CN113205462A - Photon reflectivity image denoising method based on neural network learning prior - Google Patents
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Abstract
The invention provides a photon reflectivity image denoising method based on neural network learning prior, which mainly comprises the construction of an imaging model and the networking of the model. Firstly, constructing a photon counting imaging model, solving the model to obtain a corresponding subproblem, then networking the model of the subproblem, constructing a convolutional neural network, giving a training set, learning corresponding parameters of a prior and the model, and finally obtaining a denoising result of a photon reflectivity image. Experiments prove that the method provided by the invention networks the model through learning prior, and adopts the convolutional neural network to denoise the image, so that the indexes of the denoised image are close to ideal values.
Description
Technical Field
The invention belongs to the field of photon counting imaging, and relates to a photon reflectivity image denoising method based on neural network learning prior, which is suitable for various photon counting imaging application scenes.
Background
Photon counting imaging can be used to detect targets in extremely low light conditions, while other imaging techniques have difficulty acquiring valid data in extremely low light conditions. Therefore, the method has attracted extensive research interest in a variety of fields such as spatial monitoring, biological imaging, fluorescence and microscopy. Unlike most imaging techniques that measure the intensity of reflected light from a target, photon counting imaging computes each photon collected from reflected light from a different spatial point. Under the condition of extremely low illumination, the background noise is relatively large.
Taking into account the effects of noise under low light conditions, a poisson distribution is often used to measure the process of counting reflected photons. To remove poisson noise, the poisson distribution may be approximated with a gaussian distribution using a variance-stabilized transform (VST), and denoised using conventional denoising algorithms such as block matching and three-dimensional filtering (BM 3D). However, in most single photon counting imaging applications, this approximation is inaccurate because the number of photons received is very low, resulting in high frequency artifacts. In recent work on single photon counting imaging, reconstruction from the count data has always been done by minimizing the negative poisson log-likelihood term. In 2014, the Ahmed Kirmani team published a First-photon imaging (FPI) system on Science, which proposed to recover 3D structure and reflectivity information from the First detected photon of each pixel. Dongeek Shin proposed a reliable method to estimate the reflectivity based on FPI that would allow better reflectivity images using a fixed dwell time for each pixel. The deep learning method is also applied to single photon counting imaging, but the existing methods are all based on a black box model and cannot combine a real physical model with a network. How to effectively remove the noise in the photon counting image has become a focus of attention and research of many researchers at home and abroad.
Disclosure of Invention
Aiming at the defects of the prior art, the invention provides a photon reflectivity image denoising method based on neural network learning prior.
The technical scheme adopted by the invention is as follows: a photon reflectivity image denoising method based on neural network learning prior mainly comprises the construction of an imaging model and the networking of the model. Firstly, constructing a photon counting imaging model, solving the model to obtain a corresponding subproblem, then networking the model of the subproblem, constructing a convolutional neural network, giving a training set, learning corresponding parameters of a prior and the model, and finally obtaining a denoising result of a photon reflectivity image. The method comprises the following steps:
step 1: constructing a photon counting imaging model, which can be expressed as:
where α represents the photon reflectance image, J (α) is the data fidelity term, and K (α) is the a priori constraint term.
Step 2: and solving the imaging model to obtain corresponding subproblems.
And step 3: and (4) networking the physical model of the subproblem, and constructing a convolutional neural network and a loss function.
And 4, step 4: and training the convolutional neural network, and obtaining a denoising result of the reflectivity image according to the trained network model.
Preferably, the specific implementation of step 1 comprises the following sub-steps:
step 1.1: and constructing a data fidelity item J (alpha). In general, a given photon count value ki,jReflectivity of alphai,jThe poisson negative log-likelihood function of (a) may be expressed as:
wherein N is the number of emitted pulses, η is the detection efficiency of the detector, B is the background count of the pulse repetition period, S is the signal count within the pulse repetition period, and i, j are the spatial point coordinates. The above equation is taken as a data fidelity term.
