task_id stringlengths 14 75 | capability stringclasses 9
values | domain stringclasses 6
values | prompt stringlengths 21 3.08k | tags listlengths 0 3 | data_files listlengths 0 12 |
|---|---|---|---|---|---|
IG_incar_008_20260506 | input_generation | agnostic | 为钙钛矿 BaZrO3 生成一个弹性常数计算的 VASP INCAR。使用有限差分法计算弹性张量,位移幅度 0.015 A。将完整的 INCAR 写入当前目录下的 `INCAR` 文件。 | [
"eng_vasp"
] | [] |
IG_incar_009_20260506 | input_generation | agnostic | 为有机金属氧化物 C8H12HfO4 生成一个 DFPT(密度泛函微扰理论) 介电常数计算的 VASP INCAR。需要计算介电张量和 Born 有效电荷。 将完整的 INCAR 写入当前目录下的 `INCAR` 文件。 | [
"eng_vasp"
] | [] |
IG_incar_010_20260528 | input_generation | agnostic | 为含重元素 Pb 的卤化物 Br6H6Pb2S2 生成一个 自旋轨道耦合(SOC)计算的 VASP INCAR。Pb 的 SOC 效应显著,需要高精度设置。 将完整的 INCAR 写入当前目录下的 `INCAR` 文件。 | [
"eng_vasp"
] | [] |
IG_incar_011_20260506 | input_generation | agnostic | 为三元金属间化合物 CdOs3Pt 生成一个 高精度态密度(DOS)计算的 VASP INCAR。体系为磁性金属,需要投影态密度(PDOS)。 将完整的 INCAR 写入当前目录下的 `INCAR` 文件。 | [
"eng_vasp"
] | [] |
IG_incar_012_20260528 | input_generation | agnostic | 为普鲁士蓝类似物 C24Fe8N24Na4 生成一个 NEB(nudged elastic band)+HSE06 过渡态搜索的 VASP INCAR。将完整的 INCAR 写入当前目录下的 `INCAR` 文件。 | [
"eng_vasp"
] | [] |
IG_incar_013_20260506 | input_generation | agnostic | 为三元碳化物表面 (Ta,V)2C (C33O2Ta16V16) 生成一个表面弛豫计算的 VASP INCAR。表面计算需要固定晶胞形状,体系为金属。将完整的 INCAR 写入当前目录下的 `INCAR` 文件。 | [
"eng_vasp",
"struct_surface"
] | [] |
IG_incar_014_20260523 | input_generation | agnostic | 为氢钝化的 SiO2 slab 模型 H16O24Si12 生成一个静态计算的 VASP INCAR。体系是绝缘体 slab,需要固定晶胞形状。将完整的 INCAR 写入当前目录下的 `INCAR` 文件。 | [
"eng_vasp",
"struct_surface"
] | [] |
IG_incar_015_20260508 | input_generation | agnostic | 为 BiSI 中 I 替位 S 缺陷体系生成一个 HSE06+SOC 缺陷计算的 VASP INCAR。含重元素 Bi 需要自旋轨道耦合,缺陷计算需要固定晶胞形状,使用 HSE06 获取准确缺陷能级。需要离子弛豫。将完整的 INCAR 写入当前目录下的 `INCAR` 文件。 | [
"eng_vasp"
] | [] |
IG_incar_016_20260507 | input_generation | agnostic | 为稀土硒化物 DySe 生成一个 GW 计算前驱步骤的 SCF VASP INCAR。Dy 含 f 电子(MAGMOM~7),需要保存高质量波函数供后续 GW 使用。 将完整的 INCAR 写入当前目录下的 `INCAR` 文件。 | [
"eng_vasp"
] | [] |
IG_incar_017_20260506 | input_generation | agnostic | 为简单金属 Al (FCC) 生成一个高精度结构优化的 VASP INCAR,作为后续光学计算的前驱步骤。需要高精度设置和完全优化晶胞参数。将完整的 INCAR 写入当前目录下的 `INCAR` 文件。 | [
"eng_vasp"
] | [] |
IG_incar_018_20260508 | input_generation | agnostic | 为双钙钛矿 Ca4TaOs 生成一个磁性自洽(SCF)计算的 VASP INCAR。体系含 5d 过渡金属(Ta, Os),需要自旋极化和适当的初始磁矩。将完整的 INCAR 写入当前目录下的 `INCAR` 文件。 | [
"eng_vasp"
] | [] |
IG_incar_019_20260508 | input_generation | agnostic | 为硼酸铯 B12Cs4O20 生成一个非磁性绝缘体的静态 SCF 计算 VASP INCAR。体系为非磁性,宽带隙绝缘体。将完整的 INCAR 写入当前目录下的 `INCAR` 文件。 | [
"eng_vasp"
] | [] |
IG_incar_020_20260507 | input_generation | agnostic | 为三元硒化物 Na3AlSe 生成一个磁性金属体系的静态 SCF 计算 VASP INCAR。体系为磁性金属,需要投影态密度。将完整的 INCAR 写入当前目录下的 `INCAR` 文件。 | [
"eng_vasp"
] | [] |
IG_lammps_001_20250618 | input_generation | agnostic | Generate a LAMMPS input script for a two-phase coexistence MD simulation to predict the melting temperature of Ni at standard pressure. Retrieve the FCC Ni conventional unit cell (Materials Project mp-134) from the structure database and use it to build a 14x14x28 supercell. Initialize the lower half as liquid (heated ... | [
"eng_lammps"
] | [] |
IG_lammps_001_20260428 | input_generation | agnostic | 请为一个 FCC 铜体系生成 LAMMPS 分子动力学输入文件,要求:
1. 使用 EAM 势(Cu_u3.eam),晶格常数 3.615 Å
2. 3×3×3 超胞
3. NPT 系综,温度 300 K,压力 0 bar
4. 运行 10000 步,时间步长 1 fs
5. 每 100 步输出热力学信息
输出文件名为 `in.lammps`。 | [
"eng_lammps"
] | [] |
IG_lammps_004_20250618 | input_generation | agnostic | Generate a LAMMPS input script for a two-phase coexistence MD simulation of Ni at 10 GPa external pressure. Retrieve the FCC Ni conventional unit cell from the structure database and use it to build a 14x14x28 supercell. Set up NPH ensemble with external pressure of 10 GPa, 1 fs timestep, and 120 ps production run. Sav... | [
"eng_lammps"
] | [] |
IG_lammps_deepmd_typemap_001_20260607 | input_generation | agnostic | 为含能材料 EAP(乙二胺高氯酸盐,化学式 C₂H₁₂N₂Cl₂O₈,包含 H/C/N/O/Cl 五种元素)写一个 LAMMPS DeePMD 分子动力学输入脚本。模型文件为 `model.pb`(全周期表 118元素type_map)。体系232原子,2500K NVT模拟100ps,时间步0.1fs。输出 `in.lammps`。
| [
"eng_lammps",
"code_mlip"
] | [] |
IG_lammps_eap_deepmd_preflight_001_20260602 | input_generation | agnostic | 工作区中有 `eap_model_notes.txt`,记录了 EAP(乙二胺高氯酸盐)232 原子 DeePMD 高温 MD 的体系和模型信息。请生成 LAMMPS 输入文件,不需要真实运行。
要求:
- 2500 K NVT,100 ps,时间步 0.1 fs;
- DeePMD 模型文件是 `iter23_0.pb`;
- data 文件的原子类型顺序是 H C N O Cl;
