Electric field enhancement in guided-mode resonance filters

Electric fields inside guided-mode resonance filters (GMRFs) may be intensified by resonance effects. The electric field enhancement is investigated in two GMRFs: one is resonant at normal incidence, the other at oblique incidence. It is shown that the two GMRFs exhibit different behaviors in their electric enhancement. Differences between the electric field distributions of the two GMRFs arise because coupling between counterpropagating modes occurs in the first case. It is also shown that the order of the electric field of maximum amplitude can be controlled by modulation of the dielectric constant of the grating.     

Single-layer one-dimensional nonpolarizing guided-mode resonance filters under normal incidence

We demonstrate that properly designed one-dimensional guided-mode resonance filters (GMRFs) with only one grating layer can exhibit a nonpolarizing resonant filtering effect under normal incidence. A sinusoidal profile nonpolarizing GMRF is realized by photoinduced surface-relief grating formation on thin films of polymer-azobenzene complexes and subsequent atomic layer deposition, showing the feasibility of fabrication of such compact GMRFs.     

All-Fiber Dual-Parameter Sensor Based on Cascaded Long Period Fiber Grating Pair Fabricated by Femtosecond Laser and CO2 Laser

An all-fiber dual-parameter sensor based on cascaded long period grating pair fabricated by femtosecond laser and CO₂ laser has been proposed and realized both theoretically and experimentally. The resonant wavelengths of LPFGs are 1557.80 nm and 1590.88 nm. In the strain range of 0–400 με, strain sensitivities are ?7.2 pm/με for C-LPFG and ?1.6 pm/με for F-LPFG. In the temperature range of 30–70°C, temperature sensitivities are ?41.1 pm/°C for C-LPFG and ?21.2 pm/°C for F-LPFG. By analyzing the resonant wavelength characterization, the proposed sensor can be efficiently used for dual-parameters measurement with promising application prospect and great research reference value.     

J/Ψ and Ψ′ production in hadronic Z0 decays

The production of Jψ mesons in Z⁰ decays is studied using 3.6 million hadronic events recorded by the OPAL detector at LEP. The inclusive Z⁰ to Jψ and b-quark to Jψ branching ratios are measured from the total yield of Jψ mesons, identified from their decays into lepton pairs. The Jψ momentum distribution is used to study the fragmentation of b-quarks. The production rate of ψ′ mesons, identified from their decays into a Jψ and a π⁺π^? pair, is measured as well. The following results are obtained: ${Br(Z^{0}?ghtarrow {? J}/?i X)=(3.9pm 0.2pm 0.3)cdot 10^{-3} {? and} ?op Br(Z^0?ghtarrow ?i ^?ime X)=(1.6pm 0.3pm 0.2)cdot 10^{-3}, }$ where the first error is statistical and the second systematic. Finally the Jψ sample is used to reconstruct exclusive b-hadron decays and calculate the corresponding b-hadron branching ratios and masses.     

Analysis of multimode BDK doped POF gratings for temperature sensing

We report a temperature sensor based on a Bragg grating written in a benzil dimethyl ketal (BDK) doped multimode (MM) polymer optical fiber (POF) for the first time to our knowledge. The thermal response was further analyzed in view of theory and experiment. In theory, with the order of the reflected mode increasing from 1st to 60th order, for MM silica fiber Bragg grating (FBG) the temperature sensitivity will increase linearly from 16.2 pm/°C to 17.5 pm/°C, while for MM polymer FBG the temperature sensitivity (absolute value) will increase linearly from ?79.5 pm/°C to ?104.4 pm/°C. In addition, temperature sensitivity of MM polymer FBG exhibits almost 1 order larger mode order dependence than that of MM silica FBG. In experiment, the Bragg wavelength shift will decline linearly as the temperature rises, contrary to that of MM silica FBG. The temperature sensitivity of MM polymer FBG is ranged from ?0.097 nm/°C to ?0.111 nm/°C, more than 8 times that of MM silica FBG, showing great potential used as a temperature sensor.     

