Abstract:Based on first-principles FLAPW-GGA calculation, we have investigated electronic structure of newly discovered oxygen-free 38K superconductor Ba 1-x K x Fe 2 As 2 in comparison with parent phase -tetragonal ternary iron arsenide BaFe 2 As 2 . The density of states, magnetic properties, near-Fermi bands compositions, together with Sommerfeld coefficients γ and molar Pauli paramagnetic susceptibility χ are evaluated. The results allow us to classify these systems as quasi-two-dimensional ionic metals, where the … Show more
“…Our results show that replacements in blocks [Pd(Ni) 2 Ge(As) 2 ] of the d metal atoms (Pd ↔ Ni) or p elements (Ge ↔ As) lead to anisotropic deformations of the crystal structure caused by strong anisotropy of inter-atomic bonds in "122' phases (see also [20,24]), but the type of such deformations will be quite different. Thus, going from SrPd 2 Ge 2 to SrNi 2 Ge 2 , i.e.…”
Section: Structural Propertiesmentioning
confidence: 89%
“…The superconductivity in all these systems is attributed to the [M 2 Pn 2 ] blocks which make a decisive contribution to the near-Fermi region of these materials, while the positively charged blocks (for example, [RO] δ+ or A δ+ ) serve as the so-called charge reservoirs, see [2][3][4][5][6][7][8][9]. In particular, a broad family of the mentioned "122" superconductors (SC's) with transition temperatures up to T C ~ 38K (see [2][3][4][5][10][11][12][13][14][15][16]) based on AFe 2 As 2 phases (A = Ca, Sr or Ba) was prepared by hole doping, i.e. by partial substitution of alkaline metals for alkaline earth metals; or by partial replacement of Fe (in [Fe 2 As 2 ] blocks) by other 3d transition metals as Mn, Co or Ni.…”
Section: Introductionmentioning
confidence: 99%
“…These materials, where magnetic metal (Fe) is completely replaced by the other 3d magnetic metal (Ni) or non-magnetic metals (Ru, Rh) arsenic is completely replaced by other pnictogen -phosphorus, belong to the above mentioned "122" family and are low-temperature SC's (T C ~ 0.3-3.0K), see [21][22][23][24].…”
Very recently the new low-temperature (T C ~ 3K) superconductor (SC) SrPd 2 Ge 2 has been reported. This compound is isostructural with curently intensively studied group of so-called "122" SC's (based on tetragonal AM 2 Pn 2 phases, where A are Sr, Ba; M are d metals and Pn are pnictogens: As or P), but it is pnictogen-free. Here, by means
“…Our results show that replacements in blocks [Pd(Ni) 2 Ge(As) 2 ] of the d metal atoms (Pd ↔ Ni) or p elements (Ge ↔ As) lead to anisotropic deformations of the crystal structure caused by strong anisotropy of inter-atomic bonds in "122' phases (see also [20,24]), but the type of such deformations will be quite different. Thus, going from SrPd 2 Ge 2 to SrNi 2 Ge 2 , i.e.…”
Section: Structural Propertiesmentioning
confidence: 89%
“…The superconductivity in all these systems is attributed to the [M 2 Pn 2 ] blocks which make a decisive contribution to the near-Fermi region of these materials, while the positively charged blocks (for example, [RO] δ+ or A δ+ ) serve as the so-called charge reservoirs, see [2][3][4][5][6][7][8][9]. In particular, a broad family of the mentioned "122" superconductors (SC's) with transition temperatures up to T C ~ 38K (see [2][3][4][5][10][11][12][13][14][15][16]) based on AFe 2 As 2 phases (A = Ca, Sr or Ba) was prepared by hole doping, i.e. by partial substitution of alkaline metals for alkaline earth metals; or by partial replacement of Fe (in [Fe 2 As 2 ] blocks) by other 3d transition metals as Mn, Co or Ni.…”
Section: Introductionmentioning
confidence: 99%
“…These materials, where magnetic metal (Fe) is completely replaced by the other 3d magnetic metal (Ni) or non-magnetic metals (Ru, Rh) arsenic is completely replaced by other pnictogen -phosphorus, belong to the above mentioned "122" family and are low-temperature SC's (T C ~ 0.3-3.0K), see [21][22][23][24].…”
Very recently the new low-temperature (T C ~ 3K) superconductor (SC) SrPd 2 Ge 2 has been reported. This compound is isostructural with curently intensively studied group of so-called "122" SC's (based on tetragonal AM 2 Pn 2 phases, where A are Sr, Ba; M are d metals and Pn are pnictogens: As or P), but it is pnictogen-free. Here, by means
“…[20,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51] While these differ in detail a number of common features are present. Fig.…”
Section: Crystal Structure and Chemistrymentioning
The electronic structure of the Fe-based superconductors is discussed, mainly from the point of view of first principles calculations in relation to experimental data. Comparisons and contrasts with cuprates are made. The problem of reconciling experiments indicating an s symmetry gap with experiments indicating line nodes is discussed and a possible resolution is given.
“…The valence states occupy the energy interval from E F to -6 eV, where the states from -6 eV to -4 eV and from -4 eV to -2 eV are mainly of Se 4p and As 4p character, respectively, and are hybridized with Fe 3d states. The near-Fermi states are mainly of the Fe 3d type, 31,32 As the electronic bands near the Fermi surface are involved in the formation of the superconducting state, it is important to elucidate their nature. Figure 4 shows the nearFermi bands for KFe 2 AsSe (1 and 2).…”
The ThCr 2 Si 2 -type arsenide-selenide phase KFe 2 AsSe is proposed as a parent system for a new "intermediate" group of Fe-based superconducting materials bridging the known families of Fe-pnictides (such as BaFe 2 As 2 ) and Fe-chalcogenides (such as K x Fe 2-y Se 2 ) superconductors. The characterization of the proposed charge-balanced phase by means of FLAPW-GGA approach covers the crystal structure, As/Se atomic ordering, stability, electronic bands, Fermi surface, and density of electronic states. PACS number(s): 71.18.+y, 71.15.Mb,74.25.Jb
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