Matches in SemOpenAlex for { <https://semopenalex.org/work/W1657960558> ?p ?o ?g. }
- W1657960558 abstract "We present a $^{27}mathrm{Al}$ NMR study of three giant-unit-cell complex metallic compounds, $ensuremath{beta}text{ensuremath{-}}{mathrm{Al}}_{3}{mathrm{Mg}}_{2}$, the ``Bergman-phase'' ${mathrm{Mg}}_{32}{(mathrm{Al},mathrm{Zn})}_{49}$, and ${ensuremath{xi}}^{ensuremath{'}}text{ensuremath{-}}mathrm{Al}text{ensuremath{-}}mathrm{Pd}text{ensuremath{-}}mathrm{Mn}$, which contain some hundreds up to more than a thousand atoms in the unit cell. The NMR spectra of monocrystalline samples are strongly inhomogeneously broadened by the electric quadrupole interaction and the line shapes are featureless and powderlike, but still exhibit significant orientation-dependent variation of the intensity on the satellite part of the spectrum in the magnetic field. Measuring orientation-dependent satellite intensity in appropriate frequency windows yields rotation patterns that can be related to the structure and symmetry of the giant unit cells. For a theoretical reproduction of the rotation patterns, we derived a distribution of the electric-field-gradient (EFG) tensors for each of the investigated compounds from existing structural models using point-charge and ab initio calculations. The EFG distribution yields important structural information on the manifold of different local atomic environments in the unit cell and distinguishes crystallographically inequivalent lattice sites from the equivalent ones. The distribution of the EFGs for the 1168-atom unit cell of $ensuremath{beta}text{ensuremath{-}}{mathrm{Al}}_{3}{mathrm{Mg}}_{2}$ was successfully determined by a point-charge calculation, whereas the ab initio approach was successful for the 160-atom unit cell of the ${mathrm{Mg}}_{32}{(mathrm{Al},mathrm{Zn})}_{49}$ Bergman phase. For the 258-atom unit cell of ${ensuremath{xi}}^{ensuremath{'}}text{ensuremath{-}}mathrm{Al}text{ensuremath{-}}mathrm{Pd}text{ensuremath{-}}mathrm{Mn}$, the experimental rotation patterns revealed a pseudotenfold symmetry, whereas the theoretical point-charge calculation revealed predominant twofold symmetry with traces of tenfold symmetry, so that no quantitative matching between the theory and experiment could be obtained." @default.
- W1657960558 created "2016-06-24" @default.
- W1657960558 creator A5008902557 @default.
- W1657960558 creator A5038363043 @default.
- W1657960558 creator A5041342861 @default.
- W1657960558 creator A5041954579 @default.
- W1657960558 creator A5048275594 @default.
- W1657960558 creator A5051823674 @default.
- W1657960558 creator A5078936714 @default.
- W1657960558 date "2007-01-03" @default.
- W1657960558 modified "2023-10-01" @default.
- W1657960558 title "Orientation-dependent NMR study of the giant-unit-cell intermetallics<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:mi>β</mml:mi><mml:mtext>−</mml:mtext><mml:msub><mml:mi mathvariant=normal>Al</mml:mi><mml:mn>3</mml:mn></mml:msub><mml:msub><mml:mi mathvariant=normal>Mg</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mrow></mml:math>, Bergman-phase<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:msub><mml:mi …" @default.
- W1657960558 cites W1967979326 @default.
- W1657960558 cites W1968229969 @default.
- W1657960558 cites W1970399244 @default.
- W1657960558 cites W1982664426 @default.
- W1657960558 cites W1984475108 @default.
- W1657960558 cites W1998177977 @default.
- W1657960558 cites W2013671677 @default.
- W1657960558 cites W2014318897 @default.
- W1657960558 cites W2017253235 @default.
- W1657960558 cites W2018062021 @default.
- W1657960558 cites W2028267893 @default.
- W1657960558 cites W2032152569 @default.
- W1657960558 cites W2037027420 @default.
- W1657960558 cites W2049079467 @default.
- W1657960558 cites W2055918144 @default.
- W1657960558 cites W2061359039 @default.
- W1657960558 cites W2063726339 @default.
- W1657960558 cites W2065064919 @default.