Production of orbitally excited charm mesons in semileptonic B decays

A sample of 3.6 million hadronic Z decays recorded between 1991 and 1995 with the ALEPH detector at LEP is used to investigate semileptonic decays of B mesons into final states involving orbitally excited charm mesons. Topological vertex criteria are used to search for decays involving narrow D** states as well as wide D** resonances and non-resonant D(*)π final states. The sum of the branching ratios for these processes is measured to be ${? Br}({?erline {? B}}?ghtarrow {? D}? ?l^{-}{?erline v}) + {? Br}({?erline {? B}}?ghtarrow {? D}^{?t}? ?l^{-}{?erline v})?op =(2.26 pm 0.29({? stat}) pm 0.33({? syst}))%,$which accounts for a significant fraction of the deficit between inclusive measurements and the sum of exclusive semileptonic B decay modes.     

Structural inhomogeneity and piezoelectric enhancement in ZnO nanobelts

In this work, piezoelectricity of individual ZnO nanobelts grown along the [0?1????0] direction is studied using piezoresponse force microscopy (PFM). It is found that the effective piezoelectric coefficient of these NBs, $d_{33}^{\mathrm{eff}}$ , is increasing from 2.7?pm/V at 30?kHz to 44?pm/V at 150?kHz. The results were explained by the Debye model, where structural inhomogeneity in our NBs was shown to be responsible for piezoelectric enhancement.     

A precise measurement of the ${⊼ B}_{d}^{⊼ 0}$ meson lifetime using a new technique

From data recorded by DELPHI between 1991 and 1994, which corresponds to 3.2 million hadronic Z⁰ decays, a measurement of the $?erline {{? B}_d^0}$ meson lifetime, based on the inclusive reconstruction of 3520 ± 150 semileptonic decays of the type $?erline {{? B}_d^0}?ghtarrow {? D}^{?t +}{? ? X} ?l ?erline {v_{?l}},$ has been performed. The result is: $?u ?erline {({? B_d^0})}=1.532 pm 0.041(stat.) pm 0.040(syst.)ps.$. The contribution to the systematic uncertainty which depends on external errors is ±0.015.     

强激光主镜膜厚不均匀性对偏振和光学图像的影响

本文讨论了在特定镀膜室的几何尺寸约束下,一定直径(0.8m)的主反射镜的膜层厚度分布。给出了金属增强型高反射膜系由于不均匀性对光束偏振态的影响;计算了1.06μm主激光和0.5893μm的信标光产生的相位畸变。通过修正设计得到符号相同的相位变化,从而使信标光达到预期目的。     

Nonlinear optical properties of LaCa(4)O(BO(3))(3)

We have grown LaCa(4)O (BO(3))(3) (LaCOB), an isostructural member of GdCa(4)O(BO(3))(3) (GdCOB) family and characterized its nonlinear optical properties. At 1064nm, d(eff) of 0.52+/-0.05 pm /V and an angular sensitivity of 1224+/-184(cm rad)(-1) for type I frequency doubling in LaCOB were determined relative to those of KTiOPO(4) , beta-BaB(2)O(4) , KD(2)PO(4) , LiB(3)O(5) , YCa(4)O(BO(3))(3) (YCOB), and GdCOB. The d(alphabetabeta) and d(gammabetabeta) coefficients of the nonlinear optical tensor for LaCOB, GdCOB, and YCOB were determined to be equivalent within the experimental uncertainty and have values of ?0.26+/-0.04?pm/V and ?1.69+/-0.17?pm /V , respectively. From phase-matching angle measurements at 1064 and 1047nm, we predict that LaCOB is noncritically phase matched at 1042+/-1.5 nm .     

Energy dependence of the differences between the quark and gluon jet fragmentation

Three jet events arising from decays of the Z boson, collected by the DELPHI detector, were used to measure differences in quark and gluon fragmentation. Gluon jets were anti-tagged by identifying b quark jets. Unbiased quark jets came from events with two jets plus one photon. Quark and gluon jet properties in different energy ranges were compared for the first time within the same detector. Quark and gluon jets of nearly the same energy in symmetric three jet event topologies were also compared. Using three independent methods, the average value of the ratio of the mean charged multiplicities of gluon and quark jets is $$< r >=1.241 pm 0.015 (stat.)pm 0.025 (syst.).$$ Gluon jets are broader and produce fragments with a softer energy spectrum than quark jets of equivalent energy. The string effect has been observed in fully symmetric three jet events. The measured ratio R_γ of the charged particle flow in the qq? inter-jet region of the qq?g and qq?γ samples agrees with the perturbative QCD expectation. The dependence of the mean charged multiplicity on the hadronic center-of-mass energy was analysed in photon plus n-jet events. The value for α_s(M _Z) determined from these data using a QCD prediction with corrections at leading and next-to-leading order is $$←pha_s(M_Z)=0.116pm 0.003 (stat.)pm 03009 (syst.).$$     

