Conţinutul numărului revistei |
Articolul precedent |
Articolul urmator |
600 0 |
SM ISO690:2012 SYRBU, Nicolae, TIRON, Andrew, PARVAN, Vladimir, ZALAMAI, Victor, TIGINYANU, Ion. Interference of birefractive waves in CdGa2S4 crystals(. In: Physica B: Condensed Matter, 2015, vol. 463, pp. 88-92. ISSN -. DOI: https://doi.org/10.1016/j.physb.2015.02.007 |
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Physica B: Condensed Matter | |
Volumul 463 / 2015 / ISSN - /ISSNe 0921-4526 | |
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DOI:https://doi.org/10.1016/j.physb.2015.02.007 | |
Pag. 88-92 | |
Rezumat | |
In CdGa2S4 crystals the Fabry-Perot and birefringence interference spectra were investigated. Spectral dependences of refraction indexes for ordinary (no) and extraordinary (ne) light waves are defined. The spectral dependence Δn=ne-no from the short and long-wavelength parts of isotropic wavelength λ0=485.7 nm (300 K) is determined. It is established that at λ>λ0 Δn is positive and at λ<λ0 Δn is negative. Wavelength λ0=485.7 nm shifts with decreasing temperature to short-wavelengths. The phase difference of ordinary and extraordinary light waves for λ>λ0 and λ<λ0 was determined. The band in reflection spectra observed at the isotropic wavelength has a small halfwidth (3-5 Å). Another isotropic wavelength was found in the short-wavelength region (433 nm) for crystals obtained by iodine transport method. |
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Cuvinte-cheie Birefringence, Cadmium thiogallate, Interference spectra, Isotropic wavelength, Ordinary and extraordinary waves |
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Spectral dependences of refraction indexes for ordinary (n<sub>o</sub>) and extraordinary (n<sub>e</sub>) light waves are defined. The spectral dependence Δn=n<sub>e</sub>-n<sub>o</sub> from the short and long-wavelength parts of isotropic wavelength λ<sub>0</sub>=485.7 nm (300 K) is determined. It is established that at λ>λ<sub>0</sub> Δn is positive and at λ<λ<sub>0</sub> Δn is negative. Wavelength λ<sub>0</sub>=485.7 nm shifts with decreasing temperature to short-wavelengths. The phase difference of ordinary and extraordinary light waves for λ>λ<sub>0</sub> and λ<λ<sub>0</sub> was determined. The band in reflection spectra observed at the isotropic wavelength has a small halfwidth (3-5 Å). 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