Nothing Special   »   [go: up one dir, main page]

You seem to have javascript disabled. Please note that many of the page functionalities won't work as expected without javascript enabled.
 
 
Sign in to use this feature.

Years

Between: -

Subjects

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Journals

Article Types

Countries / Regions

Search Results (16)

Search Parameters:
Keywords = eigen-subspace

Order results
Result details
Results per page
Select all
Export citation of selected articles as:
16 pages, 2967 KiB  
Technical Note
Field Programmable Gate Array (FPGA) Implementation of Parallel Jacobi for Eigen-Decomposition in Direction of Arrival (DOA) Estimation Algorithm
by Shuang Zhou and Li Zhou
Remote Sens. 2024, 16(20), 3892; https://doi.org/10.3390/rs16203892 - 19 Oct 2024
Viewed by 833
Abstract
The eigen-decomposition of a covariance matrix is a key step in the Direction of Arrival (DOA) estimation algorithms such as subspace classes. Eigen-decomposition using the parallel Jacobi algorithm implemented on FPGA offers excellent parallelism and real-time performance. Addressing the high complexity and resource [...] Read more.
The eigen-decomposition of a covariance matrix is a key step in the Direction of Arrival (DOA) estimation algorithms such as subspace classes. Eigen-decomposition using the parallel Jacobi algorithm implemented on FPGA offers excellent parallelism and real-time performance. Addressing the high complexity and resource consumption of the traditional parallel Jacobi algorithm implemented on FPGA, this study proposes an improved FPGA-based parallel Jacobi algorithm for eigen-decomposition. By analyzing the relationship between angle calculation and rotation during the Jacobi algorithm decomposition process, leveraging parallelism in the data processing, and based on the concepts of time-division multiplexing and parallel partition processing, this approach effectively reduces FPGA resource consumption. The improved parallel Jacobi algorithm is then applied to the classic DOA estimation algorithm, the MUSIC algorithm, and implemented on Xilinx’s Zynq FPGA. Experimental results demonstrate that this parallel approach can reduce resource consumption by approximately 75% compared to the traditional method but introduces little additional time consumption. The proposed method in this paper will solve the problem of great hardware consumption of eigen-decomposition based on FPGA in DOA applications. Full article
Show Figures

Figure 1

Figure 1
<p>Systolic array structure of an 8-order covariance matrix.</p>
Full article ">Figure 2
<p>(<b>a</b>) First rotational partition diagram. (<b>b</b>) Second rotational partition diagram.</p>
Full article ">Figure 3
<p>The steps of module operation.</p>
Full article ">Figure 4
<p>Block diagram of the MUSIC algorithm.</p>
Full article ">Figure 5
<p>Simulation results of eigen-decomposition iteration for (<b>a</b>) 21 times and (<b>b</b>) 28 times.</p>
Full article ">Figure 5 Cont.
<p>Simulation results of eigen-decomposition iteration for (<b>a</b>) 21 times and (<b>b</b>) 28 times.</p>
Full article ">Figure 6
<p>Illustration of the direction-finding results on the UV plane in MATLAB and FPGA.</p>
Full article ">
15 pages, 3657 KiB  
Article
Multi-Domain Joint Synthetic Aperture Radar Ship Detection Method Integrating Complex Information with Deep Learning
by Chaoyang Tian, Zongsen Lv, Fengli Xue, Xiayi Wu and Dacheng Liu
Remote Sens. 2024, 16(19), 3555; https://doi.org/10.3390/rs16193555 - 24 Sep 2024
Viewed by 734
Abstract
With the flourishing development of deep learning, synthetic aperture radar (SAR) ship detection based on this method has been widely applied across various domains. However, most deep-learning-based detection methods currently only use the amplitude information from SAR images. In fact, phase information and [...] Read more.
With the flourishing development of deep learning, synthetic aperture radar (SAR) ship detection based on this method has been widely applied across various domains. However, most deep-learning-based detection methods currently only use the amplitude information from SAR images. In fact, phase information and time-frequency features can also play a role in ship detection. Additionally, the background noise and the small size of ships also pose challenges to detection. Finally, satellite-based detection requires the model to be lightweight and capable of real-time processing. To address these difficulties, we propose a multi-domain joint SAR ship detection method that integrates complex information with deep learning. Based on the imaging mechanism of line-by-line scanning, we can first confirm the presence of ships within echo returns in the eigen-subspace domain, which can reduce detection time. Benefiting from the complex information of single-look complex (SLC) SAR images, we transform the echo returns containing ships into the time-frequency domain. In the time-frequency domain, ships exhibit distinctive features that are different from noise, without the limitation of size, which is highly advantageous for detection. Therefore, we constructed a time-frequency SAR image dataset (TFSID) using the images in the time-frequency domain, and utilizing the advantages of this dataset, we combined space-to-depth convolution (SPDConv) and Inception depthwise convolution (InceptionDWConv) to propose Efficient SPD-InceptionDWConv (ESIDConv). Using this module as the core, we proposed a lightweight SAR ship detector (LSDet) based on YOLOv5n. The detector achieves a detection accuracy of 99.5 with only 0.3 M parameters and 1.2 G operations on the dataset. Extensive experiments on different datasets demonstrated the superiority and effectiveness of our proposed method. Full article
Show Figures

Figure 1

Figure 1
<p>Flowchart of the proposed method.</p>
Full article ">Figure 2
<p>Strong scattering characteristics of ships in the image domain.</p>
Full article ">Figure 3
<p>Pulse containing a ship in <a href="#remotesensing-16-03555-f002" class="html-fig">Figure 2</a>.</p>
Full article ">Figure 4
<p>Eigenvalue of the Pulse in <a href="#remotesensing-16-03555-f003" class="html-fig">Figure 3</a>.</p>
Full article ">Figure 5
<p>Comparison of ships in different domains.</p>
Full article ">Figure 6
<p>The original images of TFSID.</p>
Full article ">Figure 7
<p>The partial images of TFSID.</p>
Full article ">Figure 8
<p>Structure of the ESIDConv.</p>
Full article ">Figure 9
<p>Overall architecture of the proposed LSDet.</p>
Full article ">Figure 10
<p>Visualization of the detection results. (<b>a</b>) The original image. (<b>b</b>) ROI in (<b>a</b>). (<b>c</b>) Results of direct detection using YOLOv5n on complete original images. (<b>d</b>) Detection results of our proposed method. Red: detection results. Yellow: missed detections. Blue: false alarms.</p>
Full article ">
13 pages, 2781 KiB  
Article
Null Broadening Beamforming for Passive Sonar Based on Weighted Similarity Vector
by Yuhao Wang and Zhenkai Zhang
J. Mar. Sci. Eng. 2023, 11(10), 1858; https://doi.org/10.3390/jmse11101858 - 25 Sep 2023
Cited by 1 | Viewed by 1005
Abstract
Beamforming technology is very important for passive sonar to detect targets. However, the performance of a beamformer is seriously degraded in practical applications due to the complex and changeable underwater environment. In this paper, a null broadening algorithm for passive sonar based on [...] Read more.
Beamforming technology is very important for passive sonar to detect targets. However, the performance of a beamformer is seriously degraded in practical applications due to the complex and changeable underwater environment. In this paper, a null broadening algorithm for passive sonar based on a weighted similarity vector is proposed for underwater fast-moving strong interference signals. First, the covariance matrix was reconstructed through the correlation between the steering vector and the subspace eigenvector, which was used to calculate the similarity vector. Then, the maximum power in the interference angle sector was used as the virtual interference source power to broaden the null in the angle sector. Next, the difference between the optimal weight vector and the similar vector was minimized, the interference-plus-noise power constraints and norm constraints were added, and the equation was written as a quadratic constrained quadratic programming (QCQP) problem, which was converted into a convex optimization problem by using the semidefinite relaxation technique. Finally, the optimal solution was calculated by using eigen decomposition. The simulation results show that the algorithm can guarantee deep nulling and effectively suppress sidelobe height under various error conditions, which shows that the proposed algorithm has a good suppression effect and strong robustness for fast strong interference. Full article
(This article belongs to the Section Ocean Engineering)
Show Figures