Step 1.2: an a priori constraint term K (α) is constructed. In the traditional method, the wavelet domain is sparse, the gradient is sparse and not necessarily accurate, and in order to obtain better effect, the invention adopts a universal methodThe nonlinear function sparsifies the reflectivity image, and the function is recorded asThe parameters of which are learnable. Inspired by strong nonlinear feature representation capability of convolutional neural network, the method is toDesigned as a combination of two linear convolution operators separated by one linear rectifying unit (ReLU), as shown in fig. 2. From this, the expression of the a priori constraint term is obtained:
step 1.3: and obtaining a final reflectivity image reconstruction model. Since η S α < 1, the following approximation can be made:
1-exp[-(ηSα+B)]≈ηSα+B
the final reconstruction model can thus be obtained:
where λ is the regularization parameter and k is the matrix of photon count values for all spatial points.
Preferably, the specific implementation of step 2 comprises the following sub-steps:
step 2.1: solving formula (1) based on an optimization strategy (A fast iterative learning algorithm for linear inverse schemes) of FISTA to obtain the following two sub-problems:
where ρ is a constant, rxIs the result of the x-th iteration calculation of the intermediate variable r, which is alphaxAnd directly reconstructing a result in the x iteration, wherein the initial value can be obtained according to the maximum likelihood estimation.
Preferably, the specific implementation of step 3 comprises the following sub-steps:
step 3.1: r isxThe model is networked, and in order to maintain the network structure and increase the flexibility of the network, the value of the parameter ρ is not fixed and is made to vary as a network parameter with the learning of the network, and then r is calculated according to equation (2)xThe model becomes:
step 3.2: alpha is alphaxAnd networking the model. To network the model, let r bexAndare respectively alpha andthe following approximation can be obtained for the mean value of:
wherein beta is a single radical ofThe associated scalar, applying the above approximation term to equation (3), yields:
introduction ofIs inverse operation ofDefinition ofFinally obtaining alphaxThe networking model of (1):
in order to maintain the flexibility of the network and increase the capacity of the network, the network is controlled by the control unitTheta varies with the iteration of the network, and thus, alpha can be obtainedxNetworked final model of (2):
FIG. 2 shows rxAnd alphaxHow the closed loop form of (a) is mapped to a deep network, first using maximum likelihood estimation from alphax-1To obtain rx,rxThrough the network layerBecome intoIn a soft threshold operationTo obtainAt the network layerOutput alphaxAnd completing a closed loop operation.
Step 3.3: a loss function is constructed. Using data setsTraining is carried out, and the network counts the photons to form an image kiGenerating a reconstruction result as an inputWe satisfy the symmetry conditionIs reduced in the case ofAnd group Truth yiFrom this, the following loss function can be designed:
wherein:
wherein N isbIs the total number of training blocks, NpNumber of network layers, NsFor each training block size, γ is a constant.
The invention mainly aims at the novel calculation imaging technology of single photon counting imaging, and provides a denoising method based on convolutional neural network learning prior, which combines the advantages of a model and a network by networking a physical model.
Drawings
FIG. 1 is a network framework diagram of the present invention.
FIG. 2 is a non-linear functionAnd its inverse functionThe structure of (1) is formed into a diagram.
Fig. 3 is a comparison of visual quality of photon reflectivity images reconstructed by using simulation data and the method of the present invention and other comparison methods, where (a) is a group Truth, (b) is a photon counting simulation image added with poisson noise and impulse noise, (c) is a denoising result of SPIRALONB, (d) is a denoising result of binomial SPIRAL TV, (e) is a denoising result of NLSPCA, (f) is a denoising result of VST + BM3D, and (g) is a reconstruction result of the method of the present invention.
Detailed Description
In order to facilitate the understanding and implementation of the present invention for those of ordinary skill in the art, the present invention will be described in further detail with reference to the accompanying drawings and examples, it is to be understood that the examples described herein are only for the purpose of illustrating the present invention and are not to be construed as limiting the present invention.
As shown in fig. 1, an embodiment of the present invention provides a photon reflectivity image denoising method based on convolutional neural network learning prior. The method specifically comprises the following steps:
step 1: constructing a photon counting imaging model, which can be expressed as:
where α represents the photon reflectance image, J (α) is the data fidelity term, and K (α) is the a priori constraint term. The specific implementation comprises the following substeps:
step 1.1: and constructing a data fidelity item J (alpha). In general, a given photon count value ki,jReflectivity of alphai,jThe poisson negative log-likelihood function of (a) may be expressed as:
the above equation is taken as a data fidelity term. Wherein N is the number of emitted pulses, η is the detection efficiency of the detector, B is the background count of the pulse repetition period, S is the signal count within the pulse repetition period, and i, j are the spatial point coordinates. In this embodiment, N is 100, η is 0.35, B is 0, and S is 1.
