TL;DR: In this paper, the first experimental measurements of the temperature distribution along silica-based optical fibres using a semiconductor laser source and an avalanche photodiode detector were reported.
Abstract: The letter reports on the first experimental measurements of the temperature distribution along silica-based optical fibres using a semiconductor laser source and an avalanche photodiode detector. Previous results by the same authors demonstrated the first use of the Raman scattering technique, but used a less practical ion laser source and a photomultiplier detector.
TL;DR: In this paper, X-ray diffraction and atom-force microscopy were applied to characterize the structure and surface morphology of the deposited ZnO films, which were characterized by photoluminescence with an Ar ion laser as a light source.
TL;DR: In this paper, the authors focused on spectral analysis of Pr3+:lead phosphate (PPbKANPr) glasses for visible lasers and optical amplifier applications and these glasses were prepared by a melt-cast technique.
TL;DR: In this article, the spectroscopic parameters of Er3+doped crystals were determined with regard to the upconversion laser parameters of the green transition 4S3/2→4I15/2.
Abstract: The spectroscopic parameters of Er3+‐doped crystals were determined with regard to the upconversion laser parameters of the green transition 4S3/2→4I15/2. The influence of excited‐state absorption on this laser channel was determined. Furthermore, upconversion pump mechanisms using ground‐state and excited‐state absorption around 810 and 970 nm were investigated by direct measurements of excited‐state absorption. The spectroscopic results confirm the pulsed room‐temperature laser experiments on the 4S3/2→4I15/2 transition. The lasers based on Er:LiYF4, Er:Y3Al5O12, and Er:Lu3Al5O12 were directly excited into the upper laser level by an excimer laser pumped dye laser in the blue spectral range. In Er:LiYF4, Er:KYF4, and Er:Y3Al5O12, laser action was achieved with two‐step upconversion pumping by a Ti:sapphire laser and a krypton ion laser. In the case of the fluorides, the additional pumping with the krypton ion laser was not necessary. The laser emission wavelengths were 551 nm for Er:LiYF4, 561 nm for Er...
TL;DR: In this article, a comparison of the relative efficiency when the scattering gas is located inside and outside the laser cavity is given for the pure rotational Raman scattering of O2, CO2 and H3CC≡CH (methylacetylene).
Abstract: Several techniques of exciting Raman spectra of low-pressure gases and vapors with cw laser radiation are described. Both the He–Ne laser with output at 6328 a and the Ar+ ion laser with output at 4880 and 5145 a have been used. The use of the He–Ne laser with a multiple-pass Raman tube inside the laser cavity yields Raman spectra which can be photographed in exposure times that are equivalent to those required with the classical Hg-arc and large-volume Raman tube as the source of scattered radiation. The Ar+-ion laser allows the photoelectric recording of rotational Raman spectra at atmospheric pressure with a signal/noise ratio of 10:1 when the Raman tube is located outside the laser cavity, and about 100:1 when the Raman tube is inside the laser cavity. A comparison is given for the relative efficiency when the scattering gas is located inside and outside the laser cavity. Pure rotational Raman spectra for N2, O2, CO2, and H3CC≡CH (methylacetylene) are presented. The depolarization ratios of both the Rayleigh and Raman lines of N2, O2, and CO2 have been determined and relative scattering cross section for the pure rotational Raman scattering of oxygen has been obtained.