- 输出 `in.eap_deepmd` 和 `run.sh`。
| [
"eng_lammps",
"code_mlip"
] | [
{
"key": "eap_model_notes",
"path": "fixtures/IG_lammps_eap_deepmd_preflight_001_20260602/eap_model_notes.txt",
"source_url": "",
"size_bytes": 279,
"sha256": "8b2a348f0587526d6a22b365a703c59f89f0cbb0025dcbaded1ea429db80b574",
"distribution": "bundled",
"available_in_repo": true
}
] |
IG_lammps_gaff_001_20260518v2 | input_generation | agnostic | 工作区中有一个 20 重复单元的聚乙烯链结构 `polyethylene.xyz`。请使用 GAFF 力场为该体系准备 LAMMPS 结构优化输入,输出 `in.lammps` 和 `data.lammps`。 | [
"eng_lammps"
] | [
{
"key": "pe_xyz",
"path": "fixtures/IG_lammps_gaff_001/polyethylene.xyz",
"source_url": "",
"size_bytes": 6635,
"sha256": "9f38bb171f6b881608860bc87705da277b655e644aa9452ffb25f5af530c04b9",
"distribution": "bundled",
"available_in_repo": true
}
] |
IG_lammps_sgcmc_001_20260523 | input_generation | agnostic | 请生成一个 LAMMPS 输入脚本,使用 `fix sgcmc` 研究 BCC Fe-10at%Cu 合金在 800K 下的短程有序(SRO)。要求:4x4x4 BCC 超胞(128原子),EAM 势,每100 MD 步尝试一次 MC swap,运行 50000 步。输出到 `in.sgcmc`。
| [
"eng_lammps"
] | [] |
IG_lammps_tensile_bond_001_20260525 | input_generation | agnostic | 生成 LAMMPS 输入文件,对 FCC Cu 单晶进行 z 方向单轴拉伸模拟,并追踪拉伸过程中键长和键角的演化。
要求:
- EAM 势
- 300K NVT 平衡后施加应变
- 输出键长分布和键角分布随应变的变化数据
- 输出为 `in.tensile_cu`
| [
"eng_lammps"
] | [] |
IG_matgl_001_20250624 | input_generation | agnostic | Generate a complete M3GNet model configuration JSON file named `m3gnet_form_energy_config.json` for training a formation energy (eV/atom) property prediction model on bulk crystals. Use the hyperparameters from the MatGL paper (Table S4) for the Matbench formation energy model. The configuration must be valid JSON with... | [
"code_mlip"
] | [] |
IG_matgl_002_20250624 | input_generation | agnostic | Generate a complete CHGNet model configuration JSON file named `chgnet_mlip_config.json` for training a universal machine learning interatomic potential (MLIP) on crystal structures. Use the hyperparameters from the MatGL paper (Table S7). The configuration must be valid JSON with the `@class`, `@module`, `@model_versi... | [
"code_mlip"
] | [] |
IG_nep_001_20260428 | input_generation | agnostic | 目录里有一份 NEP 训练数据 `train.xyz`。
请先看数据,再给出可直接训练的 `nep.in`。
要求:
- `type` 与数据中的元素一致;
- 参数不要照抄模板,要和这份数据规模匹配;
- 不要写超出 NEP 合法范围的值。
同时写一份简短说明,说明你怎么定的关键参数。
输出到当前目录:`nep.in`、`nep_input_note.md`。 | [
"eng_gpumd"
] | [
{
"key": "train_xyz",
"path": "fixtures/IG_nep_001_20260428/train.xyz",
"source_url": "",
"size_bytes": 557,
"sha256": "622628a00b8268ec047f61071d276c26f0a6a2366293b568faf64b81c622eed4",
"distribution": "bundled",
"available_in_repo": true
},
{
"key": "test_xyz",
"path": "fix... |
IG_nernst_002_20260108 | input_generation | battery | Implement the Nernst equation to compute the effective electrochemical redox potential of the H₅IO₆/HIO₃ redox couple (E° = 1.626 V) as a function of pH, following the methodology described in Wang et al. (2024) for the LiIn(IO₃)₄ aqueous synthesis system. The half-reaction is H₅IO₆ + H⁺ + 2e⁻ → HIO₃ + 3H₂O. Write a Py... | [
"char_electrochem"
] | [] |
IG_orca_001_20260522 | input_generation | agnostic | 工作区中有 `molecules.csv`,包含 5 个小分子的 SMILES。请用 ORCA 量化计算估算这些分子的 Hansen 溶解度参数(δD, δP, δH),生成可直接提交的输入文件。
要求使用 B3LYP/def2-TZVP 级别。 | [
"eng_orca"
] | [
{
"key": "molecules_csv",
"path": "fixtures/IG_orca_001/molecules.csv",
"source_url": "",
"size_bytes": 138,
"sha256": "4ebe045696d83cc05d38bdd011f94ed9078250d2e696eb733ddda073a4ed8bee",
"distribution": "bundled",
"available_in_repo": true
}
] |
IG_orca_002_20260522 | input_generation | agnostic | 请为乙醇分子生成 ORCA 输入文件,计算其红外光谱(振动频率 + IR 强度)。
要求使用 B3LYP/def2-TZVP 级别。输出为 `ethanol_ir.inp`。 | [
"eng_orca"
] | [] |
IG_orca_003_20260525 | input_generation | agnostic | 请为苯甲醛(benzaldehyde)生成 ORCA 输入文件,完成以下两步计算:
1. 几何优化(B3LYP/def2-SVP)
2. 基于优化构型的 TD-DFT 计算(PBE0/def2-SV(P),10 个激发态)
输出两个输入文件 `opt.inp` 和 `tddft.inp`,以及一个 `run.sh` 脚本按顺序执行。
| [
"eng_orca"
] | [] |
IG_pourbaix_formula_003_20260108 | input_generation | battery | Implement the Pourbaix potential formula from Wang et al. (2024) as a Python function. The Pourbaix potential (equation 3 in the paper) is:
Φ̄ = (1/N_M) × [(G − N_O·μ_H₂O) − RT·ln(10)·(2N_O − N_H)·pH − (2N_O − N_H + Q)·E]
where N_M, N_O, N_H are the number of metal, oxygen, and hydrogen atoms; Q is the charge; G is the... | [
"char_electrochem"
] | [] |
