Base image TV model based CT (Computed Tomography) beam hardening correcting method
A technology of beam hardening correction and base image, applied in 2D image generation, image enhancement, image data processing, etc., can solve problems such as low actual value and large deviation of hardening degree
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Embodiment 1
[0068] Embodiment 1: In a CT imaging system, X-ray hardening causes cupping and striping artifacts in reconstructed images, seriously affecting image quality. In this paper, by analyzing the influence of beam hardening on the original projection data, it is found that the beam hardening causes the actual value in the original projection to be lower than the ideal value, and the greater the degree of hardening, the more serious the deviation. The CT beam hardening correction method based on the basic image TV model of the present invention is completed by the following steps on the basis of establishing a beam hardening correction model with adjustable parameters: first, under different adjustable parameter conditions, the original The projection data is preprocessed and transformed by the model to obtain multiple sets of preprocessed projection sequences, and then the preprocessed projection sequences are reconstructed to obtain a series of corrected base images, and the total ...
Embodiment 2
[0070] Embodiment 2: The CT beam hardening correction method based on the basic image TV model in this embodiment first analyzes the influence of beam hardening on projection data, and then establishes a beam hardening correction model on this basis, and adopts the following method Perform an analysis of the effect of beam hardening on projection data:
[0071] The intensity attenuation formula of monoenergetic X-rays passing through homogeneous matter can be expressed by Beer’s law, as shown in formula (1),
[0072] I 1 =I 0 e -μx (1)
[0073] where I 0 Indicates the initial intensity of monoenergetic rays; I 1 Indicates the transmitted ray intensity; μ is the material attenuation coefficient, which is related to the density of the material and the energy of the ray; x indicates the length of the material that the ray passes through. Then, from formula (1), we can get:
[0074] μx = - ln I ...
Embodiment 3
[0083] Embodiment 3: The CT beam hardening correction method based on the base image TV model of this embodiment, on the basis of analyzing the influence of beam hardening on projection data in Embodiment 2, establishes a hardening correction model through the following steps:
[0084] Let P be the original projection obtained under the condition of multi-energy spectral rays, P′ be the corresponding projection data after P correction, and define the following functional relationship between P′ and P:
[0085] P'=S(P) (6)
[0086] Among them, S is a pre-correction function, S is a linear function, an exponential function or a power function, combined with a power function and an exponential function, the form of the design function S is as follows:
[0087] S(P)=P (7)
[0088] Add variable parameter n(n ∈ N + ), namely S n (P)=P n (n∈N + ), using S n (P) Fitting the calibration curve, taking different values of n to get different S n (P), which means that the projecti...
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