Shear bond strength of repairs in porcelain conditioned with laser

The aim of this study was to evaluate the shear bond strength of repairs in porcelain conditioned with laser. Sixty porcelain discs were made and six groups were formed (n = 10): G1: conditioning with laser with potency 760 mW; G2: conditioning with laser with potency 760 mW and application of 37% phosphoric acid for 15 s; G3: conditioning with laser with potency 900 mW; G4: conditioning with laser with potency 900 mW and application of 37% phosphoric acid for 15 s; G5: application of 37% phosphoric acid for 15 s (group control) and G6: application of 10% hydrofluoric acid for 2 min. The composite resin was insert of incremental layers at the porcelain surface aided with a metal matrix, and photoactivation for 20 s each increment. The specimens were submitted to a thermal cycling by 1000 cycles of 30 s in each bath with temperature between 5 and 55 degrees C. After the thermal cycling, specimens were submitted to the shear bond strength. The results were evaluated statistically through analysis of variance and Tukey's tests with 5% significance. The averages and standard deviation founded were: G1, 11.25 (+/- 3.10); G2, 12.32 (+/- 2.65); G3, 14.02 (+/- 2.38); G4, 13.44 (+/- 2,07); G5, 9.91 (-/+ 2,18); G6, 12.74 (+/- 2.67). The results showed that the femtosecond laser produced a shear bond strength of repairs in porcelain equal to the hydrofluoric acid and significantly superior to the use of phosphoric acid. Microsc. Res. Tech., 2012. (C) 2012 Wiley Periodicals, Inc.

Microbiologic results after non-surgical erbium-doped:yttrium, aluminum, and garnet laser or air-abrasive treatment of peri-implantitis: a randomized clinical trial

The purpose of this study is to assess clinical and microbiologic effects of the non-surgical treatment of peri-implantitis lesions using either an erbium-doped:yttrium, aluminum, and garnet (Er:YAG) laser or an air-abrasive subgingival polishing method.

Evaluation of the Morphological Characteristics of Laser-Irradiated Dentin

OBJECTIVE The aim of this study was to investigate the effect of different energy settings of Er:YAG laser irradiation on dentin surface morphology with respect to the number of opened dentinal tubules. BACKGROUND DATA An ideally prepared dentin surface with opened dentinal tubules is a prerequisite for adhesive fixation. No study, however, has yet compared the numbers of opened dentinal tubules with regard to statistical differences. METHODS Conventional preparations using a bur with or without additional acid etching acted as control groups. Dentin specimens were prepared from human third molars and randomly divided into eight groups according to the energy settings of the laser (1, 1.5, 4, 6, 7.5, and 8 W) and two controls (bur and bur plus acid etching). After surface preparation, dentin surfaces were analyzed with a scanning electron microscope, and the number of opened dentinal tubules in a defined area was counted. RESULTS The control groups showed smooth surfaces with (bur plus acid etching) and without opened dentinal tubules (bur), whereas all laser-irradiated surfaces showed rough surfaces. Using the energy setting of 4 W resulted in significantly more opened dentinal tubules than the conventional preparation technique using the bur with additional acid etching. In contrast, the energy setting of 8 W showed significantly fewer opened dentinal tubules, and also exhibited signs of thermal damage. CONCLUSIONS The Er:YAG laser with an energy setting of 4 W generates a dentin surface with opened dentinal tubules, a prerequisite for adhesive fixation.

