The impact of the air-fluorescence yield on the reconstructed shower parameters of ultra-high energy cosmic rays.

An accurate knowledge of the fluorescence yield and its dependence on atmospheric properties such as pressure, temperature or humidity is essential to obtain a reliable measurement of the primary energy of cosmic rays in experiments using the fluorescence technique. In this work, several sets of fluorescence yield data (i.e. absolute value and quenching parameters) are described and compared. A simple procedure to study the effect of the assumed fluorescence yield on the reconstructed shower parameters (energy and shower maximum depth) as a function of the primary features has been developed. As an application, the effect of water vapor and temperature dependence of the collisional cross section on the fluorescence yield and its impact on the reconstruction of primary energy and shower maximum depth has been studied. Published by Elsevier B.V.

盐胁迫对螺旋藻光合作用影响的研究

盐胁迫是限制高等植物和藻类生长和产量的主要环境因子之一。PSII对环境胁迫的响应被认为是光合作用适应逆境过程中最重要的一个环节。尽管盐胁迫对PSII的影响已进行了大量的研究，但有关盐胁迫对PSII作用方式和位点的研究仍存在着争议。我们主要研究了盐胁迫对螺旋藻PSII结构和功能的影响，以探讨盐胁迫对PSII的作用方式和位点以及该藻细胞PSII对盐胁迫的适应机理。主要研究结果如下： 1． 用0、0.2、0.4、0.6、0.8M NaCl处理螺旋藻细胞12小时。随盐浓度的增加，螺旋藻细胞的Chla、carotenoid、PC、APC及蛋白含量均呈下降趋势，说明盐胁迫抑制了上述色素及蛋白的合成或加速了它们的降解，从而影响了螺旋藻的光合作用。 2． 随盐浓度的增加，螺旋藻细胞光合放氧活性和PS II电子传递活性显著降低，表明盐胁迫引起藻细胞PS II活性的下降。 3． 通过放氧活性、热致发光（TL）、多相荧光瞬态上升动力学曲线的测定以及Western 杂交，来探讨盐胁迫对螺旋藻细胞PS II供体侧电子传递及OEC33蛋白含量的影响。结果显示：随盐浓度的增加，螺旋藻细胞光合放氧活性和PS II电子传递活性下降;TL B-band和Q-band强度降低，在0-0.6M NaCl下，B-band的周期性振荡清楚，最大值出现在第二次和第六次闪光，而在0.8M NaCl时，S态振荡基本上消失，S 态氧化还原循环受阻;Fm， J、I和P相荧光水平降低。以上结果都表明盐胁迫使PS II的放氧侧受损伤。且随盐浓度的增加，盐分引起螺旋藻细胞外周蛋白OEC33的降解，在蓝藻中首次提出放氧机构的S态循环受阻，放氧活性降低。 4． 通过OJIP曲线的测定以及JIP-test、闪光诱导的可变荧光衰减动力学、热致发光（TL）的分析，我们研究了盐胁迫对螺旋藻细胞PS II受体侧的影响。结果显示： JIP-test的参数Ψo和φEo随盐浓度的增加而下降,显示QA-到QB 电子传递受阻;可变荧光衰减动力学快相组分半衰期延长，所占总可变荧光百分比下降，表明QA-到QB 电子转移变慢，中相组分半衰期延长、所占百分比下降，说明空的QB位点对PQ的结合减慢，有可能PQ分子对QB位点的结合能力下降;TL B-band和Q-band的峰温度出现了位移，可能QA、QB的氧化还原电势发生了改变。以上结果表明，盐胁迫伤害了PSII受体侧的电子传递。 5． 首次运用闪光诱导下的叶绿素荧光上升及其衰减动力学来研究盐胁迫对PS II受体侧的影响。 6． 盐胁迫下，PS II供体侧和受体侧电子传递受抑制，有活性的PSII反应中心数量下降，说明盐胁迫对螺旋藻细胞PSII的伤害也可能是多位点的作用方式。此外，盐胁迫下，藻细胞放氧活性的下降快于受体侧QA 到QB电子传递所占百分比的下降，有可能PS II放氧侧先受损伤，然后是反应中心和受体侧。上述结果表明盐胁迫下PSII活性的降低是由于PSII供体侧和受体侧电子传递的抑制，有活性的PSII反应中心的减少。 7． 借助螺旋藻类囊体膜的Western杂交分析，来研究盐胁迫对螺旋藻类囊体膜PSII相关蛋白的影响。结果表明，上述PSII活性的抑制是由于类囊体膜蛋白的损失。主要与PSII反应中心CP43、CP47和OEC33蛋白含量的下降有关。 8． PS II机构对盐胁迫的适应涉及以下几个方面：降低吸收横截面，（PC/chla，APC/chla比值的降低）;光系统II光化学反应的改变，通过关闭的PS II反应中心比例的增加，使得PS II机构免于过多激发能的伤害而得以保护;提高了剩余的有活性反应中心的耗能效率（DIo/RC增加）;保持有活性反应中心高的激发能转化效率，比如，TRo/RC保持不变;另外，随盐浓度的增加，由藻胆体向光系统I的能量传递增加，避免过量激发能对 PSII的伤害，使螺旋藻细胞适应盐胁迫环境。

