48 research outputs found

    Third harmonic generation in LiKB4O7 single crystal

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    The third order nonlinear optical properties of the lithium potassium borate (LiKB4O7) single crystal have been investigated by means of the rotational Maker fringe technique using Nd:YAG laser at 1064 nm working in picosecond regime. The value of the third order nonlinear optical susceptibility was calculated using the theoretical model of Kajzar et al. and was found to be about 1.4 Γ— 10βˆ’21 m2 Vβˆ’2 that is one order higher than that of fused silica

    Influence of Ag, Cu dopants on the second and third harmonic response of ZnO films

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    Silver- and copper-doped ZnO films were prepared by radio-frequency (RF)-magnetron sputtering on glass and quartz substrates. The influence of dopants content on the microstructural evolution and optical as well as nonlinear optical (NLO) properties were investigated. It has been found that the grain sizes were enlarged with increasing of Ag, Cu dopants amount in ZnO films. The Ag or Cu doping leads to the optical band gap narrowing. Besides, the second-order NLO response of Ag- and Cu-doped ZnO films is lower than that of undoped ZnO film. The second harmonic generation (SHG) efficiency of the ZnO:Ag film was found to be higher than that of the ZnO:Cu film at the similar concentration of dopant. In addition, the decrease of the third harmonic generation (THG) response is observed in ZnO films with increasing of Ag or Cu dopant amount

    Quadratic nonlinear optical parameters of 7% MgO-doped LiNbO3 crystal

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    Pure and 7% MgO-doped lithium niobate (LiNbO3) single crystals were grown by the Czochralski technique. The shift of optical absorption edge in 7% MgO-doped crystal in direction of shorter wavelength compared to undoped crystal was observed. The second harmonic generation measurements of 7% MgO-doped LiNbO3 crystal were performed at room temperature by means of the rotational Maker fringe technique using Nd:YAG laser generating at 1064Β nm in picoseconds regime. Experimentally obtained value of nonlinear optical coefficient d33 for 7% MgO-doped LiNbO3 was found to be less than for undoped crystal but higher than for 5% MgO-doped. I-type phase-matched second harmonic generation was achieved and the value of phase-matched angle was calculated. High quadratic nonlinearity together with tolerance to intensive laser irradiation makes 7% MgO-doped LiNbO3 crystal interesting for application in optoelectronics

    Linear and nonlinear optical properties of ZnO/PMMA nanocomposite films

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    The nanoscale crystals (NCs) of ZnO were embedded into polymethylmethacrylate (PMMA) polymeric matrix and nanocomposite films were prepared by modified spin coating method. The surface of the ZnO/PMMA nanocomposite films has been investigated using atomic force and scanning electron microscopy. The prepared films are highly transparent, the ultraviolet-visible spectra show their high optical quality. The second and third harmonic generation (SHG and THG) studies of ZnO/PMMA nanocomposite films with different concentrations of ZnO NCs were carried out at Ξ»=1.064 ΞΌm and the effective values of the second and third order nonlinear susceptibilities were estimated to be higher than that of ZnO bulk for the films at low concentration of ZnO NCs. This could indicate that surface effects in ZnO/PMMA nanocomposite films have a dominant role over bulk effects for the SHG and THG processes

    Second and third order nonlinear optical properties of nanostructured ZnO thin films deposited on Ξ±-BBO and LiNbO3

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    The nanocrystalline ZnO films were deposited on Ξ±-BaB2O4 (0 0 1 2) and LiNbO3 (0 0 0 1) single crystals by RF-magnetron sputtering technique. Their structure was studied using X-ray diffractometry, scanning electron microscopy and atomic force microscopy. Besides, the optical absorption spectra were investigated. The second and third harmonic generation measurements were performed by means of the rotational Maker fringe technique using Nd:YAG laser at 1064 nm in picoseconds regime. Finally, the second and third order nonlinear susceptibilities were determined and their values have been found and compared