Fotodegradação de antibióticos de nitrofurano em condições ambientais

Ao submeter uma solução aquosa de 5-nitro-2-furaldeído (NFA) a fotólise com impulsos de luz de curta duração (produzidos por um laser de estado sólido de Nd-YAG) origina-se uma absorvância (transiente) de curta duração que é atribuída à absorção de luz pelo NFA no estado tripleto mais baixo (3NFA*). O espectro desta absorção de luz apresenta um λmax = 475 ± 5 nm, que se mostrou ser insensível à polaridade do solvente. Em solução aquosa, a absorção do 3NFA* decai para uma absorção transiente de tempo de vida mais longo e que, medida em tempos diferentes (depois do fim do impulso), revelou ser devida a um radical furiloxilo (a de λmax ≈ 375 nm) e ao anião radical NFA•‒ (a de λmax ≈ 400 nm). Estes dois radicais foram gerados independentemente um do outro, o que permitiu confirmar a atribuição daquela absorção de longo tempo de vida (obtida na fotólise de NFA em água) aos radicais furiloxilo e anião radical do NFA. O tempo de vida (τ) do 3NFA* revelou uma dependência em relação à natureza do solvente e à concentração de NFA no estado fundamental. Da propensão do 3NFA* para abstrair um átomo de hidrogénio de solventes (com átomos de H abstraíveis) concluiu-se a natureza (n, π*) do estado tripleto de menor energia do NFA. A dependência de τ em relação à concentração de NFA (no estado fundamental) forneceu evidência cinética em favor da formação de um excímero tripleto que supostamente se dissocia em iões radicais (catião e anião) como é proposto no mecanismo de auto-supressão do 3NFA* por transferência de electrão. O efeito da acididade sobre τ corrobora o mecanismo de auto-supressão por transferência de electrão. A análise cromatográfica e espectroscópica da solução fotolisada de NFA em água permitiu identificar a 5-hidroximetileno-2(5H)-furanona, o ião nitrito e uma substância desconhecida de tR 3.69 minutos como os fotoprodutos maioritários. Apresenta-se evidência conclusiva de que a 5-hidroximetileno-2(5H)-furanona provém do radical furiloxilo. Mostra-se que a substância desconhecida também pode ser obtida na foto-redução de NFA em propan-2-ol e na redução química de NFA por Fe (s) em água (em ambas, conjuntamente com produção de 5-amino-2-furaldeído). Com base na análise por espectroscopia de absorção de RMN de 1H e de 13C (com 2-D HMQC) e vibracional por FT no infravermelho médio, discute-se a possível estrutura da substância de tR 3.69 minutos obtida como um produto da foto-redução de NFA em água. Experiências de sensibilização e supressão do 3NFA* permitiram obter a energia de excitação do estado tripleto como 238 ± 2 kJ mol-1 o que, conjuntamente com o potencial de redução monoelectrónica (E71) do NFA fornece E71 (3NFA* / NFA•‒) = 2.26 V vs. SHE para o potencial de redução monoelectrónica do 3NFA* em solução aquosa neutra. Mostra-se que os aniões inorgânicos (usados como nucleófilos) são mono-oxidados pelo 3NFA* (como é indicado pela observação de NFA•‒ e do radical inorgânico) com constantes de velocidade de segunda-ordem (

Mechanisms of a change in the refractive index of an intensely pumped Yb:YAG crystal

Mechanisms of a change in the refractive index appearing in an intensely diode-pumped Yb:YAG-laser disk element are studied with the help of polarisation interferometry and dynamic grating testing. It is found that changes in the electronic component of the refractive index arising upon changing the populations of electronic levels of Yb ions (the ground F state and the upper F level of the laser transition) and caused by the difference in the polarisability of these levels are an order of magnitude greater than thermal changes in the refractive index. It is shown that the difference Δp in the polarisability at the probe wavelength of 633 nm is 1.9 × 10 cm and at the laser transition wavelength of 1029 nm is 1.6 × 10 cm. ©2006 Kvantovaya Elektronika and Turpion Ltd.

脉冲激光合金化形成含非晶相表层的微观组织

利用Nd:YAG脉冲激光在不锈钢表层合金化SiO_2纳米颗粒，在熔池最表层14μm深度范围内形成Si合金化区域，Si含量呈非均匀分布特征。表层为非晶相与奥氏体的双相组织，非昌相约不散分布并呈现特殊的环状形貌，中心为非晶，外侧为纳米尺度的超细柱晶及等轴晶。分析了非晶形成机制。

Micro-shock waves generated inside a fluid jet impinging on plane wall

An Nd:glass laser pulse (18 ns, 1.38 J) is focused in a tiny area of about 100-mum diam under ambient conditions to produce micro-shock waves. The laser is focused above a planar surface with a typical standoff distance of about 4 mm, The laser energy is focused inside a supersonic circular jet of carbon dioxide gas produced by a nozzle with internal diameter of 2.9 mm and external diameter of 8 mm, Nominal value of the Mach number of the jet is around 2 with the corresponding pressure ratio of 7.5 (stagnation pressure/static pressure at the exit of the nozzle), The interaction process of the micro-shock wave generated inside the supersonic jet with the plane wall is investigated using double-pulse holographic interferometry. A strong surface vortex field with subsequent generation of a side jet propagating outward along the plane wail is observed. The interaction of the micro-shock wave with the cellular structure of the supersonic jet does not seem to influence the near surface features of the flowfield. The development of the coherent structures near the nozzle exit due to the upstream propagation of pressure waves seems to be affected by the outward propagating micro-shock wave. Mach reflection is observed when the micro-shock wave interacts with the plane wall at a standoff distance of 4 mm, The Mach stem is slightly deflected, indicating strong boundary-layer and viscous effects near the wall. The interaction process is also simulated numerically using an axisymmetric transient laminar Navier-Stokes solver. Qualitative agreement between experimental and numerical results is good.