高温胁迫对螺旋藻光系统II影响的研究

高温胁迫是限制高等植物和藻类生长和产量的主要环境因子之一。光系统II（PSII）对环境胁迫的响应被认为是光合作用适应逆境过程中最重要的一个环节。高温胁迫对螺旋藻PSII的研究相对较少，对PSII受体侧的研究更加少了。我们借助热致发光及QA-再氧化动力学，这两种检测完整光合生物PSII供体侧和受体侧电子传递的有效、简单、无损伤的方法，为高温胁迫如何影响供体侧和受体侧的电子传递提供更直接的依据，获得高温胁迫对PSII功能影响的更精确的消息。另外，有关螺旋藻在高温胁迫下的能量传递过程研究较少，希望在荧光光谱研究的结果上探求其对高温胁迫的适应机理。主要研究结果如下： 1.高温胁迫抑制螺旋藻PS II的活性， PSII原初光能转化效率Fv/Fm随处理温度的提高而下降。高温去除后Fv/Fm可以得到部分恢复（5-15%）。 2.高温胁迫对闪光诱导的可变荧光衰减动力学有显著影响，分别代表QA-到QB 的直接电子传递和PQ分子扩散到空的QB位点后QA-到QB电子传递的快相(半衰期160 ms)和中相(半衰期2 ms)占整个可变荧光的比例，随处理温度的升高显著降低，而代表S2QA- 电荷重组的慢相（半衰期约4s）显著增加。显示高温导致QA到QB的电子传递以及PQ与QB位点的结合受阻，从而促进了QA-与放氧复合体S2态的重组过程。同时我们发现，经过5分钟的恢复，这些光系统II还原侧电子传递的功能抑制能够大部分得到恢复，显示高温胁迫对受体侧电子传递的影响具有可逆性。 3. 通过采用77K低温荧光光谱等手段，我们研究了高温胁迫对螺旋藻细胞光合能量传递的影响。研究显示，高温胁迫对580nm和436nm激发的低温荧光光谱都有显著影响。高温胁迫对PS I的发射峰F725和F751没有显著影响，显示高温没有影响藻胆体到光系统I的激发能传递。而高温胁迫引起了PBS对PS II荧光发射比值的上升，说明高温抑制了藻胆体到光系统II之间的激发能传递。但藻蓝蛋白的发射峰643nm在高温处理后基本没有变化，显示高温抑制PBS到PS II的能量传递不是由于藻蓝蛋白到别藻蓝蛋白之间的能量传递受阻造成的。结果还显示，高温胁迫对藻胆体到光系统II能量传递的抑制也不是由于藻胆体与光系统II发生分离，而是抑制了别藻蓝蛋白到CP43和CP47的能量传递，原因可能是由于藻胆体内部结构的改变引起的。 ４.热致发光（TL）和荧光衰减动力学的测定和分析结果显示，高温胁迫改变了S2QA-和S2QB-重组体的稳定性，其中S2QA-的稳定性降低，S2QB-的稳定性升高。根据具有异质性的TL信号，我们推测有活性PSII中有可能存在对高温胁迫敏感度不同的两种亚基，它们具有不同的QB/QB-氧化还原势能。当高温胁迫造成相当数量的反应中心失活，QA到QB正常的电子传递受阻时，光系统有可能通过保存更多的具有较高能量的反应中心亚基，达到促进QA到QB的电子传递的目的。 5. OJIP荧光瞬态上升曲线在高温胁迫后出现标志性K峰，说明螺旋藻的放氧复合物受到伤害，放氧S态引起的多次闪光下的TL振荡，显示这个高温处理对S1→S2的转变没有影响，却抑制了S2→S3的转变，这同OJIP荧光瞬态上升曲线的结果相一致，说明高温对螺旋藻放氧复合体造成了伤害。

