Spectral broadening of the Soret band in myoglobin: an interpretation by the full spectrum of low-frequency modes from a normal modes analysis

In this work the temperature dependence of the Soret band line shape in carbon-monoxy myoglobin is re-analyzed by using both the full correlator approach in the time domain and the frequency domain approach. The new analyses exploit the full density of vibrational states of carbon-monoxy myoglobin available from normal modes analysis, and avoid the artificial division of the entire set of vibrational modes coupled to the Soret transition into "high-frequency" and "low-frequency" subsets; the frequency domain analysis, however, makes use of the so-called short-times approximation, while the time domain one avoids it. Time domain and frequency domain analyses give very similar results, thus supporting the applicability of the short-times approximation to the analysis of hemeprotein spectra; in particular, they clearly indicate the presence of spectral heterogeneity in the Soret band of carbon-monoxy myoglobin. The analyses also show that a temperature dependence of the Gaussian width parameter steeper than the hyperbolic cotangent law predicted by the Einstein harmonic oscillator and/or a temperature dependence of inhomogeneous broadening are not sufficient to obtain quantitative information on the magnitude of an-harmonic contributions to the iron-heme plane motion. However, the dependence of the previous two quantities may be used to obtain semiquantitative information on the overall coupling of the Soret transition to the low-frequency modes and therefore on the dynamic properties of the heme pocket in different states of the protein.     

Low temperature optical absorption spectroscopy: an approach to the study of stereodynamic properties of hemeproteins

In this short review we show how suitable analysis of the temperature dependence of the optical absorption spectra of metalloproteins can give insight into their stereodynamic properties in the region of the chromophore. To this end, the theory of coupling between an intense allowed electronic transition of a chromophore and Franck-Condon active vibrations of the nearby atoms is applied to the Soret band of hemeproteins to obtain an analytical expression suitable for fitting the spectral profile at various temperatures. The reported approach enables one to separate the various contributions to the overall bandwidth together with the parameters that characterize the vibrational coupling. The thermal behavior of these quantities gives information on the dynamic properties of the active site and on their dependence upon protein structure and ligation state. The Soret band of hemeproteins appears to be coupled to high frequency vibrational modes of the heme group (as already shown by resonance Raman spectroscopy) and to a bath of low frequency modes most likely deriving from the bulk of the protein. For the deoxy derivatives inhomogeneous broadening arising from conformational heterogeneity appears to contribute substantially to the linewidth. The data indicate the onset; at temperatures near 180 K, of large scale anharmonic motions that can be attributed to jumping among different conformational substates of the protein.Abbreviations MbCO Carbonmonoxy-myoglobin - Mb Deoxymyoglobin - Mb³⁺ Aquomet-myoglobin - SWMbCO Spermwhale carbonmonoxy-myoglobin - SWMb Spermwhale deoxy-myoglobin Correspondence to: A. Cupane     

Dynamic properties of some β-chain mutant hemoglobins

The thermal behavior of the Soret band relative to the carbonmonoxy derivatives of some β-chain mutant hemoglobins is studied in the temperature range 300–10 K and compared to that of wild-type carbonmonoxy hemoglobin. The band profile at various temperatures is modeled as a Voigt function that accounts for homogeneous broadening and for the coupling with high- and low-frequency vibrational modes, while inhomogeneous broadening is taken into account with a gaussian distribution of purely electronic transition frequencies. The various contributions to the overall bandwidth are singled out With this analysis and their temperature dependence, in turn, gives information on structural and dynamic properties of the system studied. In the wildtype and mutant hemoglobins, the values of homogeneous bandwidth and of the coupling constants to high-frequency vibrational modes are not modified with respect to natural human hemoglobin, thus indicating that the local electronic and vibrational properties of the heme–CO complex are not altered by the recombinant procedures. On the contrary, differences in the protein dynamic behavior are observed. The most relevant are those relative to the “polar isosteric” βVal-67(Ell) →Thr substitution, localized in the heme pocket, which results in decreased coupling with low-frequency modes and increased anharmonic motions. Mutations involving residue βLys-144(HC1) at the C-terminal and residue βCys-112(G14) at the α₁β₁ interface have a smaller effect consisting in an increased coupling with low-frequency modes. Mutations at the β-N-terminal and at the α₁β₂ interface have no effect on the dynamic properties of the heme pocket. © 1995 Wiley-Liss, Inc.     

