Theoretical study on the partial potential energy surface and formation mechanism of the reactive resonance state of HO + CH4 → H2O + CH3 system

In the course of an extensive investigation aimed at understanding the detailed mechanism of a prototypical polyatomic reaction, several remarkable observations were uncovered. To interpret these findings, we surmise the existence of a reactive resonance in this polyatomic reaction. The concerned system is HO + CH₄ → H₂O + CH₃, of which the partial potential energy surface is constructed by the coupling between vibrational models and reactive coordinates. Then we explain the formation mechanism of the reactive resonance state by the partial potential energy surface. Finally, we estimated the lifetime of the resonance state, and it is about 45fs. The study of the reactive resonance in a polyatomic reaction is more than just an extension from a typical atom + diatom reaction. As shown here, it holds great promise to disentangle the elusive intramolecular vibrational dynamics of the transient collision complex in the critical transition‐state region. © 2007 Wiley Periodicals, Inc. Int J Quantum Chem, 2008     

Infrared-microwave double resonance study of the ν4 fundamental band of POF3

Three-level and four-level infrared-microwave double resonance effects have been observed in a POF₃ sample contained in a microwave waveguide Stark cell that was modified to permit transmission of radiation from a CO₂ infrared gas laser. In three-level double resonance experiments laser pumping of rotational states in the ν₄ = 1 vibrational state greatly increased the signal/noise for observation of Stark-shifted rotational transitions in the excited vibrational state. The frequencies of the observed excited state transitions were used to confirm the assignment of laser Stark spectra and to obtain independent measures of the rotational constant B and the dipole moment for ν₄ = 1. The observation of four level double resonances could be explained qualitatively by the assumption of dipole selection rules for collision-induced transitions. However, the intensities of the double-resonance effects could not be explained by this simple model.     

Fully resonant CARS of cresyl violet in polyacrylic acid polymer films

Multi-resonant CARS data for ground and excited electronic state resonances (593.585 cm^?1) of cresyl violet perchlorate in polyacrylic acid are reported. The intensity of the excited state resonance (585 cm^?1) depends on the location of the ω₁-field (ω_as = 2ω₁ ? ω₂) within the severely inhomogeneously broadened absorption profile of the dye. Non-photochemical hole burning is used to determine the vibronic transitions which contribute to the absorption profile. It is argued that the linear electron-phonon interaction is an important mechanism for producing an egalitarian distribution of excited dye sites with a population sufficiently high to permit observation of the excited state resonance. A marked non-photochemical hole burning effect on the intensities of the CARS resonances is used for the assignment of 585 cm^?1 as an excited state resonance. The absence of line narrowing in the CARS and CSRS spectra is reported and discussed. Finally, a novel narrowing of the 593 cm^?1 ground state resonance with increasing temperature is reported and shown to occur only for restricted values (frequency) of ω₁.     

Observation of transient resonance raman spectra of the S1 state of trans-stilbene

Transient resonance Raman spectra of trans-stilbene in n-hexane have been obtained using two pulsed lasers at 266 and 585 nm. The former was used to pump the molecule to the first excited singlet state (S₁) and the latter to proble spontaneous Raman scattering in resonance with the S_n ← S₁ electronic transition. The dependence of the pump and probe laser power, the temporal behavior, and the excitation profile of the spectra clearly indicate that they are due to the S₁ state of trans-stilbene.     

Assigning the resonance Raman spectral features of rhodopsin, isorhodopsin and bathorhodopsin in bovine photostationary state spectra.

Abstract—High resolution resonance Raman spectra of rhodopsin. isorhodopsin and photostationary state mixtures containing a high percentage of bathorhodopsin arc presented. New spectral features are detected which were not obsei-ved in lower resolution studies by other workers. All of the hands in the photostationary state spcctra arc assigned based on pure rhodopsin and isorhodopsin resonance Raman results and alterations in the photostationary state mixture. The spectral features in these spectra are invariant from 20 to 150K indicating that retinal and protein structural alteration, consistent with a model of excitation proposed by Lewis, occurs in steady-state spectra even at 20 K. In addition, the relative intensity of certain features in the photostationary state spectra are altered upon D₂O suspension. One explanation for these alterations is that the contributions of various intcrmediates to the photostationary state mixture are changed when membrane fragments are suspended in D₂O.     

Electronic structure of the 1,3-butadiyne anion studied by electron transmission and vibrational excitation spectra in the gas phase

The electron transmission and vibrational excitation spectra of the title compound are reported. Two bands, at 1.0 and 5.6 eV are found in the ETS spectrum. The 1.0 eV resonance excites mainly the CC stretch vibration ν₂ and the CH bend vibrations ν_6,8 in even quanta. It has been assigned to the ²Π_u (in linear geometry) ground state of the anion. This state is found to be bent in the equilibrium geometry and the minimum of the anion potential surface lies outside of the Franck-Condon region. The band around 5.6 eV is interpreted as the ²Π_g resonance overlapping with a σ^* resonance which excites mainly the CH stretch vibration ν₁. A remarkable feature is the excitation of high levels of the CH bend vibration near threshold, with E_r ? 0.3 eV.     

