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By Professor Dr. Bernd Hoefflinger (eds.)

ISBN-10: 3540444327

ISBN-13: 9783540444329

ISBN-10: 3540444335

ISBN-13: 9783540444336

Creating high-fidelity photos of our global has been a continual problem, while our knowing and talents have advanced. the purchase and mapping of the wealthy and complicated content material of visible info rank excessive one of the so much tough technical projects. Now digital picture sensors can checklist a dynamic diversity from shiny to darkish of greater than seven orders of significance, hence exceeding the facility of a human eye via greater than 100 instances and exhibiting 5 orders of value in brightness, leading to CRT and liquid crystal display screens with greater than 100-fold development. this primary finished account of high-dynamic-range (HDR) imaginative and prescient focusses on HDR real-time, high-speed electronic video recording and in addition systematically offers HDR video transmission and show. the facility of the eye-like, logarithmic optoelectronic conversion thought is verified in machine-vision, scientific, car, surveillance and cinematic functions, and it really is prolonged to HDR sub-retinal implants for the imaginative and prescient impaired. whereas the ebook conveys the final photo of HDR imaginative and prescient, particular wisdom of microelectronics and picture processing isn't required. It presents a quantitative precis of the key concerns to permit the review of the cutting-edge and a glimpse at destiny advancements. chosen specialists proportion their knowledge and expectancies during this swiftly evolving artwork with regards to the only strongest of our senses.

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1, ∆C increases to 11/a, rising to 1 in our example at x = 1/a for a 1. At such a low optical input, we would have to double the input intensity for a noticeable change of 1 LSB in the output. For log-response sensors we will often plot the OECF as y = f (log x) (Digits = DN) and its derivative S= dy (DN Decade−1 ), d log x S= x · dy . log e · dx To convert S into the contrast sensitivity ∆C = 100 (%), x · dy/dx −1 we observe that S = (∆C · log e) . Therefore, we represent the CSF either as S (DN Decade−1 ) or ∆C [%].

16b, the four images are shifted by the appropriate offsets resulting in identical grey-chart appearance. Now, consider a scene illuminated by a spotlight, that is with a highly nonuniform illumination. This is quite apparent in the face imaged in Fig. 16a. However, we recorded the illuminant distribution in the plane of the face with putting a white surface there and we obtained the distribution of Fig. 16b. If we subtract Fig. 16b from Fig. 16a, we obtain the image in Fig. 16c, which now has the appearance we would get from an elaborate balanced studio illumination.

4. Parameter resolution Parameter Resolution a b· c∗ 2 1 2−6 ¯ b bi improvement in order to calculate parameter c. 4 lx and measuring point 5 at 2,080 lx. The new algorithm is not as good in the dark as the logarithmic. This is due to the simple offset correction used here. Thresholds 1 and 2 are also indicated in the figure. They show that at those illuminations the approach by approximation leads to minor disadvantages. Under bright conditions, however, the approximation by lines leads to even better results.

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High-Dynamic-Range (HDR) Vision by Professor Dr. Bernd Hoefflinger (eds.)


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