182 resultados para Near infrared luminescence


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A method of manufacturing two-dimensional photonic crystals on several kinds of semiconductor materials in near infrared region by a focused ion beam is introduced, and the corresponding fabrication results are presented and show that the obtained parameters of fabricated photonic crystals are identical with the designed ones. Using the tunable laser source, the spectra of the fabricated passive photonic crystal and the active photonic crystal are measured. The experiment demonstrates that the focused ion-beam can be used to fabricate the perfect two-dimensional photonic crystals and their devices.

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The electronic structure and electron g factors of HgTe quantum dots are investigated, in the framework of the eight-band effective-mass approximation. It is found that the electron states of quantum spheres have aspheric properties due to the interaction between the conduction band and valence band. The highest hole states are S (l = 0) states, when the radius is smaller than 9.4 nm. the same as the lowest electron states. Thus strong luminescence from H-Te quantum dots with radius smaller than 9.4 nm has been observed (Rogach et al 2001 Phys. Statits Solidi b 224 153). The bandgap of H-Te quantum spheres is calculated and compared with earlier experimental results (Harrison et al 2000 Pure Appl. Chem. 72 295). Due to the quantum confinement effect, the bandgap of the small HgTe quantum spheres is positive. The electron g factors of HgTe quantum spheres decrease with increasing radius and are nearly 2 when the radius is very small. The electron g factors of HgTe quantum ellipsoids are also investigated. We found that as some of the three dimensions increase, the electron g factors decrease. The more the dimensions increase, the more the g factors decrease. The dimensions perpendicular to the direction of the magnetic field affect the g factors more than the other dimension.

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Two-dimensional photonic crystals in near infrared region were fabricated by using the focused ion beam ( FIB) method and the method of electron-beam lithography (EBL) combined with dry etching. Both methods can fabricate perfect crystals, the method of FIB is simple,the other is more complicated. It is shown that the material with the photonic crystal fabricated by FIB has no fluorescence,on the other hand, the small-lattice photonic crystal made by EBL combined with dry etching can enhance the extraction efficiency two folds, though the photonic crystal has some disorder. The mechanisms of the enhanced-emission and the absence of emission are also discussed.

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A detailed study of the characteristics of undoped GaN films, grown on either vicinal or nominal flat SiC (0001) substrates by molecular beam epitaxy, has been carried out using photoluminescence and Raman scattering techniques. The I I K photoluminescence spectra of the GaN film grown on the vicinal SiC (0001) substrate show a strong and sharp near-bandgap peak (full width at half maximum (FWHM) similar to 16 meV). This feature contrasts with that of the GaN film grown on the nominal flat SiC (0001) substrate where the I I K photoluminescence spectra exhibit the near-bandgap peak (FWHM similar to 25 meV) and the intensity is approximately seven times weaker than that of the vicinal film sample. The redshift of the near-bandgap peak associated with excitons bound to shallow donors is related to the stress caused by both the lattice mismatch and the thermal expansion coefficient difference between GaN and SiC substrates. The measured thermal activation energy of the shallow donor of 33.4 meV is determined by using an Arrhenius plot of the near-bandgap luminescence versus I IT from the slope of the graph at high temperature. The temperature dependence of the FWHM of the near-bandgap luminescence has also been studied. The Raman scattering measurements from the vicinal film reveal that the E-2 phonon peak is strengthened and the A(1)(LO) phonon peak is shifted towards the low-frequency side with enhanced intensity, in comparison to that from the nominal flat film, suggesting a reduction in the density of defects and a lower free carrier concentration in the vicinal GaN film.

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Two-dimensional photonic crystals working in near infrared region are fabricated into silicon-on-insulator wafer by 248-nm deep UV lithography. We present an efficient way to measure the photonic crystal waveguide's light transmission spectra at given polarization states.

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We report the observation of intense spontaneous emission of green light from LiF:F-2:F-3(+) centers in active channel waveguides generated in lithium fluoride crystals by near-infrared femtosecond laser radiation. While irradiating the crystal at room temperature with 405 nm light from a laser diode, yellow and green emission was seen by the naked eye. Stripe waveguides were fabricated by translating the crystal along the irradiated laser pulse, and their guiding properties and fluorescence spectra at 540 nm demonstrated. This single-step process inducing a waveguide structure offers a good prospect for the development of a waveguide laser in bulk LiF crystals.

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Micro Fabry-Perot (F-P) interferometers (MFPIs) are machined in a single-mode fiber (SMF) and a photonic crystal fiber (PCF) by using a near-infrared femtosecond laser, respectively. The strain and temperature characteristics of the two MFPIs with an identical cavity length are investigated and the experimental results show that the strain sensitivity of the PCF-based MFPI is smaller than that of the SMF-based MFPI due to their different waveguide structures, while the two MFPIs have close temperature sensitivities which are much smaller than that of an in-line SMF etalon sensor reported previously. These MFPIs in silica fibers are compact, stable, inexpensive, capable for mass-production and easy fabrication, offering great potentials for wide sensing applications. (c) 2007 Optical Society of America.