Strain and temperature discrimination technique by use of A FBG written in erbium doped fiber

We propose and demonstrate strain and temperature discrimination technique using a single fiber Bragg grating (FBG) written in the core of an erbium doped fiber. We observed that amplified spontaneous emission power varying linearly from the erbium doped fiber with temperature which determines temperature changes and strain is estimated by subtracting the wavelength shift due to temperature change, from the measured shift corresponding to the dip in the transmission spectrum of the FBG. A simple and compact FBG sensor is presented with improved rms errors of 21.2 μ? and 1 °C over ranges of 0–800 μ? and 40–95 °C, respectively. The sensor is shown to have strain and temperature sensitivity of 0.8 pm/μ? and 12 pm/°C.     

基于紫外刻写相移光栅的温度应力同时测量传感器

传统光纤光栅传感器存在温度应力交叉敏感的问题,无法同时测量被测物体的温度应力变化情况。针对这种情况,提出一种新型的利用紫外光刻写相移光栅的方法,在刻写光栅前用电极放电的方法去除掉极小一段光纤的光敏性,使光纤原有的均匀周期分布状态被破坏,从而形成相移光栅,并对其进行理论分析。此种相移光栅的透射光谱存在2个明显的谐振峰,利用2个峰对温度和应变灵敏度不同的性质,可以通过建立解调矩阵来实现温度与应力的同时测量。实验结果表明:利用此种方法制成的相移布拉格光栅能够较为精确地实现温度、应力的同时测量,所制作的传感器温度灵敏度最高可达9.51 pm/℃,灵敏度方差低于2.125×10?7,应变灵敏度最高可达0.767 pm/με,灵敏度方差低于2.156×10?10。     

Controlling on Entangled Decoherence by the Interaction Model Between Qubit and Environment

The entangling evolution of the coupled qubits interacting with non-Markov environment is investigated in terms of concurrence. The results show that the entanglement of quantum systems depends on not only the initial state of system but also the coupling ways between qubit and environment. It shows that: (1) when the system is initially in ( | 00 ?±| 11 ?)/?2( | 00 \rangle\pm| 11 \rangle)/\sqrt{2} state or in the mixed state which is produced by the state, if we can control the coupling between the qubits and the environment in a asymmetrical state, we can make the quantum system always in the entangled state. (2) For an initial state ( | 01 ?±| 10 ?)/?2( | 01 \rangle\pm| 10 \rangle)/\sqrt{2} or in its mixed state, in contrast, there will not be entangled death under the symmetric coupling. We also find that, in ( | 01 ?±| 10?)/?2( | 01 \rangle\pm| 10\rangle)/\sqrt{2} or in its mixed state, the stronger the interaction between qubits is, the better to struggle against entanglement sudden death is.     

Measurement of $D_s ^+$ meson production in Z decays and of the ${⋏r B}_s ^0$ lifetime

$D_s ^+$ mesons produced in Z⁰ → bb? events were separated from the Z⁰ → cc? component using a lifetime tag. Using a sample of 1.5 million hadronic Z decays collected with the Aleph detector the ${?r B}_s ^0$ and $D_s ^+$ yields have been measured: $$?trix {B(b?ghtarrow {?r B}_s ^0)B({?r B}_s ^0?ghtarrow D_s ^+)=0.088pm 0.020(? stat.)? pm 0.020(? syst.)? B(c?ghtarrow D_s ^+)=0.128pm 0.019(? stat.)_{-0.016} ^{+0.019}(? syst.)}$$ The ${?r B}_s ^0$ lifetime was measured in a ${?r B}_s ^0$ enriched sample reconstructing the decay length from the vertex of the $D_s ^+$ with a hadron from the ${?r B}_s ^0$ decay. The result obtained is: $${?u_B}_s=1.61_{-0.29} ^{+0.30}(? stat.)_{-0.16} ^{+0.18}(? syst.) {? ps.}$$     

