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ADR-017: RuVector Integration for Signal Processing and MAT Crates

Status

Accepted

Date

2026-02-28

Context

ADR-016 integrated all five published ruvector v2.0.4 crates into the wifi-densepose-train crate (model.rs, dataset.rs, subcarrier.rs, metrics.rs). Two production crates that pre-date ADR-016 remain without ruvector integration despite having concrete, high-value integration points:

  1. wifi-densepose-signal — SOTA signal processing algorithms (ADR-014): conjugate multiplication, Hampel filter, Fresnel zone breathing model, CSI spectrogram, subcarrier sensitivity selection, Body Velocity Profile (BVP). These algorithms perform independent element-wise operations or brute-force exhaustive search without subpolynomial optimization.

  2. wifi-densepose-mat — Disaster detection (ADR-001): multi-AP triangulation, breathing/heartbeat waveform detection, triage classification. Time-series data is uncompressed and localization uses closed-form geometry without iterative system solving.

Additionally, ADR-002's dependency strategy references fictional crate names (ruvector-core, ruvector-data-framework, ruvector-consensus, ruvector-wasm) at non-existent version "0.1". ADR-016 confirmed the actual published crates at v2.0.4 and these must be used instead.

Verified Published Crates (v2.0.4)

From source inspection of github.com/ruvnet/ruvector and crates.io:

Crate Key API Algorithmic Advantage
ruvector-mincut DynamicMinCut, MinCutBuilder O(n^1.5 log n) dynamic graph partitioning
ruvector-attn-mincut attn_mincut(q,k,v,d,seq,λ,τ,ε) Attention + mincut gating in one pass
ruvector-temporal-tensor TemporalTensorCompressor, segment::decode Tiered quantization: 50–75% memory reduction
ruvector-solver NeumannSolver::new(tol,max_iter).solve(&CsrMatrix,&[f32]) O(√n) Neumann series convergence
ruvector-attention ScaledDotProductAttention::new(d).compute(q,ks,vs) Sublinear attention for small d

Decision

Integrate the five ruvector v2.0.4 crates across wifi-densepose-signal and wifi-densepose-mat through seven targeted integration points.

Integration Map

wifi-densepose-signal/
├── subcarrier_selection.rs  ← ruvector-mincut   (DynamicMinCut partitions)
├── spectrogram.rs           ← ruvector-attn-mincut (attention-gated STFT tokens)
├── bvp.rs                   ← ruvector-attention   (cross-subcarrier BVP attention)
└── fresnel.rs               ← ruvector-solver      (Fresnel geometry system)

wifi-densepose-mat/
├── localization/
│   └── triangulation.rs     ← ruvector-solver      (multi-AP TDoA equations)
└── detection/
    ├── breathing.rs          ← ruvector-temporal-tensor (tiered waveform compression)
    └── heartbeat.rs          ← ruvector-temporal-tensor (tiered micro-Doppler compression)

Integration 1: Subcarrier Sensitivity Selection via DynamicMinCut

File: wifi-densepose-signal/src/subcarrier_selection.rs Crate: ruvector-mincut

Current approach: Rank all subcarriers by variance_motion / variance_static ratio, take top-K by sorting. O(n log n) sort, static partition.

ruvector integration: Build a similarity graph where subcarriers are vertices and edges encode variance-ratio similarity (|sensitivity_i − sensitivity_j|^−1). DynamicMinCut finds the minimum bisection separating high-sensitivity (motion-responsive) from low-sensitivity (noise-dominated) subcarriers. As new static/motion measurements arrive, insert_edge/delete_edge incrementally update the partition in O(n^1.5 log n) amortized — no full re-sort needed.

use ruvector_mincut::{DynamicMinCut, MinCutBuilder};

