FFT for real and complex signals. Split-radix real FFT + radix-2 complex FFT. Precomputed twiddle factors, typed-array buffers, zero dependencies.
import rfft from 'fourier-transform'
// magnitude spectrum (N/2 bins)
const spectrum = rfft(waveform)
import { fft } from 'fourier-transform'
// complex DFT of real input (N/2+1 bins, unnormalized)
const [re, im] = fft(waveform)
import { cfft, cifft } from 'fourier-transform'
// in-place complex FFT / inverse FFT
const re = new Float64Array(N), im = new Float64Array(N)
cfft(re, im) // forward
cifft(re, im) // inverse (1/N normalized)
rfft(input, output?) — default exportReturns magnitude spectrum as Float64Array of length N/2.
input — Float32Array, Float64Array, or plain Array. Length must be power of 2 (>= 2).output — optional Float64Array(N/2) to write into.Normalization: a unit-amplitude cosine at frequency bin k produces spectrum[k] = 1.0.
fft(input, output?) — named exportReturns complex DFT as [re, im], each Float64Array of length N/2+1 (DC through Nyquist).
output — optional [Float64Array(N/2+1), Float64Array(N/2+1)].X[k] = sum( x[n] * e^(-j*2*pi*k*n/N) ).im = 0 (real input).ifft(re, im, output?) — named exportInverse of fft() — recovers time-domain signal from complex spectrum. Returns Float64Array of length N.
re, im — Float64Array of length N/2+1 (as returned by fft()).im[0] and im[N/2] are ignored (half-complex format has no slot for them).const [re, im] = fft(signal)
// modify spectrum...
const recovered = ifft(re, im)
cfft(re, im) — named exportIn-place complex forward FFT (unnormalized). Both re and im must be Float64Array of equal power-of-2 length (>= 2). Modifies arrays in place.
cifft(re, im) — named exportIn-place complex inverse FFT (1/N normalized). Same signature as cfft.
import { stft, istft, stftBatch, stftStream, stftAnalysisStream } from 'fourier-transform/stft'
stft(signal, opts?) — analysisReturns an array of frames, each with { re, im, mag, phase, time }.
signal — Float32Array, Float64Array, or plain Array.opts.frameSize — FFT size, power of 2. Default: 2048.opts.hopSize — hop between frames. Default: frameSize / 4.time is the sample index of the frame centre in the original signal.frameSize at front and back so edge samples are fully windowed.const frames = stft(waveform, { frameSize: 2048, hopSize: 512 })
for (const f of frames) {
console.log(f.time, f.mag[100]) // time in samples, magnitude at bin 100
}
istft(frames, opts?) — synthesisReconstructs a time-domain signal from STFT frames.
frames — array of { mag, phase, time? } or { re, im, time? } objects.opts.signalLength — expected output length. Inferred from last frame if omitted.
signalLength for exact control.Float64Array.re/im are present, they are used directly (no polar round-trip). Otherwise mag/phase are converted to cartesian.const recovered = istft(frames, { frameSize: 2048, hopSize: 512, signalLength: waveform.length })
stftBatch(data, process, opts?) — batch with callbackProcesses each frame through a callback and overlap-adds the result.
process(mag, phase, state, ctx) → { mag, phase }
mag, phase — Float64Array(half + 1)state — persistent object across framesctx — { N, half, hop, anaHop, synHop, freqPerBin, frameStart, sampleRate, opts }
ctx.frameStart — sample index of the frame start in the original signal. Negative at boundaries due to zero-padding.ctx.opts — cloned copy of opts. Use this to pass custom parameters (e.g. ratio, ratioFn) through to your process callback.opts.anaHop — analysis hop (default: hopSize).opts.synHop — synthesis hop (default: hopSize). When anaHop !== synHop, the output is time-stretched or compressed.Float32Array of length round(data.length * synHop / anaHop) (same as input when anaHop === synHop).const result = stftBatch(signal, (mag, phase, state, ctx) => {
// Simple spectral gate
for (let k = 0; k < mag.length; k++) if (mag[k] < 0.1) mag[k] = 0
return { mag, phase }
}, { frameSize: 2048, hopSize: 512 })
stftStream(process, opts?) — streaming with callbackStreaming version of stftBatch. Returns { write(chunk), flush() }.
opts.anaHop / opts.synHop for time-stretching in streaming context.const stream = stftStream((mag, phase) => ({ mag, phase }), { frameSize: 2048 })
for (const chunk of audioChunks) {
const processed = stream.write(chunk)
// emit processed...
}
const tail = stream.flush()
stftAnalysisStream(opts?) — streaming analysisStreaming version of stft. Returns { write(chunk), flush() } that emit frames.
opts.anaHop for non-uniform analysis spacing.const stream = stftAnalysisStream({ frameSize: 2048, hopSize: 512 })
const frames = stream.write(chunk1)
frames.push(...stream.write(chunk2))
frames.push(...stream.flush())
rfft, fft, and ifft return internal cached buffers by default. The next call with the same N overwrites the previous result. Pass an output buffer to keep results across calls:
const out = new Float64Array(N / 2)
rfft(signal, out) // safe to keep
N=4096 real-valued FFT, complex output, 20k iterations (lower is better):
fft.js (indutny) 16.5µs ×1.0 — radix-4, interleaved output
fourier-transform 17.8µs ×1.1 — split-radix, separate re/im
ooura 23.6µs ×1.4 — Ooura C port
ml-fft 37.0µs ×2.2
dsp.js 48.1µs ×2.9 — our split-radix ancestor
kissfft-wasm 49.4µs ×3.0 — WASM KissFFT
ndarray-fft 63.1µs ×3.8
als-fft 2311.4µs ×140
fft-js 2329.2µs ×141 — naive recursive
Raw transform speed is identical to fft.js. The gap is the cost of returning separate re/im arrays vs interleaved output.
npm run benchmark to reproduce.
Forward split-radix real FFT from dsp.js by @corbanbrook, derived from RealFFT. Inverse split-radix DIF algorithm from FXT by Joerg Arndt.
MIT