IG_pymatgen_001_20260118 | input_generation | agnostic | Generate a Pt(111) surface slab structure using pymatgen. Start from bulk platinum (FCC), create a slab with the (111) Miller index, add a 10 Å vacuum layer, and ensure the slab has symmetric (identical) top and bottom terminations. Save the resulting structure to pt_111_slab.cif in the current working directory. | [
"struct_surface"
] | [] |
IG_pymatgen_002_20260118 | input_generation | agnostic | Generate a Si(111) surface slab from bulk silicon using pymatgen. Use the primitive bulk unit cell, create a slab with the (111) Miller index oriented to expose the non-polar termination (no dangling Si atoms), and add a 10 Å vacuum layer. Save the structure to si_111_slab.cif in the current working directory. | [
"struct_surface"
] | [] |
IG_pyscf_001_20260608 | input_generation | agnostic | 请用 PySCF 为水分子(H 0 0 0; H 0 0 0.96; O 居中,可用合理坐标或直接用 `O 0 0 0; H 0 0 0.96; H 0.93 0 -0.24`)写一个单点 DFT 计算脚本 `run_pyscf.py`,使用 wB97X-D 泛函、def2-TZVP 基组,打印总能量。 | [
"eng_pyscf"
] | [] |
IG_pyscf_002_20260609 | input_generation | agnostic | 请用 PySCF 为甲烷分子 CH4 写一个单点能量计算脚本 `run_pyscf.py`,使用 r2SCAN 泛函(meta-GGA)和 def2-SVP 基组,打印总能量。分子坐标可自行给出合理值。只需写出脚本本身,无需提交或运行。 | [
"eng_pyscf"
] | [] |
IG_pyscf_003_20260609 | input_generation | agnostic | 请用 PySCF 为乙烯分子 C2H4 写一个单点 DFT 脚本 `run_pyscf.py`,使用 M06-2X 泛函、cc-pVDZ 基组,打印总能量。坐标可自行给出合理值。只需写出脚本本身,无需提交或运行。 | [
"eng_pyscf"
] | [] |
IG_pyscf_004_20260609 | input_generation | agnostic | 请用 PySCF 为苯分子 C6H6 写一个单点能量脚本 `run_pyscf.py`。方法上请选用一个 带经验色散校正的范围分离杂化泛函(range-separated hybrid + dispersion),基组用 def2-SVP。 | [
"eng_pyscf"
] | [] |
IG_pyscf_005_20260608 | input_generation | agnostic | 请用 PySCF 为甲醇分子 CH3OH 写一个单点 DFT 脚本 `run_pyscf.py`,使用 wB97X-D3 泛函、def2-TZVP 基组,打印总能量。 | [
"eng_pyscf"
] | [] |
IG_pyscf_006_20260608 | input_generation | agnostic | 请用 PySCF 为甲基自由基 CH3(doublet,单重态以外的开壳层体系)写一个单点 DFT 脚本 `run_pyscf.py`,使用 PBE 泛函、def2-SVP 基组。注意正确设置自旋。 | [
"eng_pyscf"
] | [] |
IG_pyscf_007_20260608 | input_generation | agnostic | 请用 PySCF 为水分子写一个几何优化脚本 `run_pyscf.py`,在 PBE/def2-SVP 级别下用 geomeTRIC 优化器优化结构,并打印优化后的总能量。 | [
"eng_pyscf"
] | [] |
IG_pyscf_008_20260608 | input_generation | agnostic | 请用 PySCF 准备一个苯分子单点 B3LYP/def2-SVP 计算:写出 `run_pyscf.py`, 并把可直接执行的 Bohrium 提交命令(含正确的镜像和 cmd)写入 `submit_cmd.txt`。 | [
"eng_pyscf"
] | [] |
IG_pyscf_009_20260609 | input_generation | agnostic | 请用 PySCF 为甲醛分子 CH2O 写一个脚本 `run_pyscf.py`,在 B3LYP/def2-SVP 级别做单点计算,并输出 HOMO-LUMO gap 和偶极矩。只需写出脚本本身,无需提交或运行。 | [
"eng_pyscf"
] | [] |
IG_pyscf_010_20260608 | input_generation | agnostic | 请用 PySCF 为 N2 分子写一个 CCSD(T) 单点能量脚本 `run_pyscf.py`,使用 cc-pVDZ 基组,打印 CCSD(T) 总能量。 | [
"eng_pyscf"
] | [] |
IG_qe_001_20250618 | input_generation | agnostic | Generate a Quantum ESPRESSO pw.x SCF input file for diamond (primitive cell) using the parameters from Mounet & Marzari (2005): GGA-PBE functional, 40 Ry wavefunction cutoff, appropriate charge-density cutoff ratio, and an 8x8x8 Monkhorst-Pack k-mesh. Save the input as diamond_scf.in in the current directory. | [
"eng_qe"
] | [] |
IG_qe_001_20260109 | input_generation | agnostic | Generate a Quantum ESPRESSO pw.x input file (si_relax.in) for geometry relaxation of silicon (diamond-cubic, Materials Project mp-149), which you first retrieve from the structure database. Use PBE functional and precise-level convergence settings. Relax atomic positions only, keeping the cell shape and volume fixed. | [] | [] |
IG_qe_002_20250618 | input_generation | agnostic | Generate a Quantum ESPRESSO ph.x input file for a DFPT phonon calculation of diamond on an 8x8x8 q-point grid. Apply the acoustic sum rule. Use consistent parameters with the SCF run: GGA-PBE, 40 Ry wavefunction cutoff, 8x8x8 k-mesh. Save the input as diamond_phonon.in in the current directory. | [
"eng_qe"
] | [] |
IG_siesta_001_20250618 | input_generation | agnostic | Generate a SIESTA .fdf input file for a spin-polarized DFT geometry optimization of antiferromagnetic NiO. Retrieve the FCC NiO primitive cell (Fm-3m) from the structure database and use it to build the AFM-II supercell with propagation vector Q=(0.5,0.5,0.5). Apply GGA-PBE, 400 Ry mesh cutoff, 13x13x13 k-point grid, d... | [] | [] |