    Optical properties of ZnO/PMMA nanocomposite films

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    The ZnO nanocrystals (ZnO NCs) with particle size, less than 100 nm, have been blended with polymethylmethacrylate (PMMA) by solution mixing to prepare PMMA/ZnO nanocomposite films. The structure of ZnO/PMMA nanocomposite films was characterized using X-ray diffractometry. The prepared nanocomposite films are highly transparent and a clear excitonic peak is observed in their absorption spectra. Measurements of temperature evolution of the photoluminescence (PL) spectra show intensive UV emission peak corresponding to the donor-bound excitons with binding energy of 51 meV and green emission band related to the intrinsic defects in ZnO. The temperature evolution of the emission peaks energy position, intensity and integral intensity in ZnO/PMMA nanocomposite films were examined

    Room-temperature ultraviolet laser emission from ZnO hexagonal microprisms and nanowires

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    We report the observation of optically pumped laser generation in ZnO microprisms and nanowires at room temperature. The ZnO microprisms were grown on the single crystal (100) silicon substrates by a solid-vapor-phase process. The ZnO nanowires were grown on a glass substrate coated with indium tin oxide by the electrochemical deposition. Laser effect was observed at room temperature at the optically pump power higher than 685 kW cm⁻² for ZnO microprisms and 560 kW cm⁻² β€” for ZnO nanowires.ΠœΡ‹ сообщаСм ΠΎ наблюдСнии Π»Π°Π·Π΅Ρ€Π½ΠΎΠΉ Π³Π΅Π½Π΅Ρ€Π°Ρ†ΠΈΠΈ ΠΏΡ€ΠΈ оптичСской Π½Π°ΠΊΠ°Ρ‡ΠΊΠ΅ Π² ZnO ΠΌΠΈΠΊΡ€ΠΎΠΏΡ€ΠΈΠ·ΠΌΠ°Ρ… ΠΈ Π½Π°Π½ΠΎΠΏΡ€ΠΎΠ²ΠΎΠ»ΠΎΠΊΠ°Ρ… ΠΏΡ€ΠΈ ΠΊΠΎΠΌΠ½Π°Ρ‚Π½ΠΎΠΉ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π΅. ΠœΠΈΠΊΡ€ΠΎΠΏΡ€ΠΈΠ·ΠΌΡ‹ ZnO Π±Ρ‹Π»ΠΈ Π²Ρ‹Ρ€Π°Ρ‰Π΅Π½Ρ‹ Π½Π° монокристалличСских (100) ΠΊΡ€Π΅ΠΌΠ½ΠΈΠ΅Π²Ρ‹Ρ… ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠ°Ρ… с ΠΏΠ°Ρ€ΠΎΠ²ΠΎΠΉ Ρ„Π°Π·Ρ‹. ZnO Π½Π°Π½ΠΎΠΏΡ€ΠΎΠ²ΠΎΠ»ΠΎΠΊΠΈ Π±Ρ‹Π»ΠΈ Π²Ρ‹Ρ€Π°Ρ‰Π΅Π½Ρ‹ Π½Π° стСклянных ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠ°Ρ…, ΠΏΠΎΠΊΡ€Ρ‹Ρ‚Ρ‹Ρ… оксидным слоСм индия с ΠΎΠ»ΠΎΠ²ΠΎΠΌ, ΠΏΡƒΡ‚Π΅ΠΌ элСктрохимичСского осаТдСния. Π›Π°Π·Π΅Ρ€Π½Ρ‹ΠΉ эффСкт наблюдался ΠΏΡ€ΠΈ ΠΊΠΎΠΌΠ½Π°Ρ‚Π½ΠΎΠΉ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π΅ Π² Ρ‚Π΅Ρ… случаях, ΠΊΠΎΠ³Π΄Π° ΠΌΠΎΡ‰Π½ΠΎΡΡ‚ΡŒ оптичСский Π½Π°ΠΊΠ°Ρ‡ΠΊΠΈ ΠΏΡ€Π΅Π²Ρ‹ΡˆΠ°Π»Π° 685 ΠΊΠ’Ρ‚ см⁻² для ZnO ΠΌΠΈΠΊΡ€ΠΎΠΏΡ€ΠΈΠ·ΠΌ ΠΈ 560 ΠΊΠ’Ρ‚ см⁻² для ZnO Π½Π°Π½ΠΎΠΏΡ€ΠΎΠ²ΠΎΠ»ΠΎΠΊ.Ми повідомляємо ΠΏΡ€ΠΎ спостСрСТСння Π»Π°Π·Π΅Ρ€Π½ΠΎΡ— Π³Π΅Π½Π΅Ρ€Π°Ρ†Ρ–Ρ— ΠΏΡ€ΠΈ ΠΎΠΏΡ‚ΠΈΡ‡Π½ΠΎΠΌΡƒ Π½Π°Π³Π½Ρ–Ρ‚Π°Π½Π½Ρ– Π² ZnO ΠΌΡ–ΠΊΡ€ΠΎΠΏΡ€ΠΈΠ·ΠΌΠ°Ρ… Ρ– Π½Π°Π½ΠΎΠ΄Ρ€ΠΎΡ‚Π°Ρ… Π·Π° ΠΊΡ–ΠΌΠ½Π°Ρ‚Π½ΠΎΡ— Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€ΠΈ. ΠœΡ–ΠΊΡ€ΠΎΠΏΡ€ΠΈΠ·ΠΌΠΈ ZnO Π±ΡƒΠ»ΠΈ Π²ΠΈΡ€ΠΎΡ‰Π΅Π½Ρ– Π· ΠΏΠ°Ρ€ΠΎΠ²ΠΎΡ— Ρ„Π°Π·ΠΈ Π½Π° монокристалічних (100) ΠΊΡ€Π΅ΠΌΠ½Ρ–Ρ”Π²ΠΈΡ… ΠΏΡ–Π΄ΠΊΠ»Π°Π΄ΠΊΠ°Ρ…. ZnO Π½Π°Π½ΠΎΠ΄Ρ€ΠΎΡ‚ΠΈ Π±ΡƒΠ»ΠΈ Π²ΠΈΡ€ΠΎΡ‰Π΅Π½Ρ– Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΡ…Ρ–ΠΌΡ–Ρ‡Π½ΠΈΠΌ осадТСнням Π½Π° скляних ΠΏΡ–Π΄ΠΊΠ»Π°Π΄ΠΊΠ°Ρ…, ΠΏΠΎΠΊΡ€ΠΈΡ‚ΠΈΡ… оксидним ΡˆΠ°Ρ€ΠΎΠΌ Ρ–Π½Π΄Ρ–ΡŽ Π· ΠΎΠ»ΠΎΠ²ΠΎΠΌ. Π›Π°Π·Π΅Ρ€Π½ΠΈΠΉ Π΅Ρ„Π΅ΠΊΡ‚ спостСрігався ΠΏΡ€ΠΈ ΠΊΡ–ΠΌΠ½Π°Ρ‚Π½Ρ–ΠΉ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ– Π² Ρ‚ΠΈΡ… Π²ΠΈΠΏΠ°Π΄ΠΊΠ°Ρ…, ΠΊΠΎΠ»ΠΈ ΠΏΠΎΡ‚ΡƒΠΆΠ½Ρ–ΡΡ‚ΡŒ ΠΎΠΏΡ‚ΠΈΡ‡Π½ΠΎΠ³ΠΎ нагнітання ΠΏΠ΅Ρ€Π΅Π²ΠΈΡ‰ΡƒΠ²Π°Π»Π° значСння 685 ΠΊΠ’Ρ‚ см⁻² для ZnO ΠΌΡ–ΠΊΡ€ΠΎΠΏΡ€ΠΈΠ·ΠΌ Ρ– 560 ΠΊΠ’Ρ‚ см⁻² для ZnO Π½Π°Π½ΠΎΠ΄Ρ€ΠΎΡ‚Ρ–Π². Ρ„Π°Π·ΠΈ Π½Π° монокристалічних (100) ΠΊΡ€Π΅ΠΌΠ½Ρ–Ρ”Π²ΠΈΡ… ΠΏΡ–Π΄ΠΊΠ»Π°Π΄ΠΊΠ°Ρ…. ZnO Π½Π°Π½ΠΎΠ΄Ρ€ΠΎΡ‚ΠΈ Π±ΡƒΠ»ΠΈ Π²ΠΈΡ€ΠΎΡ‰Π΅Π½Ρ– Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΡ…Ρ–ΠΌΡ–Ρ‡Π½ΠΈΠΌ осадТСнням Π½Π° скляних ΠΏΡ–Π΄ΠΊΠ»Π°Π΄ΠΊΠ°Ρ…, ΠΏΠΎΠΊΡ€ΠΈΡ‚ΠΈΡ… оксидним ΡˆΠ°Ρ€ΠΎΠΌ Ρ–Π½Π΄Ρ–ΡŽ Π· ΠΎΠ»ΠΎΠ²ΠΎΠΌ. Π›Π°Π·Π΅Ρ€Π½ΠΈΠΉ Π΅Ρ„Π΅ΠΊΡ‚ спостСрігався ΠΏΡ€ΠΈ ΠΊΡ–ΠΌΠ½Π°Ρ‚Π½Ρ–ΠΉ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ– Π² Ρ‚ΠΈΡ… Π²ΠΈΠΏΠ°Π΄ΠΊΠ°Ρ…, ΠΊΠΎΠ»ΠΈ ΠΏΠΎΡ‚ΡƒΠΆΠ½Ρ–ΡΡ‚ΡŒ ΠΎΠΏΡ‚ΠΈΡ‡Π½ΠΎΠ³ΠΎ нагнітання ΠΏΠ΅Ρ€Π΅Π²ΠΈΡ‰ΡƒΠ²Π°Π»Π° значСння 685 ΠΊΠ’Ρ‚ см⁻² для ZnO ΠΌΡ–ΠΊΡ€ΠΎΠΏΡ€ΠΈΠ·ΠΌ Ρ– 560 ΠΊΠ’Ρ‚ см⁻² для ZnO Π½Π°Π½ΠΎΠ΄Ρ€ΠΎΡ‚Ρ–Π²

