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simulation_id int64 | radius float64 | gravity float64 | rotation_period float64 | surface_pressure float64 | co2 float64 | ch4 float64 | stellar_flux float64 | stellar_temperature float64 | gcm_label string | is_target_gcm bool | in_target_physical_domain bool | planet_id int64 | source string |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
0 | 5,850,000 | 8.07 | 11.5 | 146,000 | 0 | 0 | 1,160 | 2,910 | exocam | true | true | 0 | this work |
1 | 6,550,000 | 8.86 | 8.6 | 164,000 | 0 | 0.000054 | 1,070 | 2,750 | exocam | true | true | 1 | this work |
2 | 7,440,000 | 14 | 11.1 | 113,000 | 0.00828 | 0 | 1,030 | 2,800 | exocam | true | true | 2 | this work |
3 | 6,580,000 | 8.4 | 18.6 | 206,000 | 0 | 0 | 964 | 3,290 | exocam | true | true | 3 | this work |
4 | 6,520,000 | 9.12 | 10.8 | 330,000 | 0 | 0 | 1,240 | 2,830 | exocam | true | true | 4 | this work |
5 | 7,340,000 | 13.2 | 12.3 | 98,000 | 0 | 0.000017 | 811 | 2,820 | exocam | true | true | 5 | this work |
6 | 7,650,000 | 13.4 | 7.05 | 134,000 | 0.000003 | 0 | 1,190 | 2,600 | exocam | true | true | 6 | this work |
7 | 6,630,000 | 9.98 | 13.7 | 336,000 | 0.000418 | 0 | 884 | 3,200 | exocam | true | true | 7 | this work |
8 | 6,720,000 | 9.03 | 50.7 | 105,000 | 0 | 0 | 881 | 3,690 | exocam | true | true | 8 | this work |
9 | 6,450,000 | 7.61 | 93.6 | 191,000 | 0.00126 | 0 | 1,050 | 4,220 | exocam | true | true | 9 | this work |
10 | 6,160,000 | 8.86 | 14.2 | 251,000 | 0.00571 | 0.000173 | 1,370 | 3,040 | exocam | true | true | 10 | this work |
11 | 6,910,000 | 10.5 | 55 | 150,000 | 0 | 0 | 1,190 | 3,960 | exocam | true | true | 11 | this work |
12 | 5,930,000 | 7.55 | 5.39 | 410,000 | 0 | 0.00003 | 1,060 | 2,780 | exocam | true | true | 12 | this work |
13 | 7,620,000 | 12.2 | 7.54 | 219,000 | 0 | 0.000003 | 1,260 | 2,930 | exocam | true | true | 13 | this work |
14 | 7,310,000 | 11.1 | 10.6 | 96,100 | 0 | 0 | 1,130 | 2,870 | exocam | true | true | 14 | this work |
15 | 7,590,000 | 12.1 | 5.8 | 411,000 | 0.000022 | 0 | 1,410 | 2,630 | exocam | true | true | 15 | this work |
16 | 6,260,000 | 9.2 | 7.6 | 124,000 | 0.00357 | 0 | 821 | 2,600 | exocam | true | true | 16 | this work |
17 | 6,890,000 | 10.9 | 8.31 | 347,000 | 0 | 0.00172 | 1,310 | 2,690 | exocam | true | true | 17 | this work |
18 | 6,440,000 | 9.52 | 45.8 | 182,000 | 0.000002 | 0 | 1,340 | 3,710 | exocam | true | true | 18 | this work |
19 | 6,250,000 | 10.1 | 9.57 | 270,000 | 0 | 0 | 1,070 | 3,090 | exocam | true | true | 19 | this work |
20 | 5,610,000 | 8.1 | 15.7 | 393,000 | 0.48 | 0.000613 | 812 | 2,890 | exocam | true | true | 20 | this work |
21 | 6,590,000 | 8.06 | 18.4 | 136,000 | 0.116 | 0 | 1,080 | 3,040 | exocam | true | true | 21 | this work |
22 | 6,140,000 | 8.97 | 20.7 | 90,900 | 0 | 0 | 1,110 | 3,260 | exocam | true | true | 22 | this work |