IG_vasp_001_20250618 | input_generation | semiconductor | Retrieve the bulk silicon structure (diamond cubic) from the structure database, then generate two VASP INCAR files: INCAR_relax for PBE structural relaxation and INCAR_hse for one-shot HSE06 band gap calculation. Follow the AMP² computational settings described in Kim et al. (Scientific Data, 2020): PBE functional for... | [
"eng_vasp"
] | [] |
IG_vasp_001_20260109 | input_generation | agnostic | Generate VASP input files (INCAR, POSCAR, KPOINTS) for geometry relaxation of GeTe (trigonal R-3m, Materials Project mp-1189580), which you first retrieve from the structure database. Optimize atomic positions and cell shape while keeping the cell volume fixed. Use PBE functional and precise-level settings. No spin pol... | [
"eng_vasp"
] | [] |
IG_vasp_001_20260121 | input_generation | agnostic | Generate a VASP INCAR file for structural optimization of bulk pyrite FeS2 (cubic Pa-3), which you first retrieve from the structure database. Use the PBE functional with DFT+U correction (U=2.0 eV on Fe-3d). Save the INCAR to the working directory. | [
"eng_vasp"
] | [] |
IG_vasp_001_20260508 | input_generation | alloy | Generate a VASP INCAR file for a two-stage geometry optimization of a 128-atom BCC solid solution alloy. Use GGA-PBE functional, 350 eV plane-wave cutoff, 2×2×2 k-point mesh, Methfessel-Paxton smearing with 0.2 eV broadening. The first stage uses PREC=Low and the second stage uses PREC=Normal. Set convergence criteria ... | [
"eng_vasp"
] | [] |
IG_vasp_001_20260618 | input_generation | agnostic | Generate a VASP INCAR file for a spin-polarized GGA+U calculation of NiO. Use Dudarev's simplified U-J approach (LDAUTYPE=2) with U=6.4 eV on Ni 3d orbitals, a 550 eV plane-wave cutoff, PAW pseudopotentials, and settings appropriate for full structural relaxation (ionic and cell degrees of freedom). Include reasonable ... | [
"eng_vasp"
] | [] |
IG_vasp_001_20260625 | input_generation | agnostic | Generate a VASP INCAR file for PBEsol geometry optimization of the primitive CsPbI₃ perovskite structure, which you first retrieve from the structure database (e.g. Materials Project). The INCAR must use the PBEsol functional, a 500 eV plane-wave cutoff, Γ-centered k-point sampling, and convergence criteria of 1e-5 eV ... | [
"eng_vasp"
] | [] |
IG_vasp_002_20260121 | input_generation | agnostic | Generate a VASP INCAR file for structural optimization of bulk anatase TiO2 (tetragonal I41/amd), which you first retrieve from the structure database. Use the PBE functional with DFT+U correction (U=7.3 eV on Ti-3d). Save the INCAR to the working directory. | [
"eng_vasp"
] | [] |
IG_vasp_003_20250601 | input_generation | agnostic | Generate a VASP INCAR file for DFT single-point energy and force calculations using the settings from the UNEP-v1 training data generation: PBE functional, 600 eV plane-wave energy cutoff, PREC=Accurate, Gaussian smearing with SIGMA=0.02 eV, electronic convergence threshold EDIFF=1E-6, blocked Davidson algorithm (ALGO=... | [
"eng_vasp"
] | [] |
IG_vasp_003_20260618 | input_generation | agnostic | Generate a VASP INCAR file for a spin-polarized GGA+U calculation of MnO (rock-salt, AFM). Use Dudarev's simplified U-J approach (LDAUTYPE=2) with U=4.0 eV on Mn 3d orbitals, a 550 eV plane-wave cutoff, PAW pseudopotentials, and settings appropriate for full structural relaxation. Include reasonable convergence criteri... | [
"eng_vasp"
] | [] |
IG_vasp_005_20250618 | input_generation | agnostic | Generate VASP input files (INCAR, POSCAR, KPOINTS) for a SCAN meta-GGA calculation of an isolated O2 dimer in a 15×15×15 ų cubic box. Use the parameters from Zhang et al. (npj Comput. Mater. 2018): plane-wave cutoff 520 eV, PAW potentials, gamma-point only k-mesh (appropriate for a large molecular box), convergence to... | [
"eng_vasp"
] | [] |
IG_vasp_dftu_001_20260522 | input_generation | agnostic | 工作区中有 NiO.vasp(氧化镍 POSCAR)。请生成静态计算 INCAR 文件 `INCAR`。PBE 泛函,ENCUT=550 eV。 | [
"eng_vasp"
] | [] |
IG_vasp_fenc_orr_restart_001_20260602 | input_generation | agnostic | 工作区中有 `fenc_restart_bundle.json`,记录了 FeN4/graphene ORR 中间体已有计算目录、上一版公共 INCAR 和可用的 CONTCAR 情况。请据此生成下一轮“稳定重跑”会用到的 VASP 输入文件,不需要真实提交计算。
请输出 `INCAR_restart`,并写一个 `restart_inputs/check_before_submit.sh`,用于在提交前检查 POTCAR、CONTCAR/OSZICAR 和 VASP 启动命令等基本条件。
| [
"eng_vasp"
] | [
{