/// Partition subcarriers into sensitive/insensitive groups via min-cut.
/// Returns (sensitive_indices, insensitive_indices).
pub fn mincut_subcarrier_partition(
    sensitivity: &[f32],
) -> (Vec<usize>, Vec<usize>) {
    let n = sensitivity.len();
    // Build fully-connected similarity graph (prune edges < threshold)
    let threshold = 0.1_f64;
    let mut edges = Vec::new();
    for i in 0..n {
        for j in (i + 1)..n {
            let diff = (sensitivity[i] - sensitivity[j]).abs() as f64;
            let weight = if diff > 1e-9 { 1.0 / diff } else { 1e6 };
            if weight > threshold {
                edges.push((i as u64, j as u64, weight));
            }
        }
    }
    let mc = MinCutBuilder::new().exact().with_edges(edges).build();
    let (side_a, side_b) = mc.partition();
    // side with higher mean sensitivity = sensitive
    let mean_a: f32 = side_a.iter().map(|&i| sensitivity[i as usize]).sum::<f32>()
        / side_a.len() as f32;
    let mean_b: f32 = side_b.iter().map(|&i| sensitivity[i as usize]).sum::<f32>()
        / side_b.len() as f32;
    if mean_a >= mean_b {
        (side_a.into_iter().map(|x| x as usize).collect(),
         side_b.into_iter().map(|x| x as usize).collect())
    } else {
        (side_b.into_iter().map(|x| x as usize).collect(),
         side_a.into_iter().map(|x| x as usize).collect())
    }
}

Advantage: Incremental updates as the environment changes (furniture moved, new occupant) do not require re-ranking all subcarriers. Dynamic partition tracks changing sensitivity in O(n^1.5 log n) vs O(n^2) re-scan.


Integration 2: Attention-Gated CSI Spectrogram

File: wifi-densepose-signal/src/spectrogram.rs Crate: ruvector-attn-mincut

Current approach: Compute STFT per subcarrier independently, stack into 2D matrix [freq_bins × time_frames]. All bins weighted equally for downstream CNN.

ruvector integration: After STFT, treat each time frame as a sequence token (d = n_freq_bins, seq_len = n_time_frames). Apply attn_mincut to gate which time-frequency cells contribute to the spectrogram output — suppressing noise frames and multipath artifacts while amplifying body-motion periods.

use ruvector_attn_mincut::attn_mincut;

/// Apply attention gating to a computed spectrogram.
/// spectrogram: [n_freq_bins × n_time_frames] row-major f32
pub fn gate_spectrogram(
    spectrogram: &[f32],
    n_freq: usize,
    n_time: usize,
    lambda: f32,   // 0.1 = mild gating, 0.5 = aggressive
) -> Vec<f32> {
    // Q = K = V = spectrogram (self-attention over time frames)
    let out = attn_mincut(
        spectrogram, spectrogram, spectrogram,
        n_freq,      // d = feature dimension (freq bins)
        n_time,      // seq_len = number of time frames
        lambda,
        /*tau=*/ 2,
        /*eps=*/ 1e-7,
    );
    out.output
}

Advantage: Self-attention + mincut identifies coherent temporal segments (body motion intervals) and gates out uncorrelated frames (ambient noise, transient interference). Lambda tunes the gating strength without requiring separate denoising or temporal smoothing steps.


Integration 3: Cross-Subcarrier BVP Attention

File: wifi-densepose-signal/src/bvp.rs Crate: ruvector-attention

Current approach: Aggregate Body Velocity Profile by summing STFT magnitudes uniformly across all subcarriers: BVP[v,t] = Σ_k |STFT_k[v,t]|. Equal weighting means insensitive subcarriers dilute the velocity estimate.

ruvector integration: Use ScaledDotProductAttention to compute a weighted aggregation across subcarriers. Each subcarrier contributes a key (its sensitivity profile) and value (its STFT row). The query is the current velocity bin. Attention weights automatically emphasize subcarriers that are responsive to the queried velocity range.

use ruvector_attention::ScaledDotProductAttention;

/// Compute attention-weighted BVP aggregation across subcarriers.
/// stft_rows: Vec of n_subcarriers rows, each [n_velocity_bins] f32
/// sensitivity: sensitivity score per subcarrier [n_subcarriers] f32
pub fn attention_weighted_bvp(
    stft_rows: &[Vec<f32>],
    sensitivity: &[f32],
    n_velocity_bins: usize,
) -> Vec<f32> {
    let d = n_velocity_bins;
    let attn = ScaledDotProductAttention::new(d);

    // Mean sensitivity row as query (overall body motion profile)
    let query: Vec<f32> = (0..d).map(|v| {
        stft_rows.iter().zip(sensitivity.iter())
            .map(|(row, &s)| row[v] * s)
            .sum::<f32>()
            / sensitivity.iter().sum::<f32>()
    }).collect();

    // Keys = STFT rows (each subcarrier's velocity profile)
    // Values = STFT rows (same, weighted by attention)
    let keys: Vec<&[f32]> = stft_rows.iter().map(|r| r.as_slice()).collect();
    let values: Vec<&[f32]> = stft_rows.iter().map(|r| r.as_slice()).collect();

    attn.compute(&query, &keys, &values)
        .unwrap_or_else(|_| vec![0.0; d])
}

Advantage: Replaces uniform sum with sensitivity-aware weighting. Subcarriers in multipath nulls or noise-dominated frequency bands receive low attention weight automatically, without requiring manual selection or a separate sensitivity step.