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In this paper, polarization properties and propagation characteristics of polymer photonic crystal fibres with elliptical core and non-hexagonal symmetry structure are investigated by using the full vectorial plane wave method. The results how that the birefringence of the fibreis induced by asymmetries of both the cladding and the core. Moreover, by adjusting the non-symmetrical ratio factor of cladding eta from 0.4 to 1 in step 0.1, we find the optimized design parameters f the fibre with high birefringence and limited polarization mode dispersion, operating in a single mode regime at an appropriate wavelength range. The range of wavelength approaches the visible and near-infrared which is consistent with the communication windows of polymer optical fibres.

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A kind of microstructured polymer optical fiber with elliptical core has been fabricated by adopting in-situ chemical polymerization technology and the secondary sleeving draw-stretching technique. Microscope photography demonstrates the clear hole-structure retained in the fiber. Though the holes distortion is visible, initial laser experiment indicates that light can be strongly confined in the elliptical core region, and the mode field is split obviously and presents the multi-mode characteristic. Numerical modeling is carried out for the real fiber with the measured parameters, including the external diameter of 150 pin, the average holes diameter of 3.3 mu m, and the average hole spacing of 6.3 mu m. by using full-vector plane wave method. The guided mode fields of the numerical simulation are consistent with the experiment result. This fiber shows the strong multi-mode and weak birefringence in the visible and near-infrared band, and has possibility for achieving the fiber mode convertors, mode selective couplers and so on.

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近年来,随着近红外领域研究的深入,特别是光通讯工业的发展,迫切需要一大批具有良好发光性质的近红外材料。有机材料由于成本低、工艺简单和结构易调控等优点而备受关注。目前,对近红外有机发光材料的研究主要集中在两大类:一是稀土元素配合物;二是有机离子染料。但由于稀土元素的4f-4f跃迁是宇称禁阻的,其分子的激发需通过配体与中心离子的能量转移,发光效率低。同时有机离子染料由于静电相互作用,分子容易因聚集而导致发光萃灭,其器件结构主要采用主客体掺杂技术,存在着较强的主体材料发光和器件发光效率低等缺点。传统有机非离子型材料则不受上述因素的限制,可得到聚集态下高效的发光效率。本论文通过将电子给体与受体共轭连接,设计并合成了系列非离子型的窄带隙有机小分子,研究了它们在近红外电致发光等器件中的应用,主要工作内容和结果如下: (1)在分子内同时引入电子给体和受体,将它们共轭连接,设计并合成了系列D-π-A-π-D型的有机小分子,利用分子内电荷转移,实现近红外区域的吸收和发射。我们选择三苯胺和芴为电子给体,苯并双噻二唑及其衍生物为电子受体,苯、噻吩和吡咯为连接基团,得到的系列化合物的光谱及电化学性质能在很大的范围内进行调节。化合物的吸收光谱可从600nm至1400nm,发射光谱从900nm至1600nm范围内调节。化合物的带宽可从1.19eV减小到0.56eV。由于分子间的强相互作用,化合物在混合溶剂中可自组装成带状结构。同时该系列化合物在隔绝氧气的环境中有良好的光化学稳定性,可应用于电致发光或光伏器件中。 (2)多层器件结构是提高有机电致发光效率的有效方法,但前提是发光材料最好是可真空蒸镀。我们在前部分工作的基础上,合成了系列热稳定的可蒸镀型有机小分子。通过改变受体及给体结构可调节发光波长及效率。利用“掺杂剂/主体材料的思想”制备的电致发光器件,发光波长覆盖700nm到1500nm的范围,最长中心波长为1115nm。发光波长752nm时,器件最高外量子效率为1.12%。基于化合物IV-5制备的非掺杂器件,发光波长为1080nm,外量子效率为0.28%。该效率比基于有机离子染料的器件提高了近10倍。基于化合物IV-7的器件最大发射波长为1220nm,为迄今为止非掺杂有机电致发光器件中的最长发射波长。以上结果证明,该系列分子是良好的近红外电致发光材料。 (3)我们研究了含苯并双噻二唑分子与常见阴离子的相互作用关系,发现其只对CN-离子和F-离子有响应,而对其它阴离子如Cl , Br , I , AcO , H2PO4 , HSO4 , 和NO3 等则没有任何响应。并且通过将其中噻二唑环换成硝基,可实现对CN-离子和F-离子的区分。化合物V-2可高选择性的检测氰离子,其它离子的存在不会干扰检测信号,包括氟离子。检测信号为外观颜色的改变,可作为显色传感器。化合物V-3可定量检测CN-离子,检测极限为1μM。并且检测信号包括近红外发射的萃灭、可见发射的增强和吸收光谱的改变,多重检测信号可增加检测的可靠性。由于响应信号处于近红外区的生物波段,可应用于生物领域