"key": "restart_bundle",
"path": "fixtures/IG_vasp_fenc_orr_restart_001_20260602/fenc_restart_bundle.json",
"source_url": "",
"size_bytes": 1661,
"sha256": "863e5b819a06f1c5bb1f05a5c165c947f922a8de2f71f320f03f0472b3c33749",
"distribution": "bundled",
"available_in_repo": true
}
] |
IG_vasp_he_potcar_gate_001_20260602 | input_generation | agnostic | 我想用 VASP 做 Ni 中辐照缺陷的电子结构计算:完美 Ni、一个 He4V4 氦泡模型、一个 V6 空洞模型。工作区中有 `potcar_inventory.json`,请根据这个 POTCAR 清单,在 `vasp_inputs/` 下为能准备的体系生成输入模板。
请把需要用户后续确认或补齐的信息统一写在 `vasp_inputs/README.md`。
不需要真实提交计算。
| [
"eng_vasp"
] | [
{
"key": "potcar_inventory",
"path": "fixtures/IG_vasp_he_potcar_gate_001_20260602/potcar_inventory.json",
"source_url": "",
"size_bytes": 791,
"sha256": "694d1addc913bca0cbd77a84f5bf713169b9420e631a0965223b92702f8afcb7",
"distribution": "bundled",
"available_in_repo": true
}
] |
IG_vasp_mag_001_20260508 | input_generation | agnostic | 工作区中有 Fe_bcc.vasp(体心立方铁,2个原子)。
请生成适合该体系的 SCF 计算 INCAR 文件 `INCAR_mag`。
注意:Fe 是典型的铁磁性金属,请确保计算设置正确反映其磁性。
ENCUT = 520 eV,电子步收敛精度 1E-6 eV,PBE 泛函。 | [
"eng_vasp"
] | [] |
IG_vasp_metagga_001_20260508 | input_generation | agnostic | 工作区中有 TiO2_rutile.vasp(金红石结构 TiO2,6 个原子)。
生成 r2SCAN 泛函结构优化的 INCAR 文件 `INCAR_r2scan`,要求:
- r2SCAN meta-GGA 泛函
- 结构优化(离子+晶胞)
- ENCUT = 600 eV
- 力收敛标准 0.01 eV/A | [
"eng_vasp"
] | [] |
IG_vasp_qha_pbesol_workflow_001_20260602 | input_generation | agnostic | 工作区中有 `qha_systems.json`,列出了 4 个晶体结构的原子数、元素和 QHA 体积点。请在 `qha_inputs/` 下生成 VASP + PBEsol 做 QHA 会用到的输入模板和命令脚本,不需要真实提交计算。
需要至少包含:
- `qha_inputs/dfpt/INCAR`
- `qha_inputs/finite_displacement/INCAR`
- `qha_inputs/phonopy_commands.sh`
| [
"eng_vasp"
] | [
{
"key": "qha_systems",
"path": "fixtures/IG_vasp_qha_pbesol_plan_001_20260602/qha_systems.json",
"source_url": "",
"size_bytes": 1170,
"sha256": "0e26774a8887b37d71a387c5a2c62caab84332be27b4ed78a334e0837026a42a",
"distribution": "bundled",
"available_in_repo": true
}
] |
PIG_abacus_007_20260527 | input_generation | agnostic | 请为 Si 的 ABACUS LCAO-SCF 试算准备当前目录下的 `INPUT`、`STRU`、`KPT`,并把 Bohrium 提交配置写入 `submit_job.json`。 | [
"eng_abacus"
] | [] |
PIG_abacus_008_20260527 | input_generation | agnostic | 请为 Si 的 ABACUS PW-SCF 试算准备当前目录下的 `INPUT`、`STRU`、`KPT`,并把 Bohrium 提交配置写入 `submit_job.json`。 | [
"eng_abacus"
] | [] |
PIG_abacus_bader_001_20260528 | input_generation | agnostic | 工作区中有 Al₂O₃ 的 CIF 文件 `Al2O3.cif`(刚玉结构,R-3c,10原子)。 请用 ABACUS 对其做 SCF 计算并输出电荷密度,我后续要做 Bader 电荷分析看 Al-O 之间的电荷转移。 帮我把输入文件放在 `abacus_bader/` 目录下并提交运行。 | [
"eng_abacus"
] | [
{
"key": "cif_file",
"path": "fixtures/PIG_abacus_bader_001/Al2O3.cif",
"source_url": "",
"size_bytes": 1163,
"sha256": "44cb17809379c935dbfccf09437dd57ca770236c563e05455d1e5578930a74dd",
"distribution": "bundled",
"available_in_repo": true
}
] |
PIG_abacus_convert_001_20260513 | input_generation | agnostic | 工作区中有一个 Pd(111) slab 的 CIF 文件 `Pd111_slab.cif`(16 个 Pd 原子,4 层)。
请将其转换为 ABACUS LCAO 格式并准备好 SCF 计算输入,我要直接提交跑。 | [
"eng_abacus",
"struct_surface"
] | [
{
"key": "cif_file",
"path": "fixtures/IG_abacus_convert_001_20260513/Pd111_slab.cif",
"source_url": "",
"size_bytes": 902,
"sha256": "cd35d54ef41bb186b31253848cc340b61fc50b96591db437dde69d62cb7a58eb",
"distribution": "bundled",
"available_in_repo": true
}
] |
PIG_cp2k_tm_001_20260524 | input_generation | agnostic | 工作区中有 Fe₂O₃(hematite,R-3c)的 CIF 文件 `Fe2O3.cif`(10原子原胞)。 请用 CP2K 对其做 PBE+U (U_eff=4.0 eV on Fe 3d) 的 SCF 单点能计算。 使用 DZVP-MOLOPT-SR-GTH 基组、截断能 600 Ry、k 点 Gamma only。 帮我准备好输入并跑一下。 | [
"eng_cp2k"
] | [
{
"key": "cif_file",
"path": "fixtures/PIG_cp2k_tm_001/Fe2O3.cif",
"source_url": "",
"size_bytes": 1163,
"sha256": "daf4402fd138600af8ecb18ac04fdc23622e99a717945a1d597b3fb756024b1f",
"distribution": "bundled",
"available_in_repo": true
}
] |
PWO_abacus_phonon_001_20260524 | workflow_orchestration | agnostic | 工作区中有 Si 金刚石结构的 CIF 文件 `Si.cif`(2 原子原胞)。 请用 ABACUS 计算 Si 的声子色散曲线(有限位移法),沿 G-X-K-G 路径绘制, 并报告 Gamma 点光学支频率(THz)。 | [
"eng_abacus"
] | [
{
"key": "si_cif",
"path": "fixtures/PWO_abacus_phonon_001/Si.cif",
"source_url": "",
"size_bytes": 748,
"sha256": "be8d0398dfe90f55754782edc7c1ae41b28b1518535d2c961257ddb66241d0ce",
"distribution": "bundled",
"available_in_repo": true
}
] |
PWO_dpa_finetune_001_20260603 | workflow_orchestration | agnostic | 工作区 `data/` 下是我的一份 DeePMD 格式训练数据集。帮我用 DPA3 预训练模型在这份数据上微调大约 3000 步,跑完把训练和测试(验证)的 loss 告诉我。 | [
