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 104 (1996), S. 419-429 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The magnetic circular dichroism (MCD) of CD3I is reported in the 48 700–60 100 cm−1 region. This region embraces the 5p → 6s manifold, much of the 5p →6 p manifold, and perhaps some members of the 5p → 5d Rydberg manifold of states. The results in the 5p →6 s manifold are confirmatory of the same work in CH3I [Scott et al., J. Chem. Phys. 68, 4678 (1978)]; some questions occur concerning the conferral of absorption intensity on the highly forbidden 5p →6 s[1] state of these molecules. The MCD of part of the 5p →6 p manifold of CD3I is also reported. Five possible 5 p→6 p origins have been securely identified and a sixth has been tentatively assigned. Apart from one of these, that at 58 930 cm−1, the other five origins assigned here match none of those found by MPI spectroscopy [Dobber, Buma, and de Lange, J. Chem. Phys. 99, 836 (1993)], suggesting a degree of complementarity of both data sets. Relative magnetic moments for all six observed states in the 5p → 6p region have been determined: the 58 930 cm−1 origin has been assigned as a 1Σ+ state, possibly an interloper from the 5d manifold, and the 59 630 cm−1 origin has been assigned as a 1Π1 state. The 5p → 6p manifold of CH3I is also discussed and assignments, which are largely vested in correlations of energies, absorption intensities, and MCD specifics with the corresponding excitations of CD3I, are given. © 1996 American Institute of Physics.
    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 101 (1994), S. 1959-1966 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The time dependence of the optogalvanic signals induced by 1sj→2pk (Paschen notation) pulsed laser excitations of neon in a low power ∼30 MHz radio frequency (rf) discharge at ∼5 Torr has been investigated. The method of Kumar and McGlynn [Chem. Phys. Lett. 176, 536 (1991)] has been improved and is used to separate the temporal profiles of the optogalvanic signals into two components: one attributable to ionization rate changes and the other to acoustic effects. This separation simplifies the identification of the kinetic processes which produce optogalvanic signals. Selective laser excitation of 2pk states, ones which possess quite different decay branching ratios to the metastable and nonmetastable 1sj states, reveals time dependencies due to unique perturbations of specific 1sj populations. No dimer mediated nor, indeed, any effects associable with 2pk state populations contribute to the profiles. Competitive processes which increase or decrease the ionization rates are identified at t≥1 μs. The extensive broadening of the acoustic and ionization components is caused by radiation trapping of 1s2→1S0 and 1s4→1S0 photons.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 69 (1998), S. 40-48 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: A new device, a selective digital integrator (SDI), for the acquisition of modulated polarization spectroscopy (MPS) signals is described. Special attention is given to the accurate measurement of very small signals (ac component of interest 〈10−3×dc component) buried in noise. The polarization of light is altered with fast modulators (modulation frequency ∼50 kHz). A SDI connected to a single detector is used to separately and selectively measure the polarization-dependent intensities of electronic transitions. The SDI is a major improvement over the lock-in approach: it has on-the-fly time-resolved data acquisition and integration capability, and a wide gain-switching-free dynamic range (10 orders of magnitude). This design permits a variety of applications that require detection of modulated or pulsed signals. The advantages of the MPS-SDI method are demonstrated on the first Rydberg electronic transitions of (+)-3-methylcyclopentanone. The selectively measured MPS intensities are provided in 3D form (intensity versus both wavelength and light polarization). A discussion of the scattering problems that bedevil measurements at higher optical densities is included, and ways to correct for it are outlined. © 1998 American Institute of Physics.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 3068-3073 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The optogalvanic effects (OGE) induced by pulsed laser excitation of Ne 1s2,4→2p1,3 transitions in a low power, ∼30 MHz radio frequency Ne discharge at ∼5 Torr are described. The polarity (sign) of the OGE signal is controlled by perturbations of the 1sj populations. The steady state 1s4 population is ∼101 times larger than the 1s2 population and the OGE signals for 1s4→2p1,3 excitations are correspondingly stronger than those for 1s2→2p1,3 excitations. The plasma temperature is found to be ∼1000 K. The excitations 1s2,4→2p3 are more efficient at signal production than the 1s2,4→2p1 excitations, which is contrary to prediction. The OGE signals are consequences of: (1) perturbation and reequilibration of the metastable 1s3 and 1s5 populations; (2) radiatively trapped 1s2→1S0 photons; and (3) collisionally induced 1s2, 1s4↔1s3, 1s5 energy transfer. The OGE signal components, both the ionization and photoacoustic constituents, are temporally coincident only when the immediate causative agents are trapped photons. When otherwise produced, the photoacoustic part is delayed relative to the ionization component by the time required for the acoustic wave to travel from the locus of excitation to the sensitive region(s) of the plasma. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 5
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Inorganic chemistry 7 (1968), S. 1285-1290 
    ISSN: 1520-510X
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    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 85 (1986), S. 2483-2488 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Molecular constants of electronic states, all origins as well as some vibronic bands, derived from the lowest-energy Rydberg configuration of methyl iodide, are reported. Values of the internal angular momentum parameter ζeff, which is a measure of the strength of Coriolis and vibronic coupling, indicate that the spin of the Rydberg electron is effectively uncoupled from the molecular axis in the pure electronic states and that dynamic interactions between electronic, rotational, and vibrational motions completely quench the internal angular momentum in some vibronic levels. It is concluded that the parameters ζeff, as obtained from one-photon absorption spectra, are approximately those of the alternate levels, 2E3/2 and 2E1/2, of the CH3I+ ion-core ground configuration X˜.