    Tuning a sign of magnetoelectric coupling in paramagnetic NH2(CH3)2Al1-xCrx(SO4)*6H2O crystals by metal ion substitution

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    Hybrid organometallic systems offer a wide range of functionalities, including magnetoelectric interactions. However, the ability to design on-demand ME coupling remains challenging despite a variety of host-guest configurations and ME phases coexistence possibilities. Here, we report the effect of metal-ion substitution on the magnetic and electric properties in the paramagnetic ferroelectric DMAAS crystals. Doing so we are able to induce and even tune a sign of the ME interactions in the paramagnetic ferroelectric state. Both studied samples with 6.5% and 20% of Cr become paramagnetic, contrary to the initial diamagnetic compound. Due to the isomorphous substitution with Cr the ferroelectric phase transition temperature increases nonlinearly, with the shift being larger for the sample with Cr content of 6.5%. A magnetic field applied along the polar c axis increases ferroelectricity for this sample and shifts Tc to higher values, while inverse effects are observed for sample containing 20% of Cr. The ME coupling coefficient of 1.7ns/m found for a crystal with 20% of Cr is among the highest reported up to now. The observed sign change of ME coupling coefficient with a small change in Cr content paves the way for ME coupling engineering.Comment: 7 pages, 6 figures. New Organometallic Magnetoelectric and Ferroelectric compoun
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