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The ultrafast structural dynamics in the electronic excited state of photoactive yellow protein (PYP) is studied by femtosecond stimulated Raman spectroscopy. Stimulated Raman spectra in the electronic excited state, S(1), can be obtained by using a Raman pump pulse in resonance with the S(1)-S(0) transition. This is confirmed by comparing the experimental results with numerical calculations based on the density matrix treatment. We also investigate the hydrogen-bonding network surrounding the wild-type (WT)-PYP chromophore in the ground and excited states by comparing its stimulated Raman spectra with those of the E46Q-PYP mutant. We focus on the relative intensity of the Raman band at 1555 cm(-1), which includes both vinyl bond C═C stretching and ring vibrations and is sensitive to the hydrogen-bonding network around the phenolic oxygen of the chromophore. The relative intensity for the WT-PYP decreases after actinic excitation within the 150 fs time resolution and reaches a similar intensity to that for E46Q-PYP. These observations indicate that the WT-PYP hydrogen-bonding network is immediately rearranged in the electronic excited state to form a structure similar to that of E46Q-PYP.

Perylene diimide (PDI) derivatives with cyclodextrins (PDI-CD2s) exhibit specific emission properties, which depend on the type of CDs in an aqueous solution. Herein we successfully create an emission film-kneaded PDI-CD2 derivatives via effective tumbling of the altropyranose unit. PDI-6CD2s are crosslinked with PDI between 6-amino-CDs. Although the emission intensities of PDI-6CD2s in dimethyl sulfoxide are similar regardless of the type of CD, PDI-6γCD2 has a relatively high emission intensity in aqueous solutions. In contrast, for PDIC7-3CD2s, which are linked with N,N’-bis(6-carboxylhexyl)perylene-3,4,9,10-tetracarboxyl diimide (BisC7-PDI) between 3-amino-CDs, the emission intensity of PDIC7-3βCD2 is stronger than those of PDIC7-3αCD2, PDIC7-3γCD2, and PDI-6CD2s in aqueous solutions. The selective emission behavior of PDIC7-3CD2s is due to the formation of the pseudo[1]rotaxane dimer through tumbling of the altropyranose unit in an aqueous solution. PDIC7-3βCD2 in the solid state does not demonstrate a distinctive emission due to self-quenching, whereas PDIC7-3βCD2 kneaded into the polyvinyl alcohol (PVA) film exhibits a bright yellow emission. The order of the emission intensities of PDIC7-3CD2s kneaded into PVA films is similar to those in aqueous solutions. Perylene diimide (PDI) derivatives with cyclodextrins (PDI-CD2s) exhibit specific emission properties, which depend on the type of CDs in an aqueous solution. Herein we create an emission from film kneaded PDI-CD2s derivatives via effective tumbling of the altropyranose unit. We have observed the selective emission of PDIC7-3βCD2 in aqueous solutions and prepared emission films kneaded into polyvinyl alcohol (PVA) films. The emission depends on the cavity size of the altro-CDs formed through altro-CD tumbling.

An energy transfer process was investigated using cyclodextrin-oligothiophene rotaxanes (2T-[2]rotaxane). The excited energy of 2T-[2]rotaxane is transferred to the sexithiophene derivative which is included in the cavity of β-CD stoppers of 2T-[2]rotaxane.

Picosecond time-resolved ultraviolet resonance Raman (UVRR) spectra of photoactive yellow protein (PYP) were measured. UVRR bands attributed to the vibration of tyrosine and tryptophan residues showed a spectral change upon photoreaction. It was found that the hydrogen-bond strength between the chromophore and Y42 increases in the pG* state. The ultrafast change in the tryptophan band revealed that a photoinduced structural change of the chromophore had propagated to the W119 region, located 12 A from the chromophore, within picoseconds.

Pump-dump fluorescence spectroscopy was performed for photoactive yellow protein (PYP) at room temperature. The effect of the dump pulse on the population of the potential energy surface of the electronic excited state was examined as depletion in the stationary fluorescence intensity. The dynamic behavior of the population in the electronic excited state was successfully probed in the various combinations of the pump-dump delay, the dump-pulse wavelength, the dump-pulse energy and the observation wavelength. The experimental results were compared with the results obtained by the femtosecond time-resolved fluorescence spectroscopy.

