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R A Mathies

Publications and source records attributed to R A Mathies.

At least 91 records · Page 5Linked to original sources
PubMed1991

The first step in vision: femtosecond isomerization of rhodopsin.

The kinetics of the primary event in vision have been resolved with the use of femtosecond optical measurement techniques. The 11-cis retinal prosthetic group of rhodopsin is excited with a 35-femtosecond pump pulse at 500 nanometers, and the transient changes in absorption are measured between 450 and 580 nanometers with a 10-femtosecond probe pulse. Within 200 femtoseconds, an increased absorption is observed between 540 and 580 nanometers, indicating the formation of photoproduct on this time scale. These measurements demonstrate that the first step in vision, the 11-cis----11-trans torsional isomerization of the rhodopsin chromophore, is essentially complete in only 200 femtoseconds.

Animals↗
PubMed1991

High-sensitivity two-color detection of double-stranded DNA with a confocal fluorescence gel scanner using ethidium homodimer and thiazole orange.

Ethidium homodimer (EthD; lambda Fmax 620 nm) at EthD:DNA ratios up to 1 dye:4-5 bp forms stable fluorescent complexes with double-stranded DNA (dsDNA) which can be detected with high sensitivity using a confocal fluorescence gel scanner (Glazer, A.N., Peck, K. & Mathies, R.A. (1990) Proc. Natl. Acad. Sci. U.S.A. 87, 3851-3855). However, on incubation with unlabeled DNA partial migration of EthD takes place from its complex with dsDNA to the unlabeled DNA. It is shown here that this migration is dependent on the fractional occupancy of intercalating sites in the original dsDNA-EthD complex and that there is no detectable transfer from dsDNA-EthD complexes formed at 50 bp: 1 dye. The monointercalator thiazole orange (TO; lambda Fmax 530 nm) forms readily dissociable complexes with dsDNA with a large fluorescence enhancement on binding (Lee, L.G., Chen, C. & Liu, L.A. (1986) Cytometry 7, 508-517). However, a large molar excess of TO does not displace EthD from its complex with dsDNA. When TO and EthD are bound to the same dsDNA molecule, excitation of TO leads to efficient energy transfer from TO to EthD. This observation shows the practicability of 'sensitizing' EthD fluorescence with a second intercalating dye having a very high absorption coefficient and efficient energy transfer characteristics. Electrophoresis on agarose gels, with TO in the buffer, of preformed linearized M13mp18 DNA-EthD complex together with unlabeled linearized pBR322 permits sensitive fluorescence detection in the same lane of pBR322 DNA-TO complex at 530 nm and of M13mp18 DNA-EthD complex at 620 nm. These observations lay the groundwork for the use of stable DNA-dye intercalation complexes carrying hundreds of chromophores in two-color applications such as the physical mapping of chromosomes.

Benzothiazoles↗
PubMed1991

Resonance Raman spectra of bacteriorhodopsin mutants with substitutions at Asp-85, Asp-96, and Arg-82.

Detergent solubilized bacteriorhodopsin (BR) proteins which contain alterations made by site-directed mutagenesis (Asp-96----Asn, D96N; Asp-85----Asn, D85N; and Arg-82----Gln, R82Q) have been studied with resonance Raman spectroscopy. Raman spectra of the light-adapted (BRLA) and M species in D96N are identical to those of native BR, indicating that this residue is not located near the chromophore. The BRLA states of D85N and especially R82Q contain more of the 13-cis, C = N syn (BR555) species under ambient illumination compared to solubilized native BR. Replacement of Asp-85 with Asn causes a 25 nm red-shift of the absorption maximum and a frequency decrease in both the ethylenic (-7 cm-1) and the Schiff base C = NH+ (-3 cm-1) stretching modes of BRLA. These changes indicate that Asp-85 is located close to the protonated retinal Schiff base. The BRLA spectrum of R82Q exhibits a slight perturbation of the C = NH+ band, but its M spectrum is unperturbed. The Raman spectra and the absorption properties of D85N and R82Q suggest that the protein counterion environment involves the residues Asp-85-, Arg-82+ and presumably Asp-212-. These data are consistent with a model where the strength of the protein-chromophore interaction and hence the absorption maximum depends on the overall charge of the Schiff base counterion environment.

Amino Acid Sequence↗
PubMed1991

High-sensitivity DNA detection with a laser-excited confocal fluorescence gel scanner.

