The Physics of the Hume-Rothery Electron Concentration Rule

For a long time we have shared the belief that the physics of the Hume-Rothery electron concentration rule can be deepened only through thorough investigation of the interference phenomenon of itinerant electrons with a particular set of lattice planes, regardless of whether d-states are involved near the Fermi level or not. For this purpose, we have developed the FLAPW-Fourier theory (Full potential Linearized Augmented Plane Wave), which is capable of determining the square of the Fermi diameter, ( 2 k F ) 2 , and the number of itinerant electrons per atom, e/a, as well as the set of lattice planes participating in the interference phenomenon. By determining these key parameters, we could test the interference condition and clarify how it contributes to the formation of a pseudogap at the Fermi level. Further significant progress has been made to allow us to equally handle transition metal (TM) elements and their compounds. A method of taking the center of gravity energy for energy distribution of electrons with a given electronic state has enabled us to eliminate the d-band anomaly and to determine effective ( 2 k F ) 2 , and e/a, even for systems involving the d-band or an energy gap across the Fermi level. The e/a values for 54 elements covering from Group 1 up to Group 16 in the Periodic Table, including 3d-, 4d- and 5d-elements, were determined in a self-consistent manner. The FLAPW-Fourier theory faces its limit only for elements in Group 17 like insulating solids Cl and their compounds, although the value of e/a can be determined without difficulty when Br becomes metallic under high pressures. The origin of a pseudogap at the Fermi level for a large number of compounds has been successfully interpreted in terms of the interference condition, regardless of the bond-types involved in the van Arkel-Ketelaar triangle map.

[1]  Yoshihiko Yokoyama,et al.  Stable Icosahedral Al–Pd–Mn and Al–Pd–Re Alloys , 1990 .

[2]  U. Mizutani,et al.  e/a classification of Hume–Rothery Rhombic Triacontahedron-type approximants based on all-electron density functional theory calculations , 2014 .

[3]  Cesar Pay Gómez,et al.  Comparative structural study of the disordered MCd 6 quasicrystal approximants , 2003 .

[4]  U. Mizutani,et al.  Theoretical Foundation for the Hume-Rothery Electron Concentration Rule for Structurally Complex Alloys , 2014 .

[5]  Shik Shin,et al.  Comparative study of the binary icosahedral quasicrystal Cd5.7Yb and its crystalline approximant Cd6Yb by low-temperature ultrahigh-resolution photoemission spectroscopy , 2002 .

[6]  A. Palenzona The ytterbium-cadmium system , 1971 .

[7]  J. Cahn,et al.  Metallic Phase with Long-Range Orientational Order and No Translational Symmetry , 1984 .

[8]  S. Samson The crsytal structure of the phase β Mg2Al3 , 1965 .

[9]  U. Mizutani,et al.  Hume-Rothery stabilization mechanism and e/a determination in MI-type Al–Mn, Al–Re, Al–Re–Si, Al–Cu–Fe–Si and Al–Cu–Ru–Si 1/1-1/1-1/1 approximants – a proposal for a new Hume-Rothery electron concentration rule , 2012 .

[10]  J. Ketelaar Chemical constitution : an introduction to the theory of the chemical bond , 1953 .

[11]  Uichiro Mizutani,et al.  Introduction to the Electron Theory of Metals: Superconductivity , 2001 .

[12]  E. C. STONER,et al.  Atomic Theory for Students of Metallurgy , 1947, Nature.

[13]  N. Mott,et al.  The Theory of the Properties of Metals and Alloys , 1933 .

[14]  Joseph F. Capitani,et al.  Van Arkel—Ketelaar triangles , 1993 .

[15]  Y. Nishino,et al.  Fermi surface–Brillouin-zone-induced pseudogap in γ-Mg17Al12 and a possible stabilization mechanism of β-Al3Mg2 , 2010, Journal of physics. Condensed matter : an Institute of Physics journal.

[16]  R. Nesper Structure and chemical bonding in zintl-phases containing lithium , 1990 .

[17]  W. C. Martin,et al.  Handbook of Basic Atomic Spectroscopic Data , 2005 .

[18]  Hirokazu Sato,et al.  Determination of electrons per atom ratio for transition metal compounds studied by FLAPW-Fourier calculations , 2016 .

