ALBERT

All Library Books, journals and Electronic Records Telegrafenberg

feed icon rss

Your email was sent successfully. Check your inbox.

An error occurred while sending the email. Please try again.

Proceed reservation?

Export
  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 100 (1994), S. 8212-8218 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: It has been established for some time that the bond energies for any given valence pπ excited state of Group 1 (2P) and Group 2 (1,3P) metal-atom/rare-gas (M⋅RG) van der Waals complexes tend to increase with the polarizability of the RG atom. It is also known that the binding energies of the corresponding M+⋅RG ground state ions are generally greater than those of the neutral M(pπ)⋅RG excited states with the same RG atom. However, there are two stark exceptions to these trends, both involving Group 1 metal atoms and the rare gas He; Li(2p 2P)⋅He(2Π) and Na(3p 2P)⋅He(2Π), which are the focus of the present study. We have conducted ab initio calculations of the potential energy curves of M(np 2P)⋅RG(2Π) and M+⋅RG states, where M=Li, Na and RG=He, Ne. We find that the unusual behavior of the pπ Group 1 metal atom states is due to (i) the lack of M(pπ)–RG(pπ) repulsive orbital overlap in the He case, and (ii) substantial additional attraction due to correlated motion of the RG atom's electrons and the diffuse M(npπ) electron which is absent in the M+RG cases.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 114 (2001), S. 7052-7058 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We did laser pump–probe far-wing scattering experiments to study the photochemical reactions Li*(2p,3p)+H2→LiH(v″=1,2,J″)+H. We show in this work that the Li(2p)+H2⇒LiH+H reaction takes place when the kinetic energy of the reactants are high enough. We think that the Li(2p)+H2 collisions take place preferentially in bent near-C2v geometry and that the LiH2 2A′ intermediate plays a major role where wide-amplitude internal vibrations eventually result in losing a hydrogen atom from the LiH2 complex. We also have observed the Li(3p)+H2⇒LiH+H reaction. The rotational state distribution of the LiH product for excitation in the red wing is identical to that found in the blue wing region, it does not show any preference to high or low rotational states, and no asymmetry is observed in the reactive to nonreactive branching ratio. We show different possibilities for the reactive and nonreactive collisions and provide a tentative explanation of the reaction mechanism using the highly accurate ab initio potential energy surfaces. We also show that the harpooning model cannot be used to explain the reaction mechanism in the Li*+H2 collision for all the atomic states from Li(2s) to Li(3d), and that no long range electron transfer occurs from the metal atom to the hydrogen molecule. © 2001 American Institute of Physics.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 1101-1104 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We have investigated the direct collisional energy transfer process Na*(4p)+M→Na*(3d)+M, where M=He,H2 under gas cell conditions. We have measured the temporal profiles of the Na(3d–3p) sensitized fluorescence as a function of quenching gas pressure and fit the profiles to a two-state rate equation model to obtain the quenching rate coefficients from the Na*(4p) state. The total energy transfer rate coefficient out of the 4p state for He is small [(0.5±0.2)×10−10 cm3/s]. The total quenching rate coefficient out of the 4p state is much larger for H2[(3.9±0.5)×10−10 cm3/s]. Evidence suggests that the energy transfer rate coefficient for the 4p–3d process is ∼2.0×10−10 cm3/s with the remainder of the 4p quenching being predominantly reactive. We also compare the far-red wing absorption line shapes for the NaHe and NaH2 systems.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 2115-2122 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The experimental rates of predissociation of vibrational levels of the 1B1 (Ka'=0) excited states of the Cd⋅H2 and Cd⋅D2 complexes are shown to be consistent with both semiclassical and quantum-mechanical pseudodiatomic theoretical treatments of the process. The 1B1 pseudodiatomic potential was constructed by fitting an analytical function to the experimentally estimated Rydberg–Klein–Rees (RKR) inner and outer turning points. The potential of the repulsive 3A1 state was estimated by fitting an exponential function to the ab initio points of Boatz, Gutowski, and Simons, then adjusting the exponential parameter slightly to maximize overall agreement with the observed Cd⋅H2 and Cd⋅D2 predissociation lifetimes. The best-fit repulsive curves for both the semiclassical and quantum-mechanism calculations result in slightly "outer-wall'' 1B1/3A1 crossings at only 84 and 76 cm−1, respectively, above the 1B1 potential minimum. The 1B1/3A1 coupling matrix elements derived from both treatments were ∼150–160 cm−1, much smaller than the 404 cm−1 expected if the spin–orbit interaction were unchanged from that of the asymptotic Cd(5s5p) states. It is suggested that the apparent reduction in the coupling strength could be due to the marked change in the nature of the Cd 5pσ orbital due to the strong repulsive interaction with H2 in the 3A1 state and to the neglect of the anisotropy of the 1B1/3A1 triatomic potential surface crossing.