脉冲激光离散加工熔池形态及其影响因素的研究

研究了Nd:YAG脉冲激光离散加工时功率密度和作用时间对熔池几何形态的影响，5CrMnMo 钢的实验结果表明：在本文所涉及的加工条件下，熔池存在热传导型和深熔型两种形态；激光作用时间小于4ms时，在相同作用时间下，随着激光功率密度的增加，熔池深宽比显著增加；但当作用时间大于4ms后，功率密度对深宽比的影响减弱，基于线性热传导模型的计算结果表明：熔凝起始阶段的固态加热过程可忽略；熔池几何尺寸在激光脉冲结束后某个时刻达到最大值；当平均功率密度大于5x10(5)W/cm(2),同时激光作用时间大于2ms时,热传导型激光熔池向深熔型激光熔池转变。

脉冲激光离散熔凝加工的熔池几何形态研究

研究了Nd:YAG脉冲激光离散加工时功率密度和作用时间对熔池几何形态的影响。5CrMnMo钢的实验结果表明：在一定加工条件下，熔池存在热传导型和深熔型两种形态。激光作用时间小于4ms时，随着激光功率密度的增加，熔池深宽比显著增加；作用时间超过4ms后，功率密度对深宽比的影响减弱。基于线性热传导模型的计算结果表明：熔凝起始阶段固态加热过程可忽略；熔池几何尺寸在激光脉冲结束后某个时刻达到最大值；当平均功率密度大于5×10~5W/cm~2，同时激光作用时间大于2ms时，热传导型激光熔池向深熔型激光熔池转变。

高功率脉冲染料激光振荡-放大器

报道一种用倍频Nd:YAG激光纵向泵浦、双棱镜一维扩束的染料激光系统,经过二级放大,输出总效率达31%.当泵浦光为40 mJ时,得到12.2mJ、 2MW,线宽为0.18(?)的可调谐染料激光输出,重复率可达10次/秒.

CO_2激光诱导扩散的太阳电池初步研究

<正> 以硅(Si)为代表的半导体材料激光退火是近几年比较活跃的研究领域。一般,采用红宝石、YAG、氩离子等波长较短的激光器作激光源。后来发现,硅材料在强CO_2激光辐照下由于载流子的热激发也引起强烈的吸收,这为CO_2激光用于半导体Si的加工奠定了基础。用激光试制太阳电池已有一些报道,其方法一般是先对Si作离子注入,然后用调Q红宝石激光或Nd:YAG激光进行退火。这种方法对改进电池性能虽有效果,但工艺复杂,成本高,实用性比较差。考虑到连续CO_2激光器的输出功率大、效率高、价格低,并已进入工业生产,

基于强激光辐照固体锡靶产生极紫外光源的实验研究

建立了一套利用高功率YAG激光器辐照固体锡靶产生高转换效率极紫外光(extreme ultraviolet)源的实验装置.利用建立的实验装置开展了极紫外光源的强度和转换效率与抽运激光强度关系的实验研究,发现极紫外光源的转换效率随抽运激光强度的变化具有饱和效应.实验发现:当抽运激光能量达到250mJ时,极紫外光源的转换效率最高,波长为13.5nm处0.27nm带宽范围内的极紫外光源的能量转换效率为1.6%,此时对应的激光强度为1.8×1011W/cm2.

高功率钕玻璃激光三倍频脉冲时间波形的研究

基于目前国内规模最大的激光驱动器——“神光Ⅱ”八路基频光已经实现功率平衡运行，通过改变其中若干路三倍频系统各调谐量的偏离，对输出三倍频波形进行束与束之间的横向对比研究．研究发现，对于Ⅱ类-Ⅱ类偏振失配三倍频系统，在影响转换效率的三个调谐量中，偏振分配角失配△θp，对三倍频波形影响最大；在入射基频功率密度约为1．0GW／cm^2情况下，当三倍频系统三个调谐量都处在最佳匹配时，三倍频波形半峰全宽τ最小。研究工作为最终实现“神光Ⅱ”八路光束三倍频功率平衡输出提供了晶体调试的方法。

掺钕陶瓷激光器获得236W高功率激光输出

随着1999年陶瓷制备工艺的突破性进展，透明陶瓷作为激光增益介质取得了可与单晶相比拟的光学质量。Nd：YAG单晶是目前应用最广泛的固体激光介质，然而传统提拉法生长的单晶的固有缺陷限制了它的进一步发展。