Figure 1

Figure 1
<p>Beampatterns of different algorithms in ideal state [<a href="#B19-jmse-11-01858" class="html-bibr">19</a>].</p>
Full article ">Figure 2
<p>Output SINR under different input SNRs in ideal state [<a href="#B19-jmse-11-01858" class="html-bibr">19</a>].</p>
Full article ">Figure 3
<p>Output SINR under different snapshot numbers in ideal state [<a href="#B19-jmse-11-01858" class="html-bibr">19</a>].</p>
Full article ">Figure 4
<p>Output SINR under different input SNRs with amplitude and phase perturbation errors [<a href="#B19-jmse-11-01858" class="html-bibr">19</a>].</p>
Full article ">Figure 5
<p>Output SINR under different snapshot numbers with amplitude and phase perturbation errors [<a href="#B19-jmse-11-01858" class="html-bibr">19</a>].</p>
Full article ">Figure 6
<p>Output SINR under different input SNRs with array element position error [<a href="#B19-jmse-11-01858" class="html-bibr">19</a>].</p>
Full article ">Figure 7
<p>Output SINR under different snapshot numbers with array element position error [<a href="#B19-jmse-11-01858" class="html-bibr">19</a>].</p>
Full article ">Figure 8
<p>Beampattern under different <math display="inline"><semantics> <mrow> <mi>ε</mi> </mrow> </semantics></math> conditions.</p>
Full article ">Figure 9
<p>Output SINR under different <math display="inline"><semantics> <mrow> <mi>ε</mi> </mrow> </semantics></math> conditions.</p>
Full article ">Figure 10
<p>Beampatterns with different nulling widths.</p>
Full article ">Figure 11
<p>Output SINR with different null width.</p>
Full article ">
19 pages, 4794 KiB  
Article
Sequenced Steering Vector Estimation for Eigen-Subspace Projection-Based Robust Adaptive Beamformer
by Xiangwei Chen and Weixing Sheng
Electronics 2023, 12(13), 2897; https://doi.org/10.3390/electronics12132897 - 1 Jul 2023
Viewed by 1237
Abstract
Robust adaptive beamforming (RAB) is essential in many applications to ensure signal-receiving quality when model errors exist. Eigen-subspace projection (ESP), one of the most popular RAB methods, can be used when there are arbitrary model errors. However, a major challenge of ESP is [...] Read more.
Robust adaptive beamforming (RAB) is essential in many applications to ensure signal-receiving quality when model errors exist. Eigen-subspace projection (ESP), one of the most popular RAB methods, can be used when there are arbitrary model errors. However, a major challenge of ESP is projection subspace selection. Traditional ESP (TESP) treats the signal subspace as the projection subspace; thus, source enumeration is required to obtain prior information. Another inherent defect is its poor performance at low signal-to-noise ratios (SNRs). To overcome these drawbacks, two improved ESP-based RAB methods are proposed in this study. Considering that a reliable signal-of-interest steering vector needs to be obtained via the subspace projection, the main idea underlying the proposed methods is to use sequenced steering vector estimation to invert the subspace dimension estimate for an arranged eigenvector matrix. As the proposed methods do not require source enumeration, they are simple to implement. Numerical examples demonstrate the effectiveness and robustness of the proposed methods in terms of output signal-to-interference-plus-noise ratio performance. Specifically, compared with TESP, the proposed methods present at least a 2.6 dB improvement at low SNRs regardless of the error models. Full article
(This article belongs to the Section Microwave and Wireless Communications)
Show Figures

Figure 1

Figure 1
<p>Illustration of Array Signal Model.</p>
Full article ">Figure 2
<p>Ideal condition (case (i)).</p>
Full article ">Figure 3
<p>Fixed DOA mismatch without array perturbations (case (ii)).</p>
Full article ">Figure 4
<p>Fixed DOA mismatch with array perturbations (case (iii)).</p>
Full article ">Figure 5
<p>Example 2: Output SINR versus input SNR when <span class="html-italic">K</span> = 200.</p>
Full article ">Figure 6
<p>Example 2: Output SINR versus the number of snapshots when input SNR = 10 dB.</p>
Full article ">Figure 7
<p>Example 3: Output SINR versus the input SNR when <span class="html-italic">K</span> = 200.</p>
Full article ">Figure 8
<p>Example 3: Output SINR versus the number of snapshots when input SNR = 10 dB.</p>
Full article ">Figure 9
<p>Output SINR versus DOA mismatch with array perturbations; input SNR = 10 dB and <span class="html-italic">K</span> = 200.</p>
Full article ">
22 pages, 1816 KiB  
Article
Free Vibrations of Multi-Degree Structures: Solving Quadratic Eigenvalue Problems with an Excitation and Fast Iterative Detection Method
by Chein-Shan Liu, Chung-Lun Kuo and Chih-Wen Chang
Vibration 2022, 5(4), 914-935; https://doi.org/10.3390/vibration5040053 - 18 Dec 2022
Cited by 4 | Viewed by 2262
Abstract
For the free vibrations of multi-degree mechanical structures appeared in structural dynamics, we solve the quadratic eigenvalue problem either by linearizing it to a generalized eigenvalue problem or directly treating it by developing the iterative detection methods for the real and complex eigenvalues. [...] Read more.
For the free vibrations of multi-degree mechanical structures appeared in structural dynamics, we solve the quadratic eigenvalue problem either by linearizing it to a generalized eigenvalue problem or directly treating it by developing the iterative detection methods for the real and complex eigenvalues. To solve the generalized eigenvalue problem, we impose a nonzero exciting vector into the eigen-equation, and solve a nonhomogeneous linear system to obtain a response curve, which consists of the magnitudes of the n-vectors with respect to the eigen-parameters in a range. The n-dimensional eigenvector is supposed to be a superposition of a constant exciting vector and an m-vector, which can be obtained in terms of eigen-parameter by solving the projected eigen-equation. In doing so, we can save computational cost because the response curve is generated from the data acquired in a lower dimensional subspace. We develop a fast iterative detection method by maximizing the magnitude to locate the eigenvalue, which appears as a peak in the response curve. Through zoom-in sequentially, very accurate eigenvalue can be obtained. We reduce the number of eigen-equation to n1 to find the eigen-mode with its certain component being normalized to the unit. The real and complex eigenvalues and eigen-modes can be determined simultaneously, quickly and accurately by the proposed methods. Full article
(This article belongs to the Special Issue Feature Papers in Vibration)
Show Figures

