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Volumn 82, Issue 14, 2010, Pages

Effect of interlayer interactions and lattice distortions on the magnetic ground state and spin dynamics of a geometrically frustrated triangular-lattice antiferromagnet

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EID: 78049457995     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.82.144441     Document Type: Article
Times cited : (18)

References (42)
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    • + magnetic form factor is given as Fq = j0 (q), where j0 (q) = A0 e a0 s2 + B0 e b0 s2 + C0 e c0 s2 + D0 and s=sinθ/λ=q/ 4π. The coefficients are A0 =0.3972 ( a0 =13.2442 ), B0 =0.6295 ( b0 =4.9034 ), C0 =-0.0314 ( c0 =0.3496 ), and D0 =0.0044 from Ref..
    • + magnetic form factor is given as F q = j 0 (q), where j 0 (q) = A 0 e a 0 s 2 + B 0 e b 0 s 2 + C 0 e c 0 s 2 + D 0 and s = sin θ / λ = q / 4 π. The coefficients are A 0 = 0.3972 (a 0 = 13.2442), B 0 = 0.6295 (b 0 = 4.9034), C 0 = - 0.0314 (c 0 = 0.3496), and D 0 = 0.0044 from Ref..
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    • For the doped sample, the parameters were manually adjusted to fit the data because the data sets consist of multiple three-dimensional matrices. This is different from the numerical least squares fitting used to analyze the undoped sample (Ref.).
    • For the doped sample, the parameters were manually adjusted to fit the data because the data sets consist of multiple three-dimensional matrices. This is different from the numerical least squares fitting used to analyze the undoped sample (Ref.).


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