Heme symmetry, vibronic structure, and dynamics in heme proteins: ferrous nicotinate horse myoglobin and soybean leghemoglobin

We report the visible and Soret absorption bands, down to cryogenic temperatures, of the ferrous nicotinate adducts of native and deuteroheme reconstituted horse heart myoglobin in comparison with soybean leghemoglobin-a. The band profile in the visible region is analyzed in terms of vibronic coupling of the heme normal modes to the electronic transition in the framework of the Herzberg-Teller approximation. This theoretical approach makes use of the crude Born-Oppenheimer states and therefore neglects the mixing between electronic and vibrational coordinates; however, it takes into account the vibronic nature of the visible absorption bands and allows an estimate of the vibronic side bands for both Condon and non-Condon vibrational modes. In this framework, an x-y splitting of the Q transition for native and deuteroheme reconstituted horse myoglobin is clearly assessed and attributed to electronic perturbations that, in turn, are caused by a reduction of the typical D(4h) symmetry of the system due to heme distortions of B(1g)-type symmetry and/or to an x-y asymmetric position of the nicotinate ring; in deuteroheme reconstituted horse myoglobin the asymmetric heme peripheral substituents add to the above effect(s). On the contrary, in leghemoglobin-a no spectral splitting upon nicotinate binding is observed, pointing to a planar heme configuration in which only distortions of A(1g)-type symmetry are effective and to which the nicotinate ring is bound in an x - y symmetric position. The local dynamic properties of the heme pocket of the three proteins are investigated through the temperature dependence of spectral line broadening. Leghemoglobin-a behaves as a softer matrix with respect to horse myoglobin, thus validating the hypothesis of a looser heme pocket conformation in the former protein, which allows a nondistorted heme configuration and a symmetric binding of the bulky nicotinate ligand.     

Protein dynamics: conformational disorder,vibrational coupling and anharmonicity in deoxy-hemoglobin and myoglobin

In this work we study the temperature dependence of the Soret band lineshape of deoxymyoglobin and deoxyhemoglobin, in the range 300–20 K. To fit the measured spectra we use an approach originally proposed by Champion and coworkers (Srajer et al. 1986; Srajer and Champion 1991). The band profile is modelled as a Voigt function that accounts for the coupling with low frequency vibrational modes, whereas the coupling with high frequency modes is responsible for the vibronic structure of the spectra. Moreover, owing to the position of the iron atom out of the mean heme plane, inhomogeneous broadening brings about a non-Gaussian distribution of 0–0 electronic transition frequencies. The reported analysis enables us to isolate the various contributions to the overall bandwidth, and their temperature dependence points out the relevance of low frequency vibrations and of large scale anharmonic motions starting at temperatures higher than 170 K. Information on the mean iron-heme plane distance and on its temperature dependence, as well as on the heme pocket conformational disorder, is also obtained.Abbreviations Cc Carbon monoxide - Hb Human deoxyhemoglobin A - HbCO human carbonmonoxyhemoglobin A - SWMb spermwhale deoxymyoglobin - SWMbCO spermwhale carbonmonoxymyoglobin - HbO₂ human oxyhemoglobin A - SWMb³⁺-H₂O spermwhale aquometmyoglobin     

Low temperature optical spectroscopy of low-spin ferric hemeproteins

We report the Soret absorption spectra (500-350 nm) of the cyanomet derivatives of human hemoglobin and horse myoglobin, in the temperature range 300-20 K and in two different solvents (65% v/v glycerol-water or 65% v/v ethylene glycol-water). In order to obtain information on stereodynamic properties of active site of the two hemeproteins, we perform an analysis of the band profiles within the framework of electron-vibrations coupling. This approach enables us to single out the various contributions to the spectral bandwidth, such as those arising from non-radiative decay of the excited electronic state (homogeneous broadening) and from the coupling of the electronic transition i) with high frequency modes (that determines the vibronic structure of the band) and ii) with a bath of low frequency modes (that is responsible for the temperature dependence of the experimental spectra). We discuss the relevant parameters and their temperature dependence and compare them with the ones already reported for other derivatives of the same hemeproteins in the same solvents. In particular, non-harmonic contributions to soft modes are found, for cyanomet derivatives, to be larger than those observed for liganded carbonmonoxy but smaller than those observed for unliganded deoxy derivatives. The reported data enable us to obtain information on the dependence of stereodynamic properties of the heme pocket upon iron oxidation state, dimensions of the exogenous ligand and composition of the external matrix. Correspondence to: M. Leone     

Correct interpretation of heme protein spectra allows distinguishing between the heme and the protein dynamics