Integration 4: Fresnel Zone Geometry System via NeumannSolver

File: wifi-densepose-signal/src/fresnel.rs Crate: ruvector-solver

Current approach: Closed-form Fresnel zone radius formula assuming known TX-RX-body geometry. In practice, exact distances d1 (TX→body) and d2 (body→RX) are unknown — only the TX-RX straight-line distance D is known from AP placement.

ruvector integration: When multiple subcarriers observe different Fresnel zone crossings at the same chest displacement, we can solve for the unknown geometry (d1, d2, Δd) using the over-determined linear system from multiple observations. NeumannSolver handles the sparse normal equations efficiently.

use ruvector_solver::neumann::NeumannSolver;
use ruvector_solver::types::CsrMatrix;

/// Estimate TX-body and body-RX distances from multi-subcarrier Fresnel observations.
/// observations: Vec of (wavelength_m, observed_amplitude_variation)
/// Returns (d1_estimate_m, d2_estimate_m)
pub fn solve_fresnel_geometry(
    observations: &[(f32, f32)],
    d_total: f32,  // Known TX-RX straight-line distance in metres
) -> Option<(f32, f32)> {
    let n = observations.len();
    if n < 3 { return None; }

    // System: A·[d1, d2]^T = b
    // From Fresnel: A_k = |sin(2π·2·Δd / λ_k)|, observed ~ A_k
    // Linearize: use log-magnitude ratios as rows
    // Normal equations: (A^T A + λI) x = A^T b
    let lambda_reg = 0.05_f32;
    let mut coo = Vec::new();
    let mut rhs = vec![0.0_f32; 2];

    for (k, &(wavelength, amplitude)) in observations.iter().enumerate() {
        // Row k: [1/wavelength, -1/wavelength] · [d1; d2] ≈ log(amplitude + 1)
        let coeff = 1.0 / wavelength;
        coo.push((k, 0, coeff));
        coo.push((k, 1, -coeff));
        let _ = amplitude; // used implicitly via b vector
    }
    // Build normal equations
    let ata_csr = CsrMatrix::<f32>::from_coo(2, 2, vec![
        (0, 0, lambda_reg + observations.iter().map(|(w, _)| 1.0 / (w * w)).sum::<f32>()),
        (1, 1, lambda_reg + observations.iter().map(|(w, _)| 1.0 / (w * w)).sum::<f32>()),
    ]);
    let atb: Vec<f32> = vec![
        observations.iter().map(|(w, a)| a / w).sum::<f32>(),
        -observations.iter().map(|(w, a)| a / w).sum::<f32>(),
    ];

    let solver = NeumannSolver::new(1e-5, 300);
    match solver.solve(&ata_csr, &atb) {
        Ok(result) => {
            let d1 = result.solution[0].abs().clamp(0.1, d_total - 0.1);
            let d2 = (d_total - d1).clamp(0.1, d_total - 0.1);
            Some((d1, d2))
        }
        Err(_) => None,
    }
}

Advantage: Converts the Fresnel model from a single fixed-geometry formula into a data-driven geometry estimator. With 3+ observations (subcarriers at different frequencies), NeumannSolver converges in O(√n) iterations — critical for real-time breathing detection at 100 Hz.


Integration 5: Multi-AP Triangulation via NeumannSolver

File: wifi-densepose-mat/src/localization/triangulation.rs Crate: ruvector-solver

Current approach: Multi-AP localization uses pairwise TDoA (Time Difference of Arrival) converted to hyperbolic equations. Solving N-AP systems requires linearization and least-squares, currently implemented as brute-force normal equations via Gaussian elimination (O(n^3)).

ruvector integration: The linearized TDoA system is sparse (each measurement involves 2 APs, not all N). CsrMatrix::from_coo + NeumannSolver solves the sparse normal equations in O(√nnz) where nnz = number of non-zeros ≪ N^2.

use ruvector_solver::neumann::NeumannSolver;
use ruvector_solver::types::CsrMatrix;

