Academia.edu no longer supports Internet Explorer.
To browse Academia.edu and the wider internet faster and more securely, please take a few seconds to upgrade your browser.
1994
^{27}Al and ^{63,65}Cu NMR measurements are reported for powder samples of stable AlCuFe and AlCuRu icosahedral quasicrystals and their crystalline approximants, and for a AlPdMn single grain quasicrystal. Furthermore, ^{27}Al NQR spectra at 4.2 K have been observed in the AlCuFe and AlCuRu samples. From the quadrupole perturbed NMR spectra at different magnetic fields, and from the zero field NQR spectra, a wide distribution of local electric field gradient (EFG) tensor components and principal axis system orientations was found at the Al site. A model EFG calculation based on a 1/1 AlCuFe approximant was successful in explaining the observed NQR spectra. It is concluded that the average local gradient is largely determined by the p-electron wave function at the Al site, while the width of the distribution is due to the lattice contribution to the EFG. Comparison of ^{63}Cu NMR with ^{27}Al NMR shows that the EFG distribution at the two sites is similar, but that the electronic con...
Physical review. B, Condensed matter, 1994
2 7~1 and 6 3 , 6 5~~ NMR measurements are reported for powder samples of stable Al-Cu-Fe and Al-Cu-Ru icosahedral quasicrystals and their crystalline approximants, and for an Al-Pd-Mn singlegrain quasicrystal. Furthermore, ' '~1 NQR spectra at 4.2 K have been observed in the Al-Cu-Fe and Al-Cu-Ru samples. From the quadrupole-perturbed NMR spectra at different magnetic fields, and from the zero-field NQR spectra, a wide distribution of local electric-field gradient (EFG) tensor components and principal-axis-system orientations was found at the Al site. A model EFG calculation based on a 1/1 Al-Cu-Fe approximant was successful in explaining the observed NQR spectra. The average local gradient is largely determined by the p-electron wave function at the A1 site, while the width of the distribution is due to the lattice contribution to the EFG. Comparison of "CU NMR with 27Al NMR shows the EFG distribution at the two sites is similar, but the electronic contribution to the EFG is considerably smaller at the Cu site, in agreement with a more s-type wave function of the conduction electrons. The overall spread of EFG values is well reproduced by the calculation based on the approximant. However, the experimental spectra indicate a much larger number of nonequivalent sites when compared with the simulated NQR spectra based on the 1/1 approximant. The short-range, local chemical order is well represented by the approximant, but differences in coordination must be included at intermediate range in the quasicrystal. Measurements of 27Al Knight shift, magnetic susceptibility, and nuclear spin-lattice relaxation time as a function of temperature yield results which indicate a reduction of the density of states at the Fermi level by a factor of 7 or 8 from the value in Al metal, consistent with the notion of a pseudogap for these quasicrystals. No differences in the measured parameters were detected as a function of composition of the quasicrystatline alloys, arguing against a fine structure in the density of states at the Fermi level.
Physical Review Letters, 1997
The 27 Al and 63 Cu spin-lattice relaxation rates were found to contain a large T 2 term over a wide temperature range below 400 K in several thermodynamically stable quasicrystalline alloys, including i-AlCuRu, i-AlPdRe, i-AlCuFe, and the crystalline approximant phase a-AlMnSi. The relaxation mechanism is proven to be electronic in origin. Such nonlinear temperature dependence is shown to be a clear signature of sharp features in the density of states at the Fermi level. The estimated width of this sharp feature is on the order of 20 meV. [S0031-9007(97)03655-7]
Applied Magnetic Resonance, 2000
Nuclear magnetic resonance (NMR) techniques for measuring one-dimensional absorption spectra and two-dimensional exchange spectra of solids with extremely inhomogeneously broadened lines are discussed. Among various "broad-line" solids, quasicrystals represent alloys of metallic elements, the structures of which include "forbidden" symmetry elements. NMR absorption lines of quasicrystals exhibit a strong electric-quadrupole-induced inhomogeneous broadening that originates from the lack of translational periodicity of the otherwise perfectly long-range-ordered quasiperiodic lattice. Recording an NMR spectrum of a quasi crystalline sample requires a magnetic field-sweep technique. The two-dimensional exchange experiment on quasicrystals can be performed on selectively excited portions of the NMR spectrum only. Due to the off-resonance effects in a selective excitation, the use of a simple three-pulse stimulated-echo exchange sequence is preferred. The "Al spectra of the Al-Pd-Mn and Al-Pd-Re families show interesting features like temperature-dependent frequency shifts and exchange effects due to atomic motion.
