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Zusammenfassung Die energiedispersive Röntgenmikroanalyse im Rastertransmissionselektronenmikroskop ermöglicht die Untersuchung von Teilchen mit Durchmessern bis herunter zu 10 nm. Für quantitative Messungen ist die Kenntnis der kritischen Probendicke, bis zu der die Korrekturfaktoren von der chemischen Zusammensetzung der Probe unabhängig sind, von erheblicher Bedeutung. Bislang gibt es zwar theoretische Ansätze zur Abschätzung dieser Größe, jedoch keine experimentellen Bestimmungen. Deshalb wurde an einem Stahl mit 30,1% Cr und einer Nickellegierung mit 23,9% Cr und 15,1% W die kritische Probendicke gemessen. Wie die Ergebnisse zeigen, liegt bei den untersuchten Legierungen die kritische Probendicke über 500 nm und damit bei Schichtdicken, die für elektronenmikroskopische Untersuchungen im allgemeinen nicht mehr von Interesse sind. Die im Schrifttum mitgeteilten Abschätzformeln sind nach diesen Befunden für praktische Messungen zu ungenau.
Measurement of the critical specimen thickness for the EDX analysis of thin foils
Summary It is possible to investigate small particles with diameters down to 10 nm by energy dispersive X-ray microanalysis in a STEM. For quantitative measurements, the critical foil thickness, up to which the correction factors are independent of the chemical composition of the specimen, must be known. Till now, theoretical estimations of this value had been made, but no actual measurements were carried out. Therefore, the critical foil thickness was measured on a steel with 30.1% Cr and a nickel alloy containing 23.9% Cr and 15.1% W. The results show that for the alloys investigated the critical foil thickness is larger than 500 nm and hence larger than the usual maximum thickness of the TEM specimens. The formulae dealt with in the literature are much too inaccurate to be used for actual measurements.
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This study addresses a fundamental question in surface science: the adsorption of halogens on metal surfaces. Using synchrotron radiation-based high-resolution X-ray photoelectron spectroscopy (XPS), temperature-programmed XPS, low-energy electron diffraction (LEED) and density functional theory (DFT) calculations, we investigated the adsorption and thermal stability of bromine on Rh(111) in detail. The adsorption of elemental bromine on Rh(111) at 170 K was followed in situ by XPS in the Br 3d region, revealing two individual, coverage-dependent species, which we assign to fcc hollow- and bridge-bound atomic bromine. In addition, we find a significant shift in binding energy upon increasing coverage due to adsorbate-adsorbate interactions. Subsequent heating shows a high thermal stability of bromine on Rh(111) up to above 1000 K, indicating strong covalent bonding. To complement the XPS data, LEED was used to study the long-range order of bromine on Rh(111): we observe a (√3×√3)R30° structure for low coverages (≤0.33 ML) and a star-shaped compression structure for higher coverages (0.33–0.43 ML). Combining LEED and DFT calculations, we were able to visualize bromine adsorption on Rh(111) in real space for varying coverages.  相似文献   
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We report the infrared spectra of HCl, (HCl)2, and H2O-HCl in liquid helium nanodroplets in the frequency region between 2680 and 2915 cm(-1). For the HCl monomer a line width of 1.0 cm(-1) (H35Cl) corresponding to a lifetime of 5.3 ps was observed. The line broadening indicates fast rotational relaxation similar to that previously observed for HF. For (HCl)2 the free HCl as well as the bound HCl stretching band has been observed. The nu2+ bands of (HCl)2 could be rotationally resolved, and rotational constants were deduced from the spectra. We observed both the allowed and the symmetry forbidden transition. However, the forbidden "broken symmetry" tunneling transition of the mixed dimer shows an intensity that is considerably enhanced compared to the gas phase. Upon the basis of the present measurements we were able to calculate the tunneling splitting in the excited state. The tunneling splitting is found to be reduced by 28% compared to the gas phase. Transitions from the ground state to the Ka=1 level of the free HCl stretch (nu1) are recorded and show considerable line broadening with a line width of 2 cm(-1). The excited state Ka=1 has an additional rotational energy of about 10 cm(-1), thereby allowing fast rotational relaxation by coupling to helium excitations. In addition we observed the HCl stretch of the HCl-H2O dimer, which exhibits an unusually large width (1.7 cm(-1) for H35Cl)) and large red shift (8.5 cm(-1)), compared to the gas-phase values. The large-amplitude motion originating from the libration mode of the HCl-H2O complex is supposed to act as a fast relaxation manifold.  相似文献   
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Ion hydration is of pivotal importance for many fundamental processes. Various spectroscopic methods are used to study the retardation of the hydration bond dynamics in the vicinity of anions and cations. Here we introduce THz‐FTIR spectroscopy as a powerful method to answer the open questions. We show through dissection of THz spectra that we can pinpoint characteristic absorption features that can be attributed to the rattling modes of strongly hydrating ions within their hydration cages as well as vibrationally induced charge fluctuations in the case of weakly hydrating ions. Further analysis yields information on anion–cation cooperativity, the size of the dynamic hydration shell, as well as the lifetimes of these collective ion‐hydration water modes and their connecting thermal bath states. Our study provides evidence for a non‐additive behavior, thus questioning the simplified Hofmeister model. THz spectroscopy enables ion pairing to be observed and quantified at a high salt concentration.  相似文献   
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