{"title":"Epitaxial Pr,Yb:LiYF4 Waveguides for Upconversion Lasers","authors":"P. Rogin, G. Huber","doi":"10.1364/cleo_europe.1998.cthf6","DOIUrl":"https://doi.org/10.1364/cleo_europe.1998.cthf6","url":null,"abstract":"Upconversion lasers based on lanthanide doped host materials have been known for several years. The efficiency of their multiphoton excitation schemes depends critically on the absence of competing nonradiative processes, depleting the intermediate energy levels involved as well as the upper laser level. For this reason, fluoride host materials generally outperform oxides due to their lower phonon energies and, consequently, lower multiphonon relaxation rates. In this work, we concentrate on LiYF4 (YLF) codoped with Pr3+ and Yb3+, allowing for a sensitized avalanche upconversion mechanism [1] to produce red (639.5 nm) output upon pumping at ~ 835 nm. The threshold pump intensity of this process is in the order of 105 to 106 W/cm2, requiring a tightly focused pump beam. In bulk media, the high divergency of such a beam results in a very short gain medium, where only a small part of the incident light is absorbed, giving rise to a poor overall efficiency. A longer gain medium, as demonstrated with fluoride glass fibres, allows for a far better performance. In a disordered host material, however, the inhomogeneous broadening of the spectral lines reduces the peak gain cross section. Therefore, it seems promising to combine the advantages of the fibre geometry and a crystalline host by using crystalline waveguides.","PeriodicalId":10610,"journal":{"name":"Conference on Lasers and Electro-Optics Europe","volume":"6 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1998-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"80491067","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
A. Ionin, A. Kotkov, A. P. Napartovich, L. Seleznev, P. A. Svotin
{"title":"Phase conjugation in CO2 laser medium: theory and experiment","authors":"A. Ionin, A. Kotkov, A. P. Napartovich, L. Seleznev, P. A. Svotin","doi":"10.1364/cleo_europe.1998.cthn5","DOIUrl":"https://doi.org/10.1364/cleo_europe.1998.cthn5","url":null,"abstract":"Phase conjugation (PC) processes at degenerate four-wave mixing (DFWM) in the active medium of a pulsed e-beam controlled discharge CO2-laser were studied both experimentally and theoretically. The experiment was carried out with the following parameters: laser gas mixture CO2:N2:He=1:2:4, gas pressure 0.3 bar, active medium length 1.2 m, resonator length 12 m (17.7 m for single line laser), interaction angle ~10 mrad at DFWM without optical delay between probe wave and co-propagating pump one. Integral PC reflectivity (PCR) strongly depends on such parameters as: specific input energy (Fig. 1); intensity ratio for probe J3 and co-propagating pump J1 wave (Fig.2); coherency of the laser radiation, that varied by rotation of mutual polarization or with optical delay between probe wave and co-propagating pump one; geometry of DFWM; output mirror reflectance Rout (8-80%) (PCR was maximum with Rout of 8% but best quality of PC signal was observed with Rout =80%); gas mixture composition and pressure, being maximum for a mixture with a low fraction of helium and at higher pressure (up to 0.6 bar). A periodical dependence of PCR on optical delay between probe and co-propagating pump wave with periods 10−3 and 10−5 m was observed. The PCR did not depend on spectral content and a degree of linear polarization of the laser radiation.","PeriodicalId":10610,"journal":{"name":"Conference on Lasers and Electro-Optics Europe","volume":"5 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1998-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"80169229","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Continuous-wave diode-pumped Nd3+: YAG ceramics laser","authors":"K. Yoshida, T. Taira, A. Ikesue","doi":"10.1364/cleo_europe.1998.cwf17","DOIUrl":"https://doi.org/10.1364/cleo_europe.1998.cwf17","url":null,"abstract":"Recently, we have developed a Nd:YAG ceramics with high optical quality [1]. The YAG ceramic allows high neodymium-ion doping to overcome low absorption cross-section. Table 1 shows the absorption coefficient of a 0.9 at.% Nd:YAG single crystal and Nd:YAG ceramics (1.1, 2.4, 4.8, and 9.1 at.%) in the 808 nm region. The 9.1 at.% Nd:YAG ceramic has about 10 times higher absorption coefficient than 0.9 at.% Nd:YAG single crystal. The laser chip was made from aYAG ceramic with 4.8 at.