Pressure-Induced Transitions

Updated 31 January 2026

Pressure-induced transitions are material transformations triggered by external pressure that alter structural, electronic, magnetic, and topological properties without introducing disorder.
They enable precise tuning of atomic spacings, bandwidths, and interaction strengths, leading to phenomena such as insulator–metal changes, symmetry breaking, and modified magnetic order.
Advanced high-pressure experiments and ab initio modeling reveal phase diagrams and critical parameters, offering insights for developing quantum materials and novel functional states.

Pressure-induced transitions are transformations in the structural, electronic, magnetic, or topological properties of materials driven by the application of external pressure. These phenomena span a wide range of physical systems, including elemental solids, molecular crystals, correlated oxides, quantum magnets, topological semimetals, and low-dimensional conductors. Pressure acts as a clean, continuous, and controllable thermodynamic variable, enabling the tuning of atomic spacings, electronic bandwidths, and interaction strengths without introducing disorder. This article surveys the microscopic mechanisms, experimental signatures, phase diagrams, and theories underlying pressure-induced transitions, placing emphasis on archetypal case studies from contemporary literature.

1. Mechanisms and Taxonomy of Pressure-Induced Transitions

Pressure modifies the free energy landscape by reducing interatomic distances, thereby changing overlap integrals, bandwidths ( $W$ ), crystal-field splittings ( $\Delta_{\text{CF}}$ ), exchange couplings ( $J$ ), phonon spectra, and spin-orbit coupling. This tuning can trigger several classes of transitions:

Structural transitions: Rearrangement of atomic positions, changes of symmetry, volume collapse, or reorganization of coordination polyhedra. Examples include reconstructive transitions (e.g., from layered to three-dimensional networks) and displacive transitions (e.g., distortion within a given lattice).
Electronic transitions: Insulator–metal transitions (IMT), Lifshitz transitions (Fermi surface topology changes), band inversions, and reentrant semiconducting–metallic sequences. In correlated materials, these can be Mott or charge-transfer in character.
Magnetic transitions: Modifications of long-range order (AFM/FM), quantum spin-state crossovers (high-spin to low-spin), quenching of local moments, and emergent spin-liquid or SRO phases.
Topological transitions: Changes in bulk band topology, characterized by invariant jumps (e.g., $Z_2$ , mirror Chern number), resulting in protected surface or edge states.
Superconducting transitions: Either direct onset (e.g., via enhancement of electron-phonon coupling) or suppression (e.g., by structural collapse or competing ordering).
Mixed or crossover regimes: Crossover between different dimensionalities, mixed spin or phase fractions, and coexistence of multiple electronic and/or magnetic orders.

Pressure-tuned transitions can be first-order (discontinuous in order parameter/volume), second-order (continuous), or manifest as crossover phenomena that do not involve breaking of symmetry but significant changes to electronic or lattice character.

2. Structural Transitions and Symmetry Breaking

Many pressure-driven transitions are primarily structural, characterized by abrupt or continuous changes in symmetry, lattice constants, or atomic arrangements. Key findings from several systems include:

Binary/ternary oxides and chalcogenides: Cd $_2$ V $_2$ O $_7$ undergoes a sequence of monoclinic ( $\beta$ ) $\rightarrow$ triclinic ( $y$ ) at $\Delta_{\text{CF}}$ 0 GPa, followed by cubic pyrochlore-type ( $\Delta_{\text{CF}}$ 1) at $\Delta_{\text{CF}}$ 2 GPa, involving substantial polyhedral reorganization and coordination increase from 6 (Cd) and 4 (V) to 8 (Cd) and 6 (V) (Diaz-Anichtchenko et al., 2022). TiOCl transitions from orthorhombic (Pmmn) to a 2 $\Delta_{\text{CF}}$ 3%%%%14 $J$ 15%%%% $\Delta_{\text{CF}}$ 6 $\Delta_{\text{CF}}$ 7 monoclinic (P2 $\Delta_{\text{CF}}$ 8/m) superstructure at $\Delta_{\text{CF}}$ 9 GPa, signaling a Peierls-like dimerization and dimensionality change, with a further high-pressure phase at $J$ 0 GPa (Ebad-Allah et al., 2010).
Van der Waals and quasi-1D materials: Li $J$ 1Mo $J$ 2O $J$ 3 transitions from strictly quasi-1D (P2 $J$ 4/m) to 3D-connected structural motifs via P2 $J$ 5/a at $J$ 6 GPa and further transformation near $J$ 7 GPa; these transitions are marked by abrupt volume collapse and new interlayer bond formation (Tran et al., 2021).
Complex oxides and double perovskites: La $J$ 8CoTiO $J$ 9 features pressure-induced transitions in the monoclinic phase, governed by octahedral volume "breathing" and eventually full quench of the Co moment at high pressure (Nandi et al., 2023).

