Spin-flop and metamagnetic transitions

Experiment track

In plain words

Sudden rearrangements of the atomic magnets in an as a magnetic field is turned up. In an antiferromagnet neighbouring point opposite ways, so a field along them has nothing to pull on – until, at a threshold, they give way. If they are only loosely tied to their axis, they swing round to lie across the field and tilt towards it: a spin flop. If they are firmly tied, those pointing against the field turn over all at once and the magnet becomes, in effect, a ferromagnet: a metamagnetic transition. In layered antiferromagnets the layers are only weakly coupled, so this happens in modest fields, often layer by layer.

As the site uses it

Kerr microscopy sees net magnetisation only in odd layer numbers; even ones need spin-flop signatures or tunnelling magnetoresistance.

CrPS4 · Chromium thiophosphate

Going deeper

Three panels. No field: four moments alternating up and down. A spin flop: with a field B pointing up, the moments lie almost across the field, alternating left and right, each tilted slightly towards the field. A spin flip: with the field up, all four moments point up, the two that were opposed marked as turned over. no field neighbours opposite: no net pull a field along the moments finds them balanced the antiferromagnet at rest a spin flop B moments swing across the field weak anisotropy: they flop, then tilt towards the field spin flop a spin flip B turned over the opposed moments turn over strong anisotropy: all at once, a ferromagnet in effect metamagnetic transition
A field along the moments of an antiferromagnet finds them balanced. With weak anisotropy they flop across the field and then tilt towards it; with strong anisotropy the opposed moments turn over all at once – a metamagnetic transition. Layered antiferromagnets, weakly coupled between layers, do this in modest fields.

Pushing on an antiferromagnet

A field along the moments of an antiferromagnet finds them balanced: half point along it, half against, and the net moment is zero. As the field grows, the magnet can lower its energy by turning its moments so that part of their magnetisation lines up with the field, and it does so suddenly once the gain beats the cost.

The cost depends on two things: the exchange that keeps neighbours antiparallel and the that ties each moment to its axis. With weak anisotropy the moments swing round to lie perpendicular to the field – the spin flop – and then tilt towards it as the field grows, until all point along it. With strong, anisotropy they cannot leave their axis, and the moments pointing against the field turn over all at once – a metamagnetic, or -flip, transition.

Layered antiferromagnets

Many layered magnets are ferromagnetic within each layer and antiferromagnetic from one layer to the next, with the coupling between layers far weaker than within them, so fields of a tesla or less can reorganise them. CrPS4, whose chromium moments point out of the layers, flops in an out-of-plane field below 1 T, and on powder samples followed its magnetic structure through the flop (Calder and colleagues, 2020). In MnBi2Te4 the resistance drops as the field carries the crystal across its metamagnetic transition (Yan and colleagues, 2019), and the antiferromagnet CeSiI shows metamagnetic steps near 2.5 and 4.5 T at 2 K, nearly the same in from two to fifteen layers thick.

In thin flakes the count of layers matters. An odd number leaves one layer uncompensated, so thin CrPS4 alternates between ferromagnetic odd and antiferromagnetic even layer counts (Son and colleagues, 2021), and a field turns layers over one at a time.

Reading it out

A single flake holds too little magnetic material for a , so these transitions are read through light or current. Kerr microscopy sees the net magnetisation jump; a current across a antiferromagnet changes with every layer that turns, because each layer favours electrons of one spin. In multilayer CrPS4, under in-plane and out-of-plane fields followed a spin reorientation that differs with the number of layers, matched by a model of coupled layers as a linear chain (Tian and colleagues, 2025).

For specialists

Field-driven transitions of an antiferromagnet with the field along its easy axis. When the anisotropy is weak compared with the exchange, the sublattices flop perpendicular to the field at the spin-flop field and then cant progressively to saturation; when it is strong, the antiparallel sublattice reverses abruptly – a metamagnetic, or spin-flip, transition. In layered antiferromagnets the relevant exchange is the weak : CrPS4 flops in an out-of-plane field below 1 T, MnBi2Te4 crosses a metamagnetic transition with a drop in resistance, and CeSiI shows metamagnetic steps near 2.5 and 4.5 T at 2 K in flakes of every thickness; in few-layer flakes the transitions proceed layer by layer, as tunnelling magnetoresistance shows.

Where this comes from

  1. Magnetic structure and exchange interactions in the layered semiconductor CrPS4 Calder et al. · Physical Review B 102, 024408 (2020) cited by 68
  2. Air-stable and layer-dependent ferromagnetism in atomically thin van der Waals CrPS4 Son et al. · ACS Nano 15, 16904 (2021) cited by 110
  3. Crystal growth and magnetic structure of MnBi2Te4 Yan et al. · Physical Review Materials 3, 064202 (2019)
  4. Glassy relaxation dynamics in the two-dimensional heavy fermion antiferromagnet CeSiI Torres et al. · Nano Letters 25, 6848 (2025) cited by 3
  5. Layer-dependent metamagnetic transitions in van der Waals antiferromagnet CrPS4 Tian et al. · Applied Physics Letters 127, 062403 (2025)

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