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A laser-driven martensitic transformation in a specific Ni-Mn-Ga-based epitaxial thin film took about 100 picoseconds from martensite to austenite, while a nearly complete forward-and-reverse cycle finished within 5 nanoseconds. The 100 ps figure is limited by the duration of the synchrotron probe pulse, so it is not a precisely resolved intrinsic speed or a universal limit for martensitic alloys.

What the study measured

Yuru Ge and colleagues used synchrotron time-resolved X-ray diffraction to follow a structural phase change in a Ni-Mn-Ga-based epitaxial thin film after ultrashort laser excitation. In martensite, the material has a distorted crystal structure; austenite is the higher-temperature phase toward which the film transformed after excitation. Diffraction lets researchers track changes in crystal structure over time rather than infer a transformation solely from a temperature reading.

The study was posted as a preprint on September 8, 2025, under the title “Sub-nanosecond structural dynamics of the martensitic transformation in Ni-Mn-Ga.” Its headline times are author-reported results for this film and experiment, not independently replicated values established by the sources available here.

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How to interpret the reported times

Reported interval What it describes Important qualification
270 fs Duration of the laser excitation pulse used to initiate the dynamics. This is the pump pulse duration, not the measured duration of the phase transformation.
About 100 ps Martensite-to-austenite transformation. The observed timescale is limited by the synchrotron probe-pulse duration; the experiment therefore does not precisely resolve the transformation’s intrinsic duration.
Within 5 ns A nearly complete martensite-to-austenite-to-martensite cycle. This is the reported cycle time under the study’s conditions, not a general performance figure for other alloys or devices.

The authors described the cycle as the fastest martensitic transformation reported at the time of their preprint. That wording is time-bound and specific to the report; it should not be read as proof that all martensitic materials can switch at the same rate.

Why temperature alone does not explain the response

Laser energy changes the film’s temperature, and the authors measured and calculated its temperature evolution to interpret the structural response. They also measured time-resolved strain. Those measurements led them to conclude that thermal film stress must be considered alongside temperature as a competing influence on the transformation. In practical terms, a temperature trace alone is not a complete account of what drives or constrains the changing crystal structure in this thin-film experiment.

What the simulations suggest about the delay

The team used molecular-dynamics simulations with machine-learned force fields adapted to density-functional-theory calculations. In those simulations, substantial structural distortion required coordinated motion by many atoms in the microstructure. The authors propose that this collective rearrangement delays completion of the transformation. This is a simulation-supported interpretation of the observed dynamics, not a mechanism established for every martensitic alloy.

What can—and cannot—be compared with other studies

A transformation time is meaningful only alongside the measurement and sample conditions that define it. In particular, comparisons should distinguish a one-way martensite-to-austenite transition from a complete reversible cycle, and should account for whether the reported timing is limited by the probe.

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  • Measurement: which structural observable was tracked, and what the probe-pulse duration and time resolution were.
  • Excitation: the pump-pulse duration and fluence.
  • Specimen: composition, film thickness, substrate and buffer architecture, and thermal history.
  • Thermal and mechanical conditions: how temperature was estimated and whether strain or stress was measured or constrained.
  • Transformation interval: whether the number describes the forward transition alone or a nearly complete forward-and-reverse cycle.

The study’s conference listing at the 2025 Materials Research Society Fall Meeting also restated the headline times, but that listing is not an independent experimental confirmation.

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Where to find the data and code

The associated HZDR RODARE “Data and code publication” record provides the paper’s raw data and code. The record is DOI 10.14278/rodare.4112, was published on November 13, 2025, and notes a newer version dated May 12, 2026. These artifacts let readers consult the materials associated with the study; their availability does not by itself establish independent replication.

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