Acta Armamentarii ›› 2023, Vol. 44 ›› Issue (5): 1521-1528.doi: 10.12382/bgxb.2022.0025
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SHAN Zebiao1,2,3, CHANG Limin1, LIU Xiaosong1,*(), WANG Yuxiang1
Received:
2022-01-08
Online:
2022-07-10
Contact:
LIU Xiaosong
SHAN Zebiao, CHANG Limin, LIU Xiaosong, WANG Yuxiang. DOA Estimation Based on Approximate l0 Norm of Natural Logarithm Composite Function[J]. Acta Armamentarii, 2023, 44(5): 1521-1528.
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幅度误差 | 相位误差 | 均方根误差/(°) | 成功率/% |
---|---|---|---|
N(0,0.1) | N(0,10) | 1.5845 | 91.17 |
N(0,0.2) | N(0,10) | 2.1935 | 90.57 |
N(0,0.1) | N(0,20) | 1.5743 | 91.10 |
Table 1 RMSEs and success probabilities of DOA estimation with amplitude-phase inconsistency
幅度误差 | 相位误差 | 均方根误差/(°) | 成功率/% |
---|---|---|---|
N(0,0.1) | N(0,10) | 1.5845 | 91.17 |
N(0,0.2) | N(0,10) | 2.1935 | 90.57 |
N(0,0.1) | N(0,20) | 1.5743 | 91.10 |
DOA | 30.0° | 30.2° | 30.5° | 30.7° | 30.9° |
---|---|---|---|---|---|
0° | 0.8488° | 0.8763° | 0.9042° | 0.8609° | 0.8395° |
0.2° | 0.8521° | 0.8795° | 0.9523° | 0.8830° | 0.8621° |
0.5° | 1.0237° | 1.0392° | 1.0416° | 1.0211° | 1.0199° |
Table 2 RMSEs of DOA estimation for off-grid signals
DOA | 30.0° | 30.2° | 30.5° | 30.7° | 30.9° |
---|---|---|---|---|---|
0° | 0.8488° | 0.8763° | 0.9042° | 0.8609° | 0.8395° |
0.2° | 0.8521° | 0.8795° | 0.9523° | 0.8830° | 0.8621° |
0.5° | 1.0237° | 1.0392° | 1.0416° | 1.0211° | 1.0199° |
算法 | 迭代次数/次 | 均方根误差/(°) |
---|---|---|
NLSL0 | 6 | 0.3134 |
SL0 | 8 | 0.3873 |
ISL0 | 16 | 0.3742 |
WSL0 | 19 | 0.3317 |
Table 3 Number of iterations and RMSEs required by different algorithms
算法 | 迭代次数/次 | 均方根误差/(°) |
---|---|---|
NLSL0 | 6 | 0.3134 |
SL0 | 8 | 0.3873 |
ISL0 | 16 | 0.3742 |
WSL0 | 19 | 0.3317 |
参数 | 算法 | ||||
---|---|---|---|---|---|
NLSL0 | SL0 | ISL0 | WSL0 | OMP | |
时间/s | 0.0157 | 0.0189 | 0.0185 | 0.0233 | 0.0132 |
误差/(°) | 0.7483 | 1.9039 | 1.0392 | 0.8573 | 4.5706 |
Table 4 Calculation time and RMSEs of different algorithms
参数 | 算法 | ||||
---|---|---|---|---|---|
NLSL0 | SL0 | ISL0 | WSL0 | OMP | |
时间/s | 0.0157 | 0.0189 | 0.0185 | 0.0233 | 0.0132 |
误差/(°) | 0.7483 | 1.9039 | 1.0392 | 0.8573 | 4.5706 |
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