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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 108 (1998), S. 9506-9515 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The adsorption of ethylbenzene (EB) has been studied on thin films of FeO(111) and Fe3O4(111) grown epitaxially on Pt(111) using thermal desorption spectroscopy (TDS), ultraviolet photoelectron spectroscopy (UPS) and low energy electron diffraction (LEED). Applying a threshold analysis of the TDS data, desorption energies Edes and the corresponding frequency factors are deduced. The UPS measurements are performed under adsorption–desorption equilibrium conditions: The spectra are taken at varying sample temperature at constant EB gas phase pressures. From the spectra, the EB-coverages ΘEB are deduced. From the adsorption isobars obtained in this way, isosteric heats of adsorption qst(ΘEB) are obtained which are compared to the desorption energies Edes deduced from TDS. On the oxygen-terminated FeO(111) surface, two adsorption states are observed, a physisorbed first layer (β-EB) followed by condensation (α-EB). Their UP spectra are almost identical and very similar to the spectrum of gas phase EB. On Fe3O4(111), a more strongly chemisorbed species (γ1-EB) is adsorbed first, followed by physisorbed β- and condensed α-EB. The chemisorbed phase exhibits a strong shift and split of the highest occupied π orbitals of the phenyl group. This indicates a strong interaction between the substrate and the adsorbed molecules that are adsorbed with the phenyl ring lying flat on the surface. The desorption energies Edes and the isosteric heats of adsorption qst, respectively, are 91 (85) kJ/mol for γ1-, 55 (58) kJ/mol for β- and 50 (52) kJ/mol for α-EB and agree generally well. The differences are discussed in terms of different coverage ranges accessible for both methods, the nonequilibrium character of the TDS method and to the threshold analysis which yields only data for the most loosely bound molecules desorbing first in each desorption track. © 1998 American Institute of Physics.
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  • 2
    ISSN: 1476-4687
    Source: Nature Archives 1869 - 2009
    Topics: Biology , Chemistry and Pharmacology , Medicine , Natural Sciences in General , Physics
    Notes: [Auszug] On the basis of a study of the plasma tails of comets, Bier-mann1 suggested in 1951 that there was a continuous flow of plasma outward from the Sun. The first spacecraft to reach interplanetary space, more than a decade later, found that there was indeed a continuous solar wind. Attention has ...
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Continuum mechanics and thermodynamics 8 (1996), S. 37-51 
    ISSN: 1432-0959
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Entropy is absorbed and emitted in the atmosphere and in the litho- and hydrosphere of the earth by absorption and emission of radiation. The value of the total production rate of entropy may be decomposed into the production rates of radiative entropy and of material entropy. Although the latter amounts to only 3,4% of the total, the material entropy production rate is the one that is relevant to meteorology, life science and ecology. Civilization accounts for less than 1% of the material entropy production.
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  • 4
    Electronic Resource
    Electronic Resource
    Springer
    Continuum mechanics and thermodynamics 7 (1995), S. 123-177 
    ISSN: 1432-0959
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract. The interaction of light and matter leads to the scattering of light and the scattered light carries information about the thermodynamic properties of the matter. The light scattered on dilute gases carries far more information about the gas than is comprised within the Navier-Stokes-Fourier theory of gases. It takes extended thermodynamics of many moments to satisfactorily describe the characteristic features of such light quantitatively.
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  • 5
    Electronic Resource
    Electronic Resource
    Springer
    Naturwissenschaften 73 (1986), S. 655-660 
    ISSN: 1432-1904
    Source: Springer Online Journal Archives 1860-2000
    Topics: Biology , Chemistry and Pharmacology , Natural Sciences in General
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    Springer
    Naturwissenschaften 72 (1985), S. 670-672 
    ISSN: 1432-1904
    Source: Springer Online Journal Archives 1860-2000
    Topics: Biology , Chemistry and Pharmacology , Natural Sciences in General
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    Springer
    The European physical journal 67 (1987), S. 483-487 
    ISSN: 1434-6036
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Recently results of microwave spectroscopy have shown that the water relaxation time is lengthened near the surface of aggregates of hydrogen bond-forming molecules, an effect corresponding to an enhanced viscosity [1–3]. In this communication properties of the so-called bound water are treated by a percolation calculation on the water cluster sizes. The values combined with the statistical model of the dielectric response of bulk water by Haggis et al. [4] yield the bound water relaxation time and in this way its viscosity. Fair agreement with the experimental data is obtained. The new analysis represents a keystep for a better understanding of bound water in physico-chemical and biological systems.