"code_mlip"
] | [
{
"key": "train_type_map",
"path": "fixtures/PWO_dpa_finetune_001/data/data_0/type_map.raw",
"source_url": "",
"size_bytes": 4,
"sha256": "2af2202bdb95741681b308b05c1dae7837141fe32b10d14db2a4c0ea9103e55b",
"distribution": "bundled",
"available_in_repo": true
},
{
"key": "train_ty... |
PWO_dpa_head_case_001_20260524 | workflow_orchestration | agnostic | 请使用 DPA-3.2-5M 模型对 MgO 做结构优化,输出提交配置 `opt_submit.json`。
| [
"code_mlip"
] | [] |
PWO_dpa_head_organic_001_20260521 | workflow_orchestration | agnostic | 请使用 DPA 模型对咖啡因分子做构型优化,输出为 `caffeine_optimized.cif`。 | [
"code_mlip"
] | [] |
PWO_elec_009_20260521 | workflow_orchestration | agnostic | 对 Al₂O₃ 准备 ABACUS Bader 电荷分析所需文件和 Bohrium 提交配置(文件名 `al2o3_bader_submit.json`)。本题只检验输入文件与提交 JSON,不要投递或执行计算。 | [
"eng_abacus"
] | [] |
PWO_gpumd_phonon_001_20260526 | workflow_orchestration | agnostic | 使用 GPUMD 计算 Si 金刚石结构的声子色散关系。
要求:
- 使用 NEP 势函数(Si 体系,从 GPUMD 官方 examples 或已有资源获取)
- 提交到 Bohrium 运行
- 报告 Gamma 点光学支频率
- 结果写入工作区根目录 `phonon_result.json`:`{"gamma_optical_THz": ..., "method": "gpumd"}`
| [
"eng_gpumd"
] | [] |
PWO_orca_tddft_001_20260525 | workflow_orchestration | agnostic | 请用 ORCA 计算萘 (naphthalene, C₁₀H₈) 的第一激发态吸收波长。 先做几何优化(B3LYP/def2-SVP),然后在优化结构上做 TD-DFT(PBE0/def2-SVP,5 个根)。 报告 S₁ 的激发能 (eV) 和振子强度。 | [
"eng_orca"
] | [] |
PWO_qe_bands_001_20260526 | workflow_orchestration | agnostic | 使用 Quantum ESPRESSO 计算 Si 的能带结构(金刚石结构,a=5.43 Å)。
沿 Γ-X-L-Γ 高对称路径计算能带,报告带隙类型和带隙值。
| [
"eng_qe"
] | [] |
PWO_qe_scf_001_20260524 | workflow_orchestration | agnostic | 请帮我对 MgO 岩盐结构做一次 Quantum ESPRESSO pw.x 的 SCF 单点能计算。 结构参数:Fm-3m, a=4.21 Å, Mg 在 (0,0,0), O 在 (0.5,0.5,0.5)。 使用 PBE 泛函、ecutwfc=60 Ry、4×4×4 k 点网格。帮我跑一下看看总能是多少。 | [
"eng_qe"
] | [] |
PWO_vasp_submit_001_20260521 | workflow_orchestration | agnostic | 帮我用 VASP 计算一个 O₂ 分子的平衡键长和结合能,用 PBE 泛函。 | [
"eng_vasp"
] | [
{
"key": "potcar_O",
"path": "fixtures/PWO_vasp_submit_001/POT/PAW_PBE/O/POTCAR",
"source_url": "",
"size_bytes": 220113,
"sha256": "593e090199bb912785fa070a88f396478de48a4e1c2239de14d9e81b9e668c40",
"distribution": "restricted",
"available_in_repo": false,
"restriction_kind": "licen... |
PWO_vasp_submit_002_20260528 | workflow_orchestration | agnostic | 工作区中提供了 Si 金刚石结构 `POSCAR_Si` 和对应的 `POTCAR_Si`。
请准备 VASP 自洽场计算输入,放入 `si_scf/` 目录(含 POTCAR),并输出提交配置 `submit.json`。 | [
"eng_vasp"
] | [
{
"key": "poscar_si",
"path": "fixtures/PIG_vasp_001_20260513/POSCAR_Si",
"source_url": "",
"size_bytes": 100,
"sha256": "50ef4d1c61414e15775ba85c728622acf7489ba8463bb72d89ac5f951ecbd809",
"distribution": "bundled",
"available_in_repo": true
},
{
"key": "potcar_si",
"path": "... |
PXRD_pawley_303K_001_20260502_v1 | scientific_analysis | agnostic | 文件 `pxrd_303K.xy` 是一个有机-无机杂化硝普盐在 303 K(30 °C)下采集的粉末 X 射线衍射(PXRD)数据(Cu Kα1, λ = 1.5406 Å, 2θ 范围 5°–50°, 步长 ~0.02°, 两列格式: 2θ 强度)。
该化合物为单斜晶系,空间群 P 21(No. 4)。文献参考晶胞:a ≈ 10.83 Å, b ≈ 9.62 Å, c ≈ 10.13 Å, beta ≈ 108.75°, V ≈ 1000 ų。
精修策略建议: - 建议使用 14°–50° 2θ 区间以避开低角伪影 - 基线 / 背景函数使用低阶(0–1 阶)以避免过拟合 - 若多次精修收敛到不同盆地,选择 wR 最低且体积与... | [
"char_diffraction"
] | [
{
"key": "pxrd_data",
"path": "fixtures/PXRD_pawley_303K_001_20260502_v1/pxrd_303K.xy",
"source_url": "",
"size_bytes": 54498,
"sha256": "f9be7a7941b9f3efe0862561bc201b494459db31765255459321b78ae398c58f",
"distribution": "bundled",
"available_in_repo": true
}
] |
PXRD_thermal_expansion_001_20260508 | scientific_analysis | agnostic | 文件 `_td-pxrd_test.txt` 包含一个化合物在 8 个温度下的变温粉末 X 射线衍射(PXRD)数据,温度标签对应关系为:30°C→303K、50°C→323K、70°C→343K、90°C→363K、110°C→383K、120°C→393K、130°C→403K、140°C→413K。该化合物为单斜晶系,空间群提示为 P 21(No. 4),波长为 Cu Kα1,λ = 1.5406 Å。
数据特征与精修策略: - 数据为实测变温实验数据,扣除背景前的动态范围约 10×–30×;2θ 范围 5°–50°,建议精修使用 14°–50° 区间以避开低角伪影。 - 推荐将数据按相拆分(RTP 4 点、HTP 4 点)分... | [
"char_diffraction"
] | [
{
"key": "vt_pxrd_data",
"path": "fixtures/PXRD_thermal_expansion_001_20260506/_td-pxrd_test.txt",
"source_url": "https://matmaster-test.oss-cn-zhangjiakou.aliyuncs.com/matmaster_evo/eval_data/PXRD_thermal_expansion_001_20260427_v3/1777279719__td-pxrd_test.txt",
"size_bytes": 435960,
"sha256": "... |
RT_cof_3d_001_20260629 | structure_retrieval | polymer | 从 COF 数据库检索 3D 类型、dia 拓扑的 COF 结构。
请完成以下交付:
1) `3d_dia_cof.json`:包含 `query_type`, `query_topology`, `candidate_count`, `results` (每个含 name, topology, type, formula, density, void_fraction);
