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  • 1
    Electronic Resource
    Electronic Resource
    Westerville, Ohio : American Ceramics Society
    Journal of the American Ceramic Society 83 (2000), S. 0 
    ISSN: 1551-2916
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: The dielectric properties of (Ba0.6Sr0.4)TiO3 and Al2O3-doped (Ba0.6Sr0.4)TiO3 have been characterized. The grain size of the specimen is maximum for (Ba0.6Sr0.4)TiO3 that has been doped with 1 wt% Al2O3. The density and the real part of the relative dielectric constant each decrease as the Al2O3 content increases. The loss factor is minimum for (Ba0.6Sr0.4)TiO3 that has been doped with 2 wt% Al2O3. The dielectric constant of the specimens decreases as the applied dc field increases. The influence of the dc field on the loss factor is much less than that on the dielectric constant. The tunability is ∼24% for (Ba0.6Sr0.4)TiO3 that has been doped with 1 wt% Al2O3.
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 112 (2000), S. 1797-1803 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We studied the state-resolved dynamics of S1 acetaldehyde to product channels with quantum-beat spectroscopy. Two bands near the threshold of dissociation to radical products CH3+HCO in a supersonic jet, displaying most quantum-beat features, are recorded with resolution 0.025 cm−1. Evaluated on the basis of a simple asymmetric rotor, the origins of these two bands 1402−1501 and another denoted # are 31 275.045(1) and 31 523.263(1) cm−1; effective rotational constants of excited state are A=5.7883(1), 5.0408(3), B=0.33269(2), 0.32320(2) and C=0.31026(2), 0.32091(2) cm−1, respectively; large A value results from lack of consideration of torsional motion. For these two vibrational levels most rotational states (about 70 percent) display quantum-beat features attributed to coherently excited singlet–triplet eigenstates. The linewidth in transformed spectra for level #, ∼125 cm−1 below the dissociation threshold, increases with increasing total angular momentum J whereas level 142−151 that is 375 cm−1 below shows a small linewidth independent of J. This is because correlation of the triplet state with dissociation to form radical products results in a decreased lifetime of the triplet state in the tunneling region. A systematic dependence on rotational quantum number implies Coriolis-induced vibrational coupling of triplet states to dissociating continuum on the exit side of the dissociation barrier. © 2000 American Institute of Physics.
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 109 (1998), S. 9340-9350 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Fluorescence decay of the S1 state of d4-acetaldehyde is measured. Below the dissociation threshold for formation of fragments of formyl and methyl radicals, single exponential decays of fluorescence are observed. Biexponential decay is observed when the excitation energies are near and above the dissociation threshold. Hence, in this region the mechanism for intramolecular relaxation of energy reaches the "intermediate case." Strong coupling between S1 and T1 states or reversible reaction for S1↔T1 results in this biexponential behavior in the fluorescence decay of S1. Rates of appearance of DCO from dissociation of acetaldehyde are measured. The stepwise increases in plots of both rate of appearance of formyl radicals and rate of decay of excited acetaldehyde versus excitation energy for both isotopic variants of acetaldehyde are observed. According to fits to Rice–Ramsperger–Kassel–Marcus (RRKM) theory, these sharp increases correspond to vibrational levels of transition state in the triplet surface. Frequencies of torsional and C–C–O bending modes are determined to be (73±10) and (200±10) cm−1 for the transition state of CD3CDO and the torsional frequency (80±10) cm−1 for CH3CHO. That these fitted frequencies are less than values calculated with methods B3LYP and MP2 indicates a looser transition state than calculated for dissociation. From these fits the dissociation threshold for formation of radical fragments is determined to be 31 845 for CD3CDO and 31 650 cm−1 for CH3CHO. © 1998 American Institute of Physics.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 67 (1990), S. 3194-3196 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report on the measurement of the millimeter wave transmission properties of a dielectric waveguide with a YBa2Cu3O6+x boundary layer. The transmitted power and phase shift of a 94 GHz signal propagating through the dielectric waveguide structure was measured over the temperature range of 77–150 K. The transmitted power was observed to depend upon temperature due to the dissipation of the millimeter wave signal in the YBa2Cu3O6+x boundary layer. Thereby the temperature dependence of the normal-state ac conductivity was measured. The experimental data were fitted to a Drude model for the normal-state ac conductivity of the YBa2Cu3O6+x. The temperature dependence of the Drude scattering time was obtained. The scattering time was found to decrease with decreasing temperature and was 7.5–11.2 ps in magnitude.
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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. 5089-5100 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Fluorescence excitation spectra, at resolution 0.02 cm−1, in the system A˜ 1A″−X˜ 1A′ were recorded for acetaldehyde in a supersonic jet. We performed full rotational analysis of bands 1400+150n and 1400−150n, for n=0–4, in which 140+ and 140− denote the two inversion tunneling components of the aldehyde hydrogen out of plane bending, in the vibrational ground state of A˜ 1A″. Torsional levels from near the methyl torsional barrier to beyond that barrier are assigned. Sublevels of torsional symmetry A below the barrier are fitted as an asymmetric rotor, but the resulting values of the rotational parameter A are affected significantly by the torsional motion. For the E sublevels, K doublet states split significantly with torsional quantum number vt. Anomalous transitions (ΔKa=0, ΔKc=0) to A sublevels are observed for bands 1400+1504 and 1400−1503, which cannot be simply explained from the Coriolis-type interaction of torsion and rotation. The positions of A and E sublevels in 140−15n cannot be fitted with a program involving only interaction of torsion and rotation, because for n=0–2 states the A/E splitting is reversed from those in 140+15n. Interaction with inversion evidently varies the splitting of torsional sublevels and the K structure. © 2001 American Institute of Physics.