It is shown by using the vibronic approach that the iron displacement out of the porphyrin plane in deoxyheme proteins intermixes the porphyrin pi and axial iron-histidine sigma electronic subsystems. This intermixing explains the substantial coupling of the iron-histidine vibration to the heme Soret excitation, the appearance of the iron-histidine band in the corresponding resonance Raman spectra, and a number of other experimental data, including the dependence of the iron-histidine vibrational frequency on the extent of the iron displacement out of the porphyrin plane. This dependence implies that there is an anharmonic coupling between the corresponding vibrations, which is shown to be the cause of the specific temperature dependence of the iron-histidine band. The anharmonic coupling and the dependence of the dipole transition moment of the charge transfer optical absorption band III on the iron-porphyrin distance cause the anomalous temperature and pressure dependencies of this band. It is shown that the change in both the magnitude and the distribution of the iron-porphyrin distance is expected to affect the band III intensity. Consequently, the stationarity of the band III intensity can be considered as a signature of the stationarity of the iron-porphyrin distance and its distribution in deoxyheme proteins, whereas the band III position and width could be also affected by the change in the protein electric field, caused by the protein globule dynamics.     

Local dynamic properties of the heme pocket in native and solvent-induced molten-globule-like states of cytochrome c

We report the Soret absorption band, down to cryogenic temperature, of native and molten-globule-like state of horse heart cytochrome c. The band profile is analyzed in terms of vibronic coupling of the heme normal modes to the electronic transition in the framework of the Franck-Condon approximation. From the temperature dependence of the Gaussian broadening and of the peak position, we obtain information on the 'bath' of low frequency harmonic motions of the heme group within the heme pocket. The reported data indicate that, compared to the native state, the less rigid tertiary structure of the molten globule is reflected in a higher flexibility of the heme pocket and in greater conformational disorder, allowing the transduction of large-amplitude motion of the protein to the dynamics of the heme pocket.     

Optical and IR absorption as probe of dynamics of heme proteins

The spectroscopy of horseradish peroxidase with and without the substrate analogue benzohydroxamic acid (BHA) was monitored in different solvents as a function of the temperature in the interval from 10 to 300 K. Thermal broadening of the Q(0,0) optical absorption band arises mainly from interaction of the electronic pi --> pi transition with the heme vibrations. In contrast, the width of the IR absorption band of CO bound to heme is controlled by the coupling of the CO transition moment to the electric field of the protein matrix. The IR bandwidth of the substrate free enzyme in the glycerol/H2O solvent hardly changes in the glassy matrix and strongly increases upon heating above the glass transition. Heating of the same enzyme in the trehalose/H2O glass considerably broadens the band. The binding of the substrate strongly diminishes the temperature broadening of the CO band. This result is consistent with the view that the BHA strongly reduces the amplitude of vibrations of the heme pocket environment. Unusually strong thermal broadening of the CO band above the glass transition is interpreted to be caused by thermal population of a very flexible excited conformational substate. The thermal broadening of the same band in the trehalose glass is caused by an increase of the protein vibrational amplitude in each of the conformational substates, their population being independent of the temperature in the glassy matrix.     

Ionisation of fullerenes and fullerene clusters using ultrashort laser pulses.

We give a brief review of the literature concerning the ultra-short pulse ionisation of fullerenes in the gas phase. Emphasis is placed on the excitation time dependence of different ionisation regimes as manifested by photoelectron spectroscopy. The ionisation rates are modelled for the intermediate situation where the excitation energy is equilibrated between electronic degrees of freedom but not yet coupled to vibrational degrees of freedom. The model is shown to describe many aspects of the experiments. New results are presented on the intra-cluster molecular fusion of fullerene molecules when van der Waals bound clusters of fullerenes are exposed to ultra-short laser pulses. Pump-probe measurements give a decay time constant for the intra-cluster fusion reaction of 520 +/- 55 fs. A comparison with monomer ionisation results suggests that the time window for the fusion reaction is influenced by the coupling of the electronic excitation energy to vibrational degrees of freedom of the molecules in the cluster.     

Structure-dynamics-function relationships in Asian elephant (Elephas maximus) myoglobin. An optical spectroscopy and flash photolysis study on functionally important motions.

