Tellurite Glass Optical Fiber Doped With Pbte Quantum Dots

We produced a PbTe quantum dot core doped optical fiber with tellurite glasses intended to be used in highly nonlinear ultrafast optical devices capable to operate at the optical communication window at 1300 and 1500 nm wavelength region. Attenuation peaks of the optical fiber depends on the heat treatment time as expected for dots growth and covered the whole mid infrared region near 1500 nm. The optical fiber preform was made with the rod-in-tube method and the fiber was produced with a 4 m high Heatway drawing tower. The optical fiber core can be heavily doped because tellurite glasses solubility for PbTe quantum dots is order of magnitude higher than borosilicate and phosphate glasses, for example. In order to match all the requirements for core-clad optical fibers we studied undoped and doped tellurite glasses optical and thermophysical properties as a function of the glass composition. We also followed the growth kinetics of the quantum dots by High Resolution Transmission Electron Microscopy in the bulk glass matrix and the optical fiber.5734124129Borrelli, N.F., Aitken, B.G., Newhouse, M.A., (1995) J. Non-cryst.Sol., p. 185Wise, F.W., (2000) Acc. Chem. Res., 33, p. 773Borrelli, N.F., Smith, D.W., (1994) J. Non-cryst. Sol., 180, p. 25Lipovskii, A., Kolobkova, E.A., Petrikov, V., Kang, I., Olkhovets, A., Krauus, T., Thomas, M., Kycia, S., (1997) Appl. Phys. Lett., 71, p. 3406Reynoso, V.C.S., De Paula, A.M., Cuevas, R.F., Neto, J.A.M., Alves, O.L., Cesar, C.L., Barbosa, L.C., (1995) Elect. Lett., 31 (12), pp. 1013-1014Rodriguez, E., Jimenez, E., Jacob, G.J., Neves, A., Cesar, C.L., Barbosa, L.C., Photonics West 2005, , poster 5734-22Jacob, G.J., Cesar, C.L., Barbosa, L.C., (2002) Physics and Chemistry of Glass, 43 C, pp. 250-253Tudury, G.E., Marquezini, M.V., Ferreira, L.G., Barbosa, L.C., Cesar, C.L., (2000) Phys. Rev. B, 62 (11), p. 7357Cho, S.J., Paek, U.C., Han, W.T., Heo, J., (2001) OFC2001, , ThC4-1 paperJu, S., Kim, Y.H., Han, W.T., (2004) ECOC2004, , Stockholm, Sweden, September 5-9, Th2.3.3 pape

One-dimensional Photonic Crystal For The 1.3-1.5 μm Region

Multilayer of PbTe quantum dots embedded in SiO2 were fabricated by alternatively use of Plasma Enhanced Chemical Vapor Deposition and Laser Ablation techniques. The optimal growing parameters for both the SiO2 films and the PbTe quantum dots were obtained. The refractive index and optical absorption of the sample were studied. Multilayer X-ray diffraction patterns were used to estimate the nanoparticles diameter. Morphological properties of the nanostructured material were studied using Transmission Electron Microscopy. Both absorption spectra and X-ray diffraction patterns reveled the nanoparticles are 6-8 nm in diameter, consequently appropriate for developing optical devices in the infra red region. Finally the multilayer was grown inside a Fabry Perot cavity. The transmittance of the one-dimensional photonic crystal was measured.6129Tsunetomo, K., Shunsuke, S., Koyama, T., Tanaka, S., Sasaki, F., Kobayashi, S., Ultrafast nonlinear optical response of CdTe microcrystallite-doped glasses fabricated by laser evaporation (1995) Molecular Crystals and Liquid Crystals Science and Technology Section B, Nonlinear Optics, 13 (1-3), pp. 109-126Gleiter, H., (1989) Prog. Mater. Sci., 33, p. 223Tudury, G.E., Marquezini, M.V., Ferreira, L.G., Barbosa, L.C., Cesar, C.L., Effect of band anisotropy on electronic structure of PbS, PbSe, and PbTe quantum dots (2000) Phys. Rev. B, 62 (11), pp. 7357-7364Rodriguez, E., Jimenez, E., Padilha, L.A., Neves, A.A.R., Jacob, G.J., Cesar, C.L., Barbosa, L.C., SiO2/PbTe quantum dots multilayer production and characterization (2005) Appl. Phys. Lett., 86, pp. 113117-113120Rodriguez, E., Jimenez, E., Cesar, C.L., Barbosa, L.C., 1D photonic band gap silica doped PbTe quantum dot optical device (2005) Glass Technology, 46 (2), pp. 47-49Rodriguez, E., Jimenez, E., Neves, A.A.R., Jacob, G.J., Cesar, C.L., Barbosa, L.C., Fabrication and characterization of PbTe quantum dot multilayers for Photonic Fabry-Perot Devices (2005) Physica E, 26, pp. 361-36