Figure 1

Figure 1
<p>For a generalized eigenvalue problem (<a href="#FD13-vibration-05-00053" class="html-disp-formula">13</a>), (<b>a</b>) zero response under a zero excitation, and (<b>b</b>) showing five peaks in the response curve under a nonzero excitation.</p>
Full article ">Figure 2
<p>For a 2 by 2 matrix the detection of a complex eigenvalue.</p>
Full article ">Figure 3
<p>For example 1, showing two peaks in the response curve obtained from the IDM, corresponding to eigenvalues −0.619402940600584 and 1.627440079051887.</p>
Full article ">Figure 4
<p>For example 2, showing five peaks in the response curve obtained from the IDM, corresponding to five eigenvalues.</p>
Full article ">Figure 5
<p>For example 3, (<b>a</b>) showing five picks of <math display="inline"><semantics> <mrow> <mo>∥</mo> <mi mathvariant="bold">x</mi> <mo>∥</mo> </mrow> </semantics></math> with <math display="inline"><semantics> <mrow> <mi>m</mi> <mo>=</mo> <mn>50</mn> </mrow> </semantics></math> in the interval [−0.01,0.05], and (<b>b</b>) a pick of <math display="inline"><semantics> <mrow> <mo>∥</mo> <mi mathvariant="bold">x</mi> <mo>∥</mo> </mrow> </semantics></math> is enlarged in the interval [0.005,0.015], which is a process of zoom-in.</p>
Full article ">Figure 6
<p>For example 4, showing three picks of <math display="inline"><semantics> <mrow> <mo>∥</mo> <mi mathvariant="bold">x</mi> <mo>∥</mo> </mrow> </semantics></math> in the response curve in the interval [0,1.6].</p>
Full article ">Figure 7
<p>For example 4, (<b>a</b>) showing four picks of <math display="inline"><semantics> <mrow> <mo>∥</mo> <mi mathvariant="bold">x</mi> <mo>∥</mo> </mrow> </semantics></math> in the response curve in the interval [−4,1], and (<b>b</b>) a pick of <math display="inline"><semantics> <mrow> <mo>∥</mo> <mi mathvariant="bold">x</mi> <mo>∥</mo> </mrow> </semantics></math> over the plane is enlarged in the interval <math display="inline"><semantics> <mrow> <mo>[</mo> <mo>−</mo> <mn>0.01</mn> <mo>,</mo> <mn>0.01</mn> <mo>]</mo> <mo>×</mo> <mo>[</mo> <mn>0.5</mn> <mo>,</mo> <mn>1.5</mn> <mo>]</mo> </mrow> </semantics></math>.</p>
Full article ">Figure 8
<p>For example 5, showing three picks of <math display="inline"><semantics> <mrow> <mo>∥</mo> <mi mathvariant="bold">x</mi> <mo>∥</mo> </mrow> </semantics></math> in the response curve in the interval [0,5].</p>
Full article ">Figure 9
<p>For example 5 with ten-degree, showing ten picks of <math display="inline"><semantics> <mrow> <mo>∥</mo> <mi mathvariant="bold">x</mi> <mo>∥</mo> </mrow> </semantics></math> in the response curve in the interval [0,5].</p>
Full article ">Figure 10
<p>For a five-degree MK system, (<b>a</b>) showing five picks of <math display="inline"><semantics> <mrow> <mo>∥</mo> <mi mathvariant="bold">x</mi> <mo>∥</mo> </mrow> </semantics></math> in the response curve in the interval [0,10], and (<b>b</b>) displaying the five vibration modes.</p>
Full article ">Figure 11
<p>For example 4 solved as a quadratic eigenvalue problem, showing four picks of <math display="inline"><semantics> <mrow> <mo>∥</mo> <mi mathvariant="bold">u</mi> <mo>∥</mo> </mrow> </semantics></math> in the response curve in the interval [0,3].</p>
Full article ">Figure 12
<p>For example 7, showing a pick of <math display="inline"><semantics> <mrow> <mo>∥</mo> <mi mathvariant="bold">u</mi> <mo>∥</mo> </mrow> </semantics></math> in the response surface for complex eigenvalues.</p>
Full article ">Figure 13
<p>For example 7 with different dimension, showing maximal and minimal frequencies.</p>
Full article ">Figure 14
<p>For a nonlinear perturbation of example 4, showing three picks of <math display="inline"><semantics> <mrow> <mo>∥</mo> <mi mathvariant="bold">u</mi> <mo>∥</mo> </mrow> </semantics></math> in the response curve in the interval [0,2].</p>
Full article ">
12 pages, 3331 KiB  
Article
Multiple Mainlobe Interferences Suppression Based on Eigen-Subspace and Eigen-Oblique Projection
by Yunhao Ji, Yaobing Lu, Shan Wei and Zigeng Li
Sensors 2022, 22(21), 8494; https://doi.org/10.3390/s22218494 - 4 Nov 2022
Cited by 2 | Viewed by 1705
Abstract
When the desired signal and multiple mainlobe interferences coexist in the received data, the performance of the current mainlobe interference suppression algorithms is severely challenged. This paper proposes a multiple mainlobe interference suppression method based on eigen-subspace and eigen-oblique projection to solve this [...] Read more.
When the desired signal and multiple mainlobe interferences coexist in the received data, the performance of the current mainlobe interference suppression algorithms is severely challenged. This paper proposes a multiple mainlobe interference suppression method based on eigen-subspace and eigen-oblique projection to solve this problem. First, use the spatial spectrum algorithm to calculate interference power and direction. Next, reconstruct the eigen-subspace to accurately calculate the interference eigenvector, then generate the eigen-oblique projection matrix to suppress mainlobe interference and output the desired signal without distortion. Finally, the adaptive weight vector is calculated to suppress sidelobe interference. Through the above steps, the proposed method solves the problem that the mainlobe interference eigenvector is difficult to select, caused by the desired signal and the mismatch of the mainlobe interference steering vector and its eigenvector. The simulation result proves that our method could suppress interference more successfully than the former methods. Full article
Show Figures