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 114 (2001), S. 1187-1193 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Spectra of a˜ 3B1(ν1ν2ν3)=(110) and (200)–X˜ 1A1(000) of 32SO2 and 34SO2 are obtained in a supersonic jet at a resolution 0.015 cm−1. The rotational structures are analyzed for both isotopic species to obtain precise rotational and spin constants. Two new bands at 27 032.222(1) and 27 515.41(1) cm−1 arising from vibronic interaction separately with vibrational state (110) and (200) of a˜ 3B1 are assigned to transitions to b˜ 3A2(011) and (101). The rotational structure of b˜ 3A2 is observed and analyzed for the first time. The two vibrational states are analyzed to yield effective rotational constants A=1.4348(3), 1.89(3), B=0.3610(3), 0.412(3), and C=0.2689(3), 0.239(3) cm−1, respectively. Then the difference ν1−ν2 of vibrational frequency of b˜ 3A2 is obtained to be 483.19 cm−1. Because of interaction to b˜ 3A2(011) the observed spacing of K stack and spin constants α and β for a˜ 3B1(110) are smaller whereas the state a˜ 3B1(200) is relatively unaffected and only spin constants vary significantly. © 2001 American Institute of Physics.
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 116 (2002), S. 1003-1011 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: In the fluorescence excitation spectrum of acetaldehyde cooled in a supersonic jet, we performed a full rotational analysis of combination bands 10011400+150n and 10011400−150n, n=0–4 in the system A˜1A″–X˜1A′. The vibrational frequency of the C–C–O bending mode is determined to be ν10′=373.163(3) cm−1. The rotational structures of combination bands 10011400+1502, 10011400−1502, 10011400+1503, and 10011400−1504 resemble the structures of 1400+1502, 1400−1502, 1400+1503, and 1400−1504, respectively, but the intense E lines observed for 1400−1503 are not found in 10011400−1503. Torsional spacings observed in the C–C–O bend series are slightly smaller than those in the pure torsional series 140+ and 140−; these result from a decreased torsional barrier due to the C–C–O bending motion. Inversion spacings exhibit a pattern similar to those in the series 140+ and 140−. Reversed abnormal torsional sublevel A/E splittings are found for states n=0–2 of the 101140− series, similar to those in the 140− series. For states n=3, the K rotational structures between the 140+ and 101140+ series and for n=4, the 140− and 101140− series are more similar than those between the pure torsion-inversion series 140+ and 140−. Hence, these experimental data imply that the interaction of the C–C–O bend with rotational structures of torsional states is smaller than that resulting from the aldehyde inversion. © 2002 American Institute of Physics.
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 116 (2002), S. 7779-7782 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Photodissociation of jet-cooled ethylbenzene at 248 nm was studied using VUV photoionization/multimass ion imaging techniques. The photofragment translational energy distribution obtained at 248 nm showed that after the excitation 75% of the ethylbenzene molecules dissociate from electronic excited state, and the rest 25% of the molecules dissociate through a hot molecule mechanism. This is the first experimental evidence which proves that the dissociation of alkyl-substituted benzenes can occur not only from hot molecule mechanism in this UV region. © 2002 American Institute of Physics.
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  • 9
    Electronic Resource
    Electronic Resource
    s.l. ; Stafa-Zurich, Switzerland
    Key engineering materials Vol. 336-338 (Apr. 2007), p. 14-17 
    ISSN: 1013-9826
    Source: Scientific.Net: Materials Science & Technology / Trans Tech Publications Archiv 1984-2008
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
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  • 10
    Electronic Resource
    Electronic Resource
    Springer
    Journal of materials science 35 (2000), S. 4901-4905 
    ISSN: 1573-4803
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Abstract The CaO-Li2O-Sm2O3-TiO2 system has been reported having a high dielectric constant and good temperature stability. Based on the composition of CaO : Li2O : Sm2O3 : TiO2 : = 16 : 9 : 12 : 63, the modifications of CaO and Sm2O3 were investigated. In this paper, CaO has been partially substituted by BaO and Sm2O3 by Nd2O3. It was found that the introduction of BaO leads the modified ceramics to be mixtures of two phases. The fQ value has been significantly promoted, while the dielectric constant can remain higher than 90. To obtain a higher dielectric constant, Sm2O3 has been further partially replaced by Nd2O3. The sintering temperatures for the property change were also studied. The temperature coefficient of resonant frequency could be varied from a positive value to a negative value according to the different sintering temperatures. Excellent dielectric properties of εr = 103, fQ = 7200 and τf = + 2 ppm/°C were obtained with a composition of CaO : BaO : Li2O : Sm2O3 : Nd2O3 : TiO2 = 14 : 4 : 8 : 10 : 2 : 63 (molar ratio) and sintered at 1350°C for 3 h.
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