我正在开发一个小型雷达项目，可以测量心脏和胸部产生的多普勒频移。由于我事先知道了数量，我决定选择MUSIC算法进行光谱分析。我正在获取数据并将其发送到Python进行分析。但是，我的Python代码表示，具有两个频率为1 Hz和2 Hz的混合正弦波的信号的所有频率的功率相等。我的代码在这里链接了一个示例输出：
from scipy import signal
import numpy as np
from numpy import linalg as LA
import matplotlib.pyplot as plt
import cmath
import scipy
N = 5
z = np.linspace(0,2*np.pi, num=N)
x = np.sin(2*np.pi * z) + np.sin(1 * np.pi * z) + np.random.random(N) * 0.3 # sample signal
conj = np.conj(x);
l = len(conj)
sRate = 25 # sampling rate
p = 2
flipped = [0 for h in range(0, l)]
flipped = conj[::-1]
acf = signal.convolve(x,flipped,'full')
a1 = scipy.linalg.toeplitz(c=np.asarray(acf),r=np.asarray(acf))#autocorrelation matrix that will be decomposed into eigenvectors
eigenValues,eigenVectors = LA.eig(a1)
idx = eigenValues.argsort()[::-1]
eigenValues = eigenValues[idx]
eigenVectors = eigenVectors[:,idx]
idx = eigenValues.argsort()[::-1]
eigenValues = eigenValues[idx]# soriting the eigenvectors and eigenvalues from greatest to least eigenvalue
eigenVectors = eigenVectors[:,idx]
signal_eigen = eigenVectors[0:p]#these vectors make up the signal subspace, by using the number of principal compoenets, 2 to split the eigenvectors
noise_eigen = eigenVectors[p:len(eigenVectors)]# noise subspace
for f in range(0, sRate):
sum1 = 0
frequencyVector = np.zeros(len(noise_eigen[0]), dtype=np.complex_)
for i in range(0,len(noise_eigen[0])):
frequencyVector[i] = np.conjugate(complex(np.cos(2 * np.pi * i * f), np.sin(2 * np.pi * i * f)))#creating a frequency vector with e to the 2pi *k *f and taking the conjugate of the each component
for u in range(0,len(noise_eigen)):
sum1 += (abs(np.dot(np.asarray(frequencyVector).transpose(), np.asarray( noise_eigen[u]) )))**2 # summing the dot product of each noise eigenvector and frequency vector taking the absolute value and squaring
print(1/sum1)
print("\n")
"""
(OUTPUT OF THE ABOVE CODE)
0.120681885992
0
0.120681885992
1
0.120681885992
2
0.120681885992
3
0.120681885992
4
0.120681885992
5
0.120681885992
6
0.120681885992
7
0.120681885992
8
0.120681885992
9
0.120681885992
10
0.120681885992
11
0.120681885992
12
0.120681885992
13
0.120681885992
14
0.120681885992
15
0.120681885992
16
0.120681885992
17
0.120681885992
18
0.120681885992
19
0.120681885992
20
0.120681885992
21
0.120681885992
22
0.120681885992
23
0.120681885992
24
Process finished with exit code 0
"""
以下是MUSIC算法的公式：
https://drive.google.com/file/d/0B5EG2FEWlIZwYmkteUludHNXS0k/view?usp=sharing
答案 0 :(得分：1)
在数学上，问题是 i 和 f 都是整数。因此，2 *π* i * f是2π的整数倍。允许一点点的舍入误差，这会给你一个非常接近1.0的余弦和一个非常接近0.0的sin。从一次迭代到下一次迭代，这些值几乎不会产生 frequencyVector 的变化。
我也看到了一个问题，你设置 signal_eigen矩阵，但从不使用它。这个算法不需要信号本身吗？因此，您所做的只是以2πi的间隔对噪声进行采样。
让我们尝试将一个周期切换为 sRate 均匀间隔的采样点。这导致峰值在0.24和0.76（超出范围0.0-0.99）。这与你的直觉相符吗？
signal_eigen = eigenVectors[0:p]
noise_eigen = eigenVectors[p:len(eigenVectors)] # noise subspace
print "Signal\n", signal_eigen
print "Noise\n", noise_eigen
for f_int in range(0, sRate * p + 1):
sum1 = 0
frequencyVector = np.zeros(len(noise_eigen[0]), dtype=np.complex_)
f = float(f_int) / sRate
for i in range(0,len(noise_eigen[0])):
# create a frequency vector with e to the 2pi *k *f and taking the conjugate of the each component
frequencyVector[i] = np.conjugate(complex(np.cos(2 * np.pi * i * f), np.sin(2 * np.pi * i * f)))
# print f, i, np.pi, np.cos(2 * np.pi * i * f)
# print frequencyVector
for u in range(0,len(noise_eigen)):