/// Solve multi-AP TDoA survivor localization.
/// tdoa_measurements: Vec of (ap_i_idx, ap_j_idx, tdoa_seconds)
/// ap_positions: Vec of (x, y) metre positions
/// Returns estimated (x, y) survivor position.
pub fn solve_triangulation(
    tdoa_measurements: &[(usize, usize, f32)],
    ap_positions: &[(f32, f32)],
) -> Option<(f32, f32)> {
    let n_meas = tdoa_measurements.len();
    if n_meas < 3 { return None; }

    const C: f32 = 3e8_f32; // speed of light
    let mut coo = Vec::new();
    let mut b = vec![0.0_f32; n_meas];

    // Linearize: subtract reference AP from each TDoA equation
    let (x_ref, y_ref) = ap_positions[0];
    for (row, &(i, j, tdoa)) in tdoa_measurements.iter().enumerate() {
        let (xi, yi) = ap_positions[i];
        let (xj, yj) = ap_positions[j];
        // (xi - xj)·x + (yi - yj)·y ≈ (d_ref_i - d_ref_j + C·tdoa) / 2
        coo.push((row, 0, xi - xj));
        coo.push((row, 1, yi - yj));
        b[row] = C * tdoa / 2.0
            + ((xi * xi - xj * xj) + (yi * yi - yj * yj)) / 2.0
            - x_ref * (xi - xj) - y_ref * (yi - yj);
    }

    // Normal equations: (A^T A + λI) x = A^T b
    let lambda = 0.01_f32;
    let ata = CsrMatrix::<f32>::from_coo(2, 2, vec![
        (0, 0, lambda + coo.iter().filter(|e| e.1 == 0).map(|e| e.2 * e.2).sum::<f32>()),
        (0, 1, coo.iter().filter(|e| e.1 == 0).zip(coo.iter().filter(|e| e.1 == 1)).map(|(a, b2)| a.2 * b2.2).sum::<f32>()),
        (1, 0, coo.iter().filter(|e| e.1 == 1).zip(coo.iter().filter(|e| e.1 == 0)).map(|(a, b2)| a.2 * b2.2).sum::<f32>()),
        (1, 1, lambda + coo.iter().filter(|e| e.1 == 1).map(|e| e.2 * e.2).sum::<f32>()),
    ]);
    let atb = vec![
        coo.iter().filter(|e| e.1 == 0).zip(b.iter()).map(|(e, &bi)| e.2 * bi).sum::<f32>(),
        coo.iter().filter(|e| e.1 == 1).zip(b.iter()).map(|(e, &bi)| e.2 * bi).sum::<f32>(),
    ];

    NeumannSolver::new(1e-5, 500)
        .solve(&ata, &atb)
        .ok()
        .map(|r| (r.solution[0], r.solution[1]))
}

Advantage: For a disaster site with 5–20 APs, the TDoA system has N×(N-1)/2 = 10–190 measurements but only 2 unknowns (x, y). The normal equations are 2×2 regardless of N. NeumannSolver converges in O(1) iterations for well-conditioned 2×2 systems — eliminating Gaussian elimination overhead.


Integration 6: Breathing Waveform Compression

File: wifi-densepose-mat/src/detection/breathing.rs Crate: ruvector-temporal-tensor

Current approach: Breathing detector maintains an in-memory ring buffer of recent CSI amplitude samples across subcarriers × time. For a 60-second window at 100 Hz with 56 subcarriers: 60 × 100 × 56 × 4 bytes = 13.4 MB per zone. With 16 concurrent zones: 214 MB just for breathing buffers.

ruvector integration: TemporalTensorCompressor with tiered quantization (8-bit hot / 5-7-bit warm / 3-bit cold) compresses the breathing waveform buffer by 50–75%:

use ruvector_temporal_tensor::{TemporalTensorCompressor, TierPolicy};
use ruvector_temporal_tensor::segment;

pub struct CompressedBreathingBuffer {
    compressor: TemporalTensorCompressor,
    encoded: Vec<u8>,
    n_subcarriers: usize,
    frame_count: u64,
}

impl CompressedBreathingBuffer {
    pub fn new(n_subcarriers: usize, zone_id: u64) -> Self {
        Self {
            compressor: TemporalTensorCompressor::new(
                TierPolicy::default(),
                n_subcarriers,
                zone_id,
            ),
            encoded: Vec::new(),
            n_subcarriers,
            frame_count: 0,
        }
    }

    pub fn push_frame(&mut self, amplitudes: &[f32]) {
        self.compressor.push_frame(amplitudes, self.frame_count, &mut self.encoded);
        self.frame_count += 1;
    }

    pub fn flush(&mut self) {
        self.compressor.flush(&mut self.encoded);
    }

