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---
pretty_name: "OpenH-RF — eSAF Rotational 3D US Raw Channel Data (Medical FUSION Lab, WPI)"
license: cc-by-4.0
task_categories:
  - image-to-image
tags:
  - ultrasound
  - rf
  - openh-rf
  - 3d
  - beamforming
  - elevational-saf
language:
  - en
size_categories:
  - n<1K
---

# OpenH-RF Sub-Dataset — Rotational 3D US Raw Channel Data for Elevational SAF (Simulated + Measured Phantom)

> One `.hdf5` per acquisition, zea file format. Raw **per-element channel data**
> (pre-beamforming). See `manifest.json` for the full list and `../reconstruct.py`
> + `../pipeline.yaml` for the reference reconstruction.

## Dataset Description
Synthetic rotational 3D ultrasound acquisitions of point, pair, and off-axis targets, captured
with an **elevation-focused 1D linear array** that is rotated 180° about its axial
axis (1° steps, 180 frames). Each acquisition stores the **raw per-element channel
RF** for a single normal plane-wave transmit at every rotation angle — i.e. the data
*before* in-plane beamforming — which is what enables flexible offline beamforming and
the **elevational Synthetic Aperture Focusing (eSAF)** method. The targets span a wide
depth range to capture the depth-dependent elevational beam thickness (the artifact
eSAF corrects). The release is **mostly simulated (Field II)**, complemented by a
small set of **real measured phantom** rotational scans acquired with the physical
Japan Probe 68-element array (same geometry as the simulation) over a shallow-to-focal
depth series (10–45 mm). **Simulated + measured phantom** data (no in-vivo / subjects).

## Dataset Contributor(s)
Medical FUSION Laboratory, Worcester Polytechnic Institute. Contact: Ryo Murakami.

## Dataset Creation Date
06/15/2026.

## License / Terms of Use
CC BY 4.0 (see `LICENSE`). Simulated data — no IP/consent constraints.

## Intended Usage
Advanced beamforming and **elevational resolution recovery** for rotational 3D US
(eSAF), elevation-PSF / aperture-growth studies, and as a reproducible raw-channel-data
benchmark for rotational synthetic-aperture reconstruction.

## Dataset Characterization
- **Data Collection Method:** synthetic, generated with **Field II** (Jensen) run in
  **MATLAB**. The main release is a **probe × target grid** produced by
  `../sim/batch_sim_probe_target.m` (with `../sim/sim_probe_catalog.m` /
  `../sim/sim_target_catalog.m`): for each (probe type, target) it uses `xdc_focused_array`
  + `calc_scat_multi` to produce the raw per-element channel RF at every rotation angle
  (scatterer rotated about the axial axis, transducer fixed), then `../sim/sim_dataset_to_zea.py`
  repackages every case into the zea format here. **10 probe types** span lateral aperture
  (`n_el` 32/68/128, pitch 0.1/0.2/0.3 mm), elevation height `H` (4/8/12 mm), and elevation
  focal depth `R` (25/45/90 mm + unfocused) — see the probe table in `manifest.json`.
  (The earlier 18-acquisition set generated by `../sim/batch_generate_fieldii.m` +
  `../sim/mat_to_zea.py`, and a pure-Python analytic forward model `../sim/forward_sim.py`,
  remain available as compatible alternatives with the identical schema.)
  **Measured phantom acquisitions (5):** real rotational scans of the physical Japan
  Probe 68-element array on a wire/point phantom, acquired with CPWC channel-RF capture
  (`../experiment/Ryo_SetUp_JP68_PWCompound_3D_ChannelRF.m`) and a Galil-controlled 180°
  rotation. Each scan is time-tag-synced (frames → motor angles) and reduced to the
  **single centre (normal) plane wave per angle** by `../experiment/sync_channel_rf.m`
  (so the schema matches the simulation, n_tx = 1), then converted with the same
  `../sim/sim_dataset_to_zea.py`. They span a shallow-to-focal depth series (10, 20, 30,
  40, 45 mm nominal target depth).
- **Labeling Method:** synthetic ground truth (exact target positions known; in
  `manifest.json`).
- **Acquisition system (simulated):** Japan Probe JP_Linear_68 — 68-element linear
  array, pitch 0.2 mm, element width 0.15 mm, element height 8 mm, **elevational lens
  focus 45 mm** (Field II `xdc_focused_array` with 500 elevation math sub-elements);
  center frequency 10 MHz; sampling 40 MHz (NS200BW, 4 samples/wavelength); speed of
  sound 1490 m/s; single normal plane-wave transmit per rotation angle; 180° rotation,
  1° step (180 frames). Parameters match the paper simulation (`makeslices_field2.m`).

## Dataset Format
zea file format (HDF5), one file per acquisition. Pre-processing — *simulated:* none
beyond the forward model (raw RF, not demodulated/decimated); *measured:* time-tag
frame→angle synchronisation, per-angle dwell averaging, and centre-plane-wave selection
(still raw per-element RF, not demodulated/decimated). Rotation angle per frame is
stored as a zea **custom** element at `custom/scan/rotation_angles_deg`. Every file is
written with `zea.File.create()` (`../sim/sim_dataset_to_zea.py`) and carries a
`zea_version` stamp, so zea loads it natively (not as a legacy file).

