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1 tronic state where the far-from-equilibrium, vibrationally activated HCHO molecules react with therma
2 ual observation is interpreted in terms of a vibrationally activated quantum mechanical tunneling pro
3 r loop regions of the protein systems become vibrationally activated.
4                              The presence of vibrationally active species, such as nitrate and phosph
5 5 cm(-1) These results are rationalized in a vibrationally adiabatic (VA) model in which the motion o
6 zero-point energy (ZPE) to the MEP gives the vibrationally adiabatic ground state curve, V(a)(G), whi
7 s has been explained within the contemporary vibrationally assisted activated H-tunneling (VA-AHT) mo
8 with long lifetimes (100-400 fs) that permit vibrationally assisted charge transfer between a donor a
9 ystem from the charge transfer regime to the vibrationally assisted exciton transfer regime and find
10 lained by hydride transfer occurring through vibrationally assisted tunneling.
11 y by the Boltzmann average of the zero-point vibrationally averaged JHD of two isomers.
12 8 isotopic forms have been analyzed, and the vibrationally averaged structure of the system has been
13                                   Effective (vibrationally averaged) H-D distances have also been det
14                                   We observe vibrationally coherent formation of the P1 intermediate
15 opsin to exploit two mechanisms working in a vibrationally coherent regime.
16 ired with directed molecular excitation into vibrationally cold electronic states.
17 state to produce rotationally excited CO and vibrationally cold H2.
18 sis imply that intercalated Ca-bound CO2 are vibrationally constrained and contribute to the higher f
19             Furthermore, when the FTMS has a vibrationally cooled MALDI ion source, fragile glycolipi
20 ynamics in current pump-probe experiments of vibrationally coupled electrons, highlight the importanc
21 o-active network forms an electronically and vibrationally coupled system in bR, and most likely in a
22 rces where the layers are electronically and vibrationally coupled.
23 gments due to through-bond and through-space vibrationally coupling between adjacent peptide groups.
24 bsent and bulk behaves as electronically and vibrationally decoupled monolayers stacked together.
25 ing calculations qualitatively reproduce the vibrationally dependent rotational and angular distribut
26 ed and current-driven phase transitions, the vibrationally driven bandgap collapse observed here is n
27                            The dependence of vibrationally elastic and inelastic scattering on oxygen
28 ply resonant sum frequency (TRSF) and doubly vibrationally enhanced (DOVE) spectroscopies are example
29 ional spectroscopy is performed using doubly vibrationally enhanced four-wave mixing in dilute soluti
30                                              Vibrationally enhanced ground state tunnelling has been
31 antum tunneling, driven by protein dynamics [vibrationally enhanced ground-state quantum tunneling (V
32 significant energy of activation all suggest vibrationally enhanced hydride tunneling in the TS-catal
33 f tunneling and to theoretical constructs of vibrationally enhanced tunneling in enzymatic reactions.
34          We analyse the performance of these vibrationally-enhanced squeezed states in a phase estima
35 ast conversion of the S2(pipi*) state to the vibrationally excited (1)npi* state.
36 ) or ca. 5 ps (Zn) and decay giving way to a vibrationally excited (i.e., hot) ground state via back
37 attributed either to efficient relaxation of vibrationally excited 1BpCMe by 1,2 migration of hydroge
38 +) attack saturated, acyclic ketones to make vibrationally excited adduct ions.
39 il for all processes investigated, including vibrationally excited and vibrationally inelastic collis
40       Here, we highlight a dramatic role for vibrationally excited bimolecular reactants in the oxida
41                                              Vibrationally excited CO(2) (nu(2) > 3) was observed in
42 ion, were performed for the de-excitation of vibrationally excited CO.
43 rom decomposition of initially energized and vibrationally excited Criegee intermediates, are explore
44 ationally cold CO in conjunction with highly vibrationally excited H2.
45 he LTP is from dielectronic recombination of vibrationally excited He(2)(+) ions.
46 ViBr and AllBr gave evidence of a long-lived vibrationally excited intermediate for both Direct and D
47 -band transitions, i.e., those starting from vibrationally excited levels, are needed to accurately m
48 ose studies for the prototypical reaction of vibrationally excited methane and its isotopologues in g
49 n of also rotational mode specificity in the vibrationally excited methane reactions.
50                The rotational spectra of the vibrationally excited molecular eigenstates display coal
51              The chemical dynamics of highly vibrationally excited molecules have been studied by mea
52 studies of the chemical reaction dynamics of vibrationally excited molecules reveal the ability of di
53      Pt catalyzes NTP-generated radicals and vibrationally excited molecules to produce NO.
54 = 0, J'')->Ar(+)+N(2)(v', J'), where all the vibrationally excited N(2) products are dominated by for
55 ly studied experimentally: the scattering of vibrationally excited nitric oxide molecules from a Au(1
56 cule decreases during collisions with highly vibrationally excited NO(X(2)pi((1/2)), V = 18; V is the
57                       Different rotationally-vibrationally excited OH products have markedly differen
58 stepwise route involving the intermediacy of vibrationally excited or relaxed carbene.
59 hanism of perthiyl radical generation from a vibrationally excited parent molecule that asymmetricall
60 asure the conformation isomerization rate of vibrationally excited pent-1-en-4-yne (pentenyne).
