Matches in SemOpenAlex for { <https://semopenalex.org/work/W2012094392> ?p ?o ?g. }
- W2012094392 abstract "We have investigated the magnetic susceptibility, the electrical resistivity, the specific heat, the thermoelectric power, the Hall coefficient, and the thermal conductivity of the ${text{Al}}_{13}{text{Fe}}_{4}$ and ${text{Al}}_{13}{(text{Fe},text{Ni})}_{4}$ monoclinic approximants to the decagonal quasicrystal. While the ${text{Al}}_{13}{text{Fe}}_{4}$ crystals are structurally well ordered, the ternary derivative ${text{Al}}_{13}{(text{Fe},text{Ni})}_{4}$ contains substitutional disorder and is considered as a disordered version of the ${text{Al}}_{13}{text{Fe}}_{4}$. The crystallographic-direction-dependent measurements were performed along the ${a}^{ensuremath{ast}}$, $b$, and $c$ directions of the monoclinic unit cell, where the $({a}^{ensuremath{ast}},c)$ atomic planes are stacked along the $b$ direction. The electronic transport and the magnetic properties exhibit significant anisotropy. The stacking $b$ direction is the most conducting direction for the electricity and heat. The effect of substitutional disorder in ${text{Al}}_{13}{(text{Fe},text{Ni})}_{4}$ is manifested in the large residual resistivity $ensuremath{rho}(Tensuremath{rightarrow}0)$ and significantly reduced thermal conductivity of this compound, as compared to the ordered ${text{Al}}_{13}{text{Fe}}_{4}$. Specific-heat measurements reveal that the electronic density of states at the Fermi level of both compounds is high. The anisotropic Hall coefficient ${R}_{H}$ reflects complex structure of the anisotropic Fermi surface that contains electronlike and holelike contributions. Depending on the combination of directions of the current and the magnetic field, electronlike $({R}_{H}<0)$ or holelike $({R}_{H}>0)$ contributions may dominate, or the two contributions compensate each other $({R}_{H}ensuremath{approx}0)$. Similar complicated anisotropic behavior was observed also in the thermopower. The anisotropic Fermi surface was calculated ab initio using the atomic parameters of the refined ${text{Al}}_{13}{text{Fe}}_{4}$ structural model that is also presented in this work." @default.
- W2012094392 created "2016-06-24" @default.
- W2012094392 creator A5000485523 @default.
- W2012094392 creator A5006151336 @default.
- W2012094392 creator A5015489916 @default.
- W2012094392 creator A5027977591 @default.
- W2012094392 creator A5033476336 @default.
- W2012094392 creator A5038363043 @default.
- W2012094392 creator A5041342861 @default.
- W2012094392 creator A5041954579 @default.
- W2012094392 creator A5042165141 @default.
- W2012094392 creator A5044233462 @default.
- W2012094392 creator A5046635660 @default.
- W2012094392 creator A5072072076 @default.
- W2012094392 creator A5078795883 @default.
- W2012094392 creator A5078936714 @default.
- W2012094392 creator A5085886473 @default.
- W2012094392 date "2010-05-07" @default.
- W2012094392 modified "2023-10-17" @default.
- W2012094392 title "Anisotropic physical properties of the<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:msub><mml:mrow><mml:mtext>Al</mml:mtext></mml:mrow><mml:mrow><mml:mn>13</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mtext>Fe</mml:mtext></mml:mrow><mml:mn>4</mml:mn></mml:msub></mml:mrow></mml:math>complex intermetallic and its ternary derivative<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:msub><mml:mrow><mml:mtext>…" @default.
- W2012094392 cites W114325395 @default.
- W2012094392 cites W158610827 @default.
- W2012094392 cites W1610587319 @default.
- W2012094392 cites W187152825 @default.
- W2012094392 cites W1978305833 @default.
- W2012094392 cites W1980942222 @default.
- W2012094392 cites W1988335379 @default.
- W2012094392 cites W1991478619 @default.
- W2012094392 cites W1995530362 @default.
