AIエージェントが新材料探索を加速(Scientists deploy AI agents to accelerate discovery of new materials)

2026-08-06 アルゴンヌ国立研究所(ANL)

米国アルゴンヌ国立研究所(ANL)の研究チームは、複数のAIエージェントとスーパーコンピュータを連携させた新たな材料探索基盤を開発し、新材料の発見を大幅に効率化する取り組みを発表した。開発されたフレームワーク「ChemGraph」は、大規模言語モデル(LLM)を活用した複数の専門AIエージェントが連携し、計算条件の設定、シミュレーション実行、結果解析、データ整理までの一連のワークフローを自動化する。従来は専門知識と多くの手作業を要した第一原理計算や分子動力学計算を容易に実行できるため、研究者は材料設計や仮説立案に集中できる。さらに、高性能計算機「Aurora」とAI推論サービスを組み合わせることで、大規模かつ複雑な材料探索を高速化し、電池、触媒、半導体など幅広い分野で革新的材料の発見期間短縮が期待される。本成果は、AIを研究支援ツールから自律的な研究パートナーへ発展させる重要な一歩と位置付けられている。

AIエージェントが新材料探索を加速(Scientists deploy AI agents to accelerate discovery of new materials)
Argonne researchers developed a system that uses multiple AI agents to automate atomistic simulations from start to finish. An administrator agent orchestrates the overall workflow, assigning tasks to a series of specialist agents. (Image by Argonne National Laboratory.)

<関連情報>

エンドツーエンドの原子シミュレーションのためのマルチエージェントAIフレームワーク Multi-agentic AI framework for end-to-end atomistic simulations

Aikaterini Vriza;Uma Kornu;Aditya Koneru;Henry Chan;Subramanian K. R. S. Sankaranarayanan
Digital Discovery  Published:09 December 2025
DOI:https://doi.org/10.1039/d5dd00435g

One of the main bottlenecks for the wide adoption of atomistic simulation pipelines for computational materials design is the high complexity of the workflows which many times requires the use of a diverse set of specialized toolkits and libraries. Here, we introduce a multi-agent artificial intelligence (AI) framework that autonomously performs end-to-end atomistic simulations, i.e. molecular dynamics (MD), with automated input and associated full suite of analyses, using large language models (LLMs) and multiple specialized AI agents. Our system orchestrates the entire simulation pipeline, from structure generation via Atomsk and interatomic potential discovery through automated web mining, to simulation setup and execution using LAMMPS on high-performance computing (HPC) platforms. Post-simulation, our agentic framework performs automated data analysis and visualization with popular analysis tools like OVITO and Phonopy. Each expert agent operates within a defined role, equipped with domain-specific functions and a shared memory context for coordination. Using a diverse set of representative elemental and alloy systems, we demonstrate the capability of our framework to execute a range of static and dynamic materials modeling tasks, including lattice parameter and cohesive energy estimation, elastic constants computation, phonon dispersion analysis, as well as perform MD simulations to determine dynamical properties that aid estimation of melting point. The results produced by the agents show strong agreement with those obtained by a human expert, highlighting the reliability of the agentic approach. By combining automation, reproducibility, and human-in-the-loop control, our framework lowers the barrier to the widespread adoption of scalable, AI-driven discovery tools in materials science.


液体アルゴン中の原子の運動における相関関係 Correlations in the Motion of Atoms in Liquid Argon

A. Rahman
Physical Review Journals Archive  Published :19 October, 1964
DOI: https://doi.org/10.1103/PhysRev.136.A405

Abstract

A system of 864 particles interacting with a Lennard-Jones potential and obeying classical equations of motion has been studied on a digital computer (CDC 3600) to simulate molecular dynamics in liquid argon at 94.4°K and a density of 1.374 g cm−3. The pair-correlation function and the constant of self-diffusion are found to agree well with experiment; the latter is 15% lower than the experimental value. The spectrum of the velocity autocorrelation function shows a broad maximum in the frequency region ω=0.25⁢(KBT⁢/h). The shape of the Van Hove function Gs⁡(r, t) attains a maximum departure from a Gaussian at about =3.0 ×10−12 sec and becomes a Gaussian again at about 10−11 sec. The Van Hove function Gd⁡(r, t) has been compared with the convolution approximation of Vineyard, showing that this approximation gives a too rapid decay of Gd⁡(r, t) with time. A delayed-convolution approximation has been suggested which gives a better fit with Gd⁡(r, t); this delayed convolution makes Gd⁡(r, t) decay as t4 at short times and as at long times.

1603情報システム・データ工学
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