Room-temperature, ground-state lasing for red-emitting vertically aligned InAlAs/AlGaAs quantum dots grown on a GaAs(100) substrate

The effect of the growth temperature on the properties of InAlAs/AlGaAs quantum dots grown on GaAs(100) substrates is investigated. The optical efficiency and structural uniformity are improved by increasing the growth temperature from 530 to 560 degreesC. The improvements of InAlAs/AlGaAs quantum-dot characteristics could be explained by suppressing the incorporation of oxygen and the formation of group-III vacancies. Furthermore, edge-emitting laser diodes with six quantum-dot layers grown at 560 degreesC have been fabricated. Lasing occurs via the ground state at 725 nm, with a room-temperature threshold current density of 3.9 kA/cm(2), significantly better than previously reported values for this quantum-dot systems. (C) 2002 American Institute of Physics.

Measurements of the XUV mass absorption coefficient of an overdense liquid metal

The increase in the XUV mass absorption coefficient of liquid aluminium, produced by high-power-laser shock-compression, is measured using XUV laser radiography. At a photon energy of 63 eV a change in the mass absorption coefficient by up to a factor of similar to2.2 is determined at densities close to twice that of solid and electron temperatures of the order of 1 eV. Comparison with hydrodynamic simulations indicate that the absorption coefficient scales with density as rho (1.3 +/-0.2).

Thomson spectrometer-microchannel plate assembly calibration for MeV-range positive and negative ions, and neutral atoms

We report on the absolute calibration of a microchannel plate (MCP) detector, used in conjunction with a Thomson parabola spectrometer. The calibration delivers the relation between a registered count numbers in the CCD camera (on which the MCP phosphor screen is imaged) and the number of ions incident on MCP. The particle response of the MCP is evaluated for positive, negative, and neutral particles at energies below 1 MeV. As the response of MCP depends on the energy and the species of the ions, the calibration is fundamental for the correct interpretation of the experimental results. The calibration method and arrangement exploits the unique emission symmetry of a specific source of fast ions and atoms driven by a high power laser.

Spray Pyrolysed Zinc Oxide Thin Films : Effects of Doping and Ion Beam Irradiation

In recent years scientists have made rapid and significant advances in the field of semiconductor physics. One of the most important fields of current interest in materials science is the fundamental aspects and applications of conducting transparent oxide thin films (TCO). The characteristic properties of such coatings are low electrical resistivity and high transparency in the visible region. The first semitransparent and electrically conducting CdO film was reported as early as in 1907 [1]. Though early work on these films was performed out of purely scientific interest, substantial technological advances in such films were made after 1940. The technological interest in the study of transparent semiconducting films was generated mainly due to the potential applications of these materials both in industry and research. Such films demonstrated their utility as transparent electrical heaters for windscreens in the aircraft industry. However, during the last decade, these conducting transparent films have been widely used in a variety of other applications such as gas sensors [2], solar cells [3], heat reflectors [4], light emitting devices [5] and laser damage resistant coatings in high power laser technology [6]. Just a few materials dominate the current TCO industry and the two dominant markets for TCO’s are in architectural applications and flat panel displays. The architectural use of TCO is for energy efficient windows. Fluorine doped tin oxide (FTO), deposited using a pyrolysis process is the TCO usually finds maximum application. SnO2 also finds application ad coatings for windows, which are efficient in preventing radiative heat loss, due to low emissivity (0.16). Pyrolitic tin oxide is used in PV modules, touch screens and plasma displays. However indium tin oxide (ITO) is mostly used in the majority of flat panel display (FPD) applications. In FPDs, the basic function of ITO is as transparent electrodes. The volume of FPD’s produced, and hence the volume of ITO coatings produced, continues to grow rapidly. But the current increase in the cost of indium and the scarcity of this material created the difficulty in obtaining low cost TCOs. Hence search for alternative TCO materials has been a topic of active research for the last few decades. This resulted in the development of binary materials like ZnO, SnO2, CdO and ternary materials like II Zn2SnO4, CdSb2O6:Y, ZnSO3, GaInO3 etc. The use of multicomponent oxide materials makes it possible to have TCO films suitable for specialized applications because by altering their chemical compositions, one can control the electrical, optical, chemical and physical properties. But the advantages of using binary materials are the easiness to control the chemical compositions and depositions conditions. Recently, there were reports claiming the deposition of CdO:In films with a resistivity of the order of 10-5 ohm cm for flat panel displays and solar cells. However they find limited use because of Cd-Toxicity. In this regard, ZnO films developed in 1980s, are very useful as these use Zn, an abundant, inexpensive and nontoxic material. Resistivity of this material is still not very low, but can be reduced through doping with group-III elements like In, Al or Ga or with F [6]. Hence there is a great interest in ZnO as an alternative of ITO. In the present study, we prepared and characterized transparent and conducting ZnO thin films, using a cost effective technique viz Chemical Spray Pyrolysis (CSP). This technique is also suitable for large area film deposition. It involves spraying a solution, (usually aqueous) containing soluble salts of the constituents of the desired compound, onto a heated substrate.