23 | 6,360,000 | 8.61 | 5.81 | 295,000 | 0.0149 | 0 | 1,210 | 2,790 | exocam | true | true | 23 | this work |
24 | 6,290,000 | 8.38 | 8.76 | 191,000 | 0.888 | 0 | 1,030 | 2,700 | exocam | true | true | 24 | this work |
25 | 7,008,100 | 8.74 | 10.35 | 110,000 | 0.090909 | 0 | 911.87 | 3,024 | exocam | true | true | 25 | Hammond et al. [2025] |
26 | 7,008,100 | 8.74 | 10.35 | 100,010 | 0.0001 | 0 | 911.87 | 3,024 | exocam | true | true | 26 | Hammond et al. [2025] |
27 | 7,008,100 | 8.74 | 10.35 | 200,000 | 1 | 0 | 911.87 | 3,024 | exocam | true | true | 27 | Hammond et al. [2025] |
28 | 7,836,330 | 10.61 | 13.03 | 110,000 | 0.090909 | 0 | 816.6 | 2,953 | exocam | true | true | 28 | Hammond et al. [2025] |
29 | 7,836,330 | 10.61 | 13.03 | 100,010 | 0.0001 | 0 | 816.6 | 2,953 | exocam | true | true | 29 | Hammond et al. [2025] |
30 | 7,836,330 | 10.61 | 13.03 | 200,000 | 1 | 0 | 816.6 | 2,953 | exocam | true | true | 30 | Hammond et al. [2025] |
31 | 8,709,157 | 13.1 | 8.46 | 110,000 | 0.090909 | 0 | 1,233.066 | 2,871 | exocam | true | true | 31 | Hammond et al. [2025] |
32 | 8,709,157 | 13.1 | 8.46 | 100,010 | 0.0001 | 0 | 1,233.066 | 2,871 | exocam | true | true | 32 | Hammond et al. [2025] |
33 | 8,709,157 | 13.1 | 8.46 | 200,000 | 1 | 0 | 1,233.066 | 2,871 | exocam | true | true | 33 | Hammond et al. [2025] |
34 | 7,008,100 | 10.88 | 11.2 | 110,000 | 0.090909 | 0 | 877.845 | 3,050 | exocam | true | true | 34 | Hammond et al. [2025] |
35 | 7,008,100 | 10.88 | 11.2 | 100,010 | 0.0001 | 0 | 877.845 | 3,050 | exocam | true | true | 35 | Hammond et al. [2025] |
36 | 7,008,100 | 10.88 | 11.2 | 200,000 | 1 | 0 | 877.845 | 3,050 | exocam | true | true | 36 | Hammond et al. [2025] |
37 | 5,861,320 | 8.01 | 6.1 | 110,000 | 0.090909 | 0 | 879.206 | 2,566 | exocam | true | true | 37 | Hammond et al. [2025] |
38 | 5,861,320 | 8.01 | 6.1 | 100,010 | 0.0001 | 0 | 879.206 | 2,566 | exocam | true | true | 38 | Hammond et al. [2025] |
39 | 5,861,320 | 8.01 | 6.1 | 200,000 | 1 | 0 | 879.206 | 2,566 | exocam | true | true | 39 | Hammond et al. [2025] |
40 | 6,689,550 | 9.86 | 11.41 | 110,000 | 0.090909 | 0 | 503.57 | 2,904 | exocam | true | true | 40 | Hammond et al. [2025] |
41 | 6,689,550 | 9.86 | 11.41 | 100,010 | 0.0001 | 0 | 503.57 | 2,904 | exocam | true | true | 41 | Hammond et al. [2025] |
42 | 6,689,550 | 9.86 | 11.41 | 200,000 | 1 | 0 | 503.57 | 2,904 | exocam | true | true | 42 | Hammond et al. [2025] |
43 | 6,880,680 | 10.58 | 15.6 | 110,000 | 0.090909 | 0 | 887.372 | 3,158 | exocam | true | true | 43 | Hammond et al. [2025] |
44 | 6,880,680 | 10.58 | 15.6 | 100,010 | 0.0001 | 0 | 887.372 | 3,158 | exocam | true | true | 44 | Hammond et al. [2025] |
45 | 6,880,680 | 10.58 | 15.6 | 200,000 | 1 | 0 | 887.372 | 3,158 | exocam | true | true | 45 | Hammond et al. [2025] |