These transitions are typically tracked by high-pressure synchrotron x-ray diffraction, sometimes accompanied by large changes in cell volume ( $Z_2$ 0), discontinuities or kinks in compressibility, and the appearance/disappearance of superlattice reflections.

3. Electronic and Correlated-Electron Transitions

Pressure strongly affects electronic structure, bandwidths, and interactions, and thus can induce (or suppress) insulating, metallic, and superconducting states.

Mott and correlated band insulators: FePS $Z_2$ 1 remains a Mott insulator up to $Z_2$ 2 GPa, then undergoes a sequence LP $Z_2$ 3 HP-I $Z_2$ 4 HP-II $Z_2$ 5 HP-II- $Z_2$ 6 between 4--10 GPa. The final phase is a fully 3D-connected, orbital-mixed correlated metal (Deng et al., 2022). Samarium monochalcogenides, prototypically SmS, exhibit isostructural insulator–metal transitions with first-order (SmS) or continuous character (SmSe, SmTe), governed by sharp 4 $Z_2$ 7 resonance crossings with the Fermi level. DFT+DMFT reveals intermediate valence states and a direct band insulator to metal transition without a Mott-divergence of $Z_2$ 8 (Banerjee et al., 2021).
Lifshitz and band topology transitions: ZrTe $Z_2$ 9 traverses a Lifshitz transition at $_2$ 0 GPa, with a Fermi-surface pocket closing and carrier-type reversal. Fermi surface evolution is linked to density-of-states peaks and the emergence of superconductivity. Pressure-controlled changes in $_2$ 1 (extremal FS cross-section) and diverging $_2$ 2 serve as microscopic signatures (Zhu et al., 2023).
Metallization in elemental and low-dimensional systems: Black arsenic (b-As) transforms from a semiconducting orthorhombic phase to metallic gray arsenic at $_2$ 3 GPa, with onset of superconductivity above $_2$ 4 GPa (c-As), and further $_2$ 5 enhancement in the incommensurate host–guest phase above $_2$ 6 GPa (Wu et al., 4 Feb 2025).
Superconductor-insulator transitions and anomalous metals: Amorphous InO thin films under pressure exhibit a sequence—Bose insulator $_2$ 7 superconductor $_2$ 8 low and high-resistance anomalous metallic states $_2$ 9 Anderson (fermionic) insulator. These transitions are governed by Josephson inter-island coupling, local gap suppression, and emergent granularity, with critical pressures at $_2$ 0, $_2$ 1, $_2$ 2, $_2$ 3 GPa (Song et al., 6 Apr 2025).

4. Magnetic and Spin-State Transitions

Pressure generically alters superexchange pathways, crystal-field environments, and exchange energies, leading to changes in magnetic order and spin states.

Rare-earth and double perovskite systems: La $_2$ 4CoTiO $_2$ 5 displays a high-spin to low-spin transition at $_2$ 6 GPa, tracked by a sharp drop in Co–octahedral volume ratio and a collapse of magnetic moment, leading to an AFM-insulator $_2$ 7 AFM-metal $_2$ 8 NM-metal progression (Nandi et al., 2023).
Low-dimensional magnets and multiferroics: In Tb $_2$ 9BaNiO $_7$ 0, pressure shifts the Néel temperature $_7$ 1 upward ( $_7$ 2 K/GPa), but suppresses the canting-driven ferroelectric $_7$ 3 ( $_7$ 4 K/GPa), owing to strengthening of superexchange and simultaneous stiffening of polar lattice distortions (Iyer et al., 2021).
Spin-crossover compounds and elastic interactions: In compounds such as [Fe(Fpz) $_7$ 5M(CN) $_7$ 6], pressure-induced spin transitions exhibit gradual, mixed high-spin and low-spin states due to elastic inhomogeneities and internal pressure associated with different compressibilities (quantified by volume strain $_7$ 7), in contrast to the abrupt temperature-induced transition at ambient pressure (Li et al., 2022).