2) `3d_dia_report.md`:说明 3D COF 与 2D COF 在结构上的核心区别、dia 拓扑的连接规则(四面体节点+线性连接体),以及检索到的结构是否符合预期;
3) 导出第一个候选结构为 `COF_3D_dia.cif`。 | [
"meta_database"
] | [] |
RT_cof_comparison_001_20260629 | structure_retrieval | polymer | 分别检索 hcb 拓扑和 sql 拓扑的 COF 各 3 个,对比两种拓扑在孔径(PLD/LCD)和比表面积上的差异。
请完成以下交付:
1) `topology_comparison.json`:包含 `hcb_results`(3个)和 `sql_results`(3个),每个含 name, topology, pld, lcd, surface_area_m2g;
2) `topology_comparison_report.md`:对比分析两组数据的孔径和比表面积分布差异,解释为什么不同拓扑会导致不同的孔道几何。 | [
"meta_database"
] | [] |
RT_cof_elements_001_20260629 | structure_retrieval | polymer | 检索同时含有硼(B)和氮(N)元素的 COF 结构,返回最多 5 个候选。
请完成以下交付:
1) `bn_cof_candidates.json`:包含 `query_elements`, `candidate_count`, `results`(每个含 name, formula, elements, topology, surface_area);
2) `bn_cof_report.md`:分析这些 COF 的共同特征(连接化学类型、典型拓扑、孔径范围),解释为什么 B+N 组合在 COF 中常见(硼酸酯键、硼嗪键等)。 | [
"meta_database"
] | [] |
RT_cof_name_001_20260629 | structure_retrieval | polymer | 检索 COF-LZU1 的晶体结构,并报告其基本结构信息。
请完成以下交付:
1) `COF_LZU1.cif`:导出结构文件;
2) `cof_lzu1_info.json`:包含 `name`, `topology`, `elements`, `formula`, `space_group`, `pld`, `lcd`, `surface_area`, `type`(2D/3D), `database_source`;
3) 在报告中确认这是否确实是亚胺键连接的 hcb 拓扑 COF。 | [
"meta_database"
] | [] |
RT_cof_pore_size_001_20260629 | structure_retrieval | polymer | 检索孔限径(PLD)大于 20 埃的 COF 结构,按孔径从大到小排列,返回前 5 个。
请完成以下交付:
1) `large_pore_cof.json`:包含 `filter_criterion`, `results`(每个含 name, pld, lcd, topology, surface_area, type);
2) `large_pore_cof_report.md`:分析大孔 COF 的结构特征(什么样的拓扑/连接体长度容易产生大孔);
3) 导出孔径最大的结构为 `largest_pore_cof.cif`。 | [
"meta_database"
] | [] |
RT_cof_surface_area_001_20260629 | structure_retrieval | polymer | 帮我筛选比表面积大于 2000 m²/g 的 COF 材料,我想找适合甲烷储存的高孔隙率结构。
请完成以下交付:
1) `high_sa_cof.json`:包含 `filter_criterion`, `application`, `results`(每个含 name, surface_area_m2g, void_fraction, pld, lcd, topology);
2) `gas_storage_screening.md`:从检索结果中推荐 2-3 个最适合甲烷储存的候选,说明推荐理由 (孔径匹配甲烷动力学直径~3.8Å、高空隙率、合适拓扑)。 | [
"meta_database"
] | [] |
RT_cof_topology_001_20260629 | structure_retrieval | polymer | 帮我从 COF 数据库中检索 sql 拓扑、含三嗪(triazine)节点的 COF 结构。
请完成以下交付:
1) `cof_retrieval_report.md`:说明检索条件、使用了哪个数据库、返回了多少候选、各候选的关键属性(拓扑、元素、孔径等);
2) `cof_candidates.json`:至少包含 `query_topology`, `database_source`, `candidate_count`, `results`(每个结果含 name, topology, elements, pld, lcd);
3) 将筛选出的第一个结构导出为 `COF_sql_triazine.cif`。 | [
"meta_database"
] | [] |
SA_abacus_ads_001_20260519 | scientific_analysis | agnostic | 工作区中有 ABACUS SCF 计算结果文件 `abacus_results.json`,包含 Pt(111) clean slab、CO 分子、以及 CO 吸附在 Pt(111) 上的三个体系的总能量。请计算 CO 的吸附能 E_ads = E(CO+slab) - E(slab) - E(CO),输出到 `adsorption_energy.json`,格式为 `{"E_ads": ...}`。 | [
"eng_abacus"
] | [
{
"key": "abacus_results",
"path": "fixtures/SA_abacus_ads_001/abacus_results.json",
"source_url": "",
"size_bytes": 609,
"sha256": "ab02855210715c1362b9fe4620924770a2ddcfec6f448ece9b65ebd42adeff5e",
"distribution": "bundled",
"available_in_repo": true
}
] |
SA_abacus_wf_001_20260514 | scientific_analysis | agnostic | 工作区中有一个已完成的 ABACUS slab 计算结果:
- `mock_running_scf.log`:SCF 收敛日志(含费米能级)
- `mock_ElecStaticPot_z_avg.dat`:沿 z 方向平均的静电势(两列:z 分数坐标 + 势能值)
请从这些数据中提取功函数(work function),写入 `work_function.json`,格式为 `{"work_function_eV": <数值>, "V_vacuum_eV": <数值>, "E_fermi_eV": <数值>}`。 | [
"eng_abacus"
] | [
{
"key": "scf_log",
"path": "fixtures/SA_abacus_wf_001_20260514/mock_running_scf.log",
"source_url": "",
"size_bytes": 824,
"sha256": "1318f839340374eabb0813062105e370670cbddba94d8af356685f1cc3075f2e",
"distribution": "bundled",
"available_in_repo": true
},
{
"key": "pot_data",
... |
SA_ads_site_001_20260521 | scientific_analysis | agnostic | 工作区中有一个弛豫后的 H/Zn(0001) 吸附结构 `H_on_Zn0001_relaxed.xyz`(2x2 超胞,4 层 slab + 1 个 H 原子)。请分析该 H 原子处于什么吸附位点,并给出判断依据。
输出 `site_analysis.json`,格式:`{"actual_site": "...", "coordination": ..., "distances_to_nearest_Zn_A": [...], "reasoning": "..."}` | [
"struct_surface"
] | [
{
"key": "relaxed_structure",
"path": "fixtures/SA_ads_site_001/H_on_Zn0001_relaxed.xyz",
"source_url": "https://bohrium-agent-test.oss-cn-zhangjiakou.aliyuncs.com/evomaster/evaluation/sa_ads_site_001/H_on_Zn0001_relaxed.xyz",
"size_bytes": 876,
"sha256": "03f1ee3d151d563e8863cb2888611d951a9d1ce... |