61  of interconversion between the rival highly vibrationally excited photoproducts in their ground elec
62 on barrier), we remove an electron to form a vibrationally excited singlet vinylidene-d(2) and follow
63  majority of the CO molecules to their first vibrationally excited state (v = 1), we observed infrare
64 g surfaces, for some of the complexes higher vibrationally excited states can also contribute to the
65 ble tunneling-facilitated mixing with highly vibrationally excited states of acetylene, leading to br
66     The SRS process pumps molecules to their vibrationally excited states.
67                           The electronically/vibrationally excited system then relaxes through period
68 ch transitions due to the S(1) state and the vibrationally excited triplet state(s) formed by intersy
69 results from intersystem crossing to produce vibrationally excited triplets with enough energy to lau
70 ized, suggesting average lifetimes >1 ps for vibrationally excited vinylidene-d(2).
71 et state (tau(1) </= 300 fs); (3) ESA of the vibrationally excited, ligand-centered T(1) state (tau(3
72       A striking enhancement in the yield of vibrationally-excited OH super rotors is detected when e
73                                        After vibrationally exciting a single molecular conformation o
74                              This is done by vibrationally exciting a specific species that exists in
75               Following internal conversion, vibrationally highly excited ground state molecules were
76 f 'hot' electrons leaving a metal surface as vibrationally highly excited NO molecules collide with i
77 mediate that forms in 170 fs and decays to a vibrationally hot (5)T(2g) state in 39 fs.
78                                 It is formed vibrationally hot and cools over several picoseconds, co
79 exes, where the energy dispersion hints at a vibrationally hot final state.
80  + c-C(6)H(11) in CH(2)Cl(2), which produces vibrationally hot HCN.
81 d the molecule results in the formation of a vibrationally hot ion.
82 electronically excited species rather than a vibrationally hot K intermediate.
83 orize that internal conversion of S(1A) to a vibrationally hot S(0) of 1 forms 2, whereas intersystem
84 ons, both donor and acceptor are found to be vibrationally hot, pointing to an even redistribution of
85 ng group is extruded in 1.8 ps, generating a vibrationally hot, spin-conserving closed-shell singlet
86                     The use of the probes to vibrationally image proteins and other biomolecules with
87 d to recent experimental observations of the vibrationally induced isomerization of OC-NaCl(100) to C
88    We investigate the optical stimulation of vibrationally induced molecular magnetism and estimate c
89 tigated, including vibrationally excited and vibrationally inelastic collisions.
90 orward-scattering is universally observed in vibrationally inelastic H + D(2) collisions over a broad
91                                              Vibrationally inelastic scattering is a fundamental coll
92 the o-D(2)(v' = 3, j') products suggest that vibrationally inelastic scattering is the result of a fr
93 d differential cross sections (DCSs) for the vibrationally inelastic scattering process H + o-D(2)(v
94 nctions in bonding, vibrational spectra, and vibrationally mediated negative differential resistance
95 ocesses at a gas-metal interface, can hamper vibrationally mediated selectivity in chemical reactions
96 d native conformations are still found to be vibrationally more flexible than random coil structures,
97 es, both alpha-helices and beta-hairpins are vibrationally more flexible.
98       The nonlinear signal is dominated by a vibrationally non-resonant background, obscuring the Ram
99 the laser excitation pulses, suppressing the vibrationally non-resonant background.
100  the wild-type ecDHFR (l-DHFR) to generate a vibrationally perturbed "heavy ecDHFR" (h-DHFR).
101 e sequence, we show that the pathway that is vibrationally perturbed during UV-induced electron trans
102                          Conformer-specific, vibrationally resolved electronic spectroscopy of benzyl
103 arried out in mineral oil confirmed that the vibrationally resolved lowest-energy absorption bands ar
104 is study presents the first high-resolution, vibrationally resolved optical spectra of mass-selected
105 t and apply it to evaluate time-resolved and vibrationally resolved photoelectron spectra and photoio
106                                              Vibrationally resolved photoelectron spectra have been o
107                                    We report vibrationally resolved photoelectron spectra of internal
108                                              Vibrationally resolved photoelectron spectra were obtain
109 The present study offers the first partially vibrationally resolved photoelectron spectrum of the phe
110 -of-the-art quantum chemical calculations of vibrationally resolved spectra allow, for the first time
111                                          The vibrationally resolved spectra are dominated by a long p
112                                Additionally, vibrationally resolved spectra were determined allowing
113                                              Vibrationally resolved spectra were obtained at differen
114                                              Vibrationally resolved transient spectra of (3)9 were re
115                       The spectra are nearly vibrationally resolved, with little absorption below 1 T
116                      We demonstrate that the vibrationally resonant coherent anti-Stokes Raman Scatte
117                                           In vibrationally resonant sum-frequency generation (VR-SFG)
118 tion followed in time by a surface-specific, vibrationally resonant, infrared-visible sum-frequency p
119 RS) are attractive because they have narrow, vibrationally specific spectral peaks that can be excite
120 that the body of hovering insects can not be vibrationally stabilized in a non-vertical orientation.
121 predictions when the formed radicals are not vibrationally stable.
122 gands for the QDs, coupled electronically or vibrationally to localized surface states or to the delo

 
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