Step 1.2: an a priori constraint term K (α) is constructed. In the traditional method, the wavelet domain is sparse, the gradient is sparse and not accurate, and in order to obtain a better effect, the invention adopts a general nonlinear function to carry out sparsification on the reflectivity image, and the function is recorded asThe parameters of which are learnable. Inspired by the powerful representation capability of the convolutional neural network and the general approximate property thereof, the method is toDesigned as a combination of two linear convolution operators separated by one linear rectifying unit (ReLU), as shown in fig. 2. From this, the expression of the a priori constraint term is obtained:
step 1.3: and obtaining a final reflectivity image reconstruction model. Since η S α < 1, the following approximation can be made:
1-exp[-(ηSα+B)]≈ηSα+B
the final reconstruction model can thus be obtained:
where λ is the regularization parameter and k is the matrix of photon count values for all spatial points.
Step 2: and solving the imaging model to obtain corresponding subproblems. The method specifically comprises the following steps:
step 2.1: solving formula (1) based on an optimization strategy (A fast iterative learning algorithm for linear inverse schemes) of FISTA to obtain the following two sub-problems:
where ρ is a constant, rxIs the result of the x-th iteration calculation of the intermediate variable r, which is alphaxThe direct reconstruction result at the x-th iteration, the initial value of which can be obtained from the maximum likelihood estimation, i.e.
And step 3: and (4) networking the physical model of the subproblem, and constructing a convolutional neural network and a loss function. The specific implementation comprises the following substeps:
step 3.1: r isxAnd networking the model. In order to maintain the structure of the network and increase the flexibility of the network, the value of the parameter ρ is not fixed, so that it changes as a network parameter with the learning of the network. Then, r is according to the formula (1)xThe model becomes:
step 3.2: alpha is alphaxAnd networking the model. To network the model, let r bexAndare respectively alpha andthe following approximation can be obtained for the mean value of:
wherein beta is a single radical ofScalar quantity concerned, applying the above approximation term to the equation (2) and adoptingThe image is thinned, so that the following results can be obtained:
introduction ofIs inverse operation ofDefinition ofFinally obtaining alphaxThe networking model of (1):
in order to maintain the flexibility of the network and increase the capacity of the network, the network is controlled by the control unitTheta varies with the iteration of the network, and thus, alpha can be obtainedxNetworked final model of (2):
FIG. 2 shows rxAnd alphaxHow to map to a deep network. First using maximum likelihood estimation, from alphax-1To obtain rx,rxThrough the network layerBecome intoIn a soft threshold operationTo obtainAt the network layerOutput alphaxAnd completing a closed loop operation. In the present embodiment, θ0=0.0005。
Step 3.3: a loss function is constructed. Using data setsTraining is carried out, and the network counts the photons to form an image kiGenerating a reconstruction result as an inputWe satisfy the symmetry conditionIs reduced in the case ofAnd group Truth yiFrom this, the following loss function can be designed:
wherein:
wherein N isbIs the total number of training blocks, NpNumber of network layers, NsFor each training block size, γ is a constant. In this embodiment, Nb=192000,Ns=1089,Np=9,γ=0.01。
And 4, step 4: and training the network by using the simulation data, and obtaining a denoising result of the reflectivity image according to the trained network model. In this embodiment, the training speed lr is 0.0001, the batch size is 64, the convolution kernel size is 3 × 3, and the number of channels is 32.
And obtaining a photon reflectivity image based on the operation, selecting a 'Male' image with the resolution of 1024 multiplied by 1024 in an image database of a signal and image processing research institute from southern California university as a true value image in order to quantitatively evaluate the reconstructed image, simulating the true value image to obtain a photon counting image, and selecting a peak signal-to-noise ratio (PSNR) as an evaluation index. For comparison with other methods, we used the SPIRALONB method, binomial SPIRAL TV method, NLSPCA method, and VST + BM3D method to compare with our method, we selected 100 pictures in the BSD300 data set as the training set, and the results are shown in table 1. For a comparison of the visual quality of the reconstructed images of the algorithms, see fig. 3.