High quantum fluorescence yield of Er3+ at 1.5 mu m in an Yb3+, Ce3+-codoped CaF2 crystal

For the first time, a quaternary doping system of Er3+, Yb3+, Ce3+, Na+:CaF2 single crystal was demonstrated to have high fluorescence yield in the eye-safe 1.5 mu m region under 980 nm laser diode pumping, with relatively broad and flat gain curves. A simplified model was established to illustrate the effect of Ce3+ on the branching ratio for the Er3+4I11/2 -> I-4(13/2) transition. With 0.2-at.% Er3+ and 2.0-at.% Ce3+ in the quaternary-doped CaF2 crystal, the branching ratio was estimated to be improved more than 40 times by the deactivating effect of Ce3+ on the Er3+ 4I11/2 level. The quaternary-doped CaF2, system shows great potential to achieve high laser performance in the 1.5 mu m region. (c) 2006 Elsevier B.V. All rights reserved.

Localization of the mechanism of pH-dependent non- photochemical fluorescence quenching in thylakoid membranes

Higher plants have evolved a well-conserved set of photoprotective mechanisms, collectively designated Non-Photochemical Quenching of chlorophyll fluorescence (qN), to deal with the inhibitory absorption of excess light energy by the photosystems. Their main contribution originates from safe thermal deactivation of excited states promoted by a highly-energized thylakoid membrane, detected via lumen acidification. The precise origins of this energy- or LlpH-dependent quenching (qE), arising from either decreased energy transfer efficiency in PSII antennae (~ Young & Frank, 1996; Gilmore & Yamamoto, 1992; Ruban et aI., 1992), from alternative electron transfer pathways in PSII reaction centres (~ Schreiber & Neubauer, 1990; Thompson &Brudvig, 1988; Klimov et aI., 1977), or from both (Wagner et aI., 1996; Walters & Horton, 1993), are a source of considerable controversy. In this study, the origins of qE were investigated in spinach thylakoids using a combination of fluorescence spectroscopic techniques: Pulse Amplitude Modulated (PAM) fluorimetry, pump-probe fluorimetry for the measurement of PSII absorption crosssections, and picosecond fluorescence decay curves fit to a kinetic model for PSII. Quenching by qE (,..,600/0 of maximal fluorescence, Fm) was light-induced in circulating samples and the resulting pH gradient maintained during a dark delay by the lumenacidifying capabilities of thylakoid membrane H+ ATPases. Results for qE were compared to those for the addition of a known antenna quencher, 5-hydroxy-1,4naphthoquinone (5-0H-NQ), titrated to achieve the same degree of Fm quenching as for qE. Quenching of the minimal fluorescence yield, F0' was clear (8 to 130/0) during formation of qE, indicative of classical antenna quenching (Butler, 1984), although the degree was significantly less than that achieved by addition of 5-0H-NQ. Although qE induction resulted in an overall increase in absorption cross-section, unlike the decrease expected for antenna quenchers like the quinone, a larger increase in crosssection was observed when qE induction was attempted in thylakoids with collapsed pH gradients (uncoupled by nigericin), in the absence of xanthophyll cycle operation (inhibited by DTT), or in the absence of quenching (LlpH not maintained in the dark due to omission of ATP). Fluorescence decay curves exhibited a similar disparity between qE-quenched and 5-0H-NQ-quenched thylakoids, although both sets showed accelerated kinetics in the fastest decay components at both F0 and Fm. In addition, the kinetics of dark-adapted thylakoids were nearly identical to those in qEquenched samples at F0' both accelerated in comparison with thylakoids in which the redox poise of the Oxygen-Evolving Complex was randomized by exposure to low levels of background light (which allowed appropriate comparison with F0 yields from quenched samples). When modelled with the Reversible Radical Pair model for PSII (Schatz et aI., 1988), quinone quenching could be sufficiently described by increasing only the rate constant for decay in the antenna (as in Vasil'ev et aI., 1998), whereas modelling of data from qE-quenched thylakoids required changes in both the antenna rate constant and in rate constants for the reaction centre. The clear differences between qE and 5-0H-NQ quenching demonstrated that qE could not have its origins in the antenna alone, but is rather accompanied by reaction centre quenching. Defined mechanisms of reaction centre quenching are discussed, also in relation to the observed post-quenching depression in Fm associated with photoinhibition.