In this work we report the thermal behavior (10-300 K) of the Soret band lineshape of deoxy and carbonmonoxy derivatives of Asian elephant (Elephas maximus) and horse myoglobins together with their carbon monoxide recombination kinetics after flash photolysis; the results are compared to analogous data relative to sperm whale myoglobin. The Soret band profile is modeled as a Voigt function that accounts for the coupling with high and low frequency vibrational modes, while inhomogeneous broadening is taken into account with suitable distributions of purely electronic transition frequencies. This analysis makes it possible to isolate the various contributions to the overall lineshape that; in turn, give information on structural and dynamic properties of the systems studied. The optical spectroscopy data point out sizable differences between elephant myoglobin on one hand and horse and sperm whale myoglobins on the other. These differences, more pronounced in deoxy derivatives, involve both the structure and dynamics of the heme pocket; in particular, elephant myoglobin appears to be characterized by larger anharmonic contributions to soft modes than the other two proteins. Flash photolysis data are analyzed as sums of kinetic processes with temperature-dependent fractional amplitudes, characterized by discrete pre-exponentials and either discrete or distributed activation enthalpies. In the whole temperature range investigated the behavior of elephant myoglobin appears to be more complex than that of horse and sperm whale myoglobins, which is in agreement with the increased anharmonic contributions to soft modes found in the former protein. Thus, to satisfactorily fit the time courses for CO recombination to elephant myoglobin five distinct processes are needed, only one of which is populated over the whole temperature range investigated. The remarkable convergence and complementarity between optical spectroscopy and flash photolysis data confirms the utility of combining these two experimental techniques in order to gain new and deeper insights into the functional relevance of protein fluctuations.     

Temperature dependence of the low frequency dynamics of myoglobin. Measurement of the vibrational frequency distribution by inelastic neutron scattering.

Inelastic neutron scattering spectra of myoglobin hydrated to 0.33 g water (D2O)/g protein have been measured in the low frequency range (1-150 cm-1) at various temperatures between 100 and 350 K. The spectra at low temperatures show a well-resolved maximum in the incoherent dynamic structure factor Sinc(q, omega) at approximately 25 cm-1 and no elastic broadening. This maximum becomes gradually less distinct above 180 K due to the increasing amplitude of quasielastic scattering which extends out to 30 cm-1. The vibrational frequency distribution derived independently at 100 and 180 K are very similar, suggesting harmonic behavior at these temperatures. This result has been used to separate the vibrational motion from the quasielastic motion at temperatures above 180 K. The form of the density of states of myoglobin is discussed in relation to that of other amorphous systems, to theoretical calculations of low frequency modes in proteins, and to previous observations by electron-spin relaxation of fractal-like spectral properties of proteins. The onset of quasielastic scattering above 180 K is indicative of a dynamic transition of the system and correlates with an anomalous increase in the atomic mean-squared displacements observed by M?ssbauer spectroscopy (Parak, F., E. W. Knapp, and D. Kucheida. 1982. J. Mol. Biol. 161: 177-194.) and inelastic neutron scattering (Doster, W., S. Cusack, and W. Petry, 1989. Nature [Lond.]. 337: 754-756.) Similar behavior is observed for a hydrated powder of lysozyme suggesting that the low frequency dynamics of globular proteins have common features.     

Thermal sensitivity of the red absorption tail of the photosystem II reaction center complex.

The red tail of the absorption spectrum of the D1-D2-cytb559 complex, defined as the absorption signal not described by the two Gaussian sub-bands associated with the intense electronic transitions at 680 and 683 nm, exhibits anomalous temperature behavior. This tail was analyzed in the temperature interval between 80 and 300 K in terms of the mean square deviation (sigma2) of the total Qy absorption band and by Gaussian sub-band decomposition. The value of the average optical reorganization energy (Snum) obtained from the temperature dependence of sigma2 for the whole absorption band was 32 cm(-1), and changed to 16-20 cm(-1) after subtraction of the sub-bands describing the red tail. This latter value is in agreement with the hole burning literature data for chlorophyll bound to proteins, and indicates that the rather high value for the apparent optical reorganization energy obtained by analysis of the total Qy band of the D1-D2-cytb559 complex is determined by the temperature sensitivity of the red tail. This suggests that the long wavelength absorption tail might be due to vibrational transitions associated with vibrational modes in the range of 80-150 cm(-1) which are thermally accessible and give rise to an absorption signal on the low-energy side of the (0,0) transition. On the basis of this assumption, the electron-phonon coupling strength (S) for these modes is estimated to be in the range 0.028-0.18. This interpretation furthermore supports the idea that the electronic transition near 683 nm is that of a monomer chlorophyll.     