A high-sensitivity, laser-excited confocal fluorescence gel scanner has been developed and applied to the detection of fluorescently labeled DNA. An argon ion laser (1-10 mW at 488 nm) is focused in the gel with a high-numerical aperture microscope objective. The laser-excited fluorescence is gathered by the objective and focused on a confocal spatial filter, followed by a spectral filter and photodetector. The gel is placed on a computer-controlled scan stage, and the scanned image of the gel fluorescence is stored and analyzed in a computer. This scanner has been used to detect DNA separated on sequencing gels, agarose mapping gels and pulsed field gels. Sanger sequencing gels were run on M13mp18 DNA using a fluoresceinated primer. The 400-microns-thick gels, loaded with 30 fmol of DNA fragments in 3-mm lanes, were scanned at 78-microns resolution. The high resolution of our scanner coupled with image processing allows us to read up to approximately 300 bases in four adjacent sequencing lanes. The minimum band size that could be detected and read was approximately 200 microns. This instrument has a limiting detection sensitivity of approximately 10 amol of fluorescein-labeled DNA in a 1 x 3-mm band. In applications to agarose mapping gels, we have exploited the fact that DNA can be prestained with ethidium homodimer, followed by electrophoresis and fluorescence detection to achieve picogram sensitivity. We have also developed methods using both ethidium homodimer and thiazole orange staining which permit two-color detection of DNA in one lane.(ABSTRACT TRUNCATED AT 250 WORDS)

Base Sequence↗
PubMed1990

Resonance Raman analysis of the Pr and Pfr forms of phytochrome.

Resonance Raman vibrational spectra of the Pr and Pfr forms of oat phytochrome have been obtained at room temperature. When Pr is converted to Pfr, new bands appear in the C = C and C = N stretching region at 1622, 1599, and 1552 cm-1, indicating that a major structural change of the chromophore has occurred. The Pr to Pfr conversion results in an 11 cm-1 lowering of the N-H rocking band from 1323 to 1312 cm-1. Normal mode calculations correlate this frequency drop with a Z----E isomerization about the C15 = C16 bond. A line at 803 cm-1 in Pr is replaced by an unusually intense mode at 814 cm-1 in Pfr. Calculations on model tetrapyrrole chromophores suggest that these low-wavenumber modes are hydrogen out-of-plane (HOOP) wagging vibrations of the bridging C15 methine hydrogen and that both the intensity and frequency of the C15 HOOP mode are sensitive to the geometry around the C14-C15 and C15 = C16 bonds. The large intensity of the 814-cm-1 mode in Pfr indicates that the chromophore is highly distorted from planarity around the C15 methine bridge. If the Pr----Pfr conversion does involve a C15 = C16 Z----E isomerization, then the intensity of the C15 HOOP mode in Pfr argues that the chromophore has an E,anti conformation. On the basis of a comparison with the vibrational calculations, the low frequency (803 cm-1) and the reduced intensity of the C15 HOOP mode in Pr suggest that the chromophore in Pr adopts the C15-Z,syn conformation.

Edible Grain↗
PubMed1990

Structure of the retinal chromophore in 7,9-dicis-rhodopsin.

Bovine rhodopsin was bleached and regenerated with 7,9-dicis-retinal to form 7,9-dicis-rhodopsin, which was purified on a concanavalin A affinity column. The absorption maximum of the 7,9-dicis pigment is 453 nm, giving an opsin shift of 1600 cm-1 compared to 2500 cm-1 for 11-cis-rhodopsin and 2400 cm-1 for 9-cis-rhodopsin. Rapid-flow resonance Raman spectra have been obtained of 7,9-dicis-rhodopsin in H2O and D2O at room temperature. The shift of the 1654-cm-1 C = N stretch to 1627 cm-1 in D2O demonstrates that the Schiff base nitrogen is protonated. The absence of any shift in the 1201-cm-1 mode, which is assigned as the C14-C15 stretch, or of any other C-C stretching modes in D2O indicates that the Schiff base C = N configuration is trans (anti). Assuming that the cyclohexenyl ring binds with the same orientation in 7,9-dicis-, 9-cis-, and 11-cis-rhodopsins, the presence of two cis bonds requires that the N-H bond of the 7,9-dicis chromophore points in the opposite direction from that in the 9-cis or 11-cis pigment. However, the Schiff base C = NH+ stretching frequency and its D2O shift in 7,9-dicis-rhodopsin are very similar to those in 11-cis- and 9-cis-rhodopsin, indicating that the Schiff base electrostatic/hydrogen-bonding environments are effectively the same. The C = N trans (anti) Schiff base geometry of 7,9-dicis-rhodopsin and the insensitivity of its Schiff base vibrational properties to orientation are rationalized by examining the binding site specificity with molecular modeling.

Animals↗
PubMed1990

Solid-state NMR studies of the mechanism of the opsin shift in the visual pigment rhodopsin.

Solid-state 13C NMR spectra have been obtained of bovine rhodopsin and isorhodopsin regenerated with retinal selectively 13C labeled along the polyene chain. In rhodopsin, the chemical shifts for 13C-5, 13C-6, 13C-7, 13C-14, and 13C-15 correspond closely to the chemical shifts observed in the 11-cis protonated Schiff base (PSB) model compound. Differences in chemical shift relative to the 11-cis PSB chloride salt are observed for positions 8 through 13, with the largest deshielding (6.2 ppm) localized at position 13. The localized deshielding at C-13 supports previous models of the opsin shift in rhodopsin that place a protein perturbation in the vicinity of position 13. Spectra obtained of isorhodopsin regenerated with 13C-labeled 9-cis-retinals reveal large perturbations at 13C-7 and 13C-13. The similar deshielding of the 13C-13 resonance in both pigments supports the presence of a protein perturbation near position 13. However, the chemical shifts at positions 7 and 12 in isorhodopsin are not analogous to those observed in rhodopsin and suggest that the binding site interactions near these positions are different for the two pigments. The implications of these results for the mechanism of the opsin shift in these proteins are discussed.