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 99 (1993), S. 3815-3822 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Of the excited 1Π1 electronic states of van der Waals complexes of Mg, Zn, and Cd atoms (M) with rare-gas (RG) atoms, only the Zn⋅Xe (1Π1) and Cd⋅Xe (1Π1) states predissociate to form the lower-lying triplet states, Zn(4s4p 3P2) and Cd(4s4p 3P2), respectively. It has been postulated that such predissociations occur by means of potential curve crossings between bound 1Π1 levels and repulsive M⋅RG (3Σ1+) states. Since the M⋅RG (1Π1) states become more bound as the RG atom becomes more polarizable, from Ne through Xe, and the M⋅RG(3∑+) states should become more repulsive as the RG atom becomes larger in the same order, the likely reason that only the Zn⋅Xe and Cd⋅Xe 1Π1 states predissociate is that they are the only states which have 1Π1/3Σ1+ curve crossings below the energies which are accessed spectroscopically. We have carried out ab initio electronic structure calculations using various basis sets, and at various levels of correlation, to examine the repulsive 3Σ1+ potential curves of Zn⋅Ar, Zn⋅Kr, Zn⋅Xe, Mg⋅Ar, and Mg⋅Xe. These calculations support the general mechanism proposed, and show that the likely reason the Mg⋅Xe(1Π1) state does not predissociate is because the 1Π1/3Σ1+ curve crossing lies slightly above the energy region probed experimentally. It was necessary to utilize very good quality basis sets and high levels of correlated calculations to obtain agreement with experimental observations. In all cases, there was a regular decrease in the repulsive character of the M⋅RG(3Σ+) states as the basis quality and level of correlation was increased.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 96 (1992), S. 213-217 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The nascent rotational quantum state distributions of NaH and NaD products resulting from the reactions of Na*(4 2Pj) with H2, D2, and HD have been determined using the laser pump–probe technique. We have observed a bimodal rotational distribution with a minor component peaking at low J and a major component peaking at high J. We have observed no evidence for a kinematic isotope effect on the product distribution. Our results are consistent with a model wherein the reaction occurs predominantly on the attractive 2B2 potential energy surface in near C2v geometry with the rotational distribution being determined late in the exit channel.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 96 (1992), S. 218-229 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We have used a "half-collision'' pump–probe technique to measure the far wing absorption profiles of the NaH2 collision complex leading to the nonreactive formation of Na* and to four distinct final rotational states of the reaction product NaH(v‘=1, J‘=3, 4, 11, and 13). We have observed reaction on both the attractive potential energy surfaces and over a barrier on the repulsive surface. We have observed the effect of the Na* reagent electronic orbital alignment on the NaH final product rotational state distribution. Specifically, absorption to the repulsive surface leads preferentially to low-rotational product states, while absorption to the attractive surfaces leads preferentially to high-rotational product states of NaH. Isotopic substitution experiments give evidence of a kinematic isotope effect on the product rotational state distribution for reactive trajectories on the repulsive surface. We have developed a simple model using a quantum mechanical line shape calculation to estimate the NaH2 absorption probability as a function of wavelength. We then make simple phenomenological dynamical arguments to predict final state branching. There is an overall qualitative agreement between the experimental results and theoretical model predictions.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 8
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 99 (1995), S. 7878-7890 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 9
    Publication Date: 1993-09-01
    Print ISSN: 0021-9606
    Electronic ISSN: 1089-7690
    Topics: Chemistry and Pharmacology , Physics
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 10
    Publication Date: 1995-05-01
    Print ISSN: 0022-3654
    Electronic ISSN: 1541-5740
    Topics: Chemistry and Pharmacology , Physics
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
Close ⊗
This website uses cookies and the analysis tool Matomo. More information can be found here...