beamform_delay_sum — RANGEDOPPLER beamform op

데이터 종류: beatcubesignal

호출: import rangedoppler; rangedoppler.beamform_delay_sum(cube, wavelength_m=0.0038934, element_spacing_m=None, angles_deg=None, range_bin=None, doppler_bin=None, normalize=False)(또는 opsrangedoppler.get("beamform_delay_sum"))

사용법

하나의 거리-도플러 셀에 대한 지연 합(Bartlett) 각도 스펙트럼.

> 아래 상세 설명은 원문입니다 —— 요약과 제목은 번역되어 있습니다.

Takes the per-antenna complex value at a single range-Doppler cell — by

default the strongest one — and for each steering angle removes the expected

inter-element phase and sums:

`P(theta) = |sum_k conj(exp(1j*2*pi*d*k*sin(theta)/lambda)) * x_k|^2`

which peaks at the true arrival angle with value `(N_a * |a|)^2`: the

aperture gives `N_a in amplitude, N_a^2` in power. That is the exact

ground truth the tests pin. Measured with 8 elements: the peak power is

bit-exactly `(N_a*N_c*N_s)^2 = 268435456` (relative error 0.0), and

sweeping the true angle from -80 to +80 degrees in 5-degree steps (33 cases)

the reported angle matches the truth with a maximum error of 0.0 degrees.

The steering grid defaults to `arange(-90, 90.5, 1.0). normalize=True`

divides by `N_a^2 * N_c^2 * N_s^2` so that a unit-amplitude bin-centred

target peaks at 1.0.

Returns a 1-D float64 array of powers, one per grid angle — a plain signal,

so :mod:dsp's `find_peaks and :mod:funct1d`'s smoothing apply to it.

Use :func:beamform_doa if you want the angles themselves.

*range_bin* is a plain `0..N_s-1` index; *doppler_bin* is the signed

velocity bin, the same convention :func:range_doppler_peaks reports, so a

detection can be handed straight back in. Both or neither — half a cell

address raises rather than quietly beamforming the strongest cell instead.

Raises `ValueError`: no aperture — either a single element, or many

elements packed into under ~0.28 wavelengths. In both cases the spectrum is

flat to within float noise and `argmax` returns the first grid angle, i.e.

a confident report of -90 degrees that is pure tie-breaking (measured: 8

elements at 1e-12 m spacing gave a peak-to-trough spread of exactly 0.0 and

reported -90.0). Also: an all-zero cube or an all-zero selected cell; only

one of *range_bin* / *doppler_bin*; an out-of-bounds bin index; an angle grid

outside `[-90, 90]`; an FFT that overflows to NaN; plus the usual cube and

scalar refusals.

자세한 사용 가이드

fmcw_range_doppler 패밀리 가이드

참고(샘플 데이터·문헌)

• 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.

실행 가능한 예제(이 연산자를 실제로 호출하는 검증된 샘플)

fmcw_range_dopplerpy -3.11 examples/fmcw_range_doppler.py

타입이 이어지는 다음 연산자(signal 를 입력으로 받는 것)

같은 카테고리(beamform)

beamform_doa


*Provenance: rangedoppler.py — RANGEDOPPLER 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.