Heme geometry in the 10 K photoproduct from sperm whale carbonmonoxymyoglobin

We have measured the Soret band of the photoproduct obtained by complete photolysis of sperm whale carbonmonoxymyoglobin at 10 K. The experimental spectrum has been modeled with an analytical expression that takes into account the homogeneous bandwidth, the coupling of the electronic transition with both high and low frequency vibrational modes, and the effects of static conformational heterogeneity. The comparison with deoxymyoglobin at low temperature reveals three main differences. In the photoproduct, the Soret band is shifted to red. The band is less asymmetric, and an enhanced coupling to the heme vibrational mode at 674 cm⁻¹ is observed. These differences reflect incomplete relaxation of the active site after ligand dissociation. The smaller band asymmetry of the photoproduct can be explained by a smaller displacement of the iron atom from the mean porphyrin plane, in quantitative agreement with the X-ray structure analysis. The enhanced vibrational coupling is attributed to a subtle heme distortion from the planar geometry that is barely detectable in the X-ray structure.     

Dynamic properties of oxy- and carbonmonoxyhemoglobin probed by optical spectroscopy in the temperature range of 300-20 K

We have studied the absorption bands of oxy- and carbonmonoxyhemoglobin in the wavelength range of 650–350 nm (visible and Soret bands) and in the temperature range of 300–20 K. The spectra in the whole temperature range have been successfully deconvoluted in terms of gaussian components. The analysis of the temperature dependence of the first and second moment of the bands enables us to compare dynamic properties of the heme group in oxy- and carbonmonoxyhemoglobin. The results of the analysis indicate that the “mean-effective” frequency of the nuclear motion coupled to the electronic transition responsible for the visible bands is higher in carbonmonoxy- than in oxyhemoglobin. The possible functional relevance of this finding is discussed.     

Qy-excitation resonance Raman scattering from the special pair in Rhodobacter sphaeroides reaction centers. Implications for primary charge separation.

Qy-excitation resonance Raman (RR) spectra are reported for reaction centers (RCs) from Rhodobacter sphaeroides 2.4.1. The RR spectra were acquired for both chemically reduced and oxidized RCs at 25 and 201 K by using a variety of excitation wavelengths in the range 800-920 nm. This range spans the Qy absorption bands of the special pair (P) and the accessory bacteriochlorophylls (BChls). The RR studies indicate that both P and the accessory BChls exhibit rich RR spectra in the 30-1800-cm-1 region. For both types of pigments, at least 20 bands are observed in the 30-750-cm-1 range. Although the frequencies of the modes of P and the accessory BChls are different, it is possible to make one-to-one correlations of the bands observed for the two types of pigments. This result suggests that the vibronically active low-frequency modes of P are derived from monomer-like vibrations (although they may be coupled monomer-like modes) rather than being vibrations resulting from the additional degrees of freedom present in the dimer. A plausible set of vibrational assignments for the low-frequency modes of both P and the accessory BChls is proposed on the basis of a semiempirical normal coordinate calculation. Comparison of the RR intensities of the low-frequency modes of P with those of the analogous modes of the accessory BChls indicates that the intensities of the modes of the former pigments are considerably larger than those of the latter. Collectively, the spectral data indicate that a large number of low-frequency modes of P are strongly coupled to the Qy electronic transition.(ABSTRACT TRUNCATED AT 250 WORDS)     

Investigations of optical line shapes and kinetic hole burning in myoglobin.

We present the results of an extensive investigation of the optical line shapes of deoxymyoglobin (Mb), the ligand-bound form (MbCO), and the low-temperature photoproduct (Mb*). The thermal properties and the pH dependence of the Soret band and the near infrared band III (approximately 760 nm) are analyzed, taking into account the underlying vibrational properties of the absorption bands. The strong temperature dependence associated with the Soret band of MbCO and band III of Mb indicates significant coupling to low-frequency modes that may not be directly observed in the resonance Raman spectra. On the basis of analogous line-shape studies in a variety of heme systems, we assign the low-frequency coupling in MbCO to torsional motions of the CO molecule. The low-frequency mode coupled to band III (approximately 70 cm-1) is found to lie quite close to the value for the heme-doming motion (approximately 50 cm-1) calculated by using the kinetically determined value of the force constant (17 N/m). Significant inhomogeneous broadening in the Soret region of Mb and Mb* is found to be due to a "nonkinetic" coordinate that we associate with the orientation of the proximal histidine. A "kinetic" coordinate, associated with the equilibrium displacement of the iron atom from the porphyrin plane (a) is found to contribute to the inhomogeneous broadening of both the Soret band and band III. The relaxation of the heme as the system evolves from from Mb* to Mb is followed optically as a function of temperature, and a sharp transition temperature is found at 185 K. The blue shifts of the Soret band and band III as Mb* evolves to Mb are found to be nearly identical (delta v*ABS approximately 140 cm-1) and attributed to changes in the mean value of a between Mb* (a*0) and Mb (a0 = 0.45 A). A simple quadratic model for the coordinate coupling that simultaneously accounts for the observed shift, delta v*ABS, the low-temperature kinetics and the kinetic hole burning predicts a*0 = 0.2 +/- 0.05 A and EA = 16 +/- 2 kJ/mol for the room temperature Arrhenius barrier height at the heme. A simple quantitative method for the analysis of kinetic hole-burning experiments is also developed and applied to recent studies involving quaternary and subunit-specific hemoglobin structures.     