- W1657960558 cites W2066351024 @default.
- W1657960558 cites W2073264984 @default.
- W1657960558 cites W2090636414 @default.
- W1657960558 cites W2108439616 @default.
- W1657960558 cites W2334955751 @default.
- W1657960558 cites W2909654362 @default.
- W1657960558 cites W4232486186 @default.
- W1657960558 doi "https://doi.org/10.1103/physrevb.75.014202" @default.
- W1657960558 hasPublicationYear "2007" @default.
- W1657960558 type Work @default.
- W1657960558 sameAs 1657960558 @default.
- W1657960558 citedByCount "14" @default.
- W1657960558 countsByYear W16579605582012 @default.
- W1657960558 countsByYear W16579605582013 @default.
- W1657960558 countsByYear W16579605582015 @default.
- W1657960558 countsByYear W16579605582020 @default.
- W1657960558 countsByYear W16579605582022 @default.
- W1657960558 crossrefType "journal-article" @default.
- W1657960558 hasAuthorship W1657960558A5008902557 @default.
- W1657960558 hasAuthorship W1657960558A5038363043 @default.
- W1657960558 hasAuthorship W1657960558A5041342861 @default.
- W1657960558 hasAuthorship W1657960558A5041954579 @default.
- W1657960558 hasAuthorship W1657960558A5048275594 @default.
- W1657960558 hasAuthorship W1657960558A5051823674 @default.
- W1657960558 hasAuthorship W1657960558A5078936714 @default.
- W1657960558 hasConcept C121332964 @default.
- W1657960558 hasConcept C149635348 @default.
- W1657960558 hasConcept C16345878 @default.
- W1657960558 hasConcept C184779094 @default.
- W1657960558 hasConcept C185592680 @default.
- W1657960558 hasConcept C192562407 @default.
- W1657960558 hasConcept C2524010 @default.
- W1657960558 hasConcept C26873012 @default.
- W1657960558 hasConcept C2781442258 @default.
- W1657960558 hasConcept C33923547 @default.
- W1657960558 hasConcept C39984356 @default.
- W1657960558 hasConcept C41008148 @default.
- W1657960558 hasConcept C58312451 @default.
- W1657960558 hasConcept C62520636 @default.
- W1657960558 hasConcept C8010536 @default.
- W1657960558 hasConceptScore W1657960558C121332964 @default.
- W1657960558 hasConceptScore W1657960558C149635348 @default.
- W1657960558 hasConceptScore W1657960558C16345878 @default.
- W1657960558 hasConceptScore W1657960558C184779094 @default.
- W1657960558 hasConceptScore W1657960558C185592680 @default.
- W1657960558 hasConceptScore W1657960558C192562407 @default.
- W1657960558 hasConceptScore W1657960558C2524010 @default.
- W1657960558 hasConceptScore W1657960558C26873012 @default.
- W1657960558 hasConceptScore W1657960558C2781442258 @default.
- W1657960558 hasConceptScore W1657960558C33923547 @default.
- W1657960558 hasConceptScore W1657960558C39984356 @default.
- W1657960558 hasConceptScore W1657960558C41008148 @default.
- W1657960558 hasConceptScore W1657960558C58312451 @default.
- W1657960558 hasConceptScore W1657960558C62520636 @default.
- W1657960558 hasConceptScore W1657960558C8010536 @default.
- W1657960558 hasIssue "1" @default.
- W1657960558 hasLocation W16579605581 @default.
- W1657960558 hasOpenAccess W1657960558 @default.
- W1657960558 hasPrimaryLocation W16579605581 @default.
- W1657960558 hasRelatedWork W1966160131 @default.
- W1657960558 hasRelatedWork W1994021569 @default.
- W1657960558 hasRelatedWork W1997086491 @default.
- W1657960558 hasRelatedWork W1998992221 @default.
- W1657960558 hasRelatedWork W2049827859 @default.
- W1657960558 hasRelatedWork W2608355329 @default.
- W1657960558 hasRelatedWork W3091729581 @default.
- W1657960558 hasRelatedWork W3160306610 @default.
- W1657960558 hasRelatedWork W4232922591 @default.
- W1657960558 hasRelatedWork W4243897261 @default.
- W1657960558 hasVolume "75" @default.