TABLE 1 PSNR (dB) comparison of different reconstruction methods (ideal: +∞)
It can be seen that the method provided by the inventor networks the model through learning prior, and adopts the convolutional neural network to denoise the image, so that the indexes of the denoised image are close to ideal values.
The method mainly aims at the application requirement of the photon counting imaging image denoising. In consideration of the defects of the traditional method, the photon counting image denoising method based on the learning prior is provided, an optimal sparse representation mode is obtained through learning, and the parameter design process is further simplified through a model networking mode, so that an optimal result is obtained.
It should be understood that parts of the specification not set forth in detail are well within the prior art.
It should be understood that the above-mentioned embodiments are described in some detail, and not intended to limit the scope of the invention, and those skilled in the art will be able to make alterations and modifications without departing from the scope of the invention as defined by the appended claims.
Claims (5)
1. A photon reflectivity image denoising method based on neural network learning prior is characterized by comprising the following steps:
step 1, constructing a photon counting imaging model, wherein the photon counting imaging model is expressed as follows:
wherein alpha represents a photon reflectivity image, J (alpha) is a data fidelity term, and K (alpha) is a priori constraint term;
step 2, solving the imaging model to obtain corresponding subproblems;
step 3, networking the physical model of the sub-problem, and constructing a convolutional neural network and a loss function;
and 4, training the convolutional neural network, and obtaining a denoising result of the reflectivity image according to the trained network model.
2. The method of claim 1, wherein the method comprises: the specific implementation of the step 1 comprises the following substeps:
step 1.1, constructing a data fidelity term J (alpha), and giving a photon counting value ki,jReflectivity of alphai,jThe poisson negative log-likelihood function of (a) may be expressed as:
wherein N is the number of emitted pulses, eta is the detection efficiency of the detector, B is the background count of the pulse repetition period, S is the signal count within the pulse repetition period, i, j are the coordinates of spatial points, and the above formula is used as a data fidelity term;
step 1.2, constructing a prior constraint term K (alpha),
wherein the content of the first and second substances,is a combination of two linear convolution operators separated by one linear rectifying unit;
step 1.3, obtaining a final reflectivity image reconstruction model, wherein because eta S alpha is less than 1, the following approximation can be carried out:
1-exp[-(ηSα+B)]≈ηSα+B
the final reconstruction model can thus be obtained:
where λ is the regularization parameter and k is the matrix of photon count values for all spatial points.
3. The method of claim 2, wherein the method comprises: the specific implementation of step 2 comprises the following sub-steps,
step 2.1, solving the formula (1) based on the optimization strategy of FISTA to obtain the following two subproblems:
where ρ is a constant, rxIs the result of the x-th iteration calculation of the intermediate variable r, which is alphaxAnd directly reconstructing a result in the x iteration, wherein the initial value can be obtained according to the maximum likelihood estimation.
4. The method of claim 3, wherein the method comprises: the specific implementation of the step 3 comprises the following substeps:
step 3.1, rxNetworking of the model, in which the value of the parameter p varies as the network is learned, r according to equation (2)xThe model becomes:
step 3.2, alphaxModeling, assuming r for modelingxAndare respectively alpha andthe following approximation can be obtained for the mean value of:
wherein beta is a single radical ofThe associated scalar, applying the above approximation term to equation (3), yields:
introduction ofIs inverse operation ofDefinition ofFinally obtaining alphaxThe networking model of (1):
in order to maintain the flexibility of the network and increase the capacity of the network, the network is controlled by the control unitTheta varies with the iteration of the network, and thus, alpha can be obtainedxNetworked final model of (2):
step 3.3, constructing a loss function and adopting a data setTraining is carried out, and the network counts the photons to form an image kiGenerating a reconstruction result as an inputWhen the symmetric condition is satisfiedIn the state ofUnder the condition of reducingAnd group Truth yiFrom which the following loss function is designed:
wherein:
wherein N isbIs the total number of training blocks, NpNumber of network layers, NsFor each training block size, γ is a constant.
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CN114692509A (en) * | 2022-04-21 | 2022-07-01 | 南京邮电大学 | Strong noise single photon three-dimensional reconstruction method based on multi-stage degeneration neural network |
CN115222949A (en) * | 2022-09-21 | 2022-10-21 | 自然资源部第一海洋研究所 | Shallow sea area photon denoising method based on laser satellite data |
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