Physical Review B, 1994
The distribution of nonequivalent aluminum sites was studied in Al-Cu-Fe and Al-Cu-Ru stable icosahedral quasicrystalline phases using Al NQR spectra taken at 4.2 K. The observed spectrawhich give directly the distribution of nonequivalent aluminum siteswere broad, asymmetric, and structureless. A simple electricfield-gradient model calculation accounted for the spectral width in terms of a wide distribution of local atomic environments, and an estimate for the lower limit on the number of nonequivalent aluminum sites was found.
Physica B: Condensed Matter, 1995
The crystalline approximant phases ~-AIMnSi and R-AICuFe present for alloys of metallic elements anomalou electronic transport properties, with low conductivity values and strong temperature dependences of both the conductiv ity and the Hall coefficient. In both the ct-and R-phases, the high field magnetoconductivity can be analysed by quantur interference effects. The transport behaviours are very similar to those of the high structural quality icosahedral phase~ Moreover, the R-AICuFe phase properties are identical to those of the AICuFe icosahedral phases of the sam composition. Surprisingly, the ct-AlMnSi phase, of a much simpler structure than R-AICuFe, presents the sam anomalous behaviours. Approximants are very different from the icosahedral AIMnSi counterparts which behave lik amorphous metals. The results indicate that the relevant length scale for understanding the transport properties is abo~ the size of these crystalline unit cells, i.e. one or two nanometers. * Corresponding author.
Physical Review B, 2001
The unusual magnetism of manganese atoms in an icosahedral Al72.4Pd20.5Mn7.1 single-grain quasicrystal was studied by 27Al nuclear magnetic resonance (NMR), magnetic susceptibility, and electrical resistivity measurements. Between room temperature and 50 K both the 27Al NMR linewidth and the frequency shift exhibit a Curie-Weiss-type, 1/(T-theta) temperature dependence. At lower temperatures a significant narrowing of the linewidth, concomitant with a reduction of the frequency shift is observed. These features can be explained by a gradual reduction of the local exchange magnetic field at the position of the 27Al nuclei that is transferred from the manganese d moments via the conduction electrons. Two possible origins of this phenomenon are discussed: (i) the Kondo-like screening of manganese moments by the conduction electrons and (ii) the ``resistivity''-damping of the RKKY interaction due to increasing electron localization at low temperatures.
Philosophical Magazine, 2008
This article gives a short review of some important achievements in the field of electronic properties of quasicrystals. It focuses essentially on : the nature of quasicrystals as Hume-Rothery alloys, the energetics of quasicrystals and related phases, the magnetic properties, the localization of electronic states, the transport properties. For each part one emphasizes some promising directions of research. We end by listing some problems that are related to that of electrons in a quasiperiodic potential.
Journal of Alloys and Compounds, 2019
Based on the conceptual Al-Cu-(Fe+Co) phase diagram we found an optimal initial composition and developed a method to grow Al-Cu-Fe-Co single-grain quasicrystals. Our original two-stage cooling process includes (i) fast cooling of the melt down to the quasicrystalline single phase region with rate of ~165 K/h to prevent growing of nonquasicrystalline phases in the melt, and (ii) slow cooling down with rate of ~2-3 K/h to grow large (mm-size) single-grain quasicrystals. As a result a new stable quaternary Al-based icosahedral quasicrystal has been obtained. The chemical composition of the grown quasicrystal determined by both the energy dispersive X-ray analysis and inductively coupled plasma mass spectrometry was Al 64.36 Cu 22.20 Co 3.05 Fe 10.39. Powder XRD and selected area electron diffraction were carried out for the phase identification and confirmed the icosahedral structure. The temperature dependencies of the electrical resistance measured on the oriented samples in the temperature range of 1.4 K-300 K is typical for icosahedral quasicrystals.
