Commit
·
1b9bc05
1
Parent(s):
ed4b727
Update the heatmap.jsonl
Browse files- .gitattributes +1 -0
- README.md +64 -0
- heatmap.jsonl +3 -0
.gitattributes
CHANGED
|
@@ -57,3 +57,4 @@ saved_model/**/* filter=lfs diff=lfs merge=lfs -text
|
|
| 57 |
# Video files - compressed
|
| 58 |
*.mp4 filter=lfs diff=lfs merge=lfs -text
|
| 59 |
*.webm filter=lfs diff=lfs merge=lfs -text
|
|
|
|
|
|
| 57 |
# Video files - compressed
|
| 58 |
*.mp4 filter=lfs diff=lfs merge=lfs -text
|
| 59 |
*.webm filter=lfs diff=lfs merge=lfs -text
|
| 60 |
+
*.jsonl filter=lfs diff=lfs merge=lfs -text
|
README.md
CHANGED
|
@@ -1,3 +1,67 @@
|
|
| 1 |
---
|
| 2 |
license: apache-2.0
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 3 |
---
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
---
|
| 2 |
license: apache-2.0
|
| 3 |
+
datasets:
|
| 4 |
+
- thermbench
|
| 5 |
+
tags:
|
| 6 |
+
- benchmark
|
| 7 |
+
- heatmap
|
| 8 |
+
- source-localization
|
| 9 |
+
- synthetic-data
|
| 10 |
+
pretty_name: ThermBench
|
| 11 |
---
|
| 12 |
+
|
| 13 |
+
# ThermBench 🔥: Heat Source Localization Benchmark
|
| 14 |
+
|
| 15 |
+
## Summary
|
| 16 |
+
**ThermBench** is a synthetic benchmark dataset for evaluating algorithms that infer hidden **heat sources** from a **2D heatmap**.
|
| 17 |
+
Each sample consists of an observed grid (matrix of thermal intensities) and the true underlying source positions and strengths.
|
| 18 |
+
The diffusion rule is based on inverse Manhattan distance:
|
| 19 |
+
|
| 20 |
+
\[
|
| 21 |
+
H(i,j) \;=\; \sum_{s=1}^K \frac{I_s}{d_{s,(i,j)}+1}
|
| 22 |
+
\]
|
| 23 |
+
|
| 24 |
+
where \(I_s\) is the source intensity and \(d\) is the Manhattan distance from source \(s\) to grid cell \((i,j)\).
|
| 25 |
+
|
| 26 |
+
## Dataset Structure
|
| 27 |
+
- **`input_text`**: Heatmap input following problem format:
|
| 28 |
+
- First line: grid size `N M`
|
| 29 |
+
- Second line: number of sources `K`
|
| 30 |
+
- Then `N` rows of grid heat values
|
| 31 |
+
- **`output_text`**: Ground-truth sources (row, col, intensity)
|
| 32 |
+
- **`level`**: Difficulty tier (`very_easy`, `easy`, `medium`, `hard`, `extreme`)
|
| 33 |
+
|
| 34 |
+
Example:
|
| 35 |
+
```json
|
| 36 |
+
{
|
| 37 |
+
"level": "easy",
|
| 38 |
+
"input_text": "5 5\n2\n10 8 6 5 4\n8 10 7 6 5\n...",
|
| 39 |
+
"output_text": "1 1 10.0\n5 5 10.0"
|
| 40 |
+
}
|
| 41 |
+
```
|
| 42 |
+
|
| 43 |
+
## Difficulty Levels
|
| 44 |
+
- `very_easy`: 3×3 grid, 1 source
|
| 45 |
+
- `easy`: 5×5 grid, 2 sources
|
| 46 |
+
- `medium`: 10×10 grid, 3 sources
|
| 47 |
+
- `hard`: 20×20 grid, 5 sources
|
| 48 |
+
- `extreme`: 30×30 grid, 7 sources
|
| 49 |
+
|
| 50 |
+
Each level contains **100 samples** (total: 500 entries).
|
| 51 |
+
A **fuzzy variant** (`thermbench-fuzzy`) introduces noise, source jitter, and decay variations to simulate real-world uncertainty.
|
| 52 |
+
|
| 53 |
+
## Usage
|
| 54 |
+
```python
|
| 55 |
+
from datasets import load_dataset
|
| 56 |
+
|
| 57 |
+
ds = load_dataset("username/thermbench", split="train")
|
| 58 |
+
print(ds[0])
|
| 59 |
+
```
|
| 60 |
+
|
| 61 |
+
## Applications
|
| 62 |
+
- Algorithmic evaluation of source localization
|
| 63 |
+
- Benchmarking robustness against noise
|
| 64 |
+
- Teaching problem-solving with synthetic physics-based data
|
| 65 |
+
|
| 66 |
+
## License
|
| 67 |
+
Apache License, Version 2.0
|
heatmap.jsonl
ADDED
|
@@ -0,0 +1,3 @@
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
version https://git-lfs.github.com/spec/v1
|
| 2 |
+
oid sha256:dbf1335bc5e3b0c199466b2d62520855aecca41f1af6b64ca1984a02d0b85e78
|
| 3 |
+
size 655819
|