Figure 1

Figure 1
<p>Processing diagram of the proposed method.</p>
Full article ">Figure 2
<p>Comparison of beam pattern.</p>
Full article ">Figure 3
<p>Comparison of array output data.</p>
Full article ">Figure 4
<p>Analysis of the impact of Input SNR on Output SINR.</p>
Full article ">Figure 5
<p>Analysis of the impact of snapshots number on output SINR.</p>
Full article ">Figure 6
<p>Analysis of the impact of input SNR on ISR.</p>
Full article ">
20 pages, 1216 KiB  
Article
Efficient Design of Thermoelastic Structures Using a Krylov Subspace Preconditioner and Parallel Sensitivity Computation
by Yu Fu, Li Li and Yujin Hu
Appl. Sci. 2022, 12(18), 8978; https://doi.org/10.3390/app12188978 - 7 Sep 2022
Cited by 2 | Viewed by 1306
Abstract
The repeated updating of parametric designs is computationally challenging, especially for large-scale multi-physics models. This work is focused on proposing an efficient modal modification method for gradient-based topology optimization of thermoelastic structures, which is essential when dealing with their complex eigenproblems and global [...] Read more.
The repeated updating of parametric designs is computationally challenging, especially for large-scale multi-physics models. This work is focused on proposing an efficient modal modification method for gradient-based topology optimization of thermoelastic structures, which is essential when dealing with their complex eigenproblems and global sensitivity analysis for a huge number of design parameters. The degrees of freedom of the governing equation of thermoelastic structures is very huge when its parametric partial differential equation is discretized using the numerical technique. A Krylov subspace preconditioner is constructed based on the Neumann series expansion series so that the thermoelastic eigenproblem can be solved in an efficient low-dimension solver, rather than its original high-fidelity solver. In the construction of Krylov reduced-basis vectors, the computational cost of the systemic matrix inverse becomes a critical issue, which is solved efficiently by means of constructing a diagonal systemic matrix with the lumped mass and heat generation submatrices. Then, the reduced-basis preconditioner can provide an efficient optimal solver for both the thermoelastic eigenproblem and its eigen sensitivity. Furthermore, a master-slave pattern parallel method is developed to reduce the computational time of computing the global sensitivity numbers, and therefore, the global sensitivity problem can be efficiently discretized into element-scale problems in a parallel way. The sensitivity numbers can thus be solved at the element scale and aggregated to the global sensitivity number. Finally, two case studies of the iterative topology optimization process, in which the proposed modal modification method and the traditional method are implemented, are used to illustrate the effectiveness of the proposed method. Numerical examples show that the proposed method can reduce the computational cost remarkably with acceptable accuracy. Full article
(This article belongs to the Section Mechanical Engineering)
Show Figures

Figure 1

Figure 1
<p>Sketch map of the regime of thermoelastic damping (TED). As the clamped-clamped microbeam resonator vibrates in a purely flexural mode, one side along the thickness of the beam stretches, which causes the temperature of the region to decrease. The temperature of the compressed side increases, causing a temperature gradient along the thickness of the beam. The irreversible heat flux induced by the temperature gradient causes the dissipation of energy.</p>
Full article ">Figure 2
<p>Flowchart of the topology optimization process.</p>
Full article ">Figure 3
<p>Flowchart of the modal repeated analysis method.</p>
Full article ">Figure 4
<p>Sketch map of the parallel method of the master-slave pattern.</p>
Full article ">Figure 5
<p>Topology optimization results for a clamped-clamped microbeam resonator. (<b>a</b>) The original structure. (<b>b</b>) The optimization result where the traditional subspace method is implemented in the finite element analysis step. (<b>c</b>) The optimization result where the proposed method is implemented in the finite element analysis step.</p>
Full article ">Figure 6
<p>Topology optimization results for a clamped-free microbeam resonator. (<b>a</b>) The original structure. (<b>b</b>) The optimization result where the traditional subspace method is implemented in the finite element analysis step. (<b>c</b>) The optimization result where the proposed method is implemented in the finite element analysis step.</p>
Full article ">
17 pages, 5617 KiB  
Article
A Novel Method for SAR Ship Detection Based on Eigensubspace Projection
by Gaofeng Shu, Jiahui Chang, Jing Lu, Qing Wang and Ning Li
Remote Sens. 2022, 14(14), 3441; https://doi.org/10.3390/rs14143441 - 18 Jul 2022
Cited by 6 | Viewed by 2096
Abstract
Synthetic Aperture Radar (SAR) is a high-resolution radar that operates all day and in all weather conditions, so it has been widely used in various fields of science and technology. Ship detection using SAR images has become important research in marine applications. However, [...] Read more.
Synthetic Aperture Radar (SAR) is a high-resolution radar that operates all day and in all weather conditions, so it has been widely used in various fields of science and technology. Ship detection using SAR images has become important research in marine applications. However, in complex scenes, ships are easily submerged in sea clutter, which cause missed detection. Due to this, strong sidelobes in SAR images generate false targets and reduce the detection accuracy. To solve these problems, a ship detection method based on eigensubspace projection (ESSP) in SAR images is proposed. First, the image is reconstructed into a new observation matrix along the azimuth direction, and the phase space matrix of the reconstructed image is constructed by using the Hankel characteristic, which preliminarily determines the approximate position of the ship. Then, the autocorrelation matrix of the reconstructed image is decomposed by eigenvalue decomposition (EVD). According to the size of the eigenvalues, the corresponding eigenvectors are divided into two parts, which constitute the basis of the ship subspace and the clutter subspace. Finally, the original image is projected into the ship subspace, and the ship data in the ship subspace are rearranged to obtain the precise position of the ship with significantly suppressed clutter. To verify the effectiveness of the proposed method, the ESSP method is compared with other detection methods on four images at different sea conditions. The results show that the detection accuracy of the ESSP method reaches 89.87% in complex scenes. Compared with other methods, the proposed method can extract ship targets from sea clutter more accurately and reduce the number of false alarms, which has obvious advantages in terms of detection accuracy and timeliness. Full article
Show Figures