Spectroscopy of highly excited vibrational states of HCN in its ground electronic state

An experimental technique based on a scheme of vibrationally mediated photodissociation has been developed and applied to the spectroscopic study of highly excited vibrational states in HCN, with energies between 29 000 and 30 000 cm(-1). The technique consists of four sequential steps: in the first one, a high power laser is used to vibrationally excite the sample to an intermediate state, typically (0,0,4), the nu(3) mode being approximately equivalent to the C-H stretching vibration. Then a second laser is used to search for transitions between this intermediate state and highly vibrationally excited states. When one of these transitions is found, HCN molecules are transferred to a highly excited vibrational state. Third, a ultraviolet laser photodissociates the highly excited molecules to produce H and CN radicals in its A (2)Pi electronic state. Finally, a fourth laser (probe) detects the presence of the CN(A) photofragments by means of an A-->B-->X laser induced fluorescence scheme. The spectra obtained with this technique, consisting of several rotationally resolved vibrational bands, have been analyzed. The positions and rotational parameters of the states observed are presented and compared with the results of a state-of-the-art variational calculation. (C) 2004 American Institute of Physics.

Equation of state for hot dense matter using a relativistic screened hydrogenic model

The study of matter under conditions of high density, pressure, and temperature is a valuable subject for inertial confinement fusion (ICF), astrophysical phenomena, high-power laser interaction with matter, etc. In all these cases, matter is heated and compressed by strong shocks to high pressures and temperatures, becomes partially or completely ionized via thermal or pressure ionization, and is in the form of dense plasma. The thermodynamics and the hydrodynamics of hot dense plasmas cannot be predicted without the knowledge of the equation of state (EOS) that describes how a material reacts to pressure and how much energy is involved. Therefore, the equation of state often takes the form of pressure and energy as functions of density and temperature. Furthermore, EOS data must be obtained in a timely manner in order to be useful as input in hydrodynamic codes. By this reason, the use of fast, robust and reasonably accurate atomic models, is necessary for computing the EOS of a material.

Avaliação in vivo e in vitro de diferentes protocolos no tratamento da hipersensibilidade dentinária cervical