# sum the squared dot product of each noise eigenvector and frequency vector.
sum1 += (abs(np.dot(np.asarray(frequencyVector).transpose(), np.asarray( noise_eigen[u]) )))**2
print f, 1/sum1
输出
Signal
[[ -3.25974386e-01 3.26744322e-01 -5.24205744e-16 -1.84108176e-01
-7.07106781e-01 -6.86652798e-17 2.71561652e-01 3.78607948e-16
4.23482344e-01]
[ 3.40976541e-01 5.42419088e-02 -5.00000000e-01 -3.62655793e-01
-1.06880232e-16 3.53553391e-01 -3.89304223e-01 -3.53553391e-01
3.12595284e-01]]
Noise
[[ -3.06261935e-01 -5.16768248e-01 7.82012443e-16 -3.72989138e-01
-3.12515753e-16 -5.00000000e-01 5.19589478e-03 -5.00000000e-01
-2.51205535e-03]
[ 3.21775774e-01 8.19916352e-02 5.00000000e-01 -3.70053622e-01
1.44550753e-16 3.53553391e-01 4.33613344e-01 -3.53553391e-01
-2.54514258e-01]
[ -4.00349040e-01 4.82750272e-01 -8.71533036e-16 -3.42123880e-01
-2.68725150e-16 2.42479504e-16 -4.16290671e-01 -4.89739378e-16
-5.62428795e-01]
[ 3.21775774e-01 8.19916352e-02 -5.00000000e-01 -3.70053622e-01
-2.80456498e-16 -3.53553391e-01 4.33613344e-01 3.53553391e-01
-2.54514258e-01]
[ -3.06261935e-01 -5.16768248e-01 1.08027782e-15 -3.72989138e-01
-1.25036869e-16 5.00000000e-01 5.19589478e-03 5.00000000e-01
-2.51205535e-03]
[ 3.40976541e-01 5.42419088e-02 5.00000000e-01 -3.62655793e-01
-2.64414807e-16 -3.53553391e-01 -3.89304223e-01 3.53553391e-01
3.12595284e-01]
[ -3.25974386e-01 3.26744322e-01 -4.97151703e-16 -1.84108176e-01
7.07106781e-01 -1.62796158e-16 2.71561652e-01 2.06561854e-16
4.23482344e-01]]
0.0 0.115397176866
0.04 0.12355071192
0.08 0.135377011677
0.12 0.136669716901
0.16 0.148772917566
0.2 0.195742574649
0.24 0.237792763699
0.28 0.181921271171
0.32 0.12959840172
0.36 0.121070836044
0.4 0.139075881122
0.44 0.139216853056
0.48 0.117815494324
0.52 0.117815494324
0.56 0.139216853056
0.6 0.139075881122
0.64 0.121070836044
0.68 0.12959840172
0.72 0.181921271171
0.76 0.237792763699
0.8 0.195742574649
0.84 0.148772917566
0.88 0.136669716901
0.92 0.135377011677
0.96 0.12355071192
我也不确定正确的实施方式;有更多关于公式背景的论文会有所帮助。我不确定 f 值的范围和采样。当我使用FFT软件时， f 以较小的增量扫过波形，通常2π/ sRate 。
我现在没有得到那些独特的尖峰 - 不确定我之前做过什么。我做了一个小的参数化更改，添加了一个num_slice变量：
num_slice = sRate * N
for f_int in range(0, num_slice + 1):
sum1 = 0
frequencyVector = np.zeros(len(noise_eigen[0]), dtype=np.complex_)
f = float(f_int) / num_slice
当然，您可以随意计算它，但随后的循环只运行一个周期。这是我的输出：
0.0 0.136398199883
0.008 0.136583829848
0.016 0.13711117893
0.024 0.137893463111
0.032 0.138792904453
0.04 0.139633157335
0.048 0.140219450839