Figure 1

Figure 1
<p>The experimental data. (<b>a</b>) Level 1 sea state in the nearshore scene; (<b>b</b>) level 3 sea state in the nearshore scene; (<b>c</b>) level 1 sea state in the offshore scene; (<b>d</b>) level 4 sea state in the offshore scene.</p>
Full article ">Figure 2
<p>The gray-scale spatial distribution of background and ship targets.</p>
Full article ">Figure 3
<p>Diagram of low-rank and sparse decomposition of SAR image.</p>
Full article ">Figure 4
<p>The flow chart of the ESSP method.</p>
Full article ">Figure 5
<p>The construction process of phase space matrix.</p>
Full article ">Figure 6
<p>Schematic diagram of image reconstruction.</p>
Full article ">Figure 7
<p>Detection results of the different methods in the first image. (<b>a</b>) Original SAR image; (<b>b</b>) RPCA method; (<b>c</b>) SP-CFAR method; (<b>d</b>) the ESSP method.</p>
Full article ">Figure 8
<p>Detection results of the different methods in the second image. (<b>a</b>) Original SAR image; (<b>b</b>) RPCA method; (<b>c</b>) SP-CFAR method; (<b>d</b>) the ESSP method.</p>
Full article ">Figure 9
<p>Detection results of the different methods in the third image. (<b>a</b>) Original SAR image; (<b>b</b>) RPCA method; (<b>c</b>) SP-CFAR method; (<b>d</b>) the ESSP method.</p>
Full article ">Figure 10
<p>Detection results of the different methods in the fourth image. (<b>a</b>) Original SAR image; (<b>b</b>) RPCA method; (<b>c</b>) SP-CFAR method; (<b>d</b>) the ESSP method.</p>
Full article ">
10 pages, 435 KiB  
Article
Some Information Geometric Aspects of Cyber Security by Face Recognition
by C. T. J. Dodson, John Soldera and Jacob Scharcanski
Entropy 2021, 23(7), 878; https://doi.org/10.3390/e23070878 - 9 Jul 2021
Cited by 1 | Viewed by 2380
Abstract
Secure user access to devices and datasets is widely enabled by fingerprint or face recognition. Organization of the necessarily large secure digital object datasets, with objects having content that may consist of images, text, video or audio, involves efficient classification and feature retrieval [...] Read more.
Secure user access to devices and datasets is widely enabled by fingerprint or face recognition. Organization of the necessarily large secure digital object datasets, with objects having content that may consist of images, text, video or audio, involves efficient classification and feature retrieval processing. This usually will require multidimensional methods applicable to data that is represented through a family of probability distributions. Then information geometry is an appropriate context in which to provide for such analytic work, whether with maximum likelihood fitted distributions or empirical frequency distributions. The important provision is of a natural geometric measure structure on families of probability distributions by representing them as Riemannian manifolds. Then the distributions are points lying in this geometrical manifold, different features can be identified and dissimilarities computed, so that neighbourhoods of objects nearby a given example object can be constructed. This can reveal clustering and projections onto smaller eigen-subspaces which can make comparisons easier to interpret. Geodesic distances can be used as a natural dissimilarity metric applied over data described by probability distributions. Exploring this property, we propose a new face recognition method which scores dissimilarities between face images by multiplying geodesic distance approximations between 3-variate RGB Gaussians representative of colour face images, and also obtaining joint probabilities. The experimental results show that this new method is more successful in recognition rates than published comparative state-of-the-art methods. Full article
Show Figures

Figure 1

Figure 1
<p>Adopted landmark topology in the FEI Face Database with varying face poses and expressions [<a href="#B18-entropy-23-00878" class="html-bibr">18</a>].</p>
Full article ">
12 pages, 1022 KiB  
Communication
Signal Subspace Reconstruction for DOA Detection Using Quantum-Behaved Particle Swarm Optimization
by Rui Zhang, Kaijie Xu, Yinghui Quan, Shengqi Zhu and Mengdao Xing
Remote Sens. 2021, 13(13), 2560; https://doi.org/10.3390/rs13132560 - 30 Jun 2021
Cited by 8 | Viewed by 2492
Abstract
Spatial spectrum estimation, also known as direction of arrival (DOA) detection, is a popular issue in many fields, including remote sensing, radar, communication, sonar, seismic exploration, radio astronomy, and biomedical engineering. MUltiple SIgnal Classification (MUSIC) and Estimation Signal Parameter via Rotational Invariance Technique [...] Read more.
Spatial spectrum estimation, also known as direction of arrival (DOA) detection, is a popular issue in many fields, including remote sensing, radar, communication, sonar, seismic exploration, radio astronomy, and biomedical engineering. MUltiple SIgnal Classification (MUSIC) and Estimation Signal Parameter via Rotational Invariance Technique (ESPRIT), which are well-known for their high-resolution capability for detecting DOA, are two examples of an eigen-subspace algorithm. However, missed detection and estimation accuracy reduction often occur due to the low signal-to-noise ratio (SNR) and snapshot deficiency (small time-domain samples of the observed signal), especially for sources with different SNRs. To avoid the above problems, in this study, we develop a DOA detection approach through signal subspace reconstruction using Quantum-Behaved Particle Swarm Optimization (QPSO). In the developed scheme, according to received data, a noise subspace is established through performing an eigen-decomposition operation on a sampling covariance matrix. Then, a collection of angles randomly selected from the observation space are used to build a potential signal subspace on the basis of the steering matrix of the array. Afterwards, making use of the fact that the signal space is orthogonal to the noise subspace, a cost function, which contains the desired DOA information, is designed. Thus, the problem of capturing the DOA information can be transformed into the optimization of the already constructed cost function. In this respect, the DOA finding of multiple signal sources—that is, the multi-objective optimization problem—can be regarded as a single objective optimization problem, which can effectively reduce the probability of missed detection of the signals. Subsequently, the QPSO is employed to determine an optimal signal subspace by minimizing the orthogonality error so as to obtain the DOA. Ultimately, the performance of DOA detection is improved. An explicit analysis and derivation of the developed scheme are provided. The results of computer simulation show that the proposed scheme has superior estimation performance when detecting signals with very different SNR levels and small snapshots. Full article
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>The modeling scheme of measured data.</p>
Full article ">Figure 2
<p>Diagram of Quantum-Behaved Particle Swarm Optimization (QPSO) algorithm.</p>
Full article ">Figure 3
<p>(<b>a</b>) Root mean square errors (RMSE) versus number of snapshots (signals with the same signal-to-noise ratio (SNR)). (<b>b</b>) The cost function and the RMSE versus the number of iterations.</p>
Full article ">Figure 4
<p>(<b>a</b>) RMSE versus number of snapshots (signals with different SNRs). (<b>b</b>) The cost function and the RMSE versus the number of iterations.</p>
Full article ">
21 pages, 934 KiB  
Article
A Spatial-Temporal Approach Based on Antenna Array for GNSS Anti-Spoofing
by Yuqing Zhao, Feng Shen, Guanghui Xu and Guochen Wang
Sensors 2021, 21(3), 929; https://doi.org/10.3390/s21030929 - 30 Jan 2021
Cited by 7 | Viewed by 3102
Abstract
The presence of spoofing signals poses a significant threat to global navigation satellite system (GNSS)-based positioning applications, as it could cause a malfunction of the positioning service. Therefore, the main objective of this paper is to present a spatial-temporal technique that enables GNSS [...] Read more.
The presence of spoofing signals poses a significant threat to global navigation satellite system (GNSS)-based positioning applications, as it could cause a malfunction of the positioning service. Therefore, the main objective of this paper is to present a spatial-temporal technique that enables GNSS receivers to reliably detect and suppress spoofing. The technique, which is based on antenna array, can be divided into two consecutive stages. In the first stage, an improved eigen space spectrum is constructed for direction of arrival (DOA) estimation. To this end, a signal preprocessing scheme is provided to solve the signal model mismatch in the DOA estimation for navigation signals. In the second stage, we design an optimization problem for power estimation with the estimated DOA as support information. After that, the spoofing detection is achieved by combining power comparison and cross-correlation monitoring. Finally, we enhance the genuine signals by beamforming while the subspace oblique projection is used to suppress spoofing. The proposed technique does not depend on external hardware and can be readily implemented on raw digital baseband signal before the despreading of GNSS receivers. Crucially, the low-power spoofing attack and multipath can be distinguished and mitigated by this technique. The estimated DOA and power are both beneficial for subsequent spoofing localization. The simulation results demonstrate the effectiveness of our method. Full article
(This article belongs to the Special Issue Advanced Interference Mitigation Techniques for GNSS-Based Navigation)
Show Figures