[19]  U. Mizutani,et al.  Hume–Rothery Stabilization Mechanism in Low-Temperature Phase Zn6Sc Approximant and e/a Determination of Sc and Y in M–Sc and M–Y (M=Zn, Cd and Al) Alloy Systems , 2013 .

[20]  U. Mizutani,et al.  Hume-Rothery stabilization mechanism and e/a determination for RT- and MI-type 1/1-1/1-1/1 approximants studied by FLAPW-Fourier analyses. , 2012, Chemical Society reviews.

[21]  Fujiwara Electronic structure in the Al-Mn alloy crystalline analog of quasicrystals. , 1989, Physical review. B, Condensed matter.

[22]  W. Steurer The Samson phase, β-Mg2Al3, revisited , 2007 .

[23]  M. Inukai,et al.  Hume-Rothery Stabilization Mechanism in Tsai-Type Cd 6 Ca Approximant and e/a Determination of Ca and Cd Elements in the Periodic Table , 2013 .

[24]  U. Mizutani,et al.  e/a determination for 4d- and 5d-transition metal elements and their intermetallic compounds with Mg, Al, Zn, Cd and In , 2013 .

[25]  A. Tsai A test of Hume-Rothery rules for stable quasicrystals , 2004 .

[26]  Isamu Akasaki,et al.  Breakthroughs in Improving Crystal Quality of GaN and Invention of the p–n Junction Blue-Light-Emitting Diode , 2006 .

[27]  Shuji Nakamura,et al.  Ridge‐geometry InGaN multi‐quantum‐well‐structure laser diodes , 1996 .

[28]  T. Ishimasa,et al.  Low-temperature phase of the Zn–Sc approximant , 2007 .

[29]  Leland C. Allen,et al.  Electronegativity is the average one-electron energy of the valence-shell electrons in ground-state free atoms , 1989 .

[30]  R. Asahi,et al.  Verification of Hume-Rothery electron concentration rule inCu5Zn8andCu9Al4γbrasses byab initioFLAPW band calculations , 2005 .

[31]  Hase,et al.  Evidence for molecular dissociation in bromine near 80 GPa. , 1989, Physical review letters.

[32]  Linus Pauling,et al.  The Nature of the Interatomic Forces in Metals , 1938 .

[33]  K. Kimura,et al.  Composition dependence of thermoelectric properties of AlPdRe icosahedral quasicrystals , 2002 .

[34]  Y. Ishii,et al.  First-principles studies for structural transitions in ordered phase of cubic approximant Cd6Ca , 2008, 0806.1376.

[35]  U. Mizutani,et al.  Origin of the DOS pseudogap and Hume–Rothery stabilization mechanism in RT-type Al48Mg64Zn48 and Al84Li52Cu24 1/1-1/1-1/1 approximants , 2011 .

[36]  U. Mizutani,et al.  NFE approximation for the e/a determination for 3d-transition metal elements and their intermetallic compounds with Al and Zn , 2013 .

[37]  U. Mizutani,et al.  Electron Theory of Complex Metallic Alloys , 2014 .

[38]  U. Mizutani Hume-Rothery rules for structurally complex alloy phases , 2010 .

[39]  Luo,et al.  beta -Po phase of sulfur at 162 GPa: X-ray diffraction study to 212 GPa. , 1993, Physical review letters.

[40]  H. Skriver The LMTO Method , 1984 .

[41]  Hirokazu Sato,et al.  Electrons per atom ratio determination and Hume-Rothery electron concentration rule for P-based polar compounds studied by FLAPW-fourier calculations. , 2015, Inorganic chemistry.

[42]  G. Raynor Progress in the theory of alloys , 1949 .

[43]  M. Palm,et al.  Structure and stability of Laves phases. Part I. Critical assessment of factors controlling Laves phase stability , 2004 .

[44]  Yoshihiko Yokoyama,et al.  Formation Criteria and Growth Morphology of Quasicrystals in Al–Pd–TM (TM=Transition Metal) Alloys , 1991 .

[45]  Akihisa Inoue,et al.  New Stable Icosahedral Al-Cu-Ru and Al-Cu-Os Alloys , 1988 .