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How can I simulate PSF of incoherent light? |
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| Mar1-13, 02:33 AM | #18 |
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How can I simulate PSF of incoherent light?Thanks, Here I've enclosed one attachment, which is according to your suggestion. I = 1/2[I_r + I_t]. I was confused the difference between incoherent light and unpolarized light. I think I = 1/2[I_r + I_t] is more suitable for unpolarized light. do you think <<1/2[I_r + I_t]>> can reflect the incoherent but linear polarized light ? (such as the light from white light source + filter+polarizer). thanks again Regards |
| Mar1-13, 03:11 AM | #19 |
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I looked at the definition of the PSF and found that the answer to your original question is very simple: The point spread function defines the spread of light from a point source when passing through some optics. But the light from a point source is always completely spatially coherent and, if monochromatic, also temporally coherent.
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| Mar1-13, 03:25 AM | #20 |
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Thank you very much for your post. I tried with small angle. please find the attachment. I also put the formula for PSF. Thanks again for your help, |
| Mar1-13, 03:26 AM | #21 |
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| Mar1-13, 03:33 AM | #22 |
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What are r_P, theta_P, phi_P, and theta, phi? Where is the point light source?
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| Mar1-13, 03:55 AM | #23 |
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theta is open angle of objective lens, theta=arcsin(NA/n). phi is spatial angle at lens coordinate. there is one papar from wolf explain detailly about transfrom from Cartesian coordinate to polar coordinate. Here it is the paper . please find the attachment. Thanks for your help. Regards. the meaning of formula is the supperposition of all light rays which is diffracted from lens aperture. |
| Mar1-13, 04:01 AM | #24 |
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Can't see the paper
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| Mar1-13, 04:07 AM | #25 |
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if it still not be able to upload, please find it on google by title "Electromagnetic diffraction in optical systems II. Structure of the image field in an aplanatic system" Sorry for the incontinence. Regards. |
| Mar1-13, 06:08 AM | #26 |
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It didn't work but I had a look at the paper.
As I said I don't see any problem as the light from a point source is always coherent. Incoherence enters when you want to calculate the image of an extended object or source. |
| Mar1-13, 01:45 PM | #27 |
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| Mar1-13, 01:47 PM | #28 |
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| Mar1-13, 03:16 PM | #29 |
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Richards, B., & Wolf, E. (1959). Electromagnetic diffraction in optical systems. II. Structure of the image field in an aplanatic system. Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences, 253(1274), 358-379. |
| Mar4-13, 10:46 AM | #30 |
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