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光通讯近年来发展迅速,正在从元件向集成发展,迫切需要利于集成的元件。主要的一些光学元件如激光器、放大器等均采用无机材料,连接和集成存在困难。发展易于集成的有机光学元件是目前该领域研发的一个热点。电致变色是一个古老的题目,一般都在可见区,而光通讯波长主要是1300和1550nm,是近红外区。在近红外区的工作刚刚开始,.用于光衰减器的研究已有报道,但还没有达到实际要求,寻找新型的电致变色材料及其适合这些材料的新的器件构型是目前研究的重点。本文研究了三种新的有机近红外电致变色材料及其器件:PEDOT:PSS、Ru星状化合物和酞警噜。本文通过电化学、吸收光谱、X射线衍射、AFM等实验方法和手段表征了样品的本体性质、近红外电致变色,性质和器件性能。结果如下:本论文首先研究了PEDOT:PSS的近红外电致变色性质。实验结果首次表明通过掺杂如Liclo4的电解质可以提高近红外电致变色器件的性能。通过掺杂,褪色时间从30秒缩短到2.8秒,着色时间从9.2秒缩短到2.7秒,变色效率从105cm2/C提高到3llcm2/C。掺杂后薄膜离子导电率提高是器件性能改善的原因。另外还制备了基于不同厚度的PEDOT:PSS薄膜的器件,发现对于一定掺杂浓度有一个最佳的厚度,在这个厚度下器件有较大的调制能力和较小的透过损失。本论文第二部分研究Ru星状化合物。通过对基于Ru星状化合物溶液的动力学的研究,证明了调制能力与溶液浓度和外加电压的关系。之后研究开发了有新构型的近红外电致变色器件,以Ru(II,II)态化合物溶液代替其交联薄膜和电解质层来形成固液型器件,同时改善了氧化钨的制备方法。将器件对1550nm光的调制能力从文献报道的2dB提高到16dB。本论文还首次报道了酞警噜的近红外电致变色性质,发现它既可以作为阳极电致变色材料也可以作为阴极电致变色材料。酞普噜的溶液和薄膜均可用于制备电致变色器件,器件的响应速度分别为23秒和1秒。但因为中性态酞警噜对1300nm和1550nm的光吸收较小,器件的调制能力也较小(-0.3dB)。 论文的最后部分详细阐述了有机光电器件表征系统的搭建及测量方法,包括电调制光的电致变色器件测试系统、光转换为电的有机光电二极管或太阳能电池等光电器件测试系统和电转换为光的有机电致发光二极管的器件测试系统。本论文的结果证明采用新构型可以提高近红外电致变色器件的性能;通过掺杂可以缩短电致变色器件的响应时间和提高其变色效率;同时还首次报道了酞瞥噜的近红外电致变色性质。

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The electronic absorption of EL2 centers has been clarified to be related to the electron acid hole photoionizations, and the transition from its ground state to metastable state, respectively. Under an illumination with a selected photon energy in the near infrared region, these three processes with different optical cross sections will show different kinetics against the illumination time. It has recently been shown that the photosensitivity (measured under 1.25 eV illumination) of the local vibrational mode absorption induced by some deep defect centers in SI-GaAs is a consequence of the electron and hole photoionizations of EL2. This paper directly measures the kinetics of the electronic transition associated with EL2 under 1.25 eV illumination, which implies the expected charge transfer among different charge states of the EL2 center. A calculation based on a simple rate equation model is in good agreement with the experimental results.

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Recent infrared spectroscpic observations of local vibrational mode absorptions have revealed a number of photosensitive centers in semi-insulating GaAs. They include (OVAs) center which has three modes at 730 cm(-1) (A), 715 cm(-1) (B), and 714 cm(-1) (C), respectively, a suggested NH center related to a line at 983 cm(-1) (X(1)), and centers related to hydrogen, such as (H-O) or (H-N) bonds, corresponding to a group of peaks in the region of 2900-3500 cm(-1). The photosensitivity of various local vibration centers was observed to have similar time dependence under near-infrared illumination and was suggested to be due to their charge-state interconversion. Mainly described in this work is the effect of the 1.25-eV illumination. It is confirmed that this photoinduced kinetic process results from both electron capture and hole capture, which are closely related to the photoionization behavior and metastability of the EL2 center.

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A near-infrared single-photon detection system is established by using pigtailed InGaAs/InP avalanche photodiodes. With a 50GHz digital sampling oscilloscope, the function and process of gated-mode (Geiger-mode) single-photon detection are intuitionally demonstrated for the first time. The performance of the detector as a gated-mode single-photon counter at wavelengths of 1310 and 1550nm is investigated. At the operation temperature of 203K,a quantum efficiency of 52% with a dark count probability per gate of 2. 4 * 10~(-3), and a gate pulse repetition rate of 50kHz are obtained at 1550nm. The corresponding parameters are 43% , 8. 5 * 10~(-3), and 200kHz at 238K.

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Using electrochemical deposition, Cu nanowire arrays have been successfully fabricated by home-made polycarbonate ion-track templates. The diameters were well controlled by etching time of templates. The minimum diameter is 15 nm. The morphologies and structures were analyzed by scanning electron microscopy, transmission electron microscopy and X-ray diffraction. The wires prefer [1 1 0] growth direction due to H ions absorption. The optical properties of Cu nanowire arrays are studied by an ultraviolet/visible/near-infrared spectrophotometer. Two extinction peaks were observed in spectra. The optical mechanism is discussed based on surface plasmon resonance