46 | 6,371,000 | 9.807 | 1 | 100,000 | 0 | 0 | 740.384 | 2,600 | exocam-pre2022 | false | true | 46 | Komacek and Abbot [2019] |
47 | 6,371,000 | 9.807 | 6.49 | 100,000 | 0 | 0 | 740.384 | 2,600 | exocam-pre2022 | false | true | 47 | Komacek and Abbot [2019] |
48 | 6,371,000 | 9.807 | 1 | 100,000 | 0 | 0 | 907.787 | 2,600 | exocam-pre2022 | false | true | 48 | Komacek and Abbot [2019] |
49 | 6,371,000 | 9.807 | 5.57 | 100,000 | 0 | 0 | 907.787 | 2,600 | exocam-pre2022 | false | true | 49 | Komacek and Abbot [2019] |
50 | 6,371,000 | 9.807 | 1 | 100,000 | 0 | 0 | 1,110.576 | 2,600 | exocam-pre2022 | false | true | 50 | Komacek and Abbot [2019] |
51 | 6,371,000 | 9.807 | 4.79 | 100,000 | 0 | 0 | 1,110.576 | 2,600 | exocam-pre2022 | false | true | 51 | Komacek and Abbot [2019] |
52 | 6,371,000 | 9.807 | 4.51 | 100,000 | 0 | 0 | 1,200.402 | 2,600 | exocam-pre2022 | false | true | 52 | Komacek and Abbot [2019] |
53 | 6,371,000 | 9.807 | 4.37 | 100,000 | 0 | 0 | 1,250.759 | 2,600 | exocam-pre2022 | false | true | 53 | Komacek and Abbot [2019] |
54 | 6,371,000 | 9.807 | 4.25 | 100,000 | 0 | 0 | 1,299.755 | 2,600 | exocam-pre2022 | false | true | 54 | Komacek and Abbot [2019] |
55 | 6,371,000 | 9.807 | 4.13 | 100,000 | 0 | 0 | 1,350.112 | 2,600 | exocam-pre2022 | false | true | 55 | Komacek and Abbot [2019] |
56 | 6,371,000 | 9.807 | 4.07 | 100,000 | 0 | 0 | 1,375.971 | 2,600 | exocam-pre2022 | false | true | 56 | Komacek and Abbot [2019] |
57 | 6,371,000 | 9.807 | 1 | 100,000 | 0 | 0 | 1,497.1 | 2,600 | exocam-pre2022 | false | true | 57 | Komacek and Abbot [2019] |
58 | 6,371,000 | 4.9035 | 1 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | false | 58 | Komacek and Abbot [2019] |
59 | 6,371,000 | 6.933549 | 1 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | true | 59 | Komacek and Abbot [2019] |
60 | 6,371,000 | 13.867098 | 1 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | true | 60 | Komacek and Abbot [2019] |
61 | 6,371,000 | 9.807 | 1 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | true | 61 | Komacek and Abbot [2019] |
62 | 6,371,000 | 9.807 | 0.25 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | true | 62 | Komacek and Abbot [2019] |
63 | 6,371,000 | 9.807 | 0.5 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | true | 63 | Komacek and Abbot [2019] |
64 | 6,371,000 | 9.807 | 10 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | true | 64 | Komacek and Abbot [2019] |
65 | 6,371,000 | 9.807 | 12 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | true | 65 | Komacek and Abbot [2019] |
66 | 6,371,000 | 9.807 | 16 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | true | 66 | Komacek and Abbot [2019] |
67 | 6,371,000 | 9.807 | 2 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | true | 67 | Komacek and Abbot [2019] |