A versatile method to take femtosecond spectral snapshots of fluorescence has been developed based on a double gating technique in the combination of an optical Kerr gate and an image intensifier as an electrically driven gate set in front of a charge-coupled device detector. The application of a conventional optical-Kerr-gate method is limited to molecules with the short fluorescence lifetime up to a few hundred picoseconds, because long-lifetime fluorescence itself behaves as a source of the background signal due to insufficiency of the extinction ratio of polarizers employed for the Kerr gate. By using the image intensifier with the gate time of 200 ps, we have successfully suppressed the background signal and overcome the application limit of optical-Kerr-gate method. The system performance has been demonstrated by measuring time-resolved fluorescence spectra for laser dye solution and the riboflavin solution as a typical sample of biomolecule.

Time-resolved spectra of a photoactive yellow protein (PYP) containing cyano-p-coumaric acid (CHCA) were recorded. To understand the mechanism of photo-isomerization, an electron-withdrawing CN group was introduced into the PYP to alter the C[double bond, length as m-dash]C double bond character. Free CHCA chromophores in aqueous solution underwent photo-isomerization whereas PYP with a bound CHCA (PYP-CN) exhibited no photocycle at acidic or alkaline pH or in urea and other solutions. Furthermore, no photocycle was observed with PYP mutants after illumination. This phenomenon cannot be fully explained by the electron-withdrawing properties of the CN group. We conclude that the CHCA chromophore in PYP was locked in the protein cage and that the CN group interacted with the protein residues.

Vibrational energy flow in the electronic ground state of photoactive yellow protein (PYP) is studied by ultrafast infrared (IR) pump-visible probe spectroscopy. Vibrational modes of the chromophore and the surrounding protein are excited with a femtosecond IR pump pulse, and the subsequent vibrational dynamics in the chromophore are selectively probed with a visible probe pulse through changes in the absorption spectrum of the chromophore. We thus obtain the vibrational energy flow with four characteristic time constants. The vibrational excitation with an IR pulse at 1340, 1420, 1500, or 1670 cm(-1) results in ultrafast intramolecular vibrational redistribution (IVR) with a time constant of 0.2 ps. The vibrational modes excited through the IVR process relax to the initial ground state with a time constant of 6-8 ps in parallel with vibrational cooling with a time constant of 14 ps. In addition, upon excitation with an IR pulse at 1670 cm(-1), we observe the energy flow from the protein backbone to the chromophore that occurs with a time constant of 4.2 ps.

Vibrational dynamics of the chromophore in photoactive yellow protein is studied by mid-IR-pump-visible-probe spectroscopy. So-called ‘ground state intermediate’, which is believed to be a cis isomer, is directly generated by vibrational excitation.

We report a unique lambdamax shift of the absorption maximum of a photoactive yellow protein (PYP) analogue reconstituted with a fluorinated chromophore (F-PYP). The difference in lambdamax between the free chromophore and the protein was significantly larger than that with the native chromophore. We concluded that the unusual lambdamax shift is caused by the electronegative character of the fluorine atom and not by steric hindrance. This result suggests that formation of a hydrogen bond between the fluorine atom and one or more amino acid residues could neutralize its electron-withdrawing character. The properties of analogues of PYP with brominated and methylated chromophore could be explained as an effect of steric hindrance.

In order to obtain insight into the hydrogen-bonding network surrounding the chromophore in biologically photo-functional proteins, photoactive yellow protein (PYP) has been modified by a combination of a site-directed mutagenesis and a substitution of the chromophore with an analogue. Fluorescence excitation and emission spectroscopies have been performed to evaluate the inhomogeneous nature of the spectra originated from the variation of conformational substates of the modified proteins. Noticeable inhomogeneity including contributions from two distinct substates has been observed for a PYP hybrid with the E46Q mutation and a substitution of the p-coumaric acid chromophore with caffeic acid. Transient absorption spectroscopy has been also conducted to clarify whether inhomogeneity affects the recovering kinetics or not. For the PYP hybrid, a remarkable difference of the recovery time from the signaling state has been observed, depending on the wavelength of the excitation light triggering the photocycle. Although this observation is preliminary, it indicates that kinetically inhomogeneous species likely exist in the PYP hybrid.