- W2012094392 cites W2010204034 @default.
- W2012094392 cites W2010844172 @default.
- W2012094392 cites W2015762944 @default.
- W2012094392 cites W2019845198 @default.
- W2012094392 cites W2020815194 @default.
- W2012094392 cites W2023414699 @default.
- W2012094392 cites W2026017313 @default.
- W2012094392 cites W2035223648 @default.
- W2012094392 cites W2035799879 @default.
- W2012094392 cites W2037884445 @default.
- W2012094392 cites W2041713471 @default.
- W2012094392 cites W2045596260 @default.
- W2012094392 cites W2046973870 @default.
- W2012094392 cites W2049079467 @default.
- W2012094392 cites W2052558259 @default.
- W2012094392 cites W2060524866 @default.
- W2012094392 cites W2060692741 @default.
- W2012094392 cites W2060867255 @default.
- W2012094392 cites W2071728968 @default.
- W2012094392 cites W2081415419 @default.
- W2012094392 cites W2081870935 @default.
- W2012094392 cites W2084803885 @default.
- W2012094392 cites W2084833029 @default.
- W2012094392 cites W2085165785 @default.
- W2012094392 cites W2085679340 @default.
- W2012094392 cites W2086967155 @default.
- W2012094392 cites W2124360154 @default.
- W2012094392 cites W2135843168 @default.
- W2012094392 cites W2147804311 @default.
- W2012094392 cites W279556495 @default.
- W2012094392 cites W3103887024 @default.
- W2012094392 doi "https://doi.org/10.1103/physrevb.81.184203" @default.
- W2012094392 hasPublicationYear "2010" @default.
- W2012094392 type Work @default.
- W2012094392 sameAs 2012094392 @default.
- W2012094392 citedByCount "69" @default.
- W2012094392 countsByYear W20120943922012 @default.
- W2012094392 countsByYear W20120943922013 @default.
- W2012094392 countsByYear W20120943922014 @default.
- W2012094392 countsByYear W20120943922015 @default.
- W2012094392 countsByYear W20120943922016 @default.
- W2012094392 countsByYear W20120943922017 @default.
- W2012094392 countsByYear W20120943922018 @default.
- W2012094392 countsByYear W20120943922019 @default.
- W2012094392 countsByYear W20120943922020 @default.
- W2012094392 countsByYear W20120943922021 @default.
- W2012094392 countsByYear W20120943922022 @default.
- W2012094392 countsByYear W20120943922023 @default.
- W2012094392 crossrefType "journal-article" @default.
- W2012094392 hasAuthorship W2012094392A5000485523 @default.
- W2012094392 hasAuthorship W2012094392A5006151336 @default.
- W2012094392 hasAuthorship W2012094392A5015489916 @default.
- W2012094392 hasAuthorship W2012094392A5027977591 @default.
- W2012094392 hasAuthorship W2012094392A5033476336 @default.
- W2012094392 hasAuthorship W2012094392A5038363043 @default.
- W2012094392 hasAuthorship W2012094392A5041342861 @default.
- W2012094392 hasAuthorship W2012094392A5041954579 @default.
- W2012094392 hasAuthorship W2012094392A5042165141 @default.
- W2012094392 hasAuthorship W2012094392A5044233462 @default.
- W2012094392 hasAuthorship W2012094392A5046635660 @default.
- W2012094392 hasAuthorship W2012094392A5072072076 @default.
- W2012094392 hasAuthorship W2012094392A5078795883 @default.
- W2012094392 hasAuthorship W2012094392A5078936714 @default.
- W2012094392 hasAuthorship W2012094392A5085886473 @default.
- W2012094392 hasConcept C112625512 @default.
- W2012094392 hasConcept C115624301 @default.
- W2012094392 hasConcept C121332964 @default.
- W2012094392 hasConcept C134112204 @default.
- W2012094392 hasConcept C16889073 @default.
- W2012094392 hasConcept C185592680 @default.
- W2012094392 hasConcept C192562407 @default.