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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 97 (1992), S. 2809-2812 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: State-to-state threshold photoionization cross sections from specific spin–rotation levels N'=7, J'=8.5, v'=3 of C 4∑− VO to specific levels N+J+ of X 3∑− VO+ show a remarkable propensity for large, positive ΔN. Observed transitions span the ranges ΔN=−5 to +7 and ΔJ=−5.5 to +4.5. The adiabatic ionization potential of VO is 7.2386±0.0004 eV. The mean bond length of v+=0, X 3∑− VO+ is 1.561±0.003 A(ring).
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 854-855 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We have measured the adiabatic ionization potential of the aluminum dimer, AIP(Al2)=5.989±0.002 eV (±2σ uncertainty), using threshold photoelectron spectroscopy with resonant two photon ionization (ω1 fixed and ω2 scanned). We obtain the Al+2 , X 2Σ+g vibrational constants ωe =178±8 cm−1 and ωexe =2±2 cm−1 (±2σ uncertainty), the first spectroscopic data for a cationic Al cluster. These results are in excellent agreement with ab initio calculations.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 90 (1989), S. 1415-1428 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We apply the techniques of resonance enhanced multiphoton ionization (REMPI) and time-of-flight photoelectron spectroscopy (TOF-PES) to TiO molecules cooled in a pulsed nozzle expansion to obtain vibronic spectra of gas phase TiO+. The adiabatic first ionization energy is refined to I1(TiO)=54 999±52 cm−1=6.819±0.006 eV, which yields D0(Ti+–0) =159.9±2.2 kcal/mol. For the X 2Δ state of TiO+, we resolve spin–orbit pairs of vibrational levels for v=0–14, yielding ωe=1045±7 cm−1 and ωexe =4±1 cm−1. The spin–orbit splitting ΔEso =210±6 cm−1 permits confirmation of the state symmetry by comparison with the known spin–orbit splittings of the X 3Δ state of TiO. We also observe a new excited B 2∑+ state at T0=11 227±17 cm−1 with ωe =1020±9 cm−1 and ωexe =6±2 cm−1. This state is distinct from the A 2∑+ state (average frequency 860±60 cm−1) previously observed by Dyke and co-workers. From components of certain PESs apparently due to one or more metastable states of TiO, we infer the existence of a previously unobserved state of neutral TiO at T0=2980 cm−1, possibly the 3∑− state. Finally, we discuss the electronic structure and vibrational frequencies of TiO, TiO+, and other third row metal oxides from both molecular orbital and ligand field points of view in order to understand the ordering of electronic states and certain trends in vibrational frequencies. The molecular orbital model readily explains why nominally isoelectronic neutral and cationic metal oxides, such as TiO+ and ScO, are electronically quite dissimilar.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 91 (1989), S. 3854-3868 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Resonant two-photon ionization of gas phase Cu2 in a cold molecular beam in conjunction with time-of-flight photoelectron spectroscopy provides new vibronic state spectroscopic information for the dimer cation Cu+2. One color ionization via the 0–0, 1–0, and 2a–0 bands of Smalley's System V neutral Cu2 resonant states (J←X transition) accesses Cu+2 states in the range 0–1.4 eV. The electron kinetic energy measurements slightly refine the first adiabatic ionization energy of Cu2 to I1(Cu2)=7.899±0.007 eV. We observe two electronic states of Cu+2 which we assign as X 2Σ+g and an excited 2Π spin–orbit pair of sublevels with origins at T0(2Π3/2)=1.143±0.002 eV and T0(2Π1/2)=1.256±0.002 eV. The absence of spin–orbit splitting identifies the ground state 2Σ symmetry; the spin–orbit splitting of 898±8 cm−1 identifies the excited states as 2Π. Within X 2Σ+g we observe a remarkably long vibrational progression, perhaps extending from v=0–80. The vibrational intervals determine the constants ωe=188±4 cm−1 and ωexe=0.75±0.09 cm−1. The 2Π vibrational intervals determine ωe=244±6 cm−1. The adiabatic bond dissociation energy of ground state Cu+2 is D0(Cu+–Cu)=1.84±0.08 eV. The intensity pattern of the X 2Σ+g vibrational bands exhibits multiple peaks whose positions and amplitudes are sensitive to the resonant J state vibrational level. For 0–0 excitation, we observe reproducible band intensity alternation. We present preliminary mass spectral and photoelectron data indicating that the cause of the highly non-Franck–Condon band intensities is excitation of long lived, dissociative autoionization states which undergo extensive nuclear motion on the time scale of electron ejection. We propose an autoionization mechanism that includes a description of the Cu2 J state and explains the observed phenomena invoking only one electron transition.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 115 (2001), S. 3099-3104 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Collisional removal of the v′=0 level of the A 2Σ+ state of the OH radical has been studied as a function of rotational level N′ at room temperature. OH in high rotational levels of the X 2Πi state were created by 193 nm photolysis of HNO3 and excited to A 2Σ+ by a tunable dye laser. Time decays of fluorescence at varying pressures were measured. For O2 and H2, the quenching cross section σQ decreased with increasing N′ until N′∼10; for higher N′ it appears to remain approximately constant. Xe behaves the same way except that the decrease continues to N′=15. For Kr, σQ appears to decrease to within experimental error of zero at N′=10; and for N2 it was within error of zero above N′=10. These results have implications for laser-induced fluorescence atmospheric monitoring of OH and combustion temperature determinations, as well as a fundamental understanding of collisional quenching. Quenching of OH, N′∼1, by HNO3 was found to be 81±8 Å2. © 2001 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    New York : Cambridge University Press
    Central European history 25 (1992), S. 52-75 
    ISSN: 0008-9389
    Source: Cambridge Journals Digital Archives
    Topics: History
    Notes: Long before Melanchthon and Erasmus drew their parallels, paternal and political authority had enjoyed a long and successful association in Greco-Roman thought. The apparent resurgence of this patriarchal metaphor in sixteenth-century European literature and polemic, however, has led some historians to suggest a more socially significant transformation in the actual legal or moral authority of one or both of these father figures. Beginning with the pioneering work of Phillippe Ariès many historians of the family, particularly Lawrence Stone, have identified the sixteenth century as a time of greater paternal authority within the household and the beginning of the modern nuclear family throughout most of Europe. Others, expanding on references by Aries and Stone to a new state paternalism, have focused on the political half of the patriarchal analogy, especially the almost ubiquitous association among sixteenth-century German authors of the Hausvater (head of the household) with the Landesvater (political ruler). For most of these scholars, paternalistic language was a natural and even necessary component of the ambitious absolutist state-building of early modern Europe.
    Type of Medium: Electronic Resource
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  • 7
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    Atlanta : Periodicals Archive Online (PAO)
    Central European History. 25:1 (1992:Spring) 52 
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