68 | 6,371,000 | 9.807 | 4.11 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | true | 68 | Komacek and Abbot [2019] |
69 | 6,371,000 | 9.807 | 4 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | true | 69 | Komacek and Abbot [2019] |
70 | 6,371,000 | 9.807 | 8 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | true | 70 | Komacek and Abbot [2019] |
71 | 6,371,000 | 9.807 | 1 | 25,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | false | 71 | Komacek and Abbot [2019] |
72 | 6,371,000 | 9.807 | 1 | 50,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | true | 72 | Komacek and Abbot [2019] |
73 | 6,371,000 | 9.807 | 1 | 200,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | true | 73 | Komacek and Abbot [2019] |
74 | 6,371,000 | 9.807 | 1 | 400,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | true | 74 | Komacek and Abbot [2019] |
75 | 3,185,500 | 9.807 | 1 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | false | 75 | Komacek and Abbot [2019] |
76 | 4,504,297 | 9.807 | 1 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | true | 76 | Komacek and Abbot [2019] |
77 | 9,008,594 | 9.807 | 1 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | false | 77 | Komacek and Abbot [2019] |
78 | 12,742,000 | 9.807 | 1 | 100,000 | 0 | 0 | 1,361 | 2,600 | exocam-pre2022 | false | false | 78 | Komacek and Abbot [2019] |
79 | 6,371,000 | 9.807 | 35.78 | 100,000 | 0 | 0 | 740.384 | 3,300 | exocam-pre2022 | false | true | 79 | Komacek and Abbot [2019] |
80 | 6,371,000 | 9.807 | 30.7 | 100,000 | 0 | 0 | 907.787 | 3,300 | exocam-pre2022 | false | true | 80 | Komacek and Abbot [2019] |
81 | 6,371,000 | 9.807 | 26.39 | 100,000 | 0 | 0 | 1,110.576 | 3,300 | exocam-pre2022 | false | true | 81 | Komacek and Abbot [2019] |
82 | 6,371,000 | 9.807 | 22.66 | 100,000 | 0 | 0 | 1,361 | 3,300 | exocam-pre2022 | false | true | 82 | Komacek and Abbot [2019] |
83 | 6,371,000 | 9.807 | 1 | 100,000 | 0 | 0 | 740.384 | 4,000 | exocam-pre2022 | false | true | 83 | Komacek and Abbot [2019] |
84 | 6,371,000 | 9.807 | 117.4 | 100,000 | 0 | 0 | 740.384 | 4,000 | exocam-pre2022 | false | true | 84 | Komacek and Abbot [2019] |
85 | 6,371,000 | 9.807 | 1 | 100,000 | 0 | 0 | 907.787 | 4,000 | exocam-pre2022 | false | true | 85 | Komacek and Abbot [2019] |
86 | 6,371,000 | 9.807 | 100.7 | 100,000 | 0 | 0 | 907.787 | 4,000 | exocam-pre2022 | false | true | 86 | Komacek and Abbot [2019] |
87 | 6,371,000 | 9.807 | 1 | 100,000 | 0 | 0 | 1,110.576 | 4,000 | exocam-pre2022 | false | true | 87 | Komacek and Abbot [2019] |
88 | 6,371,000 | 9.807 | 86.6 | 100,000 | 0 | 0 | 1,110.576 | 4,000 | exocam-pre2022 | false | true | 88 | Komacek and Abbot [2019] |
89 | 6,371,000 | 9.807 | 1 | 100,000 | 0 | 0 | 1,667.225 | 4,000 | exocam-pre2022 | false | false | 89 | Komacek and Abbot [2019] |
