2015
DOI: 10.1117/12.2078697
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Highly sensitive absorption measurements in lithium niobate using whispering gallery resonators

Abstract: The absorption coefficient of undoped, congruently grown lithium niobate (LiNbO3) for ordinarily and extraordinarily polarized light is measured in the wavelength range from 390 to 2600 nm using whispering gallery resonators (WGRs). These monolithic cavities guide light by total internal reflection. Their high Q-factor provides several hundred meters of propagation for the coupled light in millimetre size resonators allowing for the measurement of absorption coefficients below 10-2 cm-1, where standard methods… Show more

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Cited by 3 publications
(2 citation statements)
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“…Photon losses can also be introduced by phase modulators due to absorption by their optical media and SLMs because of their limited resolution and fabrication error. Such losses can be made very low 35 52 53 54 ( Supplementary Note 3 ), and further reduced by the fact that the auxiliary cavity is designed using destructive interference with very few photons in it. The low-reflectivity pinhole manifests as an photon loss that decreases rapidly with the OAM number ( Supplementary Note 3 ).…”
Section: Discussionmentioning
confidence: 99%
“…Photon losses can also be introduced by phase modulators due to absorption by their optical media and SLMs because of their limited resolution and fabrication error. Such losses can be made very low 35 52 53 54 ( Supplementary Note 3 ), and further reduced by the fact that the auxiliary cavity is designed using destructive interference with very few photons in it. The low-reflectivity pinhole manifests as an photon loss that decreases rapidly with the OAM number ( Supplementary Note 3 ).…”
Section: Discussionmentioning
confidence: 99%
“…Photon losses can also be introduced by phase modulators due to absorption by their optical media and SLMs because of their limited resolution and fabrication error. Such losses can be made very low [31,[48][49][50] (see Supplementary Materials), and further reduced by the fact that the auxiliary cavity is designed using destructive interference with very few photons in it. The low reflectivity pinhole manifests as an photon loss that decreases rapidly with the OAM number (see Supplementary Materials).…”
Section: Discussionmentioning
confidence: 99%