Abstract:We report on the measurement of the three-dimensional electron momentum density ͑EMD͒ of a 22 nm Cu/22 nm Ni sandwich foil and of a Cu 0.50 Ni 0.50 alloy film with the same thickness, which was obtained from an identical sandwich by interdiffusion. The EMD's were measured by coincident detection of a Compton scattered photon with its recoil electron. The experiments were performed at the High-Energy beamline of the European Synchrotron Radiation Facility. The experimentally observed small change of the EMD due… Show more
“…non-coincident Compton scattering experiments on Cu-Ni single crystals, absolute values of experimental CPs are difficult to interpret due to the presence of a background contribution of uncertain origin. The solid line in figure 12 represents KKR-CPA theory [46,53]. In view of the smallness of the effect, a reasonable agreement between theory and experiment is observed.…”
Section: Cu-ni Alloymentioning
confidence: 59%
“…In this section we will report on the influence of alloying by comparing the EMD of Cu 0.50 Ni 0.50 with those of its pure constituents [46]. The electronic structure of this 3d transition-metal solid-solution alloy has received extensive attention.…”
We report on the measurement of the three-dimensional electron momentum density (EMD) of solids by means of the (γ , eγ ) reaction. Fixing the reaction kinematics by a coincidence condition, the triple-differential cross section for Compton scattering is proportional to the EMD. The experiments were performed either at the wiggler beamline of the European Synchrotron Radiation Facility (ESRF) or the undulator beamline of the PETRA storage ring at Deutsches Elektronen-Synchrotron (DESY) with photon energies of about 150 keV. Experimental three-dimensional EMDs of graphite, fullerene and aluminium are compared with theoretical ones obtained from band-structure calculations like the full-potential linear muffin-tin orbital, augmented-planewave and pseudopotential formulations. In addition, the change of the EMD caused by alloy formation has been studied in the Cu-Ni system and the results are compared with the Korringa-Kohn-Rostoker coherent potential approximation.
“…non-coincident Compton scattering experiments on Cu-Ni single crystals, absolute values of experimental CPs are difficult to interpret due to the presence of a background contribution of uncertain origin. The solid line in figure 12 represents KKR-CPA theory [46,53]. In view of the smallness of the effect, a reasonable agreement between theory and experiment is observed.…”
Section: Cu-ni Alloymentioning
confidence: 59%
“…In this section we will report on the influence of alloying by comparing the EMD of Cu 0.50 Ni 0.50 with those of its pure constituents [46]. The electronic structure of this 3d transition-metal solid-solution alloy has received extensive attention.…”
We report on the measurement of the three-dimensional electron momentum density (EMD) of solids by means of the (γ , eγ ) reaction. Fixing the reaction kinematics by a coincidence condition, the triple-differential cross section for Compton scattering is proportional to the EMD. The experiments were performed either at the wiggler beamline of the European Synchrotron Radiation Facility (ESRF) or the undulator beamline of the PETRA storage ring at Deutsches Elektronen-Synchrotron (DESY) with photon energies of about 150 keV. Experimental three-dimensional EMDs of graphite, fullerene and aluminium are compared with theoretical ones obtained from band-structure calculations like the full-potential linear muffin-tin orbital, augmented-planewave and pseudopotential formulations. In addition, the change of the EMD caused by alloy formation has been studied in the Cu-Ni system and the results are compared with the Korringa-Kohn-Rostoker coherent potential approximation.
“…Neither data processing like a deconvolution procedure accompanied by frequency filtering nor background subtraction has been applied to our data. The solid line in Figure 8.5 represents KKR-CPA theory [20,22]. In view of the smallness of the effect a reasonable agreement between theory and experiment is observed.…”
Section: Cu-ni Alloymentioning
confidence: 60%
“…In this chapter we will report on the influence of alloying by comparing the EMD of Cu 0.50 Ni 0.50 with those of its pure constituents [20]. The electronic structure of this 3d transition-metal solid-solution alloy has received extensive attention.…”
“…In the context of this work it is worth mentioning an interesting study of the Ni-Cu system by Metz et al [28], who observed directly the effects of alloying close to the Fermi energy, using the (γ , eγ ) coincidence technique. Their observations generally agree with the predictions of KKR-CPA theory; however, it is difficult to compare them directly with our results, mainly because of the very different composition of the alloys studied.…”
We report high-resolution Compton profiles (CPs) of
Ni75Cu25
and Ni75Co25
disordered, ferromagnetic alloys measured along [100], [110] and [111] crystallographic
directions. The directional CP anisotropies, profile derivatives and reciprocal form factors
B(z)
are analysed in detail and compared with first-principles KKR-CPA
(Korringa–Kohn–Rostoker coherent potential approximation) calculations.
Good overall agreement is found between the experimental and theoretical
anisotropies. It follows from experiment that the majority-spin Fermi surface of the
Ni75Cu25 and
Ni75Co25 alloys
occurs at higher momentum than the theory predicts. Also, a splitting in the secondary maxima in
experimental B(z)
functions of the alloys is observed, which is not predicted by the KKR-CPA calculations.
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