Materials Science and Engineering: A, 2000
We analyze the criterion for the appearance of magnetic moments in quasicrystals approximants and liquids Al-Mn. In a Hartree-Fock scheme, it is shown that the Stoner criterion (U n d (EF) ≥ 1) does not apply to these systems due to the presence of the pseudogap in the density of states. We give an generalized criterion that can take into account the particular density of state. The main result is that the appearance of a magnetic moment on a Mn atom depends strongly on its position in the crystalline structure. Indeed some particular positions of the Mn atoms lead to magnetic moments whereas other positions are more stable when the Mn is non-magnetic. This criterion is used to analyzed the electronic structure of two approximants (1/1-Al-Pd-Mn-Si and T-Al-Pd-Mn) calculated by the self-consistent LMTO-ASA method.
Hyperfine Interactions, 1990
Al65Cu20Fe15 quasicrystalline ribbons exhibit similar paramagnetic spectra in the temperature range 45 mK-300 K, evidencing for no magnetic change down to 45 mK. Analysis of in field Mssbauer spectra by both negative and positive EFG distribution shows an only slightly dominant negative contribution (59%).
Physical Review Letters, 2012
We use hard x-ray photoemission to resolve a controversial issue regarding the mechanism for the formation of quasicrystalline solids, i.e., the existence of a pseudogap at the Fermi level. Our data from icosahedral fivefold Al-Pd-Mn and Al-Cu-Fe quasicrystals demonstrate the presence of a pseudogap, which is not observed in surface sensitive low energy photoemission because the spectrum is affected by a metallic phase near the surface. In contrast to Al-Pd-Mn, we find that in Al-Cu-Fe the pseudogap is fully formed; i.e., the density of states reaches zero at E F indicating that it is close to the metal-insulator phase boundary.
Journal of alloys and …, 1997
We have studied the electrical resistivity and magnetoresistance for the system Al 65 Cu 20 Co 15−x Fe x (0≤x≤15). The sample with x=0 could be indexed as the decagonal (D) phase, whereas the sample with x=15 forms the icosahedral (I) phase. The sample with intermediate x ...
Acta Materialia, 2003
Cu NMR has been used to observe the evolution of the precipitate structures in the solution treated and quenched dilute alloy Al-1.7 at%Cu following thermal aging. The distinguishable phases in this alloy form in the following sequence (i) fcc a-phase with Cu in random substitutional sites, (ii) Guinier-Preston zones, (iii) qЉ-phase, (iv) qЈ-phase and finally (v) q-phase, where the last two phases are structural variants of CuAl 2 . The Cu site in all five of these phases has been detected as a resolved line in the 63 Cu FT-NMR spectrum at room temperature, together with a line assigned to surface Cu sites on qЈ-phase platelets. Two additional lines have been observed in spectra from specimens containing the q-phase due to Cu substituting for Al in the CuAl 2 structure, and Cu in the CuAl h 2 -phase. Density functional based ab initio electronic structure calculations have been used to reproduce accurately the observed electric field gradient (V zz ) at the Cu site in q-phase CuAl 2 and to explain the relatively narrow 63 Cu lines observed for GPzones, qЉ-phase and qЈ-phase.
Crystals, 2019
The standard approach applies the Gaussian distribution function to estimate atomic displacements due to thermal vibrations in periodic and aperiodic systems, which is used in a form of the Debye–Waller factor during the structure refinement. Acoustic phonons provide the largest contribution to the Gaussian correction although the character of other phonon modes remains relatively unclear. In this paper, we provide an alternative description of localized and dispersionless phonons based on an assumption of the harmonic displacement distribution function, which was recently proposed for model quasicrystals, and apply this approach for a decagonal Al-Cu-Rh quasicrystal that was previously studied by Kuczera et al. in 2012. We used the same X-ray diffraction data and the statistical method of structural analysis of the aperiodic systems. The correction function for phonons takes the form of a Bessel function instead of a conventional (Gaussian) Debye–Waller factor. This allowed us to a...
