Analysis of mode characteristics for deformed square resonators by FDTD technique

The mode frequencies and quality factors (Q-factors) in two-dimensional (2-D) deformed square resonators are analyzed by finite-difference time-domain (FDTD) technique. The results show that the deformed square cavities with circular and cut corners have larger Q-factors than the perfect ones at certain conditions. For a square cavity with side length of 2 mu m and refractive index of 3.2, the mode Q-factor can increase 13 times as the perfect corners are replaced by a quarter of circle with radius of 0.3 pm. Furthermore the blue shift with the increasing deformations is found as a result of the reduction in effective resonator area. In square cavities with periodic roughness at sidewalls which maintains the symmetry of the square, the Q-factors of the whisperin gallery (WG)-like modes are still one order of magnitude larger that those of non-WG-like modes. However, the Q-tactors of these two types of modes are of the same order in the square cavity with random roughness. We also find that the rectangular and rhombic deformation largely reduce the Q-factors with the increasing offset and cause the splitting of the doubly degenerate modes due to the breaking of certain symmetry properties.

Lasing of CdSSe quantum dots in glass spherical microcavity

Glass spherical microcavities containing CdSSe semiconductor quantum dots (QDs) of a few microns in diameter are fabricated using a physical method. When a single glass microspherical cavity is excited by a laser beam at room temperature, very strong and sharp whispering gallery modes are shown on the background of PL spectra of CdSSe QDs, which confirms that coupling between the optical emission of embedded QDs and spherical cavity modes is realized. For a glass microsphere only 4.6 mum in diameter, it was found that the energy separation is nearly up to 26 nm both for TE and TM modes. With the increasing excitation intensity, the excitation intensity dependence of the emission intensity is not linear in the double-logarithmic scale. Above the threshold value, the linewidths of resonance modes become narrower. The lasing behavior is achieved at relatively low excitation intensity at room temperature. High optical stability and low threshold value make this optical system promising in visible microlaser applications. (C) 2002 Elsevier Science B.V. All rights reserved.

Lasing of CdSexS1-x quantum dots in a glass spherical microcavity

A glass spherical microcavity only a few microns in diameter embedded with CdSexS1-x quantum dots (QDs) was fabricated using a physical method; it exhibited good optical stability under continuous-wave laser excitation with high power. We investigated the excitation power dependences of the emission intensity and the linewidth of both transverse electric and transverse magnetic resonance peaks of whispering gallery modes. Stimulated emission behaviour of multi-frequency modes is observed at room temperature. The low threshold value and large mode separation makes QD-containing microspheres promising for visible microlaser applications.

Photoluminescence behavior of quantum dots in spherical glass microcavity

Micrometer-sized spherical glass microspheres were fabricated. CdSeS semiconductor nanometer clusters were incorporated into spherical microcavities. When a single microsphere was excited by a laser beam, the whispering gallery mode resonance of the photoluminescence of CdSeS quantum dots in the spherical microcavities was realized by the multiple total internal reflections at the spherical interface. The coupling of restricted electronic and photonic states was realized.

Photoluminescence study of CdSexS1-x quantum dots in a glass spherical microcavity

The photoluminescence (PL) of CdSexS1-x semiconductor quantum dots (QDs) in a glass spherical microcavity is investigated. The CdSexS1-x semiconductor clusters embedded in a glass matrix are fabricated by using the heat treatment method. Periodical structures consisting of sharp spectral lines are observed in the PL spectra of CdSexS1-x QDs, which can be well explained by the coupling with the whispering gallery modes of the spherical microcavity based on Mie scattering theory.

Quantum dots in glass spherical microcavity

Glass spherical microcavities containing CdSexS1-x semiconductor quantum dots (QDs) are fabricated. The coupling between the optical emission of embedded CdSexS1-x QDs and spherical cavity modes is realized. When the luminescence of QDs is excited by a laser beam, the strong whispering gallery mode resonance with high Q factors is achieved in the photoluminescence spectra. (C) 2001 American Institute of Physics.

