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About McStas Download Documentation |
9.9 The Magnon_bcc McStas ComponentA sample for AFM or FM magnon scattering based on cross section expressions from Squires, Ch.8.2
Identification
DescriptionSingle-cylinder shape. Absorption included. No multiple scattering. No incoherent scattering emitted. No attenuation from coherent scattering. No Bragg scattering. bcc crystal n.n. and n.n.n. interactions only Can do either FM or AFM order upon a flag Assume J>0 for both FM and AFM. MUST BE CHANGED FOR CONSISTENCY If AFM, the order is two-sublattice, e.g. the AFM Bragg ordering vectors are Q = (1 0 0) and equivalent. One magnon branch only Assume spin along z Possible easy axis anisotropy along z No external field KNOWN BUGS: Gives zero scattering for too large J values (for AFM J=0.362, h approx 1). Probably this is a malfunction of zridd or call thereof The value of the absolute scattered intensity is clearly too high. This is probably due to unit confusion. The relative intensity scaling seems about right. Algorithm: 0. Always perform the scattering if possible (otherwise ABSORB) 1. Choose direction within a focusing solid angle 2. Calculate the zeros of (E_i-E_f-hbar omega(kappa)) as a function of k_f 3. Choose one value of k_f (always at least one is possible!) 4. Perform the correct weight transformation
Input parametersParameters in boldface are required; the others are optional.
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