Library

feed icon rss

Your email was sent successfully. Check your inbox.

An error occurred while sending the email. Please try again.

Proceed reservation?

Export
  • 1
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Acta crystallographica 20 (1966), S. 312-313 
    ISSN: 0001-5520
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 64 (1988), S. 4772-4774 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: X-ray diffraction was used to evaluate the structures of amorphous samples of Cu50Zr50 prepared by three different methods, namely, melt spinning, mechanical alloying, and irradiation by 2-MeV protons. The results demonstrate conclusively for the first time that, within experimental error, the short-range atomic distribution in an amorphous alloy is the same, regardless of how it is prepared.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 63 (1988), S. 4769-4770 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Differential scanning calorimetry measurements of mercuric iodide (HgI2 ) do not suggest the existence of the α'-HgI2 phase, as previously reported, when the necessary precautions are taken to avoid any chemical reaction with the sample holder. This conclusion is supported by variable temperature Raman spectroscopic measurements performed in the vicinity of the melting point, where the α' was supposed to exist.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 4
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 1 (1968), S. 199-208 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Ag–Ge films of thickness 1 to 3 microns were prepared by co-evaporation of Ag and Ge onto 0.005′′ thick vitreous silica plates held at liquid nitrogen temperature. The pressure during evaporation was 3 × 10−7 Torr or less. The X-ray scattering of the films and substrates was measured at room temperature with monochromatic Mo Kα and Cu Kα radiation. After correction for substrate scattering, the interference function I(K) was evaluated for each alloy as a function of K = 4π sin &thgr;/λ. The Fourier transform of K[I(K)−1] yielded the reduced distribution function G(r) = 4πrV(r)[ρ(r)−ρ0], where ρ(r) is the weighted atomic density at a distance r from a reference atom, ρ0 is the average atomic density and V(r) is the size factor of the coherently diffracting domains in the sample. Both I(K) and G(r) indicate that the alloy films consist of the Ag solid solution and Ge. The Ag phase cannot be characterized as amorphous, but is micropolycrystalline. The sizes of the coherently diffracting domains or the correlation distances determined from G(r) increased from 12 Å in Ge to 30 Å in Ag-40 at. %Ge. Fourier analyses of the (111) peak profiles of Ge and Ag yielded particle sizes of 13 Å for Ge and 16 Å for the Ag phase in the Ag-83 at. %Ge alloy. The Ag phase particles increased with increasing Ag concentration, reaching a value of 45 Å in the Ag-28 at. %Ge alloy.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 5
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 2 (1969), S. 149-155 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A horizontal diffractometer has been set up for transmission studies of liquid samples. An asymmetric, singly bent LiF monochromator in the primary X-ray beam focuses the radiation on the receiving slit of the diffractometer. The sample rotates at half the angular speed of that of the X-ray detector to retain focusing at all angles of diffraction. A high temperature furnace assembly (camera) has been constructed which fits on the diffractometer. Its heating element consists of a thin-walled, pyrolitic graphite tube 38 mm in diameter. A special sample holder for the liquids is mounted on a boron nitride stool bolted to the bottom plate of the camera. The entire set-up allows the measurement of the diffracted intensity between 2&thgr; = 2° and 2&thgr; = 90° corresponding to K = 4πsin&thgr;/λ = 0.3 Å−1 at 12.4 Å−1 when Mo Kα radiation is used. Correction procedures to obtain the scattered intensity per atom from the raw data are discussed, and a comparison is made between the transmission and reflection methods with liquid tin.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 6
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 9 (1976), S. 159-168 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Amorphous films of AgCu and CuMg2, approximately 3000 Å in thickness, were prepared by co-evaporation of Ag and Cu, and Cu and Mg, respectively, onto 25 μm thick Be sheets, held at liquid nitrogen temperature. Mo Kα X-rays were used as a radiation probe to determine the structure of the films, at room temperature, and of the liquid alloys of Cu with 50 at.% Ag and with 0 and 67 at.% Mg at 50°C above the liquidus temperature. With the transmission technique, the interference functions (or structure factors) I(K) were determined in the range of K = 4π sin &thgr;/λ between 0.8 Å−1 and 12.5 Å−1, and then Fourier transformed to obtain the radial distribution functions (RDF). The I(K) and RDF of the amorphous AgCu and CuMg2 films were compared with those of the liquid Ag–Cu and Cu–Mg alloys, respectively. It was found that the structures of the amorphous and liquid Ag–Cu alloys were similar with a more well defined short-range order occurring in the solid alloys, whose I(K) exhibited the well known shoulder on the second peak. The I(K) and RDF of the amorphous CuMg2 and the liquid Cu–Mg alloys cannot be explained by a common structure, although I(K) showed a small premaximum below the first main peak in both the amorphous and liquid alloys, a feature observed in many liquid Mg alloys.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 7