90 | 6,371,000 | 4.9035 | 1 | 100,000 | 0 | 0 | 1,361 | 4,000 | exocam-pre2022 | false | false | 90 | Komacek and Abbot [2019] |
91 | 6,371,000 | 6.933549 | 1 | 100,000 | 0 | 0 | 1,361 | 4,000 | exocam-pre2022 | false | true | 91 | Komacek and Abbot [2019] |
92 | 6,371,000 | 13.867098 | 1 | 100,000 | 0 | 0 | 1,361 | 4,000 | exocam-pre2022 | false | true | 92 | Komacek and Abbot [2019] |
93 | 6,371,000 | 9.807 | 1 | 100,000 | 0 | 0 | 1,361 | 4,000 | exocam-pre2022 | false | true | 93 | Komacek and Abbot [2019] |
94 | 6,371,000 | 9.807 | 0.25 | 100,000 | 0 | 0 | 1,361 | 4,000 | exocam-pre2022 | false | true | 94 | Komacek and Abbot [2019] |
95 | 6,371,000 | 9.807 | 0.5 | 100,000 | 0 | 0 | 1,361 | 4,000 | exocam-pre2022 | false | true | 95 | Komacek and Abbot [2019] |
96 | 6,371,000 | 9.807 | 16 | 100,000 | 0 | 0 | 1,361 | 4,000 | exocam-pre2022 | false | true | 96 | Komacek and Abbot [2019] |
97 | 6,371,000 | 9.807 | 2 | 100,000 | 0 | 0 | 1,361 | 4,000 | exocam-pre2022 | false | true | 97 | Komacek and Abbot [2019] |
98 | 6,371,000 | 9.807 | 4 | 100,000 | 0 | 0 | 1,361 | 4,000 | exocam-pre2022 | false | true | 98 | Komacek and Abbot [2019] |
99 | 6,371,000 | 9.807 | 74.3 | 100,000 | 0 | 0 | 1,361 | 4,000 | exocam-pre2022 | false | true | 99 | Komacek and Abbot [2019] |
ThousandWorlds
ThousandWorlds is a benchmark for emulating exoplanet climates: 1760 simulations across 5 GCMs, 8 planet parameters, and atmospheric variables on a 32 x 64 x 10 latitude-longitude-pressure grid. It includes three nested benchmark subsets, two evaluation protocols, and eight released baseline methods.
Inputs are 8 continuous planet parameters plus the source GCM label. Outputs are time-averaged climate fields on a 32 x 64 latitude-longitude grid: three-dimensional variables are stored as pressure-level channels, and two-dimensional variables are stored as single-level fields.
Want to look around before downloading anything? Try the ThousandWorlds Explorer! Built by Hamza Ali Shahjahan!
Quickstart
The easiest way to use the benchmark is through the Python code:
git clone https://github.com/edstevenson/ThousandWorlds.git
cd ThousandWorlds
pip install -e .
import thousandworlds as tw
tw.download_dataset()
bundle = tw.load("single-complete", data_dir="dataset")
See the GitHub repository for the full quickstart, notebooks, baseline code, evaluation utilities, and reproducing paper results.
Files
The release includes:
archives/dataset.tar.gz: the ThousandWorlds dataset.archives/results-baselines-*.tar.gz: baseline predictions for the 3 subsets.croissant.json: Croissant metadata.archives/*.sha256: checksum sidecars.
Dataset Contents
The dataset contains gridded fields (NumPy), input metadata (CSV), predefined train/test splits, normalization statistics, and spherical harmonic coefficients plus inverse-SHT weights for spectral methods.