Este estudo possui duas partes distintas: 1. in vivo (randomizado e longitudinal) que teve como objetivo avaliar protocolos de tratamento para hipersensibilidade dentinária com laser de baixa potência (com diferentes dosagens), laser de alta potência e agente dessensibilizante, por um período de 12 e 18 meses; e 2. in vitro que teve como objetivo analisar a perda de estrutura de dois dentifrícios distintos (Colgate Total 12 e Colgate Pró Alívio) e analisar a permeabilidade dentinária dos tratamentos da etapa 01, associados aos dentifrícios, após diferentes ciclos de abrasão. Na parte in vivo, as lesões cervicais não cariosas de 32 voluntários, previamente submetidos aos critérios de elegibilidade ou exclusão, foram divididas em nove grupos (n=10): G1: Gluma Desensitizer (Heraeus Kulzer), G2: Laser de baixa potência com baixa dosagem (Photon Lase, DMC) (três pontos de irradiação vestibulares e um ponto apical: 30 mW, 10 J/cm2, 9 seg por ponto com o comprimento de onda de 810nm). Foram realizadas três sessões com um intervalo de 72 horas), G3: Laser de baixa potência com alta dosagem (um ponto cervical e um ponto apical: 100 mW, 90 J/cm2, 11 seg por ponto com o comprimento de onda de 810nm. Foram realizadas três sessões com um intervalo de 72 horas), G4: Laser de baixa potência com baixa dosagem + Gluma Desensitizer, G5: Laser de baixa potência com alta dosagem + Gluma Desensitizer, G6: Laser de Nd:YAG (Power LaserTM ST6, Lares Research®), em contato com a superfície dental: 1,0W, 10 Hz e 100 mJ, ? 85 J/cm2, com o comprimento de onda de 1064nm, G7: Laser de Nd:YAG + Gluma Desensitizer, G8: Laser de Nd:YAG + Laser de baixa potência com baixa dosagem, G9: Laser de Nd:YAG + Laser de baixa potência com alta dosagem. O nível de sensibilidade de cada voluntário foi avaliado através da escala visual analógica de dor (VAS) com auxílio do ar da seringa tríplice e exploração com sonda após 12 e 18 meses do tratamento. Na parte 02, in vitro, foram utilizados terceiros molares humanos não irrompidos e recém-extraídos. Todos foram limpos e tiveram suas raízes separadas das coroas. As raízes foram seccionadas em quadrados de dentina com dimensões de 4x4x2 mm, os quais foram embutidos em resina Epoxi e devidamente polidos até uma curvatura de 0,3 ?m, analisados em perfilometria ótica. Estes foram imersos em solução de EDTA 17% por 2min para abertura dos túbulos e armazenados em uma solução de Soro Fetal Bovino diluído em salina tamponada com fosfato. Os espécimes foram divididos aleatoriamente em 12 grupos (n=10) G1: Sem tratamento de superfície, sem dentifrício; G2: Nd:YAG/sem dentifrício; G3: Gluma/sem dentifrício; G4: Nd:YAG + Gluma/sem dentifrício; G5: Sem tratamento de superfície/Colgate Total 12; G6: Nd:YAG/Colgate Total 12; G7: Gluma/Colgate Total 12; G8: Nd:YAG + Gluma/Colgate Total 12; G9: Sem tratamento de superfície/Colgate Pró Alívio; G10: Nd:YAG/Colgate Pró Alívio; G11: Gluma/Colgate Pró Alívio; G12: Nd:YAG + Gluma/Colgate Pró Alívio. Em seguida, as superfícies receberam a aplicação de fitas adesivas nas duas margens, mantendo uma área central de teste exposta de 4 x 1 mm, onde foram realizados os tratamentos de superfície e os ciclos de abrasão correspondentes a 1, 7, 30 e 90 dias de escovação (52 ciclos, 210 segundos de contato com o slurry; 361 ciclos, 1470 segundos de contato com o slurry; 1545 ciclos, 6300 segundos de contato com o slurry; 4635 ciclos, 18900 segundos de contato com o slurry, respectivamente). A cada etapa de abrasão, foi realizada análise em Perfilometria Ótica. Para as analises de permeabilidade e Microscopia Eletrônica de Varredura, foram utilizadas amostras circulares de 6 mm de diâmetro e 1 mm de espessura de dentina obtidas das coroas dentais. Estas foram divididas aleatoriamente nos mesmos grupos já descritos anteriormente, sendo que 120 espécimes foram utilizados para permeabilidade (n=10) e 36 para MEV (n=3). Ambas as análises foram realizadas após imersão no EDTA; após tratamentos para a sensibilidade; pós 1 dia, 7 dias, 30 dias e 90 dias de escovação. Após análise estatística pode-se concluir que, in vivo, todos os tratamentos foram eficazes para a redução da hipersensibilidade dentinária. Ainda que o nível da sensibilidade dos pacientes aumentou numericamente, estes não são considerados estatisticamente diferentes a partir de 12 meses. Portanto, até a avaliação de 18 meses, podemos concluir que não houve um aumento na sensibilidade dentinária desde a sua diminuição pós-tratamento. In vitro, pode-se concluir que todos os tratamentos foram capazes de diminuir a permeabilidade dentinária. O dentifrício Total 12 apresentou-se como o mais abrasivo em comparação com o dentifrício Pro Alivio, pois este último promoveu uma perda de estrutura menor, porém ambos não apresentaram aumento na permeabilidade nos tempos de escovação. As microscopias eletrônicas de varredura mostram a formação da smear layer, obliterando os túbulos para ambos os dentifricios. Como conclusão, pode-se afirmar que todos os agentes dessensibilizantes foram efetivos, mesmo apresentando estratégias de ação diferentes. Os dentifrícios são igualmente interessantes para o uso caseiro por ocasionarem oclusão tubular e a associação de tratamentos (caseiro e de consultório) parece ser uma alternativa eficaz no tratamento da hipersensibilidade dentinária.

Dissipative nonlinear structures in optical fiber systems III : dissipative solitons via nonlinear mapping

In the third and final talk on dissipative structures in fiber applications, we discuss mathematical techniques that can be used to characterize modern laser systems that consist of several discrete elements. In particular, we use a nonlinear mapping technique to evaluate high power laser systems where significant changes in the pulse evolution per cavity round trip is observed. We demonstrate that dissipative soliton solutions might be effectively described using this Poincaré mapping approach.

