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Resonance Methods for Increasing Sensitivity of Interferometry, Fluorescence, Dynamic Holography

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Biomedical and Resonance Optics

Part of the book series: Bioanalysis ((BIOANALYSIS,volume 11))

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Abstract

Coherent-optical—holographic [1,2,3,4], interference [5,6,7,8,9,10,11,12] and fluorescent [13,14,15] methods make different demands to the light source depending on the tasks: By considerable energy output and power of the radiance, it can be its high spatial coherence and monochromaticity; tunable wavelength in a broad spectral range, two and more generation lines of the radiance with the controlled spectral interval, different width of pulse generation of the radiance, and also generation of two or several pulses with the controlled time interval, the radiance with given and changeable direction of vector polarization and so on.

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Notes

  1. 1.

    The dye laser “Raduga-3M” with laser pumping was for the first time mounted by the author from the separately developed drawings into the instrument version in the Institute of Physics of the Academy of Sciences of the BSSR and was made in the optical mechanics departments of the Leningrad Physics and Technology Institute named after A. E. Ioffe of the Academy of Sciences of the USSR (1971). During the process of producing, several changes were added to this laser device. In particular, the length of the resonator was increased, and the Fabry–Perot interferometer was introduced in it with the basis of 100 μm, what gave the possibility to narrow the width of generator spectrum up to 0.01–0.03 nm and carry out the regime of one-and four-frequency generation with the pulse energy of \( 10^{ - 3} \,{\text{J}} \) and power of about 0.1 mW. These changes made it appropriate for the usage in holography purposes and resonance interferometry.

  2. 2.

    It becomes possible when the path difference of the points r1 and r2 is considerably lower than the coherence length of the light emission L = cτ, where с is the speed of light that can be easily carried out for the quasi-monochromatic light, the effective spectral bandwidth δν of which is connected with the frequency v by the relation: δν/v ≪ 1.

  3. 3.

    The idea of calculations of plots in Fig. 1.13a belongs to G. V. Ostrovskaya.

  4. 4.

    Relative shift of interference fringes means the difference in shift of interference fringes on interferograms produced in different wavelength λ1 and λ2.

  5. 5.

    In the case of strong effects or very large length of a cell, the dependence is more complicated: \( I^{\left( C \right)} L\sim \sin^{2} A\left| E \right|^{2} L/2\sqrt \varepsilon \).

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  1. CJSC Holography Industry, Minsk, Belarus

    Leonid V. Tanin

  2. Belarusian Medical Academy of Postgraduate Education, Minsk, Belarus

    Andrei L. Tanin

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Tanin, L.V., Tanin, A.L. (2021). Resonance Methods for Increasing Sensitivity of Interferometry, Fluorescence, Dynamic Holography. In: Biomedical and Resonance Optics. Bioanalysis, vol 11. Springer, Cham. https://doi.org/10.1007/978-3-030-60773-9_1

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