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How to Use Find Γ

Find Γ reads a magnetic structure from its MCIF and works out its spin space symmetry and what that symmetry allows, following Spin Space Symmetry Without Spin Space Groups. Here is what a report says, what you can do with it, and where to click.

What the Report Says

A report describes a magnetic order by a few objects, each in a row of its own.

Crystal Space Group (\(\boldsymbol{G_0}\))
The structure's symmetry with its moments left out (the report's Crystal SG).
Parent Space Group (\(\boldsymbol{G}\))
The operations of \(G_0\) that keep the magnetic order, up to one transformation of spin space for all its moments. Where \(G = G_0\) the order is regular.
Defining Representation (\(\boldsymbol{\Gamma}\))
For each operation \(g\) of \(G\), the matrix \(\Gamma(g)\) that carries the moments, the spin space group's elements being \([\Gamma(g)\,\Vert\,g]\). It is one-, two- or three-dimensional for collinear, coplanar or non-coplanar order, \(\det\Gamma(g) = -1\) meaning time reversal with it, and is written as its irreducible parts (\(\Gamma = B_{2g}\)).
Wavevectors (\(\boldsymbol{\vec{k}}\)) and Propagation Vectors (\(\boldsymbol{\vec{Q}}\))
Γ's wavevector content, the stars of the wavevectors \(\vec{k}\) of its parts, in \(G\). The propagation vectors \(\vec{Q}\) are those the structure itself has weight on, in \(G_0\).
Exterior Powers (\(\boldsymbol{\Lambda^1\Gamma}\), \(\boldsymbol{\Lambda^2\Gamma}\), \(\boldsymbol{\Lambda^3\Gamma}\))
How a spin vector, a spin pseudovector and a spin pseudoscalar transform. \(\Lambda^1\Gamma = \Gamma\); \(\Lambda^2\Gamma\) is 0 for collinear order, \(\Lambda^3\Gamma\) unless it is non-coplanar.
Allowed and Forbidden
A response is allowed (✓) where the \(\vec{k} = \vec{0}\) part of its exterior power overlaps the multipole's representation beside it (its required overlap), and forbidden (✗) where it does not. A magnet is compensated where \(\Gamma\) holds no trivial irrep: no net magnetization.
Magnet Classes
An altermagnet is collinear and compensated, with a spin texture of even rank; an odd-parity magnet is compensated, with a spin texture of odd rank and none of even rank; a Luttinger compensated candidate is collinear, its magnetization allowed but its net moment below 0.01 μB. The wave (d, g, … or p, f, …) is the texture's lowest rank.
Two Regimes
Non-relativistic: spin and space transform apart, by the spin space group. Relativistic: spin–orbit coupling turns the moments with the crystal, and the magnetic space group takes the spin space group's place, written in the same way.

Analyse a Structure

Analyse a magnetic structure of your own, or open one that is already done.

Find Γ's front page: the box to choose or drop an MCIF file, the tolerances and the examples.
The front page

The Report

A report opens with what the order is and what it allows, the structure as the file gives it, and its symmetry.

MnF₂'s report: its banner, the regime and notation switches, the structure's and the symmetry's panels.
MnF2

Structure

The cell is drawn with its moments and its magnetic ions' polyhedra; fill the window for the sidebar.

MnF₂ filling the window: a manganese atom chosen, its card in the sidebar.
MnF2: an Mn atom chosen

Symmetry

The Symmetry page lists the group's elements, each \(\{U\,\Vert\,R\,|\,\vec{t}\}\), and plays each one on the structure.

MnF₂'s Symmetry page: a fourfold screw rotation caught as it plays, its axis and angle drawn.
MnF2: \(\{\bar{1}\,\Vert\,4^{+}_{001}\,|\,\tfrac{1}{2}\,\tfrac{1}{2}\,\tfrac{1}{2}\}\) as it plays

Responses

Which responses the symmetry allows, each with the overlap that decides it.

MnF₂'s non-relativistic responses: piezomagnetism and the time-odd spin conductivity allowed, a d-wave spin texture.
MnF2
MnF₂'s even-rank spin texture: its constraint, overlap table, form and sphere.
MnF2: its spin texture of even rank

Representation

How the point group's multipoles decompose, and Γ itself, operation by operation.

MnF₂'s multipoles, Λ¹Γ's irreps in bold and a quadrupole's functions in a card, and the start of its representation.
MnF2

Brillouin Zones

Where the wavevectors are: the zones of \(G_0\) and \(G\), their points of symmetry, and the stars of \(\vec{Q}\) and \(\vec{k}\). Turn the structure's panel over to them (where \(\vec{Q}\) or \(\vec{k}\) is not 0).

CoTa₃S₆'s Brillouin zones filling the window: a point's card, the key, and the sidebar.
CoTa3S6, a triple-\(\vec{Q}\) order

Display

How the structure is drawn: the sidebar's Display, View, Export Image and Settings.

MnF₂'s Display settings: moments, ligands, polyhedra and bonds.
MnF2