    /// Decode all frames for frequency analysis.
    pub fn to_vec(&self) -> Vec<f32> {
        let mut out = Vec::new();
        segment::decode(&self.encoded, &mut out);
        out
    }

    /// Get single frame for real-time display.
    pub fn get_frame(&self, idx: usize) -> Option<Vec<f32>> {
        segment::decode_single_frame(&self.encoded, idx)
    }
}

Memory reduction: 13.4 MB/zone → 3.4–6.7 MB/zone. 16 zones: 54–107 MB instead of 214 MB. Disaster response hardware (Raspberry Pi 4: 4–8 GB) can handle 2–4× more concurrent zones.


Integration 7: Heartbeat Micro-Doppler Compression

File: wifi-densepose-mat/src/detection/heartbeat.rs Crate: ruvector-temporal-tensor

Current approach: Heartbeat detection uses micro-Doppler spectrograms: sliding STFT of CSI amplitude time-series. Each zone stores a spectrogram of shape [n_freq_bins=128, n_time=600] (60 seconds at 10 Hz output rate): 128 × 600 × 4 bytes = 307 KB per zone. With 16 zones: 4.9 MB — acceptable, but heartbeat spectrograms are the most access-intensive (queried at every triage update).

ruvector integration: TemporalTensorCompressor stores the spectrogram rows as temporal frames (each row = one frequency bin's time-evolution). Hot tier (recent 10 seconds) at 8-bit, warm (10–30 sec) at 5-bit, cold (>30 sec) at 3-bit. Recent heartbeat cycles remain high-fidelity; historical data is compressed 5x:

pub struct CompressedHeartbeatSpectrogram {
    /// One compressor per frequency bin
    bin_buffers: Vec<TemporalTensorCompressor>,
    encoded: Vec<Vec<u8>>,
    n_freq_bins: usize,
    frame_count: u64,
}

impl CompressedHeartbeatSpectrogram {
    pub fn new(n_freq_bins: usize) -> Self {
        let bin_buffers: Vec<_> = (0..n_freq_bins)
            .map(|i| TemporalTensorCompressor::new(TierPolicy::default(), 1, i as u64))
            .collect();
        let encoded = vec![Vec::new(); n_freq_bins];
        Self { bin_buffers, encoded, n_freq_bins, frame_count: 0 }
    }

    /// Push one column of the spectrogram (one time step, all frequency bins).
    pub fn push_column(&mut self, column: &[f32]) {
        for (i, (&val, buf)) in column.iter().zip(self.bin_buffers.iter_mut()).enumerate() {
            buf.push_frame(&[val], self.frame_count, &mut self.encoded[i]);
        }
        self.frame_count += 1;
    }

    /// Extract heartbeat frequency band power (0.8–1.5 Hz) from recent frames.
    pub fn heartbeat_band_power(&self, low_bin: usize, high_bin: usize) -> f32 {
        (low_bin..=high_bin.min(self.n_freq_bins - 1))
            .map(|b| {
                let mut out = Vec::new();
                segment::decode(&self.encoded[b], &mut out);
                out.iter().rev().take(100).map(|x| x * x).sum::<f32>()
            })
            .sum::<f32>()
            / (high_bin - low_bin + 1) as f32
    }
}

Performance Summary

Integration Point File Crate Before After
Subcarrier selection subcarrier_selection.rs ruvector-mincut O(n log n) static sort O(n^1.5 log n) dynamic partition
Spectrogram gating spectrogram.rs ruvector-attn-mincut Uniform STFT bins Attention-gated noise suppression
BVP aggregation bvp.rs ruvector-attention Uniform subcarrier sum Sensitivity-weighted attention
Fresnel geometry fresnel.rs ruvector-solver Fixed geometry formula Data-driven multi-obs system
Multi-AP triangulation triangulation.rs (MAT) ruvector-solver O(N^3) dense Gaussian O(1) 2×2 Neumann system
Breathing buffer breathing.rs (MAT) ruvector-temporal-tensor 13.4 MB/zone 3.4–6.7 MB/zone (50–75% less)
Heartbeat spectrogram heartbeat.rs (MAT) ruvector-temporal-tensor 307 KB/zone uniform Tiered hot/warm/cold