Animals↗
PubMed1990

Optimization of high-sensitivity fluorescence detection.

We present general expressions for the number of photons emitted by a fluorescent chromophore as a function of the intensity and the duration of illumination. The aim is to find optimal conditions for detecting fluorescent molecules in the presence of both ground-state depletion and photodestruction. The key molecular parameters are the absorption coefficient epsilon, the excited singlet-state lifetime tau f, the excited triplet-state decay rate kT, the intersystem crossing rate kI, and the intrinsic photodestruction time tau d. When only singlet saturation and photochemistry are important, the signal-to-noise ratio depends on two fundamental variables: k, the ratio of the absorption rate ka to the observed fluorescence decay rate kf, and tau, the ratio of the duration of illumination taut to the intrinsic photodestruction time tau d. Equations are also developed for the more complicated cases when triplet formation and photochemistry are important. This theory was tested by measuring the fluorescence from a solution of beta-phycoerythrin flowed through a focused argon ion laser beam. The dependence of the fluorescence on the incident light intensity and the illumination time agrees well with the theoretical prediction for singlet saturation and photochemistry. The signal-to-noise ratio is optimal when the light intensity and the flow rate are adjusted so that both K and tau are close to unity (5 X 10(22) photons cm-2 s-1 and a transit time tau t of 700 mus). This analysis should be useful for optimizing fluorescence detection in DNA sequencing, chromatography, fluorescence microscopy, and single-molecular fluorescence detection.

Fluorescence↗
PubMed1990

The role of back-reactions and proton uptake during the N----O transition in bacteriorhodopsin's photocycle: a kinetic resonance Raman study.

The kinetics of bacteriorhodopsin's photocycle have been analyzed at pH 5, 6, 7, 8, and 8.6 by using time-resolved resonance Raman spectroscopy. The concentrations of the various intermediates as a function of time were determined by following their resonance Raman intensities using 502-nm (L550, N550, BR568), 458-nm (M412), and 752-nm (O640) excitation. The spectral contributions to the pump + probe data from each intermediate were quantitatively separated by least-squares decomposition. These relative concentrations were then converted to absolute concentrations by using a conservation of molecules constraint. This enabled the unambiguous refinement of a variety of kinetic models to find the simplest one that accurately describes the data. The kinetic data, including the biphasic decay of L550 and M412, are best reproduced by a sequential scheme including back-reactions (BR----L----M----N----O----BR). In addition, the kinetics of the L----M and N----O steps are found to be pH-dependent. Both the forward and reverse rate constants connecting L550 and M412 increase with pH, confirming earlier proposals of catalyzed Schiff base deprotonation at alkaline pH. Below pH 7, the N550----O640 rate constant is independent of pH, but it decreases linearly with pH above 7. This indicates that the protein must pick up a proton during the N550----O640 transition and that this process becomes rate determining above pH 7. There must, therefore, be an intermediate between N550 and O640 which we denote as N+550. A molecular graphics model is presented which incorporates these observations into a mechanism for proton pumping.

Bacteriorhodopsins↗
PubMed1990

A stable double-stranded DNA-ethidium homodimer complex: application to picogram fluorescence detection of DNA in agarose gels.

The complex between double-stranded DNA and ethidium homodimer (5,5'-diazadecamethylene)bis(3,8-diamino-6-phenylphenanthridini um) cation, formed at a ratio of 1 homodimer per 4 or 5 base pairs, is stable in agarose gels under the usual conditions for electrophoresis. This unusual stability allows formation of the complex before electrophoresis and then separation and detection in the absence of background stain. Competition experiments between the preformed DNA-ethidium homodimer complex and a 50-fold molar excess of unlabeled DNA show that approximately one-third of the dye is retained within the original complex independent of the duration of the competition. However, dye-extraction experiments show that these are not covalent complexes. After electrophoretic separation, detection of bands containing 25 pg of DNA was readily achieved in 1-mm thick agarose gels with laser excitation at 488 nm and a scanning confocal fluorescence imaging system. The band intensity was linear with the amount of DNA applied from 0.2 to 1.0 ng per lane and with the number of kilobase pairs (kbp) per band within a lane. Analysis of an aliquot of a polymerase-chain-reaction mixture permitted ready detection of 80 pg of a 1.6-kbp amplified fragment. The use of the ethidium homodimer complex together with laser excitation for DNA detection on gels is at least two orders of magnitude more sensitive than conventional fluorescence-based procedures. The homodimer-DNA complex exemplifies a class of fluorescent probes where the intercalation of dye chromophores in DNA forms a stable, highly fluorescent ensemble.

DNA↗
PubMed1990

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↗
PubMed1990

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↗
PubMed1989

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↗
PubMed1989

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↗
PubMed1989

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↗
PubMed1989

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↗