**Paired pre-/post-SAF labels (the dataset's target output).** Each file also carries
the **elevational-SAF reconstructed 3D B-mode volume** at
`custom/labels/saf_bmode_volume` (with `custom/labels/saf_{x,y,z}_mm` axes). This is
the *post*-SAF **output/label** paired with the *pre*-beamformed **input** (`data/raw_data`):
the raw channel RF is back-projected through the published eSAF algorithm
(`../matlab/saf/safrot_backproj.m`: in-plane DAS → `recon_3d``safrot_backproj`,
elevational focus 45 mm, f-number 45/8) into a 3D volume `B_SAF(x,y,z)`, generated by
`../sim/make_saf_all.m``../experiment/run_esaf_synced.m` and written into the zea
file by `../sim/pack_saf_labels.py`. The stored volume is the normalized envelope over
a thin depth window (±2 mm) about the target; per-case arc-FWHM before/after and gain
are in `manifest.json` and on the dataset (`arc_fwhm_before_after_mm` attribute).

A **MATLAB `.mat` version** of the same raw channel data + metadata, plus a
**reference eSAF-beamformed** result and a `_ref.png` figure, is provided **per
acquisition** alongside the source grid as `sim_dataset_out/<probe>/<target>.mat`
and `..._ref.png` (each `.mat` holds the raw RF, the in-plane DAS, the metadata and
the eSAF output produced with the published algorithm `../matlab/saf/safrot_backproj.m`:
in-plane DAS → `recon_3d``safrot_backproj`, f-number 45/8). A FWHM-vs-depth
overview across probes is `sim_dataset_out/dataset_overview_r4.png`
(`../sim/dataset_overview.m`). The zea `.hdf5` acquisitions are **hosted on Hugging
Face** at <https://huggingface.co/datasets/RyoMurakami/OpenH-RF-eSAF> (git-LFS; not
committed to the GitHub code repo). The MATLAB `.mat`/`_ref.png` intermediates are
reproducible from source and kept on lab storage.

## Dataset Quantification
- **Acquisitions:** **195** = **190 simulated** + **5 measured phantom**.
  - *Simulated (190):* **10 probe types × 19 targets** (16 single points over depth
    {20,45,80,130} mm × radial offset from the rotation centre {0,2,4,6} mm, plus 3
    pair/oblique cases). The probe and target axes are listed in `manifest.json`. (The
    earlier compatible set has 18 acquisitions.)
  - *Measured (5):* real rotational phantom scans at nominal depths {10,20,30,40,45} mm
    (`experiment__acq_exp_*.hdf5`), centre plane wave, ~182 measured rotation angles
    over ~180°.
- **Frames per acquisition:** simulated 180 (one per 1° step); measured ~182 (the
  actual encoder angles are stored in `custom/scan/rotation_angles_deg`, not necessarily
  uniform).
- **Total size on disk:** simulated ~0.6–5 MB per case (zea gzip; point-target RF is
  sparse), measured ~80–92 MB per case (dense tissue RF); **~1.5 GB** for the full set
  (including the paired `saf_bmode_volume` labels).
- **Train/val/test split:** N/A (benchmark / characterization set; the probe × depth ×
  radius axes are the intended study dimensions).

### Per-sample feature table
| field (HDF5 path)                 | shape                          | dtype   | units | description |
|-----------------------------------|--------------------------------|---------|-------|-------------|
| `data/raw_data`                   | (180, 1, n_ax, 68, 1)          | float32 | a.u.  | raw per-element channel RF; dims = (frame=rotation, tx, axial, element, ch) |
| `scan/probe_geometry`             | (68, 3)                        | float32 | m     | element positions (lateral x, 0, 0) |
| `scan/sampling_frequency`         | scalar                         | float32 | Hz    | 4.0e7 |
| `scan/center_frequency`           | scalar                         | float32 | Hz    | 1.0e7 |
| `scan/sound_speed`                | scalar                         | float32 | m/s   | 1490 |
| `scan/initial_times`              | (1,)                           | float32 | s     | t0 (first-sample time) |
| `scan/t0_delays`                  | (1, 68)                        | float32 | s     | transmit delays (0; normal plane wave) |
| `scan/polar_angles`               | (1,)                           | float32 | rad   | transmit steering (0) |
| `custom/scan/rotation_angles_deg` | (180,)                         | float32 | deg   | probe rotation angle per frame (zea custom element) |
| `custom/labels/saf_bmode_volume`  | (n_el, n_el, n_z)              | float32 | a.u.  | **paired label**: elevational-SAF reconstructed 3D B-mode volume `B_SAF(x,y,z)` (normalized envelope) |
| `custom/labels/saf_x_mm` / `saf_y_mm` | (n_el,)                    | float32 | mm    | lateral / elevation axes of `saf_bmode_volume` |
| `custom/labels/saf_z_mm`          | (n_z,)                         | float32 | mm    | depth axis of `saf_bmode_volume` (target ± ~2 mm) |

