techniques have been used to study the primary photoprocesses in the light-driven transmembrane proton pump bacteriorhodopsin. Light-adapted bacteriorhodopsin was excited with a 60-femtosecond pump pulse at 618 nanometers, and the transient absorption spectra from 560 to 710 nanometers were recorded from -50 to 1000 femtoseconds by means of 6-femtosecond probe pulses. By 60 femtoseconds, a broad transient hole appeared in the absorption spectrum whose amplitude remained constant for about 200 femtoseconds. Stimulated emission in the 660- to 710-nanometer region and excited-state absorption in the 560- to 580-nanometer region appeared promptly and then shifted and decayed from 0 to approximately 150 femtoseconds. These spectral features provide a direct observation of the 13-trans to 13-cis torsional isomerization of the retinal chromophore on the excited-state potential surface. Absorption due to the primary ground-state photoproduct J appears with a time constant of approximately 500 femtoseconds.
Bacteriorhodopsins↗
Structure and function of rhodopsins from solid state NMR and resonance Raman spectroscopy of isotopic retinal derivatives.
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Animals↗
Excited-state structure and isomerization dynamics of the retinal chromophore in rhodopsin from resonance Raman intensities.
Resonance Raman excitation profiles have been measured for the bovine visual pigment rhodopsin using excitation wavelengths ranging from 457.9 to 647.1 nm. A complete Franck-Condon analysis of the absorption spectrum and resonance Raman excitation profiles has been performed using an excited-state, time-dependent wavepacket propagation technique. This has enabled us to determine the change in geometry upon electronic excitation of rhodopsin's 11-cis-retinal protonated Schiff base chromophore along 25 normal coordinates. Intense low-frequency Raman lines are observed at 98, 135, 249, 336, and 461 cm-1 whose intensities provide quantitative, mode-specific information about the excited-state torsional deformations that lead to isomerization. The dominant contribution to the width of the absorption band in rhodopsin results from Franck-Condon progressions in the 1,549 cm-1 ethylenic normal mode. The lack of vibronic structure in the absorption spectrum is shown to be caused by extensive progressions in low-frequency torsional modes and a large homogeneous linewidth (170 cm-1 half-width) together with thermal population of low-frequency modes and inhomogeneous site distribution effects. The resonance Raman cross-sections of rhodopsin are unusually weak because the excited-state wavepacket moves rapidly (approximately 35 fs) and permanently away from the Franck-Condon geometry along skeletal stretching and torsional coordinates.
Animals↗
Bacteriorhodopsin's L550 intermediate contains a C14-C15 s-trans-retinal chromophore.
Conformational changes of the retinal chromophore about the C14-C15 bond in bacteriorhodopsin (BR) have been proposed in models for the mechanism of light-driven proton transport. To determine the C14-C15 conformation in BR's L550 intermediate, we have examined the resonance Raman spectra of BR derivatives regenerated with retinal deuterated at the 14 and 15 positions. Vibrational calculations show that the C14-2H and C15-2H rocking modes form symmetric (A) and antisymmetric (B) combinations in [14,15-2H]retinal chromophores. When there is a trans conformation about the single bond between C14 and C15 (14-s-trans), a small frequency separation or splitting is observed between the A and B modes, which are found at approximately equal to 970 cm-1. In 14-s-cis molecules, the splitting is large, and the Raman-active symmetric A mode is predicted at approximately equal to 850 cm-1. In addition, the monodeuterium rock should appear at an unusually low frequency (920-930 cm-1) in the 14-2H-labeled 14-s-cis molecules. These patterns are insensitive to computational details: similar results are predicted by a modified Urey-Bradley force field and by MNDO (modified neglect of differential overlap) calculations for twisted chromophores and for highly delocalized protonated Schiff base cations. Time-resolved resonance Raman spectra were obtained of BR's L550 intermediate regenerated with [14-2H]-, [15-2H]- and [14,15-2H]retinal. The symmetric A rock in L550 is found at 968 cm-1, within 4 cm-1 of the frequencies for the monodeuterio derivatives, and no scattering is observed between 800 and 940 cm-1. The rocking frequencies of deuterated L550 are within 5 cm-1 of those observed in BR568, which contains a 14-s-trans chromophore. These results show that L550 contains a 14-s-trans chromophore and suggest that only 14-s-trans structures are involved in the proton pumping photocycle of BR.
Bacteriorhodopsins↗
Resonance Raman spectra of the Pr-form of phytochrome.
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Molecular Structure↗
Raman spectroscopic study of left-handed Z-RNA.
The solvent conditions that induce the formation of a left-handed Z form of poly[r(G-C)] have been extended to include 6.5 M NaBr at 35 degrees C and 3.8 M MgCl2 at room temperature. The analysis of the A----Z transition in RNA by circular dichroism (CD), 1H and 31P NMR, and Raman spectroscopy shows that two distinct forms of left-handed RNA exist. The ZR-RNA structure forms in high concentrations of NaBr and NaClO4 and exhibits a unique CD signature. ZD-RNA is found in concentrated MgCl2 and has a CD signature similar to the Z form of poly[d(G-C)]. The loss of Raman intensity of the 813-cm-1 A-form marker band in both the A----ZR-RNA and A----ZD-RNA transitions parallels the loss of intensity at 835 cm-1 in the B----Z transition of DNA. A guanine vibration that is sensitive to the glycosyl torsion angle shifts from 671 cm-1 in A-RNA to 641 cm-1 in both ZD- and ZR-RNA, similar to the B----Z transition in DNA in which this band shifts from 682 to 625 cm-1. Significant differences in the glycosyl angle and sugar pucker between Z-DNA and Z-RNA are suggested by the 16-cm-1 difference in the position of this band. The Raman evidence for structural difference between ZD- and ZR-RNA comes from two groups of bands: First, Raman intensities between 1180 and 1600 cm-1 of ZD-RNA differ from those for ZR-RNA, corroborating the CD evidence for differences in base-stacking geometry. Second, the phosphodiester stretching bands near 815 cm-1 provide evidence of differences in backbone geometry between ZD- and ZR-RNA.
Circular Dichroism↗
Structure of the retinal chromophore in the hRL intermediate of halorhodopsin from resonance raman spectroscopy.
Time-resolved resonance Raman spectra of the hRL intermediate of halorhodopsin have been obtained. The structurally sensitive fingerprint region of the hRL spectrum is very similar to that of bacteriorhodopsin's L550 intermediate, which is known to have a 13-cis configuration. This indicates that hRL contains a 13-cis chromophore and that an all-trans----13-cis isomerization occurs in the halorhodopsin photocycle. hRL exhibits a Schiff base stretching mode at 1644 cm-1, which shifts to 1620 cm-1 in D2O. This demonstrates that the Schiff base linkage to the protein is protonated. The insensitivity of the C-C stretching mode frequencies to N-deuteriation suggests that the Schiff base configuration is anti. The 24 cm-1 shift of the Schiff base mode in D2O indicates that the Schiff base proton in hRL has a stronger hydrogen-bonding interaction with the protein than does hR578.
Bacteriorhodopsins↗