% Nd3+ doping level, cut to a 1.61 mm thickness. In an only polished chip Nd:YAG ceramics, single mode oscillation power of 213 mW with LD pump power of 1.6 W and a laser threshold of 334.6 mW was obtained. The slope efficiency was 17.6 %. Fig. 1 shows the longitudinal modes of the Nd:YAG ceramics laser with 200 mW output power.","PeriodicalId":10610,"journal":{"name":"Conference on Lasers and Electro-Optics Europe","volume":"345 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1998-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"75114695","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Self-mode-locked semiconductor laser in a ring cavity","authors":"P. Langlois, M. Piché","doi":"10.1364/cleo_europe.1998.cpd1.3","DOIUrl":"https://doi.org/10.1364/cleo_europe.1998.cpd1.3","url":null,"abstract":"We report on the generation of short (2 ps) pulses directly from a self-mode-locked semiconductor amplifier inserted in a ring cavity. The amplifier is in fact a superluminescent diode consisting of a 500 mm long double quantum-well InGaAlAs ridge waveguide with strained InGaAs active layers ; an angled stripe geometry provides a low coherence emission with a broad spectrum centered near 855 nm. The amplifier is placed in a ring cavity with three gold minors and a 83% transmission output coupler. Collimation of the laser output and careful alignment of the cavity mirrors allows laser emission with a threshold bias current Ith near 46 mA. Self-mode locking is achieved when the dc bias current is set at ~1.2 Ith, and when the cavity is slightly misaligned. Figures 1 and 2 show typical non-colinear autocorrelation traces and optical spectra of the pulses circulating in the clockwise (cw) and counterclockwise (ccw) directions. The counterpropagating pulses have similar temporal profiles with durations from 2 to 6 ps (after deconvolution) and characterized by a weak pedestal that falls to zero. Remarkably, the pulse respective optical spectra are different, as the spectrum of the ccw pulse has a 2.9 nm bandwidth peaked at 864 nm, whereas that of the cw pulse is peaked near 867 nm with a bandwidth of 0.9 nm. Both circulating pulses have a time-bandwidth product exceeding several times the Fourier-transformed limit, which suggests that they can be compressed to subpicosecond durations.","PeriodicalId":10610,"journal":{"name":"Conference on Lasers and Electro-Optics Europe","volume":"75 2-3 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1998-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"78138595","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Progress in Chemical Oxygen-Iodine Lasers","authors":"K. Truesdell","doi":"10.1364/cleo_europe.1998.cthe1","DOIUrl":"https://doi.org/10.1364/cleo_europe.1998.cthe1","url":null,"abstract":"Summary not available.","PeriodicalId":10610,"journal":{"name":"Conference on Lasers and Electro-Optics Europe","volume":"15 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1998-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"84996476","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
A. Braud, S. Girard, J. Doualan, R. Moncorgé, M. Diaf, M. Thuau
{"title":"Excited-state dynamics and energy transfer processes involved in the 1.5 and 2.3µm laser transitions in Yb:Tm doped LiYF4 and KY3F10 single crystals","authors":"A. Braud, S. Girard, J. Doualan, R. Moncorgé, M. Diaf, M. Thuau","doi":"10.1364/cleo_europe.1998.ctuk2","DOIUrl":"https://doi.org/10.1364/cleo_europe.1998.ctuk2","url":null,"abstract":"Tm doped fluoride crystals sensitized with Yb ions were early recognized as very efficient upconversion laser materials for visible room temperature operation under infrared excitation. Recently, the advantage of ytterbium as codopant was pointed out to enhance the 1.5µm emission 3H4→3F4 and to avoid the bottlenecking effect on this laser transition[1]. In order to determine several energy-transfer parameters involved in the excitation processes of Yb-Tm doped laser materials, samples of Tm:Yb:LiYF4 and Tm:Yb:KY3F10 with different dopant concentrations were grown by Czochralski technique, oriented and cut. Energy transfer processes and upconversion effects in Tm:Yb codoped fluoride crystals were quantitatively studied with classical energy transfer models (direct dipole-dipole interaction - Förster-Dexter model extended by Inokuti-Hirayama and migration assisted energy transfer - Yokota-Tanimoto or Burshtein models), using absorption, emission and excited-state absorption cross sections experimental data as input parameters. The results were systematically compared, in the case of fast energy migration, with those deduced from the adjustement between the rate equation model and the measured kinetics of the excited state levels of the Yb (2F5/2) and Tm (3F4,3H4, 1G4 and 1D2) ions. Both decay times after short pulse excitation and rise times after square-pulse shape excitation on the Yb ions were investigated to obtain a complete description of the excitation scheme for the Tm upper energy levels.","PeriodicalId":10610,"journal":{"name":"Conference on Lasers and Electro-Optics Europe","volume":"32 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1998-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"85531921","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Single-pass distortion correction using innovative holographic methods in rhodium-doped barium titanate","authors":"L. Corner, M. Damzen","doi":"10.1364/cleo_europe.1998.cpd2.4","DOIUrl":"https://doi.org/10.1364/cleo_europe.1998.cpd2.4","url":null,"abstract":"An important problem in the area of optical image processing is that of removing distortions introduced onto the image. Methods of distortion correction include phase conjugation [1] and holography [2], but these methods generally involve a double pass through the distorter. This either returns the image to its starting position, or requires a pass through a second distortion as close as possible to the original.","PeriodicalId":10610,"journal":{"name":"Conference on Lasers and Electro-Optics Europe","volume":"17 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1998-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"87178922","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