Caught in the Hinact: Crystal Structure and Spectroscopy Reveal a Sulfur Bound to the Active Site of an O2‐stable State of [FeFe] Hydrogenase

[FeFe] hydrogenases are the most active H₂ converting catalysts in nature, but their extreme oxygen sensitivity limits their use in technological applications. The [FeFe] hydrogenases from sulfate reducing bacteria can be purified in an O₂‐stable state called H_inact. To date, the structure and mechanism of formation of H_inact remain unknown. Our 1.65 Å crystal structure of this state reveals a sulfur ligand bound to the open coordination site. Furthermore, in‐depth spectroscopic characterization by X‐ray absorption spectroscopy (XAS), nuclear resonance vibrational spectroscopy (NRVS), resonance Raman (RR) spectroscopy and infrared (IR) spectroscopy, together with hybrid quantum mechanical and molecular mechanical (QM/MM) calculations, provide detailed chemical insight into the H_inact state and its mechanism of formation. This may facilitate the design of O₂‐stable hydrogenases and molecular catalysts.     

Theoretical Study on Resonance Raman Spectra of Tetraoxaporphyrin Dication by TDDFT Calculation

The B state excited resonance Raman scattering of tetraoxaporphyrin dication (TOP²⁺) was theoretically studied with DFT/TDDFT calculations and the sum-over-states approach of polarizability including both the A and B terms contributions. The resonance Raman spectra calculated with PBE1PBE, B3LYP, Cam-B3LYP, and B3LYP-D3 functionals are similar to each other in general, with PBE1PBE and B3LYP being better in reproducing resonance Raman intensities in comparison with the experiment. The calculated relative intensities of the totally symmetric modes are excellently consistent with the experiment. The TDDFT calculations manifested a considerable deformation of the B state along theυ2,υ6, υ7, and υ8 modes, which is responsible for the strong resonance Raman intensities of these modes. The resonance Raman intensities of non-totally symmetric modes were calculated to be weaker than the totally symmetric modes by one or two order of magnitude, whichqualitatively agrees with the experiment. However, the resonance Raman intensity of the υ10 mode (C_βC_β stretch, B_1g symmetry) predicted by TDDFT calculations is unexpectedly small whereas that of the υ11 mode (symmetric C_αC_m stretch, B_1g symmetry) is too large, which is assumed to be caused by the Jahn-Teller instability for the B state of TOP²⁺.     

Magnetic resonance studies of the deuteration effect on intersystem crossing in the anthracene molecule

The intersystem crossing decay constants from the ³B_2u state into the ground state of anthracene-d₁₀ in a phenazine crystal have been determined by magnetic resonance techniques at 1.5°K both at high magnetic field and, by a parameterization procedure, at zero magnetic field. A comparison of the anthracene-d₁₀ zero-field results with those for anthracene-h₁₀ show the effects of deuterium substitution to be largest for the in-plane spin levels of the anthracene triplet state.     

A performance criterion for information theoretic data analysis

A previously unobserved electronic state in fluorobenzene appears as a two-photon resonance in the multiphoton resonance ionization spectrum. The band system is assigned to the 3s Rydberg ← b₂(π) HOMO transition with a quantum defect of 0.83 and an origin at 50 914 ± 15 cm^?1. Its correspondence to the benzene state characterized by Johnson in the same region assigns that state to E_1g 3s Rydberg.     

A novel and efficient excitation- and ionization-scheme for laser resonance ionization of mercury

A novel, efficient scheme for mercury atomic resonance ionization is proposed and experimentally studied with wavelengths λ₁=254 nm, λ₂=313 nm and λ₃=626 nm. The cross-sections of mercury photoionization from different excited states were estimated using a new imaging method of resonance ionization signal measurement. Almost 100% efficiency of Hg resonance ionization was achieved using the first harmonic of a dye laser at 626 nm to ionize mercury atoms excited into the 6³D₂ state. The photoionization cross-section from this state was found to be 1.5×10⁻¹⁸ cm². Suppression of the ionization signal by coherent effects (electromagnetically-induced transparency) and the efficiency of resonance ionization were also studied.     

Application of time-resolved resonance Raman spectroscopy to the study of rapid intramolecular radiationless transitions

It is shown that the decay rate γ₂ of the excited state of a molecule can be determined by measuring the decrease of the resonance Raman intensity on a time scale much longer than γ^?1₂, provided that the time needed for repopulation of the ground state, following rapid intramolecular radiationless transitions from the excited state to a molecular quasicontinuum, is itself much longer than γ^?1₂. Thus, it should be possible to avoid the use of ultrashort pulses in the study of very fast intramolecular decay process.     

Resonant two photon ionization of phenanthrene via its transientS 2 state

We report the vibrationally resolved photoelectron spectrum of phenanthrene obtained by two photon ionization via theS ₂ electronic state. The experiments were performed with picosecond laser pulses with a bandwidth sufficiently large to span a significant fraction of the intermediate resonance state. Therefore the photoelectron spectrum is dominated by signal corresponding to the unrelaxed intermediate resonance, in spite of this state's 420 fs lifetime.     