    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 85 (1986), S. 5401-5404 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Rotational envelopes of some of the lowest-energy (R6s) Rydberg transitions [i.e., the two electronically degenerate B3E(1) and C1E(1) band systems and the totally symmetric A1(0+) band system] of methyl iodide are calculated for a two-photon absorption process and compared to the experimental spectra obtained using the technique of two-photon resonant multiphoton ionization (MPI). The rotational band shapes, which were computed with molecular constants extracted from a simulation of high-resolution, one-photon absorption data, reproduce all significant features of the experimental MPI spectra, including temperature and polarization dependencies. Since one- and two-photon processes are governed by different selection rules, the present results are an independent verification of spin uncoupling in these R6s states. These results, therefore substantiate the conclusion that the R6s electron uncouples from the molecular frame during the evolution of the Rydberg state and that, consequently, the molecular constants extracted from experimental band shape analysis pertain to the freely rotating, electronically degenerate, molecular–ion core.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 84 (1986), S. 6808-6815 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The photoinization of 9-phenylanthracene (PhA) and the role of the radical cation in the photocyanation reaction is reported. Radical cations are produced by two processes: (a) biphotonic unimolecular ionization under high intensity laser excitation and (b) a monophotonic bimolecular electron-transfer process in the presence of dicyanobenzene (DCB). In both cases, the singlet excited state is the precursor to the radical cation.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 82 (1985), S. 3929-3933 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The photoionization of perylene in two common polar solvents (acetonitrile and dimethylformamide) is reported. The transient absorption spectra differ significantly from one solvent to the other: Positive and negative ion absorption intensities invert as also do ion decay times. These differences are attributed to solute–solvent interactions in the excited state. The mechanism for the photoionization process is posited to involve electron injection from perylene to the electrophilic solvent (i.e., acetonitrile) and hole injection from perylene to the nucleophilic solvent (i.e., dimethylformamide).
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 99 (1993), S. 2560-2566 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Photoabsorption or photoionization spectra of CH3I are discussed as a function of perturber pressure for 11 different binary gas mixtures consisting of CH3I and each one of 11 different gaseous perturbers. Five of the perturbers were rare gases and six were nondipolar molecules. The energy shifts of CH3I Rydberg states become independent of n, the principal quantum number, for n≥10. The energy shifts for n≥10 vary in a linear fashion with perturber number density. The electron scattering lengths for the perturbers are extracted from the shifts using Fermi theory in which the polarization term is that of Alekseev and Sobel'man. These scattering lengths are compared with those from swarm and time-of-flight experiments. It is found that the uncorrected shift scattering lengths correspond to the zero energy or near-zero energy scattering lengths obtained from extrapolated swarm and time-of-flight data. It is found that plots of scattering length vs polarizability α (α¯ for molecules) define two linearities, one for the rare gases and one for molecules, CO2 being an exception to the latter linearity (presumably because of its large quadrupole moment). For a given polarizability, it is also found that molecules exhibit a larger scattering length than the rare gases. These results are discussed and consequences for scattering cross sections are elaborated.
    Type of Medium: Electronic Resource
    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...