C. Bellecci, P. Gaudio, M. Valentini, S. Martellucci, P. Aversa, G. Caputi, F. De Donato R. Zoccali
{"title":"TEA CO2 dial station for atmospheric water and pollutants measurements","authors":"C. Bellecci, P. Gaudio, M. Valentini, S. Martellucci, P. Aversa, G. Caputi, F. De Donato R. Zoccali","doi":"10.1364/cleo_europe.1998.ctui84","DOIUrl":"https://doi.org/10.1364/cleo_europe.1998.ctui84","url":null,"abstract":"Among the differential techniques of remote sensing employed to study the atmosphere and it’s composition, the dial is one of the most powerful, mainly in the detection of concentration of the gas traces. This technique, as known, is based on the knowledge of the interaction between the laser radiation and the molecular compound in studying. In particular it needs, with high precision, the value of the absorption coefficients for the defined wavelengths used in carrying the measurements out.","PeriodicalId":10610,"journal":{"name":"Conference on Lasers and Electro-Optics Europe","volume":"93 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1998-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"84226495","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Photorefractive Effect in Copper-Doped LiNbO3 Waveguides","authors":"S. Kostritskii, P. Moretti","doi":"10.1364/cleo_europe.1998.cthh56","DOIUrl":"https://doi.org/10.1364/cleo_europe.1998.cthh56","url":null,"abstract":"Photorefractive waveguides (PRW) are of prime interest for applications in integrated optics such as optical switching, resonant filtering or holographic memories. Therefore, investigations are to date extensively increasing to search new efficient methods of PRW’s fabrication Among the potential optical materials, lithium niobate (LiNbO3) has been subjected to extensive development, especially because crystals of good optical quality are commercially available. Comparatively to other known and mostly used methods of PRW’s elaboration in LiNbO3, the very new method of combined proton and copper exchange seems to present some interesting advantages [1,2]. This ionic exchange process enables to control easily and precisely the photorefractive response parameters since the copper concentration as well as the ratio Cu+/Cu2+ can be varied gradually in a wide range [1]. Moreover, it allows to reach an extremely high holographic sensitivity [2]. However, an undesired feature of the proton-exchanged waveguides is that the electrooptical coefficients are reduced significantly [2]. In contrast, no degradation of the latter is observed in ion-implanted waveguides [3]. Therefore, to elaborate the LiNbO3 waveguides with improved photorefractive properties, we have used a new two-step techique : First, the optical waveguides are formed by implantation of He+-ions at room temperature under a fluence of 2×1016 ions/cm2 and with an energy of 1 MeV, and second, the photorefractive sensitivity of the waveguides are increased by using the combined proton and copper exchage process, but conducted in specific conditions, i.e. when the proton exchange is minima, not sufficient to induce both an essential degradation of the electrooptical effect and a marked change of the effective refractive index.","PeriodicalId":10610,"journal":{"name":"Conference on Lasers and Electro-Optics Europe","volume":"19 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1998-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"84227255","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Nonlinear Optical Properties of Czochralski-Grown Periodically Poled LiNbO3 Crystals","authors":"O. Gliko, I. Naumova, J. Ju, H. K. Kim, M. Cha","doi":"10.1364/cleo_europe.1998.ctua7","DOIUrl":"https://doi.org/10.1364/cleo_europe.1998.ctua7","url":null,"abstract":"Bulk periodically poled LiNbO3 crystal is a promising material for nonlinear optical devices using quasi-phase matching In particular, frequency doubling of near-infrared radiation into the blue spectra range and optical parametric oscillation are of importance. The spatial modulation of the nonlinear susceptibility is realized in lithium niobate by formation of periodically reversed domain pattern. In this work the periodic domain structure was formed in LiNbO3:Nd:Mg crystals by means of the modulation of impurity incorporation during the process of crystal growth. We investigated the correlation of ferroelectric domains with Nd-concentration modulation, and the nonlinear properties of the optical superlattice.","PeriodicalId":10610,"journal":{"name":"Conference on Lasers and Electro-Optics Europe","volume":"34 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1998-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"81491642","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}