Ultra Large Amplification Bandwidth Of Er3+ And Tm3+ At S And L Band From Teo2-wo3-na2o-nb 2o5 Glass Doped Optical Fibers

Tellurite glasses optical fibers became promising for optical amplifiers due to its high rare earth ions solubility and very large amplification bandwidth. Among several tellurite glasses the TeO2-WO 3-Na2O-Nb2O5 system show one of the largest bandwidth. Our previous characterization of lifetime using the Ω2, Ω4, Ω6, Judd-Ofelt parameters indicate a quantum efficiency maximum for 7500ppm Er3+ concentration. Therefore we decided to produce jointed Er3+ and Tm3+ single mode optical fibers with this glass system keeping the 7500ppm Er3+ concentration and varying the Tm3+ concentration from 2500ppm to 15000ppm. This single mode fiber was pumped by 120mW of the semiconductor laser at 790nm and we observed a flat ASE bandwidth from 1400 to 1570nm for the 5000ppm Tm3+ concentration.5723243247Jeong, H., Oh, K., Han, S.R., Morse, T.F., Broadband amplified spontaneous emission from an Er3+-Tm 3+ - Codoped silica fibar (2003) Opt. Lett., 28, pp. 161-163Reisfeld, R., Jorgensen, C.K., (1987) Handbook on the Physics and Chemistry of Rare Earths, 9, pp. 1-90. , K. A. Gschneidner, Jr. and L. Eyring (Eds.), Elsevier ScienceChen, C.Y., Petrin, R.R., Yeh, D.C., Sibley, W.A., Concentration-dependent energy-transfer processes in Er3+-and Tm3+ -doped heavy-metal fluoride (1989) Opt. Lett., 14, pp. 432-434Miniscalco, W.J., Quimby, R.S., General procedure for the analysis of Er3+ cross sections (1991) Opt. Lett, 16, pp. 258-26

In Situ Synchrotron Radiation Small-angle X-ray Scattering Study Of The Kinetics Of Growth Of Cdte Nanocrystals In Borosilicate Glass

A number of isolator-semiconductor nanocrystal composites exhibit quantum confinement effects and nonlinear optical properties. In this work, the formation and growth of CdTe and CdTe0.9S0.1 nanocrystals immersed in a borosilicate glass host matrix were studied by small-angle x-ray scattering using synchrotron radiation during in situ annealing in the 560-580°C temperature range. The values of the average radii of the CdTe nanocrystals determined by using Guinier plots for different annealing times (20-30 Å) agree with those obtained from optical absorption spectroscopy measurements. The nanocrystal size distribution depends on the thermal history and composition of the samples. The existence of other structural heterogeneities having an average size of several hundred ångstroms was detected. © 1995 American Institute of Physics.6621338134

Pbte Quantum Dots - Sio2 Multilayers For Optical Devices Produced By Laser Ablation