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  • 8
    Electronic Resource
    Electronic Resource
    Springer
    Catalysis letters 52 (1998), S. 215-220 
    ISSN: 1572-879X
    Keywords: iron oxide ; ethylbenzene dehydrogenation ; model catalysis ; surface defects
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology
    Notes: Abstract The dehydrogenation of ethylbenzene to styrene was studied over single-crystalline iron oxide model catalyst films grown epitaxially onto Pt(111) substrates. The role of the iron oxide stoichiometry and of atomic surface defects for the catalytic activity was investigated by preparing single-phased Fe3O4(111) and α-Fe2O3(0001) films with defined surface structures and varying concentrations of atomic surface defects. The structure and composition of the iron oxide films were controlled by low-energy electron diffraction (LEED) and Auger electron spectroscopy (AES), the surface defect concentrations were determined from the diffuse background intensities in the LEED patterns. These ultrahigh vacuum experiments were combined with batch reactor experiments performed in water–ethylbenzene mixtures with a total gas pressure of 0.6 mbar. No styrene formation is observed on the Fe3O4 films. The α-Fe2O3 films are catalytically active, and the styrene formation rate increases with increasing surface defect concentration on these films. This reveals atomic surface defects as active sites for the ethylbenzene dehydrogenation over unpromoted α-Fe2O3. After 30 min reaction time, the films were deactivated by hydrocarbon surface deposits. The deactivation process was monitored by imaging the surface deposits with a photoelectron emission microscope (PEEM). It starts at extended defects and exhibits a pattern formation after further growth. This indicates that the deactivation is a site-selective process. Post-reaction LEED and AES analysis reveals partly reduced Fe2O3 films, which shows that a reduction process takes place during the reaction which also deactivates the Fe2O3 films.
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  • 9
    Electronic Resource
    Electronic Resource
    Springer
    The European physical journal 1 (1986), S. 151-156 
    ISSN: 1434-6079
    Keywords: 32.90 ; 32.30 ; 35.10
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract By optical interference and VUV spectroscopy the doublet system of SbI 5p 26s was investigated, so that now the hyperfinestructure of all 8 levels of 5p 26s (A- andB-splitting constants) are known. From the analysis we receive a spin-orbit parameter ζ5p =3,538(57) cm−1 and from the hyperfine-analysis single electron splitting constantsa 5p 01 =52.4(4.6),a 5p 10 =−1.6(7.3),a 5p 12 =72.3(2.3),a 6s 10 =91.7(4.1),b 5p 02 =−49.6(1.1) andb 5p 11 =30.4(3.2) (all values in mK). For all calculations in the fs- and hfs-analysis the 5p 26s 2 D 3/2 has to be excluded (see discussion). With the figures given above the quadrupole moment121 Q(5p 26s)=−0.44(3) barn was obtained. It is in good agreement with the121 Q(5p 3). For the core-polarization by the 5p electron in the innerfieldns-shells (n=1, 2, 3, 4, 5) and the unpaired 6s electron a field of +500(300) kG was obtained.
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  • 10
    ISSN: 1434-6079
    Keywords: 32.30 ; 32.90 ; 35.10
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract From 17 transitions in the singly ionized Sb II spectrum the hyperfine structure (A andB splitting constants) of the complete excited configurations 5p6s and 5p6p were determined by means of optical interference spectroscopy. In addition, a theoretical analysis both of the fine structure and also of the hyperfine structure was carried out (in the case of 5p6p of the general typenpn′p for the first time in literature). For the 3 levels 5p6p 3 P 1, 5p7p 3 D 2 and 5p6p 1 P 1 a different classification was found and consistent values for the fine structure parameters, mixing coefficients and single electron hyperfine structure splitting parametersa nl ik andb nl ik were obtained. The three new determinations in Sb II of the quadrupole moment (in barn) of121Sb (Q(5p6s)=−0.55(5);Q(5p6p)=−0.57(5) from the 5p-electron andQ(5p6p)=−0.7(2) from the 6p-electron) are well agreeing with each other but differ to former values from SbI. The core polarization and isotope shift of the lines, however, are compatible with our former results in SbI.
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