Laser-induced,second-order optical susceptibilities of YAB:Cr3+ single crystals

Complex temperature studies of optically stimulated second harmonic generation (SHG) at 1064?nm for pulsed 10?ns Nd:YAG laser radiation under illumination of two coherent laser beams (at 1064?nm and its 532?nm second harmonic) were carried out by means of the Maker fringe method. The bicolour coherent process allowed detection of some additionally induced non-centrosymmetry. The effect was studied at different temperatures and experimental geometries in YAB:Cr³⁺ single crystals. We found that Cr³⁺ ions play a principal role in the observed effects. The output of optically stimulated SHG was generally non-spherical in the sequence profile, contrary to the traditional non-stimulated SHG. Moreover, we also established that the optimal conditions for obtaining SHG corresponded to the fundamental/writing beam intensities ratio 6:1. A specially performed control of the photo-thermal sample heating showed that the increase of temperature did not exceed 1.2?K, which allowed the influence of photo-thermal heating to be neglected. The optimal input–output laser geometry corresponded to s-p polarisation and to the angle of about 32° between the photo-inducing and fundamental beams. Additionally in the studied temperature range (77–295?K) there was observed an enhancement of the output second-order susceptibilities from 0.72?pm/V up to 1.02?pm/V.     

Optical fiber strain and temperature sensor based on an in-line Mach–Zehnder interferometer using thin-core fiber

We propose and demonstrate a fiber in-line Mach–Zehnder interferometer using thin-core fibers. This in-line interferometer is composed of a short section of thin-core fiber inserted between two single mode fibers (SMF), and demonstrated as a strain and temperature sensor in this study. A strain sensitivity of ?1.83 pm/με with a measurement range of 0?2000 με, and the temperature sensitivity of ?72.89 pm/°C with a temperature variation of 50 °C are achieved. We also discussed that the influence of strain and temperature change on the relative power ratios among the excited cladding modes in thin-core fibers.     

Optimization of a guided-mode resonance filter by varying the thickness of the buffer layer

In this Letter, we demonstrate that by adjusting the thickness of the buffer layer, the optical responses of a guided-mode resonance filter(GMRF) can be improved for sensor applications. The GMRF is fabricated using a replica molding with a plastic substrate and a UV-curable polymer. SiO_2 buffer layers of different thicknesses are deposited before the waveguide-layer deposition. The sensitivity of the GMRFs decreases slightly with increasing SiO_2 layer thickness. By contrast, the full width at half-maximum reduces substantially with increasing SiO_2 layer thickness, resulting in the improvement of the overall figure of merit.     

Design of guided mode resonant filters for authentication applications through azimuthal angles varying

Guided mode resonant filters (GMRFs) for authentication application with low sideband reflection at O° and 90° azimuthal angles were designed. Using rigorous coupled-wave analysis, the diffractive characteristics of this kind device with different illumination angles, groove depths, and thicknesses of cover SiO<,2> layer were investigated. The structure of GMRF which satisfies the requirements for authentication applications was obtained. Illuminated at 30° for a definite polarization mode, the filter presents symmetrical reflectance shape, low sideband reflectance, two separate reflectance peaks, and definite full-width at half-maximum (FWHM) at O° and 90° azimuthal angles.     

基于马赫-曾德干涉的全光纤双参量传感器

提出一种基于S形-错位结构的全光纤马赫-曾德干涉仪（MZI）双参量传感器。该传感结构是采用单模光纤在光纤熔接机中通过简单的放电和熔接等步骤制备而成。顺时针扭转时, 传感器的传输光谱向短波长方向偏移; 逆时针扭转, 向长波长方向偏移。对传感器的实验研究结果表明,该传感器在光纤横截面上顺时针和逆时针两个旋转方向上的扭曲传感灵敏度分别为?223 pm/(rad·cm?1), 140 pm/(rad·cm?1),且可实现扭转方向的判别,在一定应变范围内的应变灵敏度为0.145×106 dB/ε(这里ε为应变),且温度交叉灵敏度极小,可忽略不计。因此,这种基于单模光纤的纤芯-包层MZI双参量传感器具有传感灵敏度高,体积小巧,工艺简单,成本低廉且可判别扭转方向的优点,有望成为众多双参量测量操作中良好的候选仪器之一。