signal op• 데이터 종류: positions → table
• 호출: import fullseye as fs; fs.ledger.point_spectrum(positions, extent=None, n_freq=2048, f_max=None, method='direct', weights=None, bins_per_period=8)(구현을 직접 호출하려면 import dsp; dsp.point_spectrum(positions, extent=None, n_freq=2048, f_max=None, method='direct', weights=None, bins_per_period=8), 원장에서 가져오려면 ops1d.get("point_spectrum"))
> 이 연산자의 설명은 아직 번역이 없습니다. 원문을 그대로 싣습니다.
Periodogram of event positions — defects, impacts, counts, arrivals.
:func:spectrum needs an evenly sampled signal, but a great deal of
industrial data arrives as a *list of positions*: where each defect was on
the web, when each particle was counted, at what angle each dent sits. The
usual workaround is to histogram the positions and FFT the histogram, which
works but hides two choices — bin width and record length — that decide the
answer. This operator makes both explicit and returns them.
*method* picks the estimator:
`"direct"`
the point-process (Bartlett) periodogram
`|sum_j w_j exp(-2 pi i f x_j) - rate * integral|^2 / sum_j w_j`,
evaluated at each requested frequency. No binning at all, so no bin
width to choose and no aliasing from one. The subtracted term is the
contribution a *uniform* process of the same rate would make; without it
every spectrum peaks at f -> 0 simply because events exist.
`"binned"`
histogram the positions, then `rfft`, with the bin width set so the
finest frequency asked for still gets `bins_per_period` samples per
cycle. Cheaper for very many events, and the result is what a
histogram-and-FFT pipeline would have produced.
The frequency resolution is a property of the record, not of the method.
Two periods closer than `1/extent` apart cannot be told apart by either
estimator, and the returned dict says so in `resolution`: read it before
reading a peak, not after.
A periodic train of events is a comb, not a line. Its harmonics at
`k/period are as tall as the fundamental, so argmax` of this spectrum
routinely returns `period/k` rather than the period. Measured on 93 events
(43 spaced 471.24 apart with 1.5 of jitter, plus 50 uniformly random) over a
record of 20000: the global maximum lands on `58.90 with direct` (the
8th harmonic) and `52.35 with binned` (the 9th), while the fundamental
is present and prominent in both — `direct` puts 0.947 of the maximum
power at `1/471.24, binned` 0.379. Take the lowest frequency whose
first few harmonics *all* stand, rather than the tallest line — see
`examples/poc_web_roll_periodicity.py`, which is what this operator was
added for.
Returns a dict: `freq (cycles per unit of *positions*), power`,
`resolution (1/extent), extent, n_events, method`, and
`bin_width (None for "direct"`).
Fail-closed: fewer than two events raises `ValueError` — a periodogram of
one point is not a weak measurement, it is not a measurement.
• 샘플 데이터 카탈로그(DL URL / 라이선스) —— 2-D 는 skimage.data(BSD/public)+ 합성, 3-D 는 실데이터 소스(Stanford/PDS 등)의 DL URL.
• 연산자의 내력·참고문헌 —— 이 연산자 족의 바탕이 된 연구/기법의 출처.
• 알고리즘의 정전(저자·연도)과 용도는 위의 패밀리 사용 가이드에 적혀 있습니다.
• poc_web_roll_periodicity — py -3.11 examples/poc_web_roll_periodicity.py
table 를 입력으로 받는 것)—
signal)lowpass · highpass · bandpass · envelope · rms · local_std · quantize · companding_mu_law
*Provenance: dsp.py — ONED 연산자 레지스트리. 이 op 노트는 tools/opdocs.py md 가 자동 생성합니다(직접 편집하지 마세요).*
© 2026 Kazufumi Furuse — Fullseye operator documentation. Licensed under Apache-2.0.