Experimental ground stateg J-factor of Ba+ in a Penning ion trap

We observed the Zeeman-splitting of the 6S _1/2 – 6P _1/2 resonance transition of Ba⁺-ions (493.4 nm) in a 6T magnetic field. The ions were stored in a Penning quadrupole trap. We polarized the ground state by optical pumping and in a microwave-optical double resonance experiment we measured the ground state Zeeman-splitting. From the resonance frequency and the cyclotron frequency of electrons stored in the same trap we derived theg-factor of the 6S _1/2 state. The result isg _J(6S _1/2)=2.002 490 6(11), in reasonable agreement with recent calculations.     

An investigation of the triplet state dynamics of zinc chlorophyll b by microwave-induced changes in the intensity of fluorescence and singlet-singlet absorption

Optical detection of magnetic resonance experiments on the triplet state of zinc-substitution chlorophyll b has provided the zero-field splitting and depopulation rate constants for the individual triplet spin sublevels. The zero field triplet state EPR transitions could be observed at 890 MHz and 1085 MHz as either microwave-induced changes in the fluorescence intensity or in the intensity of S₀ → S_n absorption. The dynamics experiments show that intersystem crossing from the Zn chlorophyll b triplet state into the ground state occurs primarily through the out-of-plane (lowest energy) spin sublevel.     

The influence of external fields on magnetically ordered FeCl3·6H2O

Mössbauer resonance has been used to study a single crystal of FeCl₃·6H₂O at 1.16°K in external magnetic fields. The spectra exhibit pronounced splittings of the resonance lines at low field, followed by compression and then expansion of the resonance spectrum with increasing field. The results demonstrate two unique sets of ionic spins, and a gradual transformation from an antiferromagnetic state to magnetically induced paramagnetism.     

Interpretation of resonance cars and shpolskii spectra with calculated molecular geometries,vibrational frequencies and relative intensities: Chrysene in it's lowest excited singlet and triplet state

Coherent anti-Stokes Raman scattering (CARS) spectra of excited molecules as well as Shpolskii spectra provide information about geometry changes between ground and excited states. Vibrational frequencies and relative intensities from recently obtained CARS spectra of the chrysene S₁ and T₁ state and earlier observed Shpolskii spectra are interpreted in terms of molecular geometry and force-field changes by means of quantum-chemical consistent force field (QCFF) and Franck-Condon factor calculations. The comparison of observed and calculated relative intensities indicates a coupling between the S₁ and S₂ state enhancing some of the vibrational radiative singlet transitions both in absorption and fluorescence spectra whereas within the phosphorescence spectra proportionality to calculated Franck-Condon factors is obeyed. The T₁ state is the more loosely bound state and its geometry change is different from that of the S₁ state. The resonance CARS transitions in the S₁ state are assigned to totally symmetric vibrations getting their intensity by a coupling scheme analogous to the A term of the resonance Raman effect: the relative intensity of a transition is shown to be proportional to the Franck-Condon factor to the higher excited state and to the squared vibrational frequency. Using this relation this state can be identified by means of its finger-print-like intensity pattern.     

Resonant photoemission and absorption spectroscopy study of the Cu<Subscript><Emphasis Type="Italic">x</Emphasis></Subscript>TiSe<Subscript>2</Subscript> electronic structure

The Cu3p and Cu2p resonance photoelectron spectra of the valence bands and core levels as well as Ti and CuL _2,3 absorption spectra for monocrystals 1T-Cu _x TiSe₂ were studied. The valence spectra obtained at Cu3p and Cu2p resonance drastically differ from each other. For Cu 3p-3d resonance, there are several bands corresponding to different channels of excited state decay. Spectra of the valence bands at Cu 2p-3d resonance are virtually identical to the spectra of pure TiSe₂. As follows from the absorption spectra, titanium atoms have the oxidation state 4+, whereas copper atoms are close to the free ion state.     

Direct measurement of the vibrational predissociation lifetime of NeBr2 in the ground electronic state

The vibrational predissociation lifetime of NeBr₂ in the ground electronic state with one vibrational quantum in the halogen stretch was measured directly in a free jet expansion. NeBr₂(X, ν = 1) was detected by optical-optical double resonance to monitor the population as a function of distance from the nozzle to the laser interaction region. The vibrational predissociation lifetime for NeBr₂(X, ν = 1) was determined to be 8 ± 3 μs.     

Application of the mössbauer effect to microgram samples with resonance sample scintillators

The possibilities of the Mössbauer effect for qualitative and quantitative measurements of microgram amounts of resonance absorbing matter are considered. The sample is placed in a plastic scintillator and the conversion electrons emitted are measured. The preparation of the resonance sample scintillators (RSS) and the methods of measurement are described in detail. Mossbauer spectra of different samples containing SnO₂ are given as an example. The sensitivity of the method is around 10^-7 g (even less in some cases). A concentration of 4 · 10^-6% SnCl₂ in aqueous solution can be measured. The methods can be used for surface studies of small particles.