Thin films of glass doped with PbTe quantum dots were successfully fabricated. The semiconducting quantum dots were grown by laser ablation of a PbTe target (99.99%) using the second harmonic of a Q-Switched Quantel Nd:YAG laser under high purity argon atmosphere. The glass matrix was fabricated by a plasma chemical vapor deposition method using vapor of tetramethoxysilane (TMOS) as precursor. The QD's and the glass matrix were alternately deposited onto a Si (100) wafer for 60 cycles. Cross-section TEM image clearly showed QD's layer well separated from each other with glass matrix layers. The influence of the ablation time on the size distribution of the quantum dots is studied. HRTEM revealed anisotropy in the size of the QD's: they were about 9nm in the high and 3-5 in diameter. Furthermore HRTEM studies revealed that the QD's basically growth in the (200) and (220) directions. The thickness of the glass matrix layer was about 20 nm. Absorption, photo luminescence and relaxation time of the multilayer were also measured.5734116123Alivisatos, A.P., (1996) Sci., 271, p. 933Warnock, J., Awschalom, D.D., (1985) Phys. Rev. B, 32, p. 5529Borrelli, N.F., May, D.W., Holland, H.J., Smith, D.W., (1987) J. Appl. Phys., 61, p. 399Potter, B.G., Simmons, J.H., (1988) Phys. Rev. B, 37, p. 10838Gleiter, H., (1989) Prog. Mater. Sci., 33, p. 223Tsunetomo, K., Shunsuke, S., Koyama, T., Tanaka, S., Sasaki, F., Kobayashi, S., (1995) Nonlinear Opt., 13, p. 109Reynoso, V.C.S., De Paula, A.M., Cuevas, R.F., Neto, J.A.M., Alves, O.L., Cesar, C.L., Barbosa, L.C., (1995) Electr. Lett., 31 (12), pp. 1013-1015Jacob, G.J., Cesar, C.L., Barbosa, L.C., (2002) Chem. Phys. Glass, 43 C, pp. 250-252Singh, R.K., Narayan, J., (1990) Phys. Rev. B, 41, p. 8843Barnes, J.P., (2002) Nanotechnology, 13, p. 465Tudury, G.E., Marquezini, M.V., Ferreira, L.G., Barbosa, L.C., Cesar, C.L., (2000) Phys. Rev. B, 62 (11), pp. 7357-7364Cesar, C.L., Jacob, G.J., Tudury, G.E., Marquezini, M.V., Barbosa, L.C., (2004) Atti della Fondazione G. Ronchi Journal, (4), pp. 519-528. , Anno LI

Preparation of hybrid organic-inorganic materials based on a di-ureasil matrix doped with lithium bis(trifluoromethanesulfonyl)imide

In this presentation we describe the preparation of solvent-free solid polymer electrolytes (SPEs) by the sol-gel route with the incorporation of controlled quantities of lithium bis(trifluoromethanesulfonyl) imide (LiTFSI) into the host matrix. The host framework of these xerogels, designated as di-ureasils and represented by d-U(900), contains oxyethylene oligomers with about 15 repeat units bonded at each end to a siliceous backbone through urea bridging links. Electrolytes were characterized by ionic conductivity measurements, cyclic voltammetry at a gold microelectrode and thermal analysis. The results obtained reveal that these hybrid materials are completely amorphous and exhibit appropriate electrochemical characteristics for a variety of applications.Fundação para a Ciência e a Tecnologia - POCI/QUI/59856/2004; POCTI/3/686; SFRH/BD/22707/2005

Carbon Nanotube Doped Tellurite Glasses

In the past it was observed that buck ball doped glasses showed enhanced optical nonlinearities. However, carbon nanotubes are much more stable than buck ball and should be a better choice for that purpose. Therefore we decided to investigate the possibility to produce carbon nanotubes doped tellurite glasses and measured their optical nonlinearities. Tellurite glasses already have a larger nonlinearity compared to silica, and other, glasses. We produced TeO 2-ZnO tellurite family glasses doped with multi wall Carbon Nanotube (CNT). The CNTs acquired from Carbolex were vigorously mechanically mixed with the tellurite glass precursors and melted in platinum crucible around 650°C in a controlled atmosphere inside an electrical induction furnace. We used the lowest temperature possible and controlled atmosphere to avoid the CNT oxidation. The glass melt was cast in a stainless steel and thermally treated at 300°C for 5 hours to relieve internal stresses. The samples were than cutted and polished to perform the optical characterization. We measured refractive index and thermo physical properties, such as vitreous transition Tg, crystallization onset Tx and melting Tf temperatures. Raman spectroscopy showed the possible presence of CNTs.6890Iijima, S., (1991) Nature, 354, p. 56http://www.ati.surrey.ac.uk/news/n, onlinearDiMaio, J., Rhyne, S., Yang, Z., Fu, K., Czerw, R., Xu, J., Webster, S., Ballato, J., (2003) Information Sciences, 149, p. 69Aoki, Y., Okubo, S., Kataura, H., Nagasawa, H., Achiba, Y., (2005) Chem. Lett, 34 (4), p. 562Misra, S.K., Watts, P.C.P., Valappil, S.P., Silva, S.R.P., Roy, I., Boccaccini, A.R., (2007) Nanotechnology, 18, p. 07570