Dissipative nonlinear structures in optical fiber systems III:dissipative solitons via nonlinear mapping

In the third and final talk on dissipative structures in fiber applications, we discuss mathematical techniques that can be used to characterize modern laser systems that consist of several discrete elements. In particular, we use a nonlinear mapping technique to evaluate high power laser systems where significant changes in the pulse evolution per cavity round trip is observed. We demonstrate that dissipative soliton solutions might be effectively described using this Poincaré mapping approach.

Stable optical vortices in nonlinear multicore fibers

The multicore fiber (MCF) is a physical system of high practical importance. In addition to standard exploitation, MCFs may support discrete vortices that carry orbital angular momentum suitable for spatial-division multiplexing in high-capacity fiber-optic communication systems. These discrete vortices may also be attractive for high-power laser applications. We present the conditions of existence, stability, and coherent propagation of such optical vortices for two practical MCF designs. Through optimization, we found stable discrete vortices that were capable of transferring high coherent power through the MCF.

Noncollinear Polarization Gating of Attosecond Pulse Trains in the Relativistic Regime

High order harmonics generated at relativistic intensities have long been recognized as a route to the most powerful extreme ultraviolet pulses. Reliably generating isolated attosecond pulses requires gating to only a single dominant optical cycle, but techniques developed for lower power lasers have not been readily transferable. We present a novel method to temporally gate attosecond pulse trains by combining noncollinear and polarization gating. This scheme uses a split beam configuration which allows pulse gating to be implemented at the high beam fluence typical of multi-TW to PW class laser systems. Scalings for the gate width demonstrate that isolated attosecond pulses are possible even for modest pulse durations achievable for existing and planned future ultrashort high-power laser systems. Experimental results demonstrating the spectral effects of temporal gating on harmonic spectra generated by a relativistic laser plasma interaction are shown.

Room temperature continuous wave operation of 1.33-micron InAs/GaAs quantum dot laser with high output power

Continuous wave operation of a semiconductor laser diode based on five stacks of InAs quantum dots (QDs) embedded within strained InGaAs quantum wells as an active region is demonstrated. At room temperature, 355-mW output power at ground state of 1.33-1.35 microns for a 20-micron ridge-waveguide laser without facet coating is achieved. By optimizing the molecular beam epitaxy (MBE) growth conditions, the QD density per layer is raised to 4*10^(10) cm^(-2). The laser keeps lasing at ground state until the temperature reaches 65 Celsius degree.

Efficacy of high intensity diode laser as an adjunct to non-surgical periodontal treatment: a randomized controlled trial

The high intensity diode laser has been studied in periodontics for the reduction of subgingival bacteria in non-surgical treatment. Our study evaluated the bacterial effect as well as changes in periodontal clinical parameters promoted by root scaling and planing associated with this wavelength. Twenty-seven patients randomly assigned in two groups underwent root scaling and planing on the tested sites, and only the experimental group received the diode laser irradiation. Among the clinical parameters studied, the clinical probing depth (CPD) and the clinical attachment level (CAL) resulted in significant enhancement in the control group when compared with the experimental group (P = 0.014 and P = 0.039, respectively). The results were similar for both groups regarding the plaque index (PI) and bleeding on probing (BP). No significant difference in the microbiological parameters was observed between the control and experimental groups. It was possible to conclude that the high power diode laser adjunct to the non-surgical periodontal treatment did not promote additional effects to the conventional periodontal treatment.

High-energy LDA switched side-pumped electro-optical Q-switched Nd : YAG ceramic laser

By employing a uniformly compact side-pumping system, a high-energy electro-optical Q-switched Nd:YAG ceramic laser has been demonstrated. With 420 W quasi-cw laser-diode-array pumping at 808 ran and a 100 Hz modulating repetition rate, 50 mJ output energy at 1064 nm was obtained with 10 ns pulse width, 5 W average output power, and 5 MW peak power. Its corresponding slope efficiency was 29.8%. The laser system operated quite stably and no saturation phenomena have been observed, which means higher output energy could be expected. Laser parameters between ceramic and single-crystal Nd:YAG lasers have been compared, and pulse characteristics of Nd:YAG ceramic with different repetition rate have been investigated in detail. The still-evolving Nd:YAG ceramics are potential super excellent media for high-energy laser applications. (C) 2007 Optical Society of America.