0.056 0.140365986349
0.064 0.139926689416
0.072 0.138822121693
0.08 0.137054535152
0.088 0.13470609994
0.096 0.131921188389
0.104 0.128879079596
0.112 0.125765649854
0.12 0.122750994163
0.128 0.119976226317
0.136 0.117549199221
0.144 0.115546862203
0.152 0.114021482029
0.16 0.113008398728
0.168 0.112533730494
0.176 0.112621097254
0.184 0.113296863522
0.192 0.114593615279
0.2 0.116551634665
0.208 0.119218062482
0.216 0.12264326497
0.224 0.126873674308
0.232 0.131940131305
0.24 0.137840727381
0.248 0.144517728837
0.256 0.151830000359
0.264 0.159526062508
0.272 0.167228413981
0.28 0.174444818009
0.288 0.180621604818
0.296 0.185241411664
0.304 0.187943197745
0.312 0.188619481273
0.32 0.187445977812
0.328 0.184829467764
0.336 0.181300320748
0.344 0.177396490666
0.352 0.173576190425
0.36 0.170171993077
0.368 0.167379359825
0.376 0.165265454514
0.384 0.163786582966
0.392 0.16280869726
0.4 0.162130870823
0.408 0.161514399035
0.416 0.160719375729
0.424 0.159546457646
0.432 0.157875982968
0.44 0.155693319037
0.448 0.153091632029
0.456 0.150251065569
0.464 0.147402137481
0.472 0.144785618099
0.48 0.14261932062
0.488 0.141076562538
0.496 0.140275496354
0.504 0.140275496354
0.512 0.141076562538
0.52 0.14261932062
0.528 0.144785618099
0.536 0.147402137481
0.544 0.150251065569
0.552 0.153091632029
0.56 0.155693319037
0.568 0.157875982968
0.576 0.159546457646
0.584 0.160719375729
0.592 0.161514399035
0.6 0.162130870823
0.608 0.16280869726
0.616 0.163786582966
0.624 0.165265454514
0.632 0.167379359825
0.64 0.170171993077
0.648 0.173576190425
0.656 0.177396490666
0.664 0.181300320748
0.672 0.184829467764
0.68 0.187445977812
0.688 0.188619481273
0.696 0.187943197745
0.704 0.185241411664
0.712 0.180621604818
0.72 0.174444818009
0.728 0.167228413981
0.736 0.159526062508
0.744 0.151830000359
0.752 0.144517728837
0.76 0.137840727381
0.768 0.131940131305
0.776 0.126873674308
0.784 0.12264326497
0.792 0.119218062482
0.8 0.116551634665
0.808 0.114593615279
0.816 0.113296863522
0.824 0.112621097254
0.832 0.112533730494
0.84 0.113008398728
0.848 0.114021482029
0.856 0.115546862203
0.864 0.117549199221
0.872 0.119976226317
0.88 0.122750994163
0.888 0.125765649854
0.896 0.128879079596
0.904 0.131921188389
0.912 0.13470609994
0.92 0.137054535152
0.928 0.138822121693
0.936 0.139926689416
0.944 0.140365986349
0.952 0.140219450839
0.96 0.139633157335
0.968 0.138792904453
0.976 0.137893463111
0.984 0.13711117893
0.992 0.136583829848
1.0 0.136398199883