Photothermal Spectroscopic Characterization In Teliurite Glasses Codoped With Rare-earth Ions

Thermal Lens (TL) and spectroscopic characterizations were performed in 70TeO2-19WO3-7Na2O-4Nb2O 5 (mol%) tellurite glasses. TL measurements were accomplished in Er3+/Tm3+ co-doped tellurite glasses in function of the Tm2O3 concentration (0.4 -1.6 ×1020 ions/cm3). Fluorescence spectra at 488 nm showed that Er 3+/Tm3+co-doped tellurite glasses present several emission bands between (500-1800) nm. However, the more iniense emission bands correspond to the Er3+ and Tm3+ transitions ( 4I13/2 → 4I15/2 and 3F4 → 3H6), respectively. The absolute nonradiative quantum efficiency (φ) was determined by TL method. Higher values of φ were obtained with the increase of Tm2O 3 concentration inside of the Er3+/Tm3+ co-doped tellurite glasses. These results are corroborated by the Judd-Ofelt calculations.6116Ryba-Romanowski, W., Effect of Temperature and activator concentration on luminescence decay of erbium-doped tellurite glass (1990) J. Lumin., 46, pp. 163-172Tanabe, S., Hirao, K., Soga, N., Upconversion fluorescences of TeO2 and Ga2O 3. based oxide glasses containing Er3+ (1990) J. Non-cryst. Solids, 122, pp. 79-82Inoue, S., Nukui, A., Yamamoto, K., Yano, T., Shibata, S., Yamane, M., Refractive index patterning of tellurite glass surfaces by ultra short pulse laser spot heating (2002) J. Mater. Sci., 37, pp. 3459-3465Huang, L., Jha, A., Shen, S., Chung, W.J., Visible emissions at 592 and 613 nm in Er3+-Eu3+ -codoped tellurite fibers (2004) Opt. Commun., 239, pp. 403-408Chillece, E.F., Rodriguez, E., Neves, A.A.R., Moreira, W.C., César, C.L., Barbosa, L.C., Er3+-Tm3+ co-doped tellurite fibers for broadband optical fiber amplifier around 1550 nm band (2005) Opt. Fiber Tech.Tanabe, S., Suzuki, K., Soga, N., Hanada, T., Mechanisms and concentration dependence of Tm3+ blue and Er3+ green up-con version in codoped glasses by red-laser pumping (1995) J. Lumin., 65, pp. 247-255Dai, S.X., Yang, J.H., Liu, Z.P., Wen, L., Hu, L.L., Jiang, Z.H., The luminescence of Er3+, Yb3+, Tm 3+-codoped tellurite glass pumped at 970 nm (2003) Acta Physica Sinica, 52, pp. 729-735Shen, S.X., Jha, A., Huang, L.H., Joshi, P., 980-nm diode-pumped Tm3+/Yb3+-codoped tellurite fiber for S-band amplification (2005) Optics Letters, 30, pp. 1437-1439Shen, X., Nie, Q., Xu, T., Peng, T., Gao, Y., Green and red upconversion emission and energy-transfer between Er 3+ and Tm3+ions in tellurite glasses (2004) Phys. Lett. A, 332, pp. 101-106Daf, S., Yang, J., Xu, S., Dai, N., Hu, L., Jiang, Z., The spectroscopic properties of Er3+, Yb3+, Tm 3+ -codoped tellurite glass (2003) Proc. SPIE, 4990, pp. 150-156. , Rare-Earth-Doped Materials and Devices Vil, S. Jiang, J. Lucas (Eds.)Lima, S.M., Sampaio, J.A., Catuncla, T., Bento, A.C., Miranda, L.C.M., Baesso, M.L., Mode-mismatched thermal lens spcctrometry for thermo-optical properties measurement in optical glasses: A review (2000) J. Non-cryst. Solids, 273, pp. 215-227Sampaio, J.A., Catunda, T., Gama, S., Baesso, M.L., Thermo-optical properties of OH-free erbium-doped low silica calcium aluminosilicate glasses measured by thermal lens technique (2001) J. Non-cryst. Solids, 284, pp. 210-216Lima, S.M., De Camargo, A.S.S., Nunes, L.A.O., Catunda, T., Fluorescence quantum efficiency measurements of excitation and nonradiative deexcitation processes of rare earth 4f-states in chalcogenide glasses (2002) Appl. Phys. Lett., 81, pp. 589-591Oliveira, S.L., Lima, S.M., Catunda, T., Nunes, L.A.O., Rohling, J.H., Bento, A.C., Baesso, M.L., High fluorescence quantum efficiency of 1.8 μm emission in Tm-dopcd low silica calcium aluminate glass determined by thermal lens spectroscopy (2004) Appl. Phys. Lett., 84, pp. 359-361Jacinto, C., Oliveira, S.L., Nunes, L.A.O., Catunda, T., Bell, M.J.V., Thermal lens study of the OH influence on the fluorescence efficiency of Yb3+ -doped phosphate glasses (2005) Appl. Phys. Lett., 86Sampaio, J.A., Gama, S., Baesso, M.L., Catunda, T., Fluorescence quantum efficiency of Er3+ in low silica calcium aluminate glasses determined by mode-mismatched thermal lens spectromctry (2005) J. Non-cryst. Solids, 351, pp. 1594-1602Pilla, V., Lima, S.M., Catunda, T., Medina, A., Baesso, M.L., Jenssen, H.P., Cassanho, A., Thermal quenching of the fluorescence quantum efficiency in colquiriite crystals measured by thermal lens spcctrometry (2004) J. Opt. Soc. Am. B., 21, pp. 1784-1791Pilla, V., Catunda, T., Balogh, D.T., Faria, R.M., Zilio, S.C., Thermal lensing in Polyvinyl alcoholVpolyaniline blends (2002) J. Polym. Sc., Part B Polym. Physics, 40, pp. 1949-1956Lima, S.M., Catunda, T., Lebullenger, R., Hernandes, A.C., Baesso, M.L., Bento, A.C., Miranda, L.C.M., Temperature dependence of thermo-optical properties of fluoride glasses determined by thermal lens spectrometry (1999) Phys. Rev. B, 60, pp. 15173-15178Lima, S.M., Sampaio, J.A., Catunda, T., De Camargo, A.S.S., Nunes, L.A.O., Baesso, M.L., Hewak, D.W., Spectroscopy, thermal and optical properties of Nd3+ -doped chalcogenide glasses (2001) J. Non-cryst. Solids, 284, pp. 274-281Zou, X., Izumitani, T., Spectroscopic properties and mechanisms of excited state absorption and energy transfer upconversion for Er3+ -doped glasses (1993) J. Non-cryst. Solids, 162, pp. 68-8

