TY - JOUR
T1 - Structure and lattice excitations of the copper substituted lead oxyapatite Pb9.06(7)Cu0.94(6)(PO3.92(4))6 O0.96(3)
AU - Zhang, Qiang
AU - Guan, Yingdong
AU - Cheng, Yongqiang
AU - Min, Lujin
AU - Keum, Jong K.
AU - Mao, Zhiqiang
AU - Stone, Matthew B.
N1 - Publisher Copyright:
© 2024 American Physical Society.
PY - 2024/1
Y1 - 2024/1
N2 - The copper substituted lead oxyapatite, Pb10-xCux(PO3.92(4))6O0.96(3) [x = 0.94(6)] was studied using neutron and x-ray diffraction and neutron spectroscopy techniques. The crystal structure of the main phase of our sample, which has come to be colloquially known as LK-99, is verified to possess a hexagonal structure with space group P63/m, alongside the presence of impurity phases Cu and Cu2S. We determine the primary substitution location of the Cu as the Pb1 (6h) site, with a small substitution at the Pb2 (4f) site. Consequently, no clear Cu-doping-induced structural distortion was observed in the investigated temperature region between 10 K and 300 K. Specially, we did not observe a reduction of coordinate number at the Pb2 site or a clear tilting of PO4 tetrahedron. Magnetic characterization reveals a diamagnetic signal in the specimen, accompanied by a very weak ferromagnetic component at 2 K. No long-range magnetic order down to 10 K was detected by the neutron diffraction. Inelastic neutron scattering measurements did not show magnetic excitations for energies up to 350 meV. There is no sign of a superconducting resonance in the excitation spectrum of this material. The measured phonon density of states compares well with density functional theory calculations performed for the main LK-99 phase and its impurity phases. Our study may shed some insight into the role of the favored substitution site of copper in the absence of structural distortion and superconductivity in LK-99.
AB - The copper substituted lead oxyapatite, Pb10-xCux(PO3.92(4))6O0.96(3) [x = 0.94(6)] was studied using neutron and x-ray diffraction and neutron spectroscopy techniques. The crystal structure of the main phase of our sample, which has come to be colloquially known as LK-99, is verified to possess a hexagonal structure with space group P63/m, alongside the presence of impurity phases Cu and Cu2S. We determine the primary substitution location of the Cu as the Pb1 (6h) site, with a small substitution at the Pb2 (4f) site. Consequently, no clear Cu-doping-induced structural distortion was observed in the investigated temperature region between 10 K and 300 K. Specially, we did not observe a reduction of coordinate number at the Pb2 site or a clear tilting of PO4 tetrahedron. Magnetic characterization reveals a diamagnetic signal in the specimen, accompanied by a very weak ferromagnetic component at 2 K. No long-range magnetic order down to 10 K was detected by the neutron diffraction. Inelastic neutron scattering measurements did not show magnetic excitations for energies up to 350 meV. There is no sign of a superconducting resonance in the excitation spectrum of this material. The measured phonon density of states compares well with density functional theory calculations performed for the main LK-99 phase and its impurity phases. Our study may shed some insight into the role of the favored substitution site of copper in the absence of structural distortion and superconductivity in LK-99.
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U2 - 10.1103/PhysRevMaterials.8.014605
DO - 10.1103/PhysRevMaterials.8.014605
M3 - Article
AN - SCOPUS:85184019949
SN - 2475-9953
VL - 8
JO - Physical Review Materials
JF - Physical Review Materials
IS - 1
M1 - 014605
ER -