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The crystal structure of the Ag36Li64 gamma-brass was determined by analyzing the powder diffraction pattern taken using a synchrotron radiation beam with wavelength 0.50226 Å. It turned out that the compound contained 52 atoms in its unit cell with the space group I\bar 43m and that the Li atom enters exclusively into inner tetrahedral (IT) and cubo-octahedral (CO) sites, whereas the Ag atom enters into those on outer tetrahedral (OT) and octahedral (OH) sites in the 26-atom cluster. Small amounts of Li also exist in OT and OH sites, resulting in chemical disorder. We discovered that the volumes of the IT and CO polyhedra shrink, while those of the OT and OH polyhedra expand relative to those of the corresponding polyhedra in the original b.c.c. (body-centered cubic) structure. This feature is universal and is found in other gamma-brasses such as Cu5Zn8 and Al8V5, for which the structure data are available. Among these gamma-brasses, we revealed the unique bond-length distribution for pairs connecting the atom on OH sites and that on CO sites, depending on the degree of d-p orbital hybridization between the transition metal elements such as Ag, Cu and V on OH sites, and the non-transition metal elements such as Li, Zn and Al on CO sites. It is suggested that this may hold a clue to resolving why some gamma-brasses such as the present Ag-Li and Cu-Zn possess a finite solid solution, but others such as Al8V5 and Mn3In exist as line compounds.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768107039092/av5091sup1.cif
Contains datablocks global, Ag36Li64

rtv

Rietveld powder data file (CIF format) https://doi.org/10.1107/S0108768107039092/av5091sup2.rtv
Contains datablock noritakeAgLiprofile

Computing details top

Cell refinement: RIETAN-2000 (Izumi and Ikeda, 2000); program(s) used to refine structure: RIETAN-2000 (Izumi and Ikeda, 2000); molecular graphics: ATOMS (Eric Dowty 1999).

silver-lithium gamma phase top
Crystal data top
Ag18.56Li33.44F(000) = 972.64
Mr = 2234.14Dx = 4.185 Mg m3
Cubic, I43mSynchrotron radiation, λ = 0.50226 Å
a = 9.6066 (8) ŵ = 3.85 mm1
V = 886.56 (13) Å3T = 300 K
Z = 1
Data collection top
BL02B2
diffractometer
k =
Si monochromatorl =
h =
Refinement top
S = 1.6752 parameters
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzBiso*/BeqOcc. (<1)
Ag10.82767 (8)0.827670.827670.9311
Li10.827670.827670.827670.0689
Ag20.35410 (10)0.00.00.9259 (9)
Li20.35410.00.00.0741
Li30.1168 (13)0.11680.1168
Li40.3150 (14)0.31500.0334 (17)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ag10.178 (3)0.1780.1780.033 (4)0.0330.033
Li10.1780.1780.1780.0330.0330.033
Ag20.136 (6)0.209 (4)0.2090.00.00.049 (8)
Li20.1360.2090.2090.00.00.049
Li30.42 (9)0.420.420.22 (8)0.220.22
Li40.46 (7)0.460.26 (14)0.07 (7)0.17 (6)0.17
Geometric parameters (Å, º) top
Ag2—Li4i2.74 (2)Ag2—Li4v3.070 (10)
Ag1—Li4ii2.77 (2)Ag2—Ag2vi2.802 (2)
Ag2—Li32.7780 (10)Ag1—Ag2ii2.9210 (10)
Ag1—Li4iii2.83 (2)Li3—Li42.810 (2)
Ag1—Li3ii2.878 (7)Li4—Li4iv2.843 (5)
Ag2—Li4iv3.05 (2)Li3—Li3vii3.17 (3)
Ag2vi—Ag2—Li4i66.7 (3)Ag2vi—Ag2—Li497.0 (3)
Ag2vi—Ag2—Li4iv55.6 (4)
Symmetry codes: (i) z+1/2, x1/2, y+1/2; (ii) x+1, y+1, z+1; (iii) x+1/2, y+1/2, z+1/2; (iv) z+1/2, x+1/2, y+1/2; (v) x, y, z; (vi) x+1, y, z; (vii) x, y, z.
 

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