The blue light receptor photoactive yellow protein (PYP) displays a photocycle that involves several intermediate states. Here we report resonance Raman spectroscopic investigations of the short-lived red-shifted intermediate denoted PYP(L). We have found that the Raman bands of the carbonyl C=O stretching mode nu(11) as well as the C=C stretching mode nu(13) for the chromophore can be resolved into two peaks, and the ratio of the two components varies as a function of pH with pK(a) approximately 6. The isotope effects on the resonance Raman spectra have confirmed a deprotonated cis-chromophore for the two components. The results indicate the presence of two conformations in the active site of PYP(L). The normal coordinate calculations based on the density functional theory provide a structural model for the two conformations, where the low pH form is possibly an active structure for the protonation reaction generating a following intermediate in the photocycle.

Photoactive yellow protein (PYP) is a bacterial blue light receptor containing a 4-hydroxycinnamyl chromophore, and its absorption maximum is 446 nm. In a dark state, the hydroxyl group of the chromophore is deprotonated and forms hydrogen bonds with Tyr42 and Glu46. Either removal of a hydrogen bond with Tyr42 or addition of chaotropes such as thiocyanate produces a blue-shifted species called an intermediate wavelength form, in which absorption maximum ranges from 355 to 400 nm. To examine the structural origin of the intermediate wavelength form, we have performed resonance Raman investigations of wild-type PYP and some mutants (Tyr42 --Ala, Tyr42 --Phe, Glu46 --Gln, and Thr50 --Val) in the presence or absence of potassium thiocyanate. These studies show that the chromophore of the intermediate wavelength form is protonated, implying an increase in a pK(a) of the chromophore. Hence, the removal of the hydrogen bond between Tyr42 and chromophore or partial protein denaturation in the presence of thiocyanate results in a spectral blue-shift. Quantum chemical calculations based on density functional theory further support the idea that the pK(a) of the chromophore is increased by removing a hydrogen bond or by increasing the dielectric constant in the vicinity of the chromophore.

The early stage in the photo-induced dynamics of photoactive yellow protein in aqueous solution has been investigated at room temperature by the femtosecond luminescence spectroscopy using an optical Kerr-gate technique. Remarkable oscillatory components have been directly observed with the time resolution of 180 fs and the spectral resolution of 5 nm . Mapping the phase of oscillations in time at each wavelength reveals that each oscillation is restricted in the respective narrow spectral region, the period and amplitude of which are 500– 800 fs and 100– 200 cm −1 , respectively. Since the mean spectral position of each component seems to be related to the molecular vibrational energy, the oscillatory components are possibly attributed to the combination of the intramolecular vibrations of the chromophore and the surrounding protein motions.

We have investigated primary processes of ultrafast photoreactions of various photoresponsive proteins by means of fs fluorescence dynamics measurements. Based on these studies, the effects of the protein nanospace (PNS), containing the chromophore, on the dynamics and mechanisms of the ultrafast and highly efficient reactions of these proteins have been elucidated. In this article, we discuss mainly the results of our studies on ultrafast photoisomerization of photoactive yellow protein (PYP), its mutants and analogues. The chromophore of the PYP, deprotonated coumaric acid thioester (O−-phenyl-CHCH–CO–S–CH2–), fixed in PNS by hydrogen (H) bonding interactions at the head part, O−-phenyl-, and by covalent bonding at the tail part, –CO–S–, undergoes ultrafast twisting by flipping the thioester bond, owing to the intrachromophore head to tail charge transfer caused by the photoexcitation. In the site-directed mutants where the PNS structure is looser and more disordered, the photoinduced twisting reaction becomes slowed compared with the wild-type PYP and moreover, the twisting becomes much slower in the denatured PYP, showing the supreme importance of more regulated PNS for the fast twisting. We found also coherent vibrations in the fluorescence decay curves which might be coupled with the twisting. Furthermore, we found for a PYP analogue with replaced chromophore ultrafast dynamic Stokes shift of fluorescence rather than the quenching due to twisting, indicating the importance of chromophore-PNS fine adjustment for the ultrafast twisting.