Subsets
The dataset is organized into three subsets of increasing complexity and realism:
| Subset | Simulations | Fields | Description |
|---|---|---|---|
single-complete |
256 | 48 | Smaller subset; simulations from a single GCM, complete observations only. |
multi-complete |
1659 | 48 | All 5 GCMs, still with no missing fields. |
multi-partial |
1760 | 53 | Full dataset; all 5 GCMs, with missing fields represented as NaNs. |
The subset split files contain:
| File | single-complete |
multi-complete |
multi-partial |
|---|---|---|---|
train.csv |
206 | 1538 | 1626 |
test.csv |
50 | 90 | 100 |
test_shared_planets_only.csv |
- | 58 | 60 |
held_out_aux.csv |
- | 31 | 34 |
held_out_aux.csv is excluded from train and test to prevent train-test leakage (it contains simulations from auxiliary GCMs that correspond to identical planets present in the test set).
Inputs
Each simulation has one row in dataset/inputs.csv, keyed by simulation_id.
The public model inputs are stellar temperature, stellar flux, radius, gravity,
rotation period, surface pressure, CO2, CH4, and gcm_label. The metadata also
includes is_target_gcm, in_target_physical_domain, planet_id, and
source.
| Parameter | Range |
|---|---|
| Radius (Earth radii) | [0.7, 1.4] |
| Surface gravity (m s^-2) | [6.0, 16.0] |
| Rotation period (days) | [0.1, 1000.0] |
| Surface pressure (bar) | [0.5, 5] |
| CO2 volume fraction (%) | [0, 100] |
| CH4 volume fraction (%) | [0, 5] |
| Incident stellar flux (W m^-2) | [500, 1500] |
| Stellar temperature (K) | [2500, 5800] |
Outputs
Target fields include surface temperature, 3D temperature, specific humidity, cloud fraction, east-west wind, north-south wind, absorbed shortwave radiation, and outgoing longwave radiation. Gridded targets are provided on a 32 x 64 latitude-longitude grid, with vertical fields stored on relative pressure levels.
| Variable | Dimensionality | Unit |
|---|---|---|
| Surface temperature | 2D | K |
| Temperature | 3D | K |
| Specific humidity | 3D | dex |
| Cloud fraction | 3D | 1 |
| East-west wind | 3D | m s^-1 |
| North-south wind | 3D | m s^-1 |
| Absorbed shortwave radiation | 2D | W m^-2 |
| Outgoing longwave radiation | 2D | W m^-2 |
The gridded field archives are:
| File | Shape | Contents |
|---|---|---|
dataset/fields/all-obs.npz |
(1760, 53, 32, 64) |
Field archive covering all 5 GCMs with structured whole-field missingness. |
dataset/fields/complete-obs-only.npz |
(1659, 48, 32, 64) |
Complete-observation field archive. |
Spectral Coefficients:
The spectral coefficient archives mirror those field archives with T21
spherical harmonic coefficients: dataset/coefficients/*.npz stores
coefficients with 484 coefficients per field and a field_mask for missing
fields. Whole-field missingness is represented as all-NaN gridded channels and
as false entries in the spectral field_mask.
Evaluation
The package includes loaders and metrics for two benchmark protocols:
- Standard: the main test protocol, ideal for ML model comparison.
- Shared-planets: evaluate on planets shared across target and auxiliary GCMs; used to assess performance relative to inter-GCM error, i.e. how close a model gets to the epistemic uncertainty floor of the problem.
Released baselines include train mean, kNN, PCA ridge, PCA-MLP, Coord-MLP, Coord-DeepONet, PPCA-ICM, and GPLFR. Baseline artifacts include predictions, resolved configs, and metrics JSON files.
Links
- DOI: https://doi.org/10.57967/hf/8695
- Code: https://github.com/edstevenson/ThousandWorlds
- Paper: https://arxiv.org/abs/2606.18338
Citation
If you use ThousandWorlds, please cite the paper:
@article{thousandworlds2026,
title = {ThousandWorlds: A benchmark for climate emulation of potentially habitable exoplanets},
author = {Stevenson, Edward T. and Mak, Mei Ting and Wolf, Eric and Sergeev, Denis E. and Hammond, Tobi and Mayne, N. J. and Cranmer, Miles},
year = {2026},
eprint = {2606.18338},
archivePrefix = {arXiv},
doi = {10.48550/arXiv.2606.18338}
}
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