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 10 (1977), S. 468-472 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The long-range order parameter, S, of pure Cu3Au and two Cu3Au alloys containing 0.64 and 1.5 at. % Co was determined over the temperature range 325 to 387°C. In principle, the state of order in the ternary alloy (Cu3Au)1−XCoX is described by two order parameters S1 = Aα − Aβ, and S2 = Bβ − Bα where Aα is the fraction of α sites occupied by A atoms, etc. It is shown that S2 − S1 = Cα − Cβ = 0 as long as the Co atoms are randomly distributed on α and β sites. The values of S were measured at temperature using Warren's method [Warren, B. E. (1969). X-Ray Diffraction. Reading, Mass.: Addison-Wesley] applied to powder samples, employing the {110}, {210}, {211}, and {221, 300} superstructure and the {111}, {200}, {220}, {311}, and {222} fundamental reflections. The results on pure Cu3Au are in relatively good agreement with earlier measurements, but in poor agreement with theoretical predictions, especially at temperatures above 360°C. Within the accuracy of the measurements, it is observed that cobalt, which is in solid solution in both alloys, has no effect on the experimentally determined values of S. The root-mean-square vibration amplitudes, 〈u2〉1/2, of the Cu and Au atoms at 640°K were also estimated from the data, and it appeared that 〈u2〉1/2Cu decreased slightly with increasing Co content while 〈u2〉1/2Au increased.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 8
    Electronic Resource
    Electronic Resource
    Springer
    The European physical journal 62 (1986), S. 189-194 
    ISSN: 1434-6036
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract We report a new method, how to derive the primary energy spectrum of an X-ray tube. As a starting point, we use scattering data of an amorphous sample taken as a function of angle in energy dispersive scans. Results are presented for the amorphous alloy Fe78B13Si9 using transmission geometry, measured with a Mo tube at 50 kV and 14 mA. The primary beam intensityI 0(E) drops monotonically when the energyE increases from 20–40 keV.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 9
    Electronic Resource
    Electronic Resource
    Springer
    Hyperfine interactions 94 (1994), S. 2239-2244 
    ISSN: 1572-9540
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The process of mechanical alloying consists of intimate mixing and mechanical working of elemental powders in a high-energy ball mill. It has been well established that this process is able to produce nanocrystalline and amorphous material. In this study, the structural effects of mechanical alloying of pure Fe, Fe50W50 and Fe50Mo50 powders were investigated by X-ray diffraction and Mössbauer spectroscopy. For all cases, nanocrystalline and/or amorphous fractions were found after milling. The resulting particle size was determined by X-ray diffraction. Pure Fe does not amorphize even after prolonged milling times. For the nanocrystalline powder, significant changes in the linewidth and the hyperfine field are found. Powder mixtures of Fe50Mo50 and Fe50W50 are completely amorphous after milling times of 10 h, as seen by Mössbauer spectroscopy, but nanocrystalline fractions of the non-iron part are still found in X-ray diffraction. Also in the amorphous state, further changes in the hyperfine parameters are found with increasing milling time.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 10
    Electronic Resource
    Electronic Resource
    Springer
    Journal of materials science 7 (1972), S. 105-114 
    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 X-ray diffraction techniques have been used to study plastic deformation in a polycrystalline Ag-30 at.% Cd alloy under tensile load. The positions and shapes of all (hkl) reflections were recorded using a parafocusing arrangement up to a maximum true strain of 0.265. The effects on the peak displacements caused by stacking faults and by macroscopic strains normal to the surface were distinguished. The longitudinal true stress in the surface layer evaluated by least square analysis was smaller than the macroscopic flow stress by an approximately constant amount over the whole range of strain (in accord with previous observations of a stress gradient near a free surface); the apparent rate of work hardening in the surface was equal to that for the specimen as a whole. The stacking fault probability α was approximately a linear function of strain and attained a maximum value of 7×10−3. Fourier analyses were performed on the profiles of (111) — (222) and (200) — (400) pairs of reflections. The effective particle sizes D e(111) and D e(100) and the estimated true domain size D decreased approximately inversely with increasing strain, tending to limiting values at high strains of 220, 150 and 300Å respectively. Similarly, the microscopic strains [〈εL 2〉hkl *]1/2 tended to limiting values at high mechanical strains. The twin fault concentration was found to be negligibly small. The particle size and microstrain parameters were compared with values for cold-worked filings of the alloy. A plot of α against 〈εL=50Å 2〉111 * for the solid specimens and for the filings was linear and yielded a stacking fault energy for Ag-30 at. % Cd of 6.1 ergs/cm2.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
Close ⊗
This website uses cookies and the analysis tool Matomo. More information can be found here...