The crystal structure of Pb
10(PO
4)
6O, the proposed matrix for the potential room-temperature superconductor LK-99, Pb
10−xCu
x(PO
4)
6O (x = 0.9–1.0), has been reinvestigated via single-crystal X-ray diffraction using crystals prepared by
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The crystal structure of Pb
10(PO
4)
6O, the proposed matrix for the potential room-temperature superconductor LK-99, Pb
10−xCu
x(PO
4)
6O (x = 0.9–1.0), has been reinvestigated via single-crystal X-ray diffraction using crystals prepared by Merker and Wondratschek (
Z. Anorg. Allg. Chem. 1960,
306, 25–29). The crystal structure is trigonal,
P,
a = 9.8109(6),
c = 14.8403(12) Å,
V = 1237.06(15),
R1 = 0.0413 using 3456 unique observed reflections. The crystal structure of Pb
10(PO
4)
6O is a superstructure with regard to the ‘standard’
P6
3/
m apatite structure type. The doubling of the
c parameter is induced through the ordering of the split sites of ‘additional’ O’ atoms within the structure channels running parallel to the
c axis and centered at (00
z). The O’ atoms form short bonds to the Pb1 atoms, resulting in splitting the Pb1 site into two, Pb1A and Pb1B. The structural distortions are further transmitted to the Pb phosphate framework formed by four Pb2 sites and PO
4 groups. The structure data previously reported by Krivovichev and Burns (
Z. Kristallogr. 2003,
218, 357–365) may either correspond to the Pb
10(PO
4)
6O
x(OH)
2−2x (x ~ 0.4) member of the Pb
10(PO
4)
6O—Pb
10(PO
4)
6(OH)
2 solid solution series, or to the high-temperature polymorph of Pb
10(PO
4)
6O (with the phase with doubled
c parameter being the low-temperature polymorph).
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