PYP (photoactive yellow protein) is a photoreceptor protein, which is activated upon photo-isomerization of the p-coumaric acid chromophore and is inactivated as the chromophore is thermally back-isomerized within a second (in PYP(M)-to-PYP(dark) conversion). Here we have examined the mechanism of the rapid thermal isomerization by analyzing mutant PYPs of Met100, which was previously shown to play a major role in facilitating the reaction [Devanathan, S. et al. (1998) Biochemistry 37, 11563-11568]. The mutation to Lys, Leu, Ala, or Glu decelerated the dark state recovery by one to three orders of magnitude. By evaluating temperature-dependence of the kinetics, it was found that the retardation resulted unequivocally from elevations of activation enthalpy (DeltaH( double dagger )) but not the other parameters such as activation entropy or heat capacity changes. Another effect exerted by the mutations was an up-shift of the apparent pK(a) of the chromophore [the pK(a) of a titratable group (X) that controls the pK(a) of the chromophore] in the PYP(M)-decay process. The pK(a) up-shift and the DeltaH( double dagger ) elevation show an approximately linear correlation. We, therefore, postulate that the role of Met100 is to reduce the energy barrier of the PYP(M)-decay process by an indirect interaction through X and that the process is thereby facilitated.

Light-activation of the PAS domain protein photoactive yellow protein (PYP) is believed to trigger a negative phototactic response in the phototropic bacterium Halorhodospira halophila. To investigate transient conformational changes of the PYP photocycle, we utilized the PYP mutant M100L that displays an increased lifetime of the putative signaling-state photointermediate PYP(M) by 3 orders of magnitude, as previously reported for the M100A mutant [Devanathan, S., Genick, U. K., Canestrelli, I. L., Meyer, T. E., Cusanovich, M. A., Getzoff, E. D., and Tollin, G. Biochemistry (1998) 37, 11563-11568]. The FTIR difference spectrum of PYP(M) and the ground state of M100L demonstrated extensive peptide-backbone structural changes as observed in the FTIR difference spectrum of the wild-type protein and PYP(M). The conformational change investigated by CD spectroscopy in the far-UV region showed reduction of the alpha-helical content by approximately 40%, indicating a considerable amount of changes in the secondary structure. The optical activity of the p-coumaric acid chromophore completely vanished upon PYP(M) in contrast to the dark state, indicating deformation of the binding pocket structure in PYP(M). The tertiary structural changes were further monitored by small-angle X-ray scattering measurements, which demonstrated a significant increase of the radius of gyration of the molecule by approximately 5% in PYP(M). These structural changes were reversed concomitantly with the chromophore anionization upon the dark state recovery. The observed changes of the quantities provided a more vivid view of the structural changes of the mutant PYP in going from PYP(M) to PYP(dark), which can be regarded as a process of folding of the secondary and the tertiary structures of the "PAS" domain structure, coupled with the p-coumaric acid chromophore deprotonation and isomerization.

Model compounds of PYP chromophore were synthesized and characterized to investigate the role of the Cys69 residue in the active center, which has the intramolecular NHOC hydrogen bond to the conjugated carbonyl oxygen and thioester linkage of the chromophore. The results of UV-vis and (13)C NMR spectroscopy of the model compounds indicated that they delocalized the negative charge of the chromophore and increased the contribution of the quinoid-like resonance structure in the phenolate anion state. Thus, the Cys69 residue plays an important role in the regulation of the color and the stabilization of the chromophore anion in the active center.

The ultrafast photo-induced dynamics of wild-type photoactive yellow protein and its site-directed mutant of E46Q in aqueous solution was studied at room temperature by femtosecond fluorescence spectroscopy using the optical Kerr-gate method. The vibronic structure appears, depending on the excitation photon energy, in the time-resolved fluorescence spectra just after photoexcitation, which winds with time and disappears on a time scale of sub-picoseconds. This result indicates that the wavepacket is localized in the electronic excited state followed by dumped oscillations and broadening, and also that the initial condition of the wavepacket prepared depending on the excitation photon energy affects much the following ultrafast dynamics in the electronic excited state.