Characteristics of triangle and square InP/InGaAsP microlasers

Directional emission triangle and square InGaAsP/InP lasers have been fabricated by standard photolithography, inductively coupled plasma etching technique combined with wet chemical etching process. In this article, the characteristics of the microcavity lasers are presented. For an equilateral triangle microcavity laser with the side length of 30 mu m, we got the laser spectra fitted very well with the mode wavelength formulate LIP to the 8(th) transverse mode at room temperature. But the laser spectra are usually more complex than the formulae for the lasers, especially for the lasers with a smaller side length. For a square microcavity laser with side length of 20 mu m, we observed the mode competition between the Fabry-Perot (FP) modes and Whispering-Gallery (WG) modes at 200K. The output spectra below the threshold have the mode interval of FP modes with a large mode interval, and the laser spectra agree very well with the WG modes, which have mode interval less than the FP modes. The output spectra are dominated by the FP modes below the threshold, because the FP modes have a higher output coupling efficiency than the WG modes.

High-quality-factor EH modes in microcylinder resonators predicted by 3D FDTD simulation

The mode characteristis of a microcylinders with center layer thickness 0.2 mu m and radius 1 mu m are investigated by the three-dimensional (31)) finite-difference time-domain (FDTD) technique and the Pade approximation. The mode quality factor (Q-factor) of the EH71 mode obtained by 3D FDTD increase with the increase of the refractive index of the cladding layer n(2) as n(2) smaller than 3.17, and can be as large as 2.4 x 10(4) as the vertical refractive index distribution is 3.17/3.4/3.17, which is much larger than that of the HE71 mode with the same vertical refractive index distribution.

AlGaInAs-InPMicrocylinder Lasers Connected With an Output Waveguide

AlGaInAs-InPmicrocylinder lasers connected with an output waveguide are fabricated by planar technology. Room-temperature continuous-wave operation with a threshold current of 8 mA is realized for a microcylinder laser with the radius of 10 mu m and the output waveguide width of 2 mu m. The mode Q-factor of 1.2 x 10(4) is measured from the laser spectrum at the threshold. Coupled mode characteristics are analyzed by 2-D finite-difference time-domain simulation and the analytical solution of whispering-gallery modes. The calculated mode Q-factors of coupled modes are in the same order as the measured value.

平面工艺制作的定向输出微腔半导体激光器

光学微腔中偶极子自发辐射受到空间和频谱调制,能实现自发辐射增强或抑制效应,而且其有源区体积可以非常小,有利于极低阈值工作和极高的调制速率.在过去的二十多年来,垂直腔面发射激光器、回音壁模式(whispering-gallery mode)微腔激光器以及光子晶体微腔激光器三类光学微腔激光器的研究取得了很大的进展.回音壁模式微腔中,模式光线由于其在微腔界面的入射角大于全反射临界角而受到限制,是一种结构非常简单的光学微腔.微盘激光器作为典型的回音壁模式微腔激光器,可利用普通的边发射激光器外延片材料,采用半导体平面工艺制作,引起了人们很大的重视.但圆对称结构的微盘激光器易于实现回音壁模式的全反射限制,却难以得到定向的激光输出,限制了它的应用.人们往往采用局部破坏圆盘的对称性、整体变形以及消逝波耦合的输出波导实现微盘激光器的定向激光输出.在圆对称的微盘结构中,模式光线在微腔与空气界面上的入射角是恒定的,而在整体变形的圆盘中,如椭圆形微腔中,模式光线在界面的入射角则不断变化,并在某些位置上小于全反射临界角而折射出光学微腔,从而实现定向输出.这种变形微盘中模式光线往往具有混沌现象,因而吸引了人们的注意.

InGaAsP/InP正方形微腔激光器

采用平面工艺制作的定向输出微腔半导体激光器是集成光学回路的理想光源.近十几年来,以微盘为代表的回音壁模式(whispering-gallery mode)微腔激光器引起人们很大的重视.但圆对称的微盘激光器缺乏定向的激光输出,人们往往利用输出波导与微盘实现消逝波耦合或通过改变微盘的对称性来实现定向输出.最近几年,多边形微腔如正三角形、正方形、长方形、六边形等多边形光学微腔也引起人们的重视.多边形光学微腔中也能有高Q值的类回音壁模式.而且由于不具有圆对称性,其模式特性有利于简单地实现定向光输出.

