# Difference between revisions of "Incommensurate magnetic structure"

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− | <Font color="blue">Structure magnétique incommensurable</font> (Fr.) | + | <Font color="blue">Structure magnétique incommensurable</font> (''Fr''). <Font color="black">Struttura magnetica incommensurabile</font> (''It''). <Font color="purple">非整合磁気構造</font> (''Ja''). |

== Definition == | == Definition == | ||

− | An ''incommensurate magnetic structure'' is a structure in which the magnetic moments are | + | An ''incommensurate magnetic structure'' is a [[crystal pattern|structure]] in which the magnetic moments are |

− | ordered, but without | + | ordered, but without periodicity that is commensurate with that of the nuclear structure |

of the crystal. In particular, the magnetic moments have a spin density with wave vectors | of the crystal. In particular, the magnetic moments have a spin density with wave vectors | ||

that have at least one irrational component with respect to the reciprocal lattice | that have at least one irrational component with respect to the reciprocal lattice | ||

of the atoms. Or, in the case of localized moments, the spin function '''S'''('''n'''+'''r'''<sub>''j''</sub>) | of the atoms. Or, in the case of localized moments, the spin function '''S'''('''n'''+'''r'''<sub>''j''</sub>) | ||

− | (where the ''j''th atom has position '''r'''<sub>''j''</sub> in the unit cell) has Fourier components | + | (where the ''j''th atom has position '''r'''<sub>''j''</sub> in the [[unit cell]]) has Fourier components |

with irrational indices with respect to the reciprocal lattice of the crystal. | with irrational indices with respect to the reciprocal lattice of the crystal. | ||

## Revision as of 14:06, 20 March 2015

Structure magnétique incommensurable (*Fr*). Struttura magnetica incommensurabile (*It*). 非整合磁気構造 (*Ja*).

## Definition

An *incommensurate magnetic structure* is a structure in which the magnetic moments are
ordered, but without periodicity that is commensurate with that of the nuclear structure
of the crystal. In particular, the magnetic moments have a spin density with wave vectors
that have at least one irrational component with respect to the reciprocal lattice
of the atoms. Or, in the case of localized moments, the spin function **S**(**n**+**r**_{j})
(where the *j*th atom has position **r**_{j} in the unit cell) has Fourier components
with irrational indices with respect to the reciprocal lattice of the crystal.

## Details

When the atoms of the basic structure are at positions **n**+**r**_{j}, where **r**_{j}
is the position of the *j*th atom in the unit cell, then the spin function for
an incommensurate magnetic structure is

[math] S( n+ r_j)~=~\sum_ {k} \hat{S}( k)_j \exp \left(2\pi i k.( n+ r_j)\right),~~ k=\sum_{i=1}^n h_i a_i^*~~(h_i ~~{\rm integer}).[/math]

This spin structure is incommensurate if one component of the basis vectors **a**_{i}^{*}
is irrational. Incommensurate magnetic structures may be linear, but occur as quite
complicated, like fan structures etc. as well. Especially, in rare-earth compounds very
complicated magnetic phase diagrams have been found.