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Electron Paramagnetic Resonance and Optical Absorption Spectra of VO2+ in CsCl Single Crystals
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The performance of base metal oxides on ceramic carriers as catalysts for air pollution control
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Thermodynamic relations between component activities and gas solubilities in binary metallic systems
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Thermohydrodynamic analysis of thrust-bearing with circular pads running on bubbly oil (BTHD-theory)
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A Portable Implementation of Index Sequential Input-Output [Part 1] / Kurbel, Karl; Pietsch, W.
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A Portable Implementation of Index Sequential Input-Output [Part 2] / Kurbel, Karl; Pietsch, W.
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A microscopic photometric method for measuring erythrocyte deformability. Artmann, Gerhard Michael
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The adsorption of fluor-carbon complexes on GaAs(110) studied by electron energy loss spectroscopy
(1986)
Dielectric Properties of Polyolefins Stressed by High Electrical Fields. Fruth, B. ; Krause, G.
(1987)
Grain boundary and surface segragation of Ba-Ti-O-Phases in rutile. O´Bryan, H. M.; Hagemann, H. J.
(1987)
E0 transitions in 106Pd studied by neutron capture / G. G. Colvin ; F. Hoyler ; S. J. Robinson
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Investigation of the InSb(110)-Sn schottky barrier by means of electron energy loss spectroscopy
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Differentiation between Phaeocystis pouchetii (Har.) Lagerheim and Phaeocystis globosa Scherffel
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Dielectric Properties of Polyolefins Stressed by High Electrical Fields / Fruth, B. ; Krause, G.
(1988)
In-beam study of ¹⁴³ Eu
(1988)
Thickness dependence of the electronic structure of ultrathin, epitaxial Ni(111)/W(110) layers.
(1988)
The spin asymmetry in deep inelastic scattering of longitudinally polarised muons by longitudinally polarised protons has been measured over a large x range (0.01<x<0.7). The spin-dependent structure function g1(x) for the proton has been determined and its integral over x found to be 0.114±0.012±0.026, in disagreement with the Ellis-Jaffe sum rule. Assuming the validity of the Bjorken sum rule, this result implies a significant negative value for the integral of g1 for the neutron. These values for the integrals of g1 lead to the conclusion that the total quark spin constitutes a rather small fraction of the spin of the nucleon.