Broadband Plasmon-Induced Transparency in Plasmonic Metasurfaces Based on Bright-Dark-Bright Mode Coupling

Plasmon-induced transparency (PIT), an analog of electromagnetically induced transparency, originates from destructive interference of plasmonic resonators with different quality factors and brings about the extreme dispersion within the narrow transparency window, promising remarkable potential for slow light, nonlinear optics and biochemical sensors. However, sometimes a broad transmission frequency band is more desirable for other applications such as bandpass filters. In general, strong coupling between bright and dark plasmon modes in coupled resonant systems leads to wide transparency bandwidth at the PIT resonance. Based on multi-oscillator coupling theory, a metasurface structure consisting of three perpendicularly connected metallic nanobars is purposefully designed and numerically demonstrated to support broadband PIT spectral response. The near-field patterns indicate that the broadening of the transparent band results from the constructive interference of dual excitations of the single non-radiative (dark) resonator by the two radiative (bright) antennas. These results show that this scheme of bright-dark-bright mode coupling is significantly beneficial for designing filters operating over a broad frequency range.

     

Optical absorption spectra of azurin and stellacyanin in glycerol/water and ethylene glycol/water solutions in the temperature range 290-20 K

We have measured the optical absorption spectra of azurin and stellacyanin in the wavelength range 1100-350 nm and in the temperature interval 290-20 K. Samples are protein aqueous solutions containing 65% (v/v) glycerol or ethylene glycol as cryoprotectants and remain homogeneous and transparent throughout the whole temperature range investigated. Spectra are deconvoluted into Gaussian components and the temperature dependence of the zeroth, first and second moments of the various bands is analyzed, within the harmonic Franck-Condon approximation, to obtain information on the stereodynamic properties of the active sites of these proteins. Sizable differences of the integrated intensities of all the bands with temperature are observed and are attributed to variations of the metal-ligand relative positions (i.e., deformations of the active site) that occur as the temperature is lowered. The mean effective frequency of the nuclear vibrations coupled to all the observed bands is about 150 cm(-1) for both proteins in both solvents used; this indicates that the electronic transitions from which the optical spectrum originates are substantially coupled with low-frequency vibrational modes, likely ligand-metal-ligand deformations. The relevance of the stereodynamic properties of azurin and stellacyanin, investigated in this work, to their functional behavior is also suggested.     

Real-time vibrational dynamics in chlorophyll a studied with a few-cycle pulse laser

We use a 6.8-fs laser as the light source for broad-band femtosecond pump-probe real-time vibrational spectroscopy to investigate both electronic relaxation and vibrational dynamics of the Q_y-band of Chl-a at 293 K. More than 25 vibrational modes coupled to the Q_y transition are observed. Eleven of them have been clarified predominantly due to the excited state, and six of them are concluded to be nearly exclusively resulting from the ground-state wave-packet motion. Moreover, thanks to the broad-band detection over 5000 cm⁻¹, the modulated signals due to the excited state vibrational coherence are observed on both sides of the 0-0 transition with equal separation. The corresponding nonlinear process has been studied using a three-level model, from which the probe wavelength dependence of the phase of the periodic modulation can be calculated. The probe wavelength dependence of the vibrational amplitude is interpreted in terms of the interaction between the “pump” or “laser,” Stokes, and anti-Stokes field intermediated by the molecular vibrations. In addition, an excited state absorption peak at ∼709 nm has been observed. To the best of our knowledge, this is the first study of broad-band real-time vibrational spectroscopy in Chl-a.