Figure 1

Figure 1
<p>Block diagram of the proposed anti-spoofing scheme.</p>
Full article ">Figure 2
<p>The root mean square error (RMSE) of direction of arrival (DOA) estimation versus SNR.</p>
Full article ">Figure 3
<p>The RMSE of power estimation versus SNR.</p>
Full article ">Figure 4
<p>Spatial spectrum estimation results.</p>
Full article ">Figure 5
<p>The cross-correlation results. (<b>a</b>) 25<math display="inline"><semantics> <msup> <mrow/> <mo>∘</mo> </msup> </semantics></math> and 30<math display="inline"><semantics> <msup> <mrow/> <mo>∘</mo> </msup> </semantics></math>; (<b>b</b>) 25<math display="inline"><semantics> <msup> <mrow/> <mo>∘</mo> </msup> </semantics></math> and 38<math display="inline"><semantics> <msup> <mrow/> <mo>∘</mo> </msup> </semantics></math>; (<b>c</b>) 25<math display="inline"><semantics> <msup> <mrow/> <mo>∘</mo> </msup> </semantics></math> and 54<math display="inline"><semantics> <msup> <mrow/> <mo>∘</mo> </msup> </semantics></math>; (<b>d</b>) 25<math display="inline"><semantics> <msup> <mrow/> <mo>∘</mo> </msup> </semantics></math> and 38<math display="inline"><semantics> <msup> <mrow/> <mo>∘</mo> </msup> </semantics></math>.</p>
Full article ">Figure 6
<p>Beam pattern for each authentic satellite.</p>
Full article ">Figure 7
<p>Spatial spectrum estimation results.</p>
Full article ">Figure 8
<p>Beam pattern for each authentic satellite.</p>
Full article ">Figure 9
<p>Spatial spectrum estimation results.</p>
Full article ">Figure 10
<p>Beam pattern for each authentic satellite.</p>
Full article ">
18 pages, 473 KiB  
Letter
Angle-Awareness Based Joint Cooperative Positioning and Warning for Intelligent Transportation Systems
by Zhi Dong and Bobin Yao
Sensors 2020, 20(20), 5818; https://doi.org/10.3390/s20205818 - 15 Oct 2020
Cited by 2 | Viewed by 2192
Abstract
In future intelligent vehicle-infrastructure cooperation frameworks, accurate self-positioning is an important prerequisite for better driving environment evaluation (e.g., traffic safety and traffic efficiency). We herein describe a joint cooperative positioning and warning (JCPW) system based on angle information. In this system, we first [...] Read more.
In future intelligent vehicle-infrastructure cooperation frameworks, accurate self-positioning is an important prerequisite for better driving environment evaluation (e.g., traffic safety and traffic efficiency). We herein describe a joint cooperative positioning and warning (JCPW) system based on angle information. In this system, we first design the sequential task allocation of cooperative positioning (CP) warning and the related frame format of the positioning packet. With the cooperation of RSUs, multiple groups of the two-dimensional angle-of-departure (AOD) are estimated and then transformed into the vehicle’s positions. Considering the system computational efficiency, a novel AOD estimation algorithm based on a truncated signal subspace is proposed, which can avoid the eigen decomposition and exhaustive spectrum searching; and a distance based weighting strategy is also utilized to fuse multiple independent estimations. Numerical simulations prove that the proposed method can be a better alternative to achieve sub-lane level positioning if considering the accuracy and computational complexity. Full article
Show Figures