Micro-size Tapered Silica Fibers For Sensing Applications

In this work we show results of controlled tapered fibers using a Vytran instrument. The tapered silica fibers were produced by pulling a 50μm length by heating time. The minimum taper diameter was around 3μm and the maximum taper length was around 600μm. The evanescent field effect, in the near infra red (NIR) region, was observed to the tapers with diameter inferior to 15μm. These micro-size tapers no modify the waveguide dispersion spectra. This device could be used to splice a conventional fiber to photonic crystal fibers and also as liquid and gas sensors In this work is reported a fiber optic sensor in the form of taper using the concept of the evanescent field. We show the sensor sensitivity using different liquid materials. © 2011 Copyright Society of Photo-Optical Instrumentation Engineers (SPIE).8120The Society of Photo-Optical Instrumentation Engineers (SPIE)Foster, M.A., Gaeta, A.L., Ultra-low threshold supercontinuum generation in sub-wavelength waveguides (2004) Opt. Express, 12 (14), pp. 3137-3143Jung, Y., Brambilla, G., Richardson, D.J., Broadband single-mode operation of standard optical fibers by using a sub-wavelength optical wire filter (2008) Opt. Express, 16 (19), pp. 14661-14667Tong, L., Gattass, R.R., Ashcom, J.B., He, S., Lou, J., Shen, M., Maxwell, I., Mazur, E., Subwavelength-diamter silica wires for low-loss optical wave guiding (2003) Nature, 426, pp. 816-819Zhang, L., Gu, F., Lou, J., Yin, X., Tong, L., Fast detection of humidity with a subwavelengthdiameter fiber taper coated with gelatin film (2008) Opt. Express, 16 (17), pp. 13349-13353Espinola, R.L., Dadap, J.I., Osgood Jr., R.M., McNab, S.J., Vlasov, Y.A., C-band wavelength conversion in silicon photonic wire waveguides (2005) Opt. Express, 13 (11), pp. 4341-4349Lizé, Y.K., Mägi, E.C., Ta'Eed, V.G., Bolger, J.A., Steinvurzel, P., Eggleton, B.J., Microstructured optical fiber photonic wires with subwavelength core diameter (2004) Opt. Express, 12 (14), pp. 3209-3217Foster, M.A., Turner, A.C., Lipson, M., Gaeta, A.L., Nonlinear optics in photonic nanowires (2008) Opt. Express, 16 (2), pp. 1300-1320Siviloglou, G.A., Suntsov, S., El-Ganainy, R., Iwanow, R., Stegeman, G.I., Christodoulides, D.N., Enchanced thirdorder nonlinear effects in optical AlGaAs nanowires (2006) Opt. Express, 14 (20), pp. 9377-9384www.orc.soton.ac.uk/ofnrd.html, Optical Fibre Nanowires and Related Devices Group, University of SouthamptonCordeiro, C.M.B., Wadsworth, W.J., Birks, T.A., Russell, P.St.J., Engineering the dispersion of tapered fibers for supercontinuum generation with a 1064 nm pump laser (2005) Opt. Lett., 30 (15), pp. 1980-1982Wadsworth, W.J., Ortigosa-Blanch, A., Knight, J.C., Birks, T.A., Man, T.-P.M., Russell, P.St.J., Supercontinuum generation in photonic crystal fibers and optical fiber tapers: A novel light source (2002) J. Opt. Soc. Am. B, 19 (9), pp. 2148-2155Shi, L., Chen, X., Liu, H., Chen, Y., Ye, Z., Liao, W., Xia, Y., Fabrication of submicron-diameter silica fibers using electric strip heater (2006) Opt. Express, 14 (12), pp. 5055-5060Sagué, G., Baade, A., Rauschenbeutel, A., Blue-detuned evanescent field surface traps for neutral atoms based on mode interference in ultra-thin optical fibres (2008) New J. Phys., 10, pp. 113008+18Nayak, K.P., Melentiev, P.N., Morinaga, M., Le Kien, F., Balykin, V.I., Hakuta, K., Optical nanofiber as an efficient tool for manipulating and probing atomic fluorescence (2007) Opt. Express, 15 (9), pp. 5431-5438Xu, F., Horak, P., Brambilla, G., Optical microfiber coil resonator refractometric sensor (2007) Opt. Express, 15 (12), pp. 7888-7893Leon-Saval, S.G., Birks, T.A., Wadsworth, W.J., Russell, P.S.J., Supercontinuum generation in submicron fibre waveguides (2004) Opt. Express, 12 (13), pp. 2864-2869Tran, T.X., Biancalana, F., An accurate envelope equation for light propagation in photonic nanowires: New nonlinear effects (2009) Opt. Express, 17 (20), pp. 17934-17949Biancalana, F., Tran, Tr.X., Stark, S., Schmidt, M.A., Russell, P.S., Emergence of geometrical optical nonlinearities in photonic crystal fiber nanowires (2010) Physical Review Letters, 105, p. 09390

