The method proposed is based at statistical properties of the Poisson flux caused by ionizing radiation detection. It works at the earliest stage of image shaping when the statistical properties of incident flux have not been lost yet and includes the analysis and processing of image forming flux taking into account local properties of it in the vicinity of each event and, as a consequence, irregularities in flux density. Hence, the existing gradient in flux density between the different sections of the same image can be magnified. Due to density of image forming flux depends on the specimen internal structure one may get to improve the contract and detection of defects. From the practical point of view we are allowed to obtain the pictures of defects with enhanced contrast in comparison to images being formed without the analysis and modification of original flux.

Fig 1: Schematic diagram of image forming.
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In classical schemes the flux y (x,y,z) comes to imagine surface where it is being integrated and shaped.
In the frames of the method we propose to process the flux y (x,y,z) before it will form the image. The processing itself is based at analysis of separate flux sections with respect to their own statistical properties and taking into account the correlation between different sections. Such the approach allows to change the level of detailisation and, subsequently, to adjust the sensitivity to discontinuities of small sizes as well as the contrasting amplification to big flaws. Moreover, the method proposed can be used either for image contrasting for low intensity flux by using the space processing of results or for getting of contrast image by means of flux processing in time scale.
To demonstrate the advantages of the method proposed we conducted modeling experiments to determine it's quantitative and qualitative characteristics. The model for flux simulation and subsequent image shaping has been developed and verified. It was assumed that incident flux is the Poisson one and during the exposure time the flux is constant.
The model developed realizes the diagram at Fig.1 to shaping the image and gives the possibility to include the program unit to process the flux y (x,y,z).To be able to estimate the results obtained, the contrasting coefficient K was proposed to be as a measure of contrast enhancement:
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| where: B0 - brightness of given part of image;
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| Bb - background brightness caused by the specimen itself.
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1. For the first set of experiments the procedure of image shaping was modeled. The "specimen" had the notches of different areas machined in the surface. The original "specimen" image is shown at Fig.2 a). The result of classical shaping image is presented at Fig.2 b). Fig.2 c) shows the result of implemented procedure. Also the contrasting coefficients K are given for both procedures.
| a)
| b)
| c)
| | Fig 2: Modeling results for exposure the specimen having notches of different areas machined in the specimen surface.
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| Methods for image
| Image sections
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| shaping
| I
| II
| III
| IV
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| Original image
| 0.4
| 0.6
| 0.8
| 0.99
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| Classical image
| 0.2
| 0.21
| 0.23
| 0.24
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| Shaped image
| 0.3
| 0.41
| 0.51
| 0.63
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| Table 2: Values of contracting coefficients both for "classical" and proposed method of image shaping. |
2. To estimate the method capabilities the image has been modeled for the specimen having notches of different depths, but the same area and located athwart to incident flux. Fig. 3 a) presents original image of the specimen. Fig 3 b) shows the picture, which is typical, i.e., obtained in classical way. Fig. 3 c) demonstrates the image processed with the method proposed. Table 1 contains the contrasting coefficients for different image sections. Analysis of results confirms that the method proposed allows to obtain the pictures of specimen with different density at the same image having kept the linearity of contrasting coefficients ratios for different image sections.
| a)
| b)
| c)
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Fig 3: Modeling results for exposure of the specimen, having notches of different depths.
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