## Subject Metadata
N/A (synthetic phantom; no subjects/PHI).

## Data Validation
`../reconstruct.py` (**runnable, verified** — official `zea` API, no fallback code)
loads one zea acquisition, reads its acquisition parameters via
`zea.Config.from_path('../pipeline.yaml')` + `File.load_parameters`, beamforms the
rotation frame closest to 90° (the frame where an off-axis target lies in-plane) with
the native `zea.Pipeline` op chain **Cast → Demodulate → Beamform(delay_and_sum) →
EnvelopeDetect → Normalize → LogCompress** defined in `../pipeline.yaml`, and writes a
two-panel PNG: the B-mode image, and the per-frame probe **rotation angle**
(`custom/scan/rotation_angles_deg`) so downstream users know how to interpret the
frame axis — the special data this dataset adds, per reviewer feedback:
```
python ../reconstruct.py --input data/<probe>__<target>.hdf5 --output out.png
```
The rotational **eSAF** across frames — the contribution of this dataset — is implemented in
`../matlab/saf` (`recon_3d``safrot_backproj`); per-probe before/after eSAF reference
images and a FWHM-vs-depth overview accompany the MATLAB `.mat` release
(`../sim/dataset_overview.m`), and the resulting paired `custom/labels/saf_bmode_volume`
is stored in every `.hdf5` (see Dataset Format above).

## Known Issues
- **Paired SAF label — on-axis targets (r0 = 0) do not narrow, by design.** eSAF
  refocuses the *rotational elevation smear*; a target sitting on the rotation axis has
  essentially no smear, so its `saf_bmode_volume` is not sharper than the input (arc-FWHM
  gain ≈ 1). This is expected physics, not a defect — the 40 on-axis cases (median gain
  1.00×) are included so the pair covers the degenerate no-smear case. Off-axis targets
  (n=120, median gain 1.75×, up to ~12×) and paired/oblique targets (n=30, median 3.71×)
  improve clearly; targets at the focal depth (~45 mm) and weak-elevation-focus probes
  (`efocus_deep_90`, `elev_unfocused`) have less smear to recover. Across all 195 cases,
  median arc-FWHM gain is 1.36× (42 cases < 1×, mostly the on-axis/near-focus group above).
  Arc-FWHM is measured on a **centred** reconstruction: the smear circle passes through both
  the rotation axis and the target (not a circle centred on the rotation axis). The eSAF
  back-projection uses a fixed elevational focus of 45 mm; per-depth focus tuning (see
  `../docs/eSAF_focus_depth_study_JP.md`) can further sharpen deep off-axis cases but was
  not applied here (single as-designed focus).
- **Measured phantom depth window.** The real reflector bead sits **~4 mm off the rotation
  axis** (not on-axis) and, for each scan, slightly deeper than the folder's nominal depth
  label; labels are reconstructed over the interactively-identified reflector depth window
  (not a naive nominal-depth ± 2 mm window), which matters because a mis-centred window can
  pick up near-axis clutter instead of the actual bead.
- **Simulated** data (Field II spatial-impulse-response model): realistic transducer
  field, but no tissue attenuation, aberration, multiple scattering, or electronic
  noise. Not a substitute for measured data.
- Speed of sound is 1490 m/s, matching the paper Table 1 and the experiment.
- A single normal plane-wave transmit per rotation angle is simulated (the dataset
  stores n_tx = 1); multi-angle compounding is left to downstream users.
- **Measured scans:** acquired as 7-angle CPWC; only the **centre (0°) plane wave** is
  kept here to match the n_tx = 1 schema. The dwell frames per angle are averaged before
  storage (noise reduction). Real reflectors are not ideal point scatterers — expect
  reverberation/clutter near the surface and specular layering; rotation angles are the
  measured encoder values (slightly non-uniform, full span ≈ 180°, sign per encoder
  direction). The elevational lens focus is the nominal 45 mm, but the effective
  back-projection focus for eSAF is depth-dependent on real data (see
  `../docs/eSAF_focus_depth_study_JP.md`).

## Raw Source Data
The raw, pre-conversion acquisition/simulation outputs that were processed into the
zea `.hdf5` files above are archived (same CC BY 4.0 license) at
<https://huggingface.co/datasets/RyoMurakami/OpenH-RF-eSAF-raw>: the raw Verasonics
per-line channel-RF captures (`RFdata_line*.mat` + encoder logs) for the 5 measured
acquisitions, and the per-case MATLAB intermediates (raw RF, in-plane DAS, eSAF
output) for the 190 simulated cases. See that repository's README for how each
maps to `data/*.hdf5` here.

## Ethical Considerations
None. The data is either fully synthetic (Field II) or measured on an **inanimate
phantom** — no human or animal subjects, no PHI, no consent/IRB constraints.