5. Topological and Quantum Phase Transitions

External pressure can modulate band inversion, open or close gaps, and change topological quantum numbers, enabling access to new quantum phases.

Topological insulators with strong correlations: YbB $_7$ 8 provides a canonical pressure-driven sequence: topological insulator–metal–topologically distinct insulating phase. Low-pressure TI-1 arises from d–p inversion ( $_7$ 9 via BHZ model), while high-pressure TI-2 is driven by d–f inversion, with a metallic window (and valence change) between the two (Zhou et al., 2015).
Topological crystalline insulators: Rock-salt IV–VI chalcogenides (PbTe, PbSe, PbS) transition from trivial to TCI phases for $\beta$ 0–5 GPa, when asymmetric cation–anion $\beta$ 1 hybridization inverts the band gap at the L point. The formation of a non-zero mirror Chern number $\beta$ 2 yields Dirac surface states protected by lattice mirror symmetry (Barone et al., 2013).
Layered antiferromagnetic TIs: In MnBi $\beta$ 3Te $\beta$ 4 and MnBi $\beta$ 5Te $\beta$ 6, pressure drives suppression of antiferromagnetism at $\beta$ 79–10 GPa, induces metal–semiconductor–metal sequences (in MnBi $\beta$ 8Te $\beta$ 9), and leads to amorphization (MnBi $\rightarrow$ 0Te $\rightarrow$ 1) or successive symmetry-lowering transitions (MnBi $\rightarrow$ 2Te $\rightarrow$ 3). Surface and bulk states respond differently, with non-monotonic resistivity as a function of pressure due to competition between localization and hybridization (Pei et al., 2020).
Topological semimetals and nodal-line systems: In ZrTe $\rightarrow$ 4, pressure gives rise to a sequence of topological transitions characterized by parity-based $\rightarrow$ 5 index changes. Notably, superconductivity and nontrivial topology coexist in a finite pressure window ( $\rightarrow$ 6– $\rightarrow$ 7 GPa), making ZrTe $\rightarrow$ 8 a candidate for topological superconductivity (Zhu et al., 2023). Optical measurements in ZrSiTe resolve Lifshitz-like transitions via discontinuities in plasma frequency and interband transitions at $\rightarrow$ 9 GPa and $y$ 0 GPa (Ebad-Allah et al., 2019).

6. Experimental Techniques and Computational Approaches

The characterization and understanding of pressure-induced transitions require integration of advanced methods:

High-pressure experimental probes: Synchrotron x-ray diffraction (with DACs and hydrostatic PTMs), Raman and infrared spectroscopy (with spectral tracking of phonons/modes and free-carrier response), four-probe electrical transport (for resistive transitions and Hall effect), magnetization under pressure, and x-ray absorption spectroscopy (valence tracking).
Ab initio modeling: DFT (GGA, hybrid, + $y$ 1), DMFT (capturing intermediate valence and correlated electron phenomena), random structure search, maximally localized Wannier functions for topology, Berry phase, and enthalpy/volume equations of state (3rd-order Birch–Murnaghan and related forms).
Transition path analysis: Nudged elastic band (NEB, SS-NEB) calculations and molecular dynamics, for mapping atomic-scale structural transformation paths and kinetic barriers, including stress dependence and nucleation rates.

Tables of transition pressures, lattice parameters, and critical temperatures are widely used to summarize phase diagrams, with LaTeX-formulated equations for state equations or fitting routines.

7. Unified View and Cross-material Trends

Pressure-induced transitions reflect deep, unifying principles of energy minimization, electron–lattice coupling, and symmetry constraints:

System/Phenomenon	Transition(s) and P (GPa)	Key Mechanisms
ZrTe $y$ 2 (Zhu et al., 2023)	Lifshitz ( $y$ 311), SC dome (8–60), topo QPTs (2,50)	FS topology, band inversion, DFT+SOC
Black As (Wu et al., 4 Feb 2025)	b-As $y$ 4g-As (1.5), g $y$ 5c-As (25.9), c $y$ 6hg-As (44.8), $y$ 7 jumps	Entropy minimization, phonon DOS, electron-phonon
SmS (Banerjee et al., 2021)	Insulator $y$ 8Metal ( $y$ 9), first-order	Intermediate valence, 4 $\Delta_{\text{CF}}$ 00 hybridization, DMFT
Li $\Delta_{\text{CF}}$ 01Mo $\Delta_{\text{CF}}$ 02O $\Delta_{\text{CF}}$ 03 (Tran et al., 2021)	1D $\Delta_{\text{CF}}$ 043D crossover (3.6,6)	Dimensionality, orbital overlap
MnBi $\Delta_{\text{CF}}$ 05Te $\Delta_{\text{CF}}$ 06 (Pei et al., 2020)	AFM $\Delta_{\text{CF}}$ 07PM (9.3), M–S–M, amorphization (17.4)	Bond angles, bulk vs. surface gap, DFT+U, Raman/XRD
Ba(Fe $\Delta_{\text{CF}}$ 08Ru $\Delta_{\text{CF}}$ 09) $\Delta_{\text{CF}}$ 10As $\Delta_{\text{CF}}$ 11 (Uhoya et al., 2013)	SC dome (3.9–11.5), collapsed T (14)	As–As bonding, negative $\Delta_{\text{CF}}$ 12-axis compressibility
(Ph $\Delta_{\text{CF}}$ 13P) $\Delta_{\text{CF}}$ 14IC $\Delta_{\text{CF}}$ 15 (Francis et al., 2012)	Dynamic $\Delta_{\text{CF}}$ 16Static JT ( $\Delta_{\text{CF}}$ 172)	Vibronic coupling, steric crowding, IR
La $\Delta_{\text{CF}}$ 18CoTiO $\Delta_{\text{CF}}$ 19 (Nandi et al., 2023)	AFM-I $\Delta_{\text{CF}}$ 20AFM-M (42), $\Delta_{\text{CF}}$ 21NM (130)	Breathing mode, spin-state switch

Notably, pressure enables reversible exploration of complex phase diagrams, decouples lattice from chemical effects, and often reveals phase competition, criticality, coexistence phenomena, and pathways to novel quantum states unavailable at ambient conditions.

References

ZrTe $\Delta_{\text{CF}}$ 22 superconductivity and topology: (Zhu et al., 2023)
Black As structural and SC transitions: (Wu et al., 4 Feb 2025)
SmX isostructural MIT: (Banerjee et al., 2021)
MnBi $\Delta_{\text{CF}}$ 23Te $\Delta_{\text{CF}}$ 24 and MnBi $\Delta_{\text{CF}}$ 25Te $\Delta_{\text{CF}}$ 26 MTIs: (Pei et al., 2020)
Topological phase transitions in chalcogenides: (Barone et al., 2013)
Samarium hexaboride, YbB $\Delta_{\text{CF}}$ 27: (Zhou et al., 2015)
FePS $\Delta_{\text{CF}}$ 28 pressure sequence: (Deng et al., 2022)
Li $\Delta_{\text{CF}}$ 29Mo $\Delta_{\text{CF}}$ 30O $\Delta_{\text{CF}}$ 31 dimensional crossover: (Tran et al., 2021)
AgClO $\Delta_{\text{CF}}$ 32: (Errandonea et al., 2012)
Cd $\Delta_{\text{CF}}$ 33V $\Delta_{\text{CF}}$ 34O $\Delta_{\text{CF}}$ 35: (Diaz-Anichtchenko et al., 2022)
(Ph $\Delta_{\text{CF}}$ 36P) $\Delta_{\text{CF}}$ 37IC $\Delta_{\text{CF}}$ 38 JT effect: (Francis et al., 2012)
Pressure-induced spin-crossover with elastic interactions: (Li et al., 2022)
Ba(Fe $\Delta_{\text{CF}}$ 39Ru $\Delta_{\text{CF}}$ 40) $\Delta_{\text{CF}}$ 41As $\Delta_{\text{CF}}$ 42 SC and T $\Delta_{\text{CF}}$ 43cT: (Uhoya et al., 2013)
Tb $\Delta_{\text{CF}}$ 44BaNiO $\Delta_{\text{CF}}$ 45 multiferroic: (Iyer et al., 2021)
ZrSiTe optical transitions: (Ebad-Allah et al., 2019)
Si phase transformations: (Rovaris et al., 2024)
Anomalous metal near SIT: (Song et al., 6 Apr 2025)

The breadth of pressure-induced transitions continues to expand, with ongoing advances in multianvil synthesis, in situ measurements, and first-principles computations enabling the discovery and control of emergent quantum phases across materials classes.