Philosophical Magazine, 2006
Journal of Applied Physics
We report the results of field and temperature dependent magnetization measurements on (Al,Ge) 65 CuMn quasicrystalline samples with ϳ22 and 24 at. % Mn. The Ge content is also kept ϳ25 at. %. The data for these samples are then compared with the data taken on samples with low Ge content ͑ϳ10 and 0 at. %͒. Al 40 Ge 25 Cu 10 Mn 25 , a composition very close to one of the alloys studied here, is reported ͓Tsai et al., Jpn. J. Appl. Phys., 27, L2252 ͑1988͔͒ in literature as a ferromagnetic, icosahedral QC with large T C . The detailed magnetic studies described here prove that the magnetism observed in these quaternary alloys is highly disordered. The two important observations made in our studies are ͑i͒ observation of short-range ferromagnetism in samples with high Ge and high Mn content, up to very high fields (Hϭ5 T) and ͑ii͒ oscillatory magnetization ͑or existence of multiple minima in the M -T curves͒ observed for the same samples for Hу1 kOe.
To address the questions on the anisotropy of bulk physical properties of decagonal quasicrystals and the intrinsic physical properties of the d-Al-Co-Ni phase, we investigated the anisotropic magnetic susceptibility, the electrical resistivity, the thermoelectric power, the Hall coefficient, and the thermal conductivity of a d-Al-Co-Ni single crystal of exceptional structural quality. Superior structural order on the local scale of atomic clusters was confirmed by 27 Al nuclear magnetic resonance spectroscopy. The measurements were performed in the 10-fold periodic direction of the structure and in three specific crystallographic directions within the quasiperiodic plane, corresponding to the 2 and 2 twofold symmetry directions and their bisector. The specific heat, being a scalar quantity, was determined as well. The measurements of the second-rank bulk tensorial properties confirm the theoretical prediction that a solid of decagonal point group symmetry should exhibit isotropic physical properties within the quasiperiodic plane and anisotropy between the in-plane and the 10-fold directions. d-Al-Co-Ni is an anisotropic diamagnet with stronger diamagnetism for the magnetic field in the 10-fold direction. Electrical and thermal transport is strongly metallic in the 10-fold direction but largely suppressed within the quasiperiodic plane, the main reason being the lack of translational periodicity that hinders the propagation of electrons and phonons in a nonperiodic lattice. The third-rank Hall-coefficient tensor shows sign-reversal anisotropy related to the direction of the magnetic field when applied in the 10-fold direction or within the quasiperiodic plane. The observed anisotropy is not a peculiarity of quasicrystals but should be a general feature of solids with broken translational periodicity in two dimensions.
Hyperfine Interactions, 2011
The Al 46 Cu 23 Fe 13 quasicrystal phase, prepared by arc-melting and nanostructured using high energy ball milling technique, was studied employing X-ray diffraction, transmission electron microscopy, ferromagnetic resonance and electric transport measurements. Fe local environments were studied by Mössbauer spectroscopy. The resistivity ratio R(4.2 K)/R(300 K) is within the expected values commonly observed in an icosahedral phase. In general, the experimental results show that an appropriate heat treatment of the as-cast alloy prepared by arc-melting makes possible to obtain good quasicrystal samples. On the other hand, for milling time longer than five hours, the average grain-size of quasicrystal phase reduces, but it preserves Fe local atomic orders. It is also observed that the quasicrystalline sample decomposes in an iron rich nano-quasicrystalline phase and a ε-Al 2 Cu 3 phase. Electric transport measurements show that at low temperatures the nanoquasicrystalline samples behave strongly different to their solid counterparts, an effect attributed to a long-range order reduction and an increasing of grain boundary regions. The presence of local magnetic moments in the nanostructured sample is also discussed.
Physical Review B, 1994
The A165Cu20Ru» icosahedral alloy was studied by ' Al nuclear magnetic resonance from 150 to 1110 K. The Knight shift of the unresolved resonance line was observed to significantly increase above 500 K. This uncommon temperature dependence of the Knight shift is interpreted in terms of the presence of a pseudogap at the Fermi level. The spin-lattice relaxation rate deviates from the linear temperature dependence of Korringa relaxation below 500 K, and above 500 K it is dominated by a thermally activated process with a small activation energy of 0.48 eV. This energy is distinctly different from the activation energy observed in simple metallic alloys.
Loading Preview
Sorry, preview is currently unavailable. You can download the paper by clicking the button above.