Figure 1

Figure 1
<p>A graphical illustration of joint cooperative positioning and warning (JCPW).</p>
Full article ">Figure 2
<p>The warning systems: (<b>a</b>) two vehicle scenario; (<b>b</b>) a qualitative deceleration-distance curve.</p>
Full article ">Figure 3
<p>A graphical representation of the task sequences. CP, cooperative positioning.</p>
Full article ">Figure 4
<p>A graphical illustration of the localization data format.</p>
Full article ">Figure 5
<p>Performance evaluation for LOS angle-of-departure (AOD) estimation with different algorithms. (<b>a</b>) RMSE performance comparison; (<b>b</b>) Average single running time comparison.</p>
Full article ">Figure 6
<p>The cumulative distribution of the average absolute angle estimation error under different conditions.</p>
Full article ">Figure 7
<p>The positioning RMSE comparison for different weighting strategies.</p>
Full article ">
26 pages, 6737 KiB  
Article
Interference Mitigation for Synthetic Aperture Radar Based on Deep Residual Network
by Weiwei Fan, Feng Zhou, Mingliang Tao, Xueru Bai, Pengshuai Rong, Shuang Yang and Tian Tian
Remote Sens. 2019, 11(14), 1654; https://doi.org/10.3390/rs11141654 - 11 Jul 2019
Cited by 66 | Viewed by 5550
Abstract
Radio Frequency Interference (RFI) is a key issue for Synthetic Aperture Radar (SAR) because it can seriously degrade the imaging quality, leading to the misinterpretation of the target scattering characteristics and hindering the subsequent image analysis. To address this issue, we present a [...] Read more.
Radio Frequency Interference (RFI) is a key issue for Synthetic Aperture Radar (SAR) because it can seriously degrade the imaging quality, leading to the misinterpretation of the target scattering characteristics and hindering the subsequent image analysis. To address this issue, we present a narrow-band interference (NBI) and wide-band interference (WBI) mitigation algorithm based on deep residual network (ResNet). First, the short-time Fourier transform (STFT) is used to characterize the interference-corrupted echo in the time–frequency domain. Then, the interference detection model is built by a classical deep convolutional neural network (DCNN) framework to identify whether there is an interference component in the echo. Furthermore, the time–frequency feature of the target signal is extracted and reconstructed by utilizing the ResNet. Finally, the inverse time–frequency Fourier transform (ISTFT) is utilized to transform the time–frequency spectrum of the recovered signal into the time domain. The effectiveness of the interference mitigation algorithm is verified on the simulated and measured SAR data with strip mode and terrain observation by progressive scans (TOPS) mode. Moreover, in comparison with the notch filtering and the eigensubspace filtering, the proposed interference mitigation algorithm can improve the interference mitigation performance, while reducing the computation complexity. Full article
(This article belongs to the Special Issue Radio Frequency Interference (RFI) in Microwave Remote Sensing)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Synthetic Aperture Radar (SAR) echoes corrupted with (<b>a</b>) and (<b>b</b>) narrow-band interference (NBI) in range-frequency azimuth-time domain and wide-band interference (WBI) in azimuth-frequency range-time domain.</p>
Full article ">Figure 2
<p>An example of the (<b>a</b>) NBI-corrupted echo in the range-time domain, (<b>b</b>) NBI-corrupted echo in the range-frequency domain, (<b>c</b>) NBI-corrupted echo in the time–frequency domain, (<b>d</b>) WBI-corrupted echo in the azimuth-time domain, (<b>e</b>) WBI-corrupted echo in the azimuth-frequency domain, and (<b>f</b>) WBI-corrupted echo in the time–frequency domain.</p>
Full article ">Figure 3
<p>The interference detection network (IDN) framework.</p>
Full article ">Figure 4
<p>Samples of echoes in time–frequency representation used for training the IDN. (<b>a</b>) Shows the NBI-corrupted echoes, (<b>b</b>) shows the WBI-corrupted echoes, and (<b>c</b>) shows the echoes without interference.</p>
Full article ">Figure 4 Cont.
<p>Samples of echoes in time–frequency representation used for training the IDN. (<b>a</b>) Shows the NBI-corrupted echoes, (<b>b</b>) shows the WBI-corrupted echoes, and (<b>c</b>) shows the echoes without interference.</p>
Full article ">Figure 5
<p>The interference mitigation network (IMN) framework.</p>
Full article ">Figure 6
<p>Workflow of the interference detection and mitigation based on a deep convolutional neural network (DCNN).</p>
Full article ">Figure 7
<p>Simulated SAR echoes in the time–frequency domain for training and testing the IMN. (<b>a</b>) the original SAR echoes without interference, and (<b>b</b>) the interference-corrupted echoes.</p>
Full article ">Figure 8
<p>The convergence curve of training accuracy with training iterations.</p>
Full article ">Figure 9
<p>Representation in the time–frequency domain. (<b>a</b>) Short-time Fourier transform (STFT) of the NBI-free pulse. (<b>b</b>) STFT of the simulated NBI-corrupted pulse. (<b>c</b>) STFT after the range spectrum notch filtering. (<b>d</b>) STFT after the eigensubspace filtering. (<b>e</b>) STFT after the IMN.</p>
Full article ">Figure 10
<p>Representation in the time–frequency domain. (<b>a</b>) STFT of the WBI-free pulse. (<b>b</b>) STFT of the simulated WBI-corrupted pulse. (<b>c</b>) STFT after the instantaneous-spectrum notch filtering. (<b>d</b>) STFT after the eigensubspace filtering. (<b>e</b>) STFT after the IMN.</p>
Full article ">Figure 11
<p>The representation of the (a) 500th and (b) 1000th measured NBI-contaminated echoes in the time–frequency domain.</p>
Full article ">Figure 12
<p>The detection probability of radar pulse before NBI mitigation, where the red line represents the threshold.</p>
Full article ">Figure 13
<p>Mitigation results. (<b>a</b>) the SAR image without interference mitigation, (<b>b</b>) the SAR image after applying the range-spectrum notch filtering, (<b>c</b>) the SAR image after applying the eigensubspace filtering, and (<b>d</b>) the SAR image after applying the IMN.</p>
Full article ">Figure 13 Cont.
<p>Mitigation results. (<b>a</b>) the SAR image without interference mitigation, (<b>b</b>) the SAR image after applying the range-spectrum notch filtering, (<b>c</b>) the SAR image after applying the eigensubspace filtering, and (<b>d</b>) the SAR image after applying the IMN.</p>
Full article ">Figure 14
<p>The representation of the measured WBI-contaminated echoes in the time–frequency domain. (<b>a</b>) The STFT of the WBI-contaminated echo before de-ramping, and (<b>b</b>) the STFT of the WBI-contaminated echo after de-ramping.</p>
Full article ">Figure 15
<p>The detection probability of radar pulse before WBI mitigation, where the red line represents the threshold.</p>
Full article ">Figure 16
<p>The SAR imaging results (a) without interference mitigation and (b) after IMN.</p>
Full article ">Figure 17
<p>Mitigation results. (<b>a</b>) The SAR image without interference mitigation, (<b>b</b>) the SAR image after applying the instantaneous-spectrum notch filtering, (<b>c</b>) the SAR image after applying the eigensubspace filtering, and (<b>d</b>) the SAR image after applying the IMN.</p>
Full article ">Figure 17 Cont.
<p>Mitigation results. (<b>a</b>) The SAR image without interference mitigation, (<b>b</b>) the SAR image after applying the instantaneous-spectrum notch filtering, (<b>c</b>) the SAR image after applying the eigensubspace filtering, and (<b>d</b>) the SAR image after applying the IMN.</p>
Full article ">Figure 18
<p>The representation of two measured WBI-contaminated echoes in the time–frequency domain.</p>
Full article ">Figure 19
<p>The detection probability of radar pulse before WBI mitigation, where the red line represents the threshold.</p>
Full article ">Figure 20
<p>Mitigation results. (<b>a</b>) The SAR image without interference mitigation, (<b>b</b>) the SAR image after applying the instantaneous-spectrum notch filtering, (<b>c</b>) the SAR image after applying the eigensubspace filtering, and (<b>d</b>) the SAR image after applying the IMN.</p>
Full article ">Figure 20 Cont.
<p>Mitigation results. (<b>a</b>) The SAR image without interference mitigation, (<b>b</b>) the SAR image after applying the instantaneous-spectrum notch filtering, (<b>c</b>) the SAR image after applying the eigensubspace filtering, and (<b>d</b>) the SAR image after applying the IMN.</p>
Full article ">
21 pages, 5490 KiB  
Article
Multilinear EigenECGs and FisherECGs for Individual Identification from Information Obtained by an Electrocardiogram Sensor
by Yeong-Hyeon Byeon, Jae-Neung Lee, Sung-Bum Pan and Keun-Chang Kwak
Symmetry 2018, 10(10), 487; https://doi.org/10.3390/sym10100487 - 12 Oct 2018
Cited by 4 | Viewed by 2541
Abstract
In this study, we present a third-order tensor-based multilinear eigenECG (MEECG) and multilinear Fisher ECG (MFECG) for individual identification based on the information obtained by an electrocardiogram (ECG) sensor. MEECG and MFECG are based on multilinear principal component analysis (MPCA) and multilinear linear [...] Read more.
In this study, we present a third-order tensor-based multilinear eigenECG (MEECG) and multilinear Fisher ECG (MFECG) for individual identification based on the information obtained by an electrocardiogram (ECG) sensor. MEECG and MFECG are based on multilinear principal component analysis (MPCA) and multilinear linear discriminant analysis (MLDA) in the field of multilinear subspace learning (MSL), respectively. MSL directly extracts features without the vectorization of input data, while MSL extracts features without vectorizing the input data while maintaining most of the correlations shown in the original structure. In contrast with unsupervised linear subspace learning (LSL) techniques such as PCA (Principal Component Analysis) and LDA (Linear Discriminant Analysis), it is less susceptible to small-data problems because it learns more compact and potentially useful representations, and it can efficiently handle large tensors. Here, the third-order tensor is formed by reordering the one-dimensional ECG signal into a two-dimensional matrix, considering the time frame. The MSL consists of four steps. The first step is preprocessing, in which input samples are centered. The second step is initialization, in which eigen decomposition is performed and the most significant eigenvectors are selected. The third step is local optimization, in which input data is applied by eigenvectors from the second step, and new eigenvectors are calculated using the applied input data. The final step is projection, in which the resultant feature tensors after projection are obtained. The experiments are performed on two databases for performance evaluation. The Physikalisch-Technische Bundesanstalt (PTB)-ECG is a well-known database, and Chosun University (CU)-ECG is directly built for this study using the developed ECG sensor. The experimental results revealed that the tensor-based MEECG and MFECG showed good identification performance in comparison to PCA and LDA of LSL. Full article
Show Figures