The ultrafast photoinduced dynamics of photoactive yellow protein in aqueous solution were studied at room temperature by femtosecond fluorescence spectroscopy using an optical Kerr-gate technique. Coherent oscillations of the wave packet were directly observed in the two-dimensional time-energy map of ultrafast fluorescence with 180 fs time resolution and 5 nm spectral resolution. The two-dimensional map revealed that four or more oscillatory components exist within the broad bandwidth of the fluorescence spectrum, each of which is restricted in the respective narrow spectral region. Typical frequencies of the oscillatory modes are 50 and 120 cm(-1). In the landscape on the map, the oscillatory components were recognized as the ridges which were winding and descending with time. The amplitude of the oscillatory and winding behaviors is a few hundred cm(-1), which is the same order as the frequencies of the oscillations. The mean spectral positions of the oscillatory components in the two-dimensional map are well explained by considering the vibrational energies of intramolecular modes in the electronic ground state of the chromophore. The entire view of the wave packet oscillations and broadening in the electronic excited state, accompanied by fluorescence transitions to the vibrational sublevels belonging to the electronic ground state, was obtained.

Photoactive yellow protein from Ectothiorhodospira halophila is a photoreceptor protein involved in the negative phototaxis of this bacterium. Its chromophore (p-coumaric acid) is deprotonated in the ground state, which is stabilized by a hydrogen-bond network between Tyr42, Glu46 and Thr50. Glu46 is a key residue as it has been suggested that the proton at Glu46 is transferred to the chromophore during its photoconversion from the dark state to the signalling state. The structure of E46Q mutant protein was determined at 1.2 A resolution, revealing that the phenolic O atom of p-coumaric acid is hydrogen bonded to NH(2) of Gln46 in E46Q with a longer distance (2.86 +/- 0.02 A) than its distance (2.51 A) to Glu46 OH in the wild type. This and the decreased thermal stability of E46Q relative to the wild type show that this hydrogen bond is weakened in the E46Q mutant compared with the corresponding bond in the wild type. Several characteristic features of E46Q such as an alkali shift in the pK(a) and the rapid photocycle can be explained by this weakened hydrogen bond. Furthermore, the red shift in the absorption maximum in E46Q can be explained by the delocalization of the electron on the phenolic oxygen of p-coumaric acid owing to the weakening of this hydrogen bond.

Ultrafast photoreactions in PNS of PYP have been studied by means of fs fluorescence up conversion method. Conclusions obtained are: (a) Photoreaction in PNS (chromophore twisting) occurs from vibrationally unrelaxed fluorescence state and coherent oscillations in the fluorescence decay curves have been observed for the first time. (b) Comparative studies on fluorescence dynamics of mutants and w.-t. PYP have proved that the w.-t. PYP is best engineered for the ultrafast reaction. (c) The coherent oscillations in the fluorescence decay completely disappeared and the reaction was much slower in the denatured state, demonstrating the supremely important role of PNS for the photoreaction.

In photosensory or photoactive proteins with chromophores absorbing in the visible region, such as rhodopsin (Rh) for vision, bacteriorhodopsin (bR), photoactive yellow protein (PYP) etc., light absorption leads to ultrafast and highly efficient reactions. Interestingly, despite quite different chromophores of these proteins, their behavior concerning the photoinduced primary processes in the protein nanospace in the course of the relaxation and twisting, including coherent processes seems to be similar. For instance, the fluorescence dynamics in all three proteins is nonexponential, no dynamic Stokes shift but a slight narrowing of the fluorescence spectra within first few picoseconds of the reaction were observed [1-3]. The spectral narrowing effect is most probably due to damping of coherently coupled intrachromophore high frequency modes and/or low frequency vibrations of environmental protein interacting with chromophore along the twisting coordinate. If this is the case, oscillatory behavior in fluorescence dynamics of photosensory proteins should be observed. To our knowledge, no such observation has been reported yet.

Ultrafast structural evolution in photoactive yellow protein (PYP) is studied by femtosecond stimulated Raman spectroscopy. A comparison between wild-type PYP and E46Q mutant reveals that the hydrogen-bonding network surrounding the chromophore of PYP is immediately rearranged in the electronic excited state.

Low-frequency vibrational modes of the native photoactive yellow protein (PYP) and its several mutant and analogue systems have been investigated in “time” (femtosecond fluorescence up-conversion) ...