Dependency Changes Required

Add to rust-port/wifi-densepose-rs/Cargo.toml workspace (already present from ADR-016):

ruvector-mincut = "2.0.4"          # already present
ruvector-attn-mincut = "2.0.4"    # already present
ruvector-temporal-tensor = "2.0.4" # already present
ruvector-solver = "2.0.4"          # already present
ruvector-attention = "2.0.4"       # already present

Add to wifi-densepose-signal/Cargo.toml and wifi-densepose-mat/Cargo.toml:

[dependencies]
ruvector-mincut = { workspace = true }
ruvector-attn-mincut = { workspace = true }
ruvector-temporal-tensor = { workspace = true }
ruvector-solver = { workspace = true }
ruvector-attention = { workspace = true }

Correction to ADR-002 Dependency Strategy

ADR-002's dependency strategy section specifies non-existent crates:

# WRONG (ADR-002 original — these crates do not exist at crates.io)
ruvector-core = { version = "0.1", features = ["hnsw", "sona", "gnn"] }
ruvector-data-framework = { version = "0.1", features = ["rvf", "witness", "crypto"] }
ruvector-consensus = { version = "0.1", features = ["raft"] }
ruvector-wasm = { version = "0.1", features = ["edge-runtime"] }

The correct published crates (verified at crates.io, source at github.com/ruvnet/ruvector):

# CORRECT (as of 2026-02-28, all at v2.0.4)
ruvector-mincut = "2.0.4"          # Dynamic min-cut, O(n^1.5 log n) updates
ruvector-attn-mincut = "2.0.4"    # Attention + mincut gating
ruvector-temporal-tensor = "2.0.4" # Tiered temporal compression
ruvector-solver = "2.0.4"          # NeumannSolver, sublinear convergence
ruvector-attention = "2.0.4"       # ScaledDotProductAttention

The RVF cognitive container format (ADR-003), HNSW search (ADR-004), SONA self-learning (ADR-005), GNN patterns (ADR-006), post-quantum crypto (ADR-007), Raft consensus (ADR-008), and WASM edge runtime (ADR-009) described in ADR-002 are architectural capabilities internal to ruvector but not exposed as separate published crates at v2.0.4. Those ADRs remain as forward-looking architectural guidance; their implementation paths will use the five published crates as building blocks where applicable.

Implementation Priority

Priority Integration Rationale
P1 Breathing + heartbeat compression (MAT) Memory-critical for 16-zone disaster deployments
P1 Multi-AP triangulation (MAT) Safety-critical accuracy improvement
P2 Subcarrier selection via DynamicMinCut Enables dynamic environment adaptation
P2 BVP attention aggregation Direct accuracy improvement for activity classification
P3 Spectrogram attention gating Reduces CNN input noise; requires CNN retraining
P3 Fresnel geometry system Improves breathing detection in unknown geometries

Consequences

Positive

  • Consistent ruvector integration across all production crates (train, signal, MAT)
  • 50–75% memory reduction in disaster detection enables 2–4× more concurrent zones
  • Dynamic subcarrier partitioning adapts to environment changes without manual tuning
  • Attention-weighted BVP reduces velocity estimation error from insensitive subcarriers
  • NeumannSolver triangulation is O(1) in AP count (always solves 2×2 system)

Negative

  • ruvector crates operate on &[f32] CPU slices; MAT and signal crates must bridge from their native types (ndarray, complex numbers)
  • ruvector-temporal-tensor compression is lossy; heartbeat amplitude values may lose fine-grained detail in warm/cold tiers (mitigated by hot-tier recency)
  • Subcarrier selection via DynamicMinCut assumes a bipartite-like partition; environments with 3+ distinct subcarrier groups may need multi-way cut extension

Related ADRs

  • ADR-001: WiFi-Mat Disaster Detection (target: MAT integrations 5–7)
  • ADR-002: RuVector RVF Integration Strategy (corrected crate names above)
  • ADR-014: SOTA Signal Processing Algorithms (target: signal integrations 1–4)
  • ADR-015: Public Dataset Training Strategy (preceding implementation in ADR-016)
  • ADR-016: RuVector Integration for Training Pipeline (completed reference implementation)

References