Figure 1

Figure 1
<p>Flowchart of multilinear principal component analysis (MPCA).</p>
Full article ">Figure 2
<p>Process of a multilinear projection.</p>
Full article ">Figure 3
<p>Process of multilinear linear discriminant analysis (MLDA).</p>
Full article ">Figure 4
<p>Comparison of multilinear subspace learning (MSL) with unsupervised linear subspace learning (LSL): (<b>a</b>) LSL; (<b>b</b>) MSL.</p>
Full article ">Figure 5
<p>Course of preprocessing: (<b>a</b>) Original signal; (<b>b</b>) regularized signal; (<b>c</b>) spike-removed signal; (<b>d</b>) detected peaks.</p>
Full article ">Figure 6
<p>Input shapes of LSL and MSL on electrocardiogram (ECG) signal.</p>
Full article ">Figure 7
<p>Course of multilinear eigenECG (MEECG) feature extraction.</p>
Full article ">Figure 8
<p>Course of MFECG feature extraction: (<b>a</b>) Parameters calculation of MFECG using training data; (<b>b</b>) Projection of the training and test data.</p>
Full article ">Figure 9
<p>Comparison of correlation by reshaping: (<b>a</b>) Correlation of a 1D vector; (<b>b</b>) correlation of a 3D tensor reshaped from a low dimension to a high dimension; (<b>c</b>) correlation of a 3D tensor; (<b>d</b>) correlation of a 1D vector reshaped from a high dimension to a low dimension.</p>
Full article ">Figure 10
<p>New correlations by reshaping.</p>
Full article ">Figure 11
<p>Diagram of base board and its real image.</p>
Full article ">Figure 12
<p>Environment for measuring ECG signals.</p>
Full article ">Figure 13
<p>Symmetric tensor.</p>
Full article ">Figure 14
<p>Comparison of the highest accuracies in each distance and each method on PTB-ECG.</p>
Full article ">Figure 15
<p>Comparison of the highest accuracies in each distance and each method on CU-ECG.</p>
Full article ">Figure 16
<p>MEECG feature space for 12 classes.</p>
Full article ">Figure 17
<p>MFECG feature space for 12 classes.</p>
Full article ">
25 pages, 3936 KiB  
Article
Mitigating Wind Induced Noise in Outdoor Microphone Signals Using a Singular Spectral Subspace Method
by Omar Eldwaik and Francis F. Li
Technologies 2018, 6(1), 19; https://doi.org/10.3390/technologies6010019 - 28 Jan 2018
Cited by 5 | Viewed by 6752
Abstract
Wind induced noise is one of the major concerns of outdoor acoustic signal acquisition. It affects many field measurement and audio recording scenarios. Filtering such noise is known to be difficult due to its broadband and time varying nature. In this paper, a [...] Read more.
Wind induced noise is one of the major concerns of outdoor acoustic signal acquisition. It affects many field measurement and audio recording scenarios. Filtering such noise is known to be difficult due to its broadband and time varying nature. In this paper, a new method to mitigate wind induced noise in microphone signals is developed. Instead of applying filtering techniques, wind induced noise is statistically separated from wanted signals in a singular spectral subspace. The paper is presented in the context of handling microphone signals acquired outdoor for acoustic sensing and environmental noise monitoring or soundscapes sampling. The method includes two complementary stages, namely decomposition and reconstruction. The first stage decomposes mixed signals in eigen-subspaces, selects and groups the principal components according to their contributions to wind noise and wanted signals in the singular spectrum domain. The second stage reconstructs the signals in the time domain, resulting in the separation of wind noise and wanted signals. Results show that microphone wind noise is separable in the singular spectrum domain evidenced by the weighted correlation. The new method might be generalized to other outdoor sound acquisition applications. Full article
Show Figures

Figure 1

Figure 1
<p>The two complementary stages of the SSA method.</p>
Full article ">Figure 2
<p>A descriptive process of the SSA method.</p>
Full article ">Figure 3
<p>Main aspects in the SSA method.</p>
Full article ">Figure 4
<p>Representation of a given time series when considering for example a window length <span class="html-italic">m</span> = 4 to construct the trajectory matrix.</p>
Full article ">Figure 5
<p>A flow chart of the experimental procedure.</p>
Full article ">Figure 6
<p>Window length optimisation using seven different values of the frame length.</p>
Full article ">Figure 7
<p>Singular spectra of clean record of birds’ chirps and a noisy one with wind noise added.</p>
Full article ">Figure 8
<p>The leading four principle components used for grouping and reconstruction and the record of birds’ chirps with additive wind noise: (<b>a</b>) Reconstruction with the first two leading pairs of the principle components; (<b>b</b>) Reconstruction with the third and fourth principle components pairs.</p>
Full article ">Figure 9
<p>Reconstructed series vs original noisy signal and residual series.</p>
Full article ">Figure 10
<p>The de-noised record was separated by retaining only the leading two pairs of the eigenvalues.</p>
Full article ">Figure 11
<p>A combination of our signals used in the experiments: (<b>a</b>) Noisy record (birds’ chirps and wind noise); (<b>b</b>) Clean record of birds’ chirps.</p>
Full article ">Figure 12
<p>Moving periodogram matrix of reconstructed components.</p>
Full article ">Figure 13
<p>Matrix of <span class="html-italic">w</span>-correlations of the selected 50 eigenvectors of the SVD of the trajectory matrix.</p>
Full article ">
Back to TopTop