Lasing of CdSSe quantum dots in glass spherical microcavity

Glass spherical microcavities containing CdSSe semiconductor quantum dots (QDs) of a few microns in diameter are fabricated using a physical method. When a single glass microspherical cavity is excited by a laser beam at room temperature, very strong and sharp whispering gallery modes are shown on the background of PL spectra of CdSSe QDs, which confirms that coupling between the optical emission of embedded QDs and spherical cavity modes is realized. For a glass microsphere only 4.6 mum in diameter, it was found that the energy separation is nearly up to 26 nm both for TE and TM modes. With the increasing excitation intensity, the excitation intensity dependence of the emission intensity is not linear in the double-logarithmic scale. Above the threshold value, the linewidths of resonance modes become narrower. The lasing behavior is achieved at relatively low excitation intensity at room temperature. High optical stability and low threshold value make this optical system promising in visible microlaser applications. (C) 2002 Elsevier Science B.V. All rights reserved.

Systematic Nonlinear Planning

This paper presents a simple, sound, complete, and systematic algorithm for domain independent STRIPS planning. Simplicity is achieved by starting with a ground procedure and then applying a general and independently verifiable, lifting transformation. Previous planners have been designed directly as lifted procedures. Our ground procedure is a ground version of Tate's NONLIN procedure. In Tate's procedure one is not required to determine whether a prerequisite of a step in an unfinished plan is guarnateed to hold in all linearizations. This allows Tate"s procedure to avoid the use of Chapman"s modal truth criterion. Systematicity is the property that the same plan, or partial plan, is never examined more than once. Systematicity is achieved through a simple modification of Tate's procedure.

Carbono da biomassa microbiana em solos de cerrado: comparacao dos metodos fumigacao-incubacao e fumigacao-extracao.

Dentre os metodos mais utilizados para determinacao do carbono da biomassa microbiana destacam-se: os de cloroformio-fumigacao-incubacao (CFI) e cloroformio-fumigacao-extracao (CFE). Trabalhos relatados na literatura tem comparado a eficiencia desses metodos em diversos locais. No entanto, para a regiao do cerrado nao existem informacoes a esse respeito. O objetivo deste trabalho foi avaliar a eficiencia dos metodos CFE e CFI na determinacao do carbono da biomassa microbiana do solo (CBMS) em areas de cerrado sob cultura anual (rotacao soja-milho) e pastagem consorciada (Andropogon gayanus e Stylosanthes guianensis) e sob tres fitofisionomias - Mata de Galeria, Campo Sujo e Cerradao. Amostras de solo coletadas em duas profundidades, 0 a 5 cm e 5 a 20 cm, foram analisadas em quatro epocas: agosto de 1998, janeiro a agosto de 1999 e janeiro de 2000. Nas areas cultivadas, os resultados obtidos com os metodos CFE e CFI foram semelhantes independentemente dos tratamentos e das epocas amostradas; as pastagens consorciadas apresentaram maiores teores de CBMS do que as areas sob culturas anuais. A integracao profundidades x metodos foi significatica. Nao houve diferencas entre a profundidade 0 a 5 cm quando se utilizou o metodo CFI, mas as diferencas obtidas com o metodo CFE foram significativas. Os metodos CFI e CFE apresentaram as mesmas tendencias nas areas ativas, independentemente dos tratamentos, profundidades ou epocas analisados; a Mata de Galeria apresentou niveis de CBMS superiores aos do Cerradao e do Campo Sujo. As interacoes profundidades x metodos e epocas x metodos foram significativas devido ao fato de que as diferencas nos teores do carbono da bimassa microbiana, nas profundidades e epocas amostradas, foram mais acentuadas com o metodo CFE. Os resultados indicaram que os metodos CFI e CFE foram apropriados para determinacao da CBMS em solos de Cerrado sob cultivo e sob vegetacao nativa.

from Webern to dance to Burton.

Commissioned by the Concorde Ensemble. Paul Roe gave the premiere performance at the RHA Gallery, Dublin, 23rd February 2014. The piece is informed by the choreography of Jiri Kylian, in particular two three minute sections of his work No More Play initially choreographed to a score by Webern (his Five Movements for String Quartet) hence the title.