Quantum Confinement Effects On The Phonons Of Pbte Quantum Dots In Tellurite Glasses

We present Raman-scattering results for PbTe quantum dots (QDs) in doped telluride glasses which clearly show the confinement effects on the phonon spectra as a function of the quantum-dot size..6892Kraus and F. Wise;Phys. Rev. Lett. 79 (25), 5102-05 (1997)Thoen, E.R., (1998) Appl, Phys. Lett, 73 (15), p. 2149Wise, F., (2000) Ace. Chem. Res, 33, pp. 773-780Tsuda, S., Cruz, C.H.B., (1991) Opt. Lett, 16, p. 1596Nakamura, A., Tokizaki, T., Akiyama, H., Kataoka, T., (1992) J. Lumin, 53, p. 105Ohtsuka, S., Koyama, T., Tsunetomo, K., Nagata, H., Tanaka, S., (1992) Appl. Phys. Lett, 61, p. 2953Tsunetomo, K., Ohtsuka, S., Koyama, T., Tanaka, S., Sasaki, F., Kobayashi, S., (1995) Nonlin. Opt, 13, p. 109Colvin, V.L., Schlamp, M.C., Alivisatos, A.P., (1995) Nature ∼London, 370, p. 354Dabbousi, M., Bawendi, G., Onitsuka, O., Rubner, M.F., (1995) Appl. Phys. Lett, 66, p. 1316Guerreiro, T., Ten, S., Borrelli, N.F., Butty, J., Jabbour, G.E., Peyghambarian, N., (1997) Appl. Phys. Lett, 71, p. 1595Murray, C.B., Kagan, C.R., Bawendi, M.G., (1995) Science, 270, p. 1335Kang, I., Wise, F.W., (1997) J. Opt. Soc. Am. B, 14, p. 1632Reynoso, V.C.S., de Paula, A.M., Cuevas, R.F., Medeiros Neto, J.A., Alves, O.L., Cesar, C.L., Barbosa, L.C., (1995) Electron. Lett, 31, p. 1013G.J.Jacob, C.L.Cesar,L.C.Barbosa, Chem.Phys.Glass 43C (2002)250-252Esch, V., Fluegel, B., Khitrova, G., Gibbs, H.M., Jiajin, X., Kang, K., Koch, S.W., Peyghambarian, N., (1990) Phys. Rev, B42, p. 7450Sercel, P.C., Valhala, K.J., (1990) Phys. Rev, B42, p. 3690Schoenlein, R.W., Mittleman, D.M., Shiang, J.J., Alivisatos, A.P., Shank, C.V., (1993) Phys. Rev. Lett, 70, p. 1014Ekimov, A.I., Hache, F., Schanne-Klein, M.C., Ricard, D., Flytzanis, C., Kudryavtsev, I.A., Yazeva, T.V., Efros, A.L., (1993) J. Opt. Soc. Am, B10, p. 100Norris, D.J., Sacra, A., Bawendi, C.B.M.M.G., (1994) Phys. Rev. Lett, 72, p. 2612de Oliveira, C.R.M., de Paula, A.M., Filho, F.O.P., Neto, J.A.M., Barbosa, L.C., Alves, O.L., Menezes, E.A., Cesar, C.L., (1995) Appl. Phys. Lett, 66, p. 439R. Ruppin and R. Englman, Rep. Prog. Phys. 33, 149 (1970)R. Ruppin, J. Phys. C: 8, 1969 (1975)Thoen, E.R., Steinmeyer, G., Langlois, P., Ippen, E.P., Tudury, G.E., Brito Cruz, C.H., Barbosa, L.C., Cesar, C.L., (1998) Appl. Phys. Lett, 73Krauss, T.D., Wise, F.W., Coherent and Acoustical Phonon in a Semiconductor Quantum DotsPhis (1997) Rev. Lett, 79, pp. 5102-510