SA_agnostic_001_20250618 | scientific_analysis | agnostic | Calculate the Debye temperature Θ_D (in K) of Ni₃Al using the Moruzzi-Janak-Schwarz approximation. The bulk modulus is B = 180 GPa, the average atomic volume is Ω = 11.14 ų/atom, and the average atomic mass is M̄ = 45.24 amu. Write your answer to a file named debye_temperature.txt in the working directory, with the nu... | [] | [] |
SA_agnostic_001_20260625 | scientific_analysis | semiconductor | Calculate the decomposition enthalpy (ΔH_decomp) in meV/atom for CsGe₀.₅Sn₀.₅Br₃. Use the formula ΔH_decomp = E(CsGe₀.₅Sn₀.₅Br₃) - E(CsBr) - 0.5*E(GeBr₂) - 0.5*E(SnBr₂). Fetch total energies per atom from Materials Project for CsBr (mp-1066996), GeBr₂ (use OQMD or estimate), SnBr₂ (mp-23215), and construct the perovski... | [
"meta_database"
] | [] |
SA_agnostic_002_20250618 | scientific_analysis | agnostic | Calculate the nearest-neighbor effective cluster interaction V_1nn (in meV/atom) for the Pd-V alloy system at T = 1000 K using the bond proportion model. The spring constants are: k_PdPd = 3.2 eV/Ų, k_VV = 2.8 eV/Ų, and k_PdV = 3.5 eV/Ų. The system is fcc (d = 3). Write your answer to a file named v1nn_meV.txt in th... | [] | [] |
SA_agnostic_002_20260625 | scientific_analysis | semiconductor | Calculate the mixing entropy ΔS_mix (in meV/atom/K) and the free-energy-corrected decomposition enthalpy ΔH_decomp - TΔS_mix (in meV/atom) at T = 298 K for a B-site alloyed perovskite with composition CsGe₀.₂₅Hg₀.₂₅Pb₀.₂₅Sn₀.₂₅Br₃. Use the ideal solid solution model: ΔS_mix = -k_B Σ x_i ln(x_i), where k_B = 8.617333262... | [] | [] |
SA_agnostic_003_20250618 | scientific_analysis | agnostic | Calculate the volumetric thermal expansion ΔV/N (in ų/atom) at T = 1000 K for an fcc alloy using the quasiharmonic approximation. The bulk modulus is B = 150 GPa and the average Grüneisen parameter is γ̄ = 2.0. Write your answer to a file named thermal_expansion.txt in the working directory, with the numeric value on ... | [] | [] |
SA_agnostic_003_20260625 | scientific_analysis | agnostic | Calculate Bartel's tolerance factor τ for CsGe₀.₅₆₂₅Sn₀.₄₃₇₅Br₃. Use Shannon ionic radii (6-coordination, in Å): Cs⁺ = 1.81, Ge²⁺ = 0.73, Sn²⁺ = 1.18, Br⁻ = 1.96. n_A = 1 (Cs oxidation state). r_B is the composition-weighted average. Use the formula: τ = r_X/r_B - n_A*(n_A - (r_A/r_B)/ln(r_A/r_B)). Write the result to ... | [] | [] |
SA_agnostic_005_20250618 | scientific_analysis | agnostic | The purely configurational order-disorder transition temperature of Ni3Al (L1₂ → fcc disordered) is T_config = 1350 K. The configurational entropy change upon disordering at 50:50 composition is ΔS_config = 0.693 k_B/atom. The vibrational entropy change upon disordering is ΔS_vib = 0.05 k_B/atom. Compute the corrected ... | [] | [] |
SA_barrier_001_20250115 | scientific_analysis | battery | From the paper 'Factors that affect Li mobility in layered lithium transition metal oxides' by Kang and Ceder, extract the activation barrier data for Li migration in LiCoO₂ as a function of Li slab distance (Figure 2). Create a CSV file named licoo2_barrier_vs_slab.csv with columns: slab_distance_angstrom and activati... | [
"analysis_data",
"meta_grounding"
] | [] |
SA_bat_formation_001_20260521 | scientific_analysis | battery | 工作区中有 ABACUS 计算结果文件 `abacus_energies.json`,包含 LiCoO2 体相、Li 金属、Co 金属和 O2 分子的总能量。请计算 LiCoO2 的生成能(每 formula unit),输出到 `formation_energy.json`,格式为 `{"E_f_per_fu": ...}`。 | [
"eng_abacus"
] | [
{
"key": "energies",
"path": "fixtures/SA_formation_energy_001/abacus_energies.json",
"source_url": "",
"size_bytes": 713,
"sha256": "e9cdbd270796124f8394c02c341dfcb57d73feaccef73439fcfef7f6898d7616",
"distribution": "bundled",
"available_in_repo": true
}
] |
SA_bat_oxpot_001_20260519 | scientific_analysis | battery | 请计算 FEC(氟代碳酸乙烯酯,SMILES: C1OC(=O)OC1F)的电化学氧化电位 vs Li/Li+,输出到 `fec_oxidation.json`,格式为 `{"E_ox_vs_Li": ...}`。 | [] | [] |
SA_battery_003_20250618 | scientific_analysis | battery | Calculate the theoretical Mn2+/Mn4+ double redox capacity (in mAh/g) of the cathode material Li2Mn2/3Nb1/3O2F. The Mn2+/Mn4+ couple involves 2 electrons per Mn ion. Use atomic masses: Li=6.94, Mn=54.94, Nb=92.91, O=16.00, F=19.00 g/mol. Save your calculation steps and result to a file named capacity_calculation.txt. | [
"char_electrochem"
] | [] |
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