Measurement of the absolute fluorescence quantum yield of rhodamine B solution using a dual-beam thermal lens technique

The dual-beam thermal lens technique has been found to be very effective for the measurement of fluorescence quantum yields of dye solutions. The concentration-dependence of the quantum yield of rhodamine B in methanol is studied here using this technique. The observed results are in line with the conclusion that the reduction in the quantum yield in the quenching region is essentially due to the non-radiative relaxation of the absorbed energy. The thermal lens has been found to become abberated above 40 mW of pump laser power. This low value for the upper limit of pump power is due to the fact that the medium is a resonantly absorbing one.

Comparison of available measurements of the absolute air-fluorescence yield and determination of its global average value

Experimental results of the absolute air-fluorescence yield are given very often in different units (photons/MeV or photons/m) and for different wavelength intervals. In this work we present a comparison of available results normalized to its value in photons/MeV for the 337 nm band at 1013 hPa and 293 K. The conversion of photons/m to photons/MeV requires an accurate determination of the energy deposited by the electrons in the field of view of the experimental set-up. We have calculated the energy deposition for each experiment by means of a detailed Monte Carlo simulation and the results have been compared with those assumed or calculated by the authors. As a result, corrections to the reported fluorescence yields are proposed. These corrections improve the compatibility between measurements in such a way that a reliable average value with uncertainty at the level of 5% is obtained.

Investigation on nonradiative decay of the (Er3+I13/2)-I-4 -> I-4(15/2) transition in different tellurite glass matrix

Three kinds of Er3+-doped tellurite glasses with different hydroxyl groups are prepared by the conventional melt-quenching method. Infrared spectra are measured to estimate the exact content of OH- groups in samples. The maximum phonon energy in glasses are obtained by measuring the Raman scattering spectra. The strength parameters Omega(t) (t = 2, 4, 6) for all the samples are calculated and compared. The nonradiative decay rate of the Er3+ I-4(13/2) -> I-4(15/2) transition are calculated for the glass samples with different phonon energy and OH- group contents. Finally, the effect of OH- groups on fluorescence decay rate of Er3+ is analysed, the constant KOH-Er Of TWN, TZPL and TZL glasses are calculated to be 9.2 x 10(-19) cm(4)s(-1), 5.9 x 10(-19) cm(4)s(-1), and 3.5 x 10(-19) cm(4)s(-1), respectively.

Effect of hydroxyl groups on nonradiative decay of Er3+: I-4(13/2)-> I-4(15/2) transition in zinc tellurite glasses

A series of zinc tellurite glasses of 75TeO(2)-20ZnO-(5-x)La2O3-xEr(2)O(3) (x=0.02, 0.05, and 0.1 mol%) with the different hydroxl groups were prepared by the conventional melt-quenching method. Infrared spectra were measured in order to estimate the exact content of OH- groups in samples. The observed increase of the fluorescence lifetime with the oxygen bubbling time has been related to the reduction in the OH- content concentration as evidenced by IR transmission spectra. Various nonradiative decay rates from I-4(13/2) of Er3+ with. the change of OH content were determined from the fluorescence lifetime and radiative decay rates were calculated on the basis of Judd-Ofelt theory. (c) 2005 Elsevier B.V. All rights reserved.

STUDY ON THE COMPLEXATION OF ACENAPHTHENE AND FLUORANTHENE WITH CYCLODEXTRINS BY MEANS OF TIME-RESOLVED FLUORESCENCE TECHNIQUE

The complexation of acenaphthene and fluoranthene with beta-cyclodextrin (CD) in aqueous solutions in the presence and absence of ethanol was investigated by means of the time-resolved fluorescence technique. The appearance of a longer lifetime component and the increase of its fraction relative to that of the shorter lifetime component with increasing CD concentration demonstrate the formation of inclusion complex between the guest molecule and CD. The formation constants for complexation were derived from the pre-exponential factor A(i) of fluorescence decay curves. The presence of ethanol in the reaction systems enhanced the inclusion to a large extent.

Solute effects on the production and decay of primary species in the flash photolysis of indole

Maximum production rates ofs and decay kinetics for the hydrated electron, the indolyl neutral radical and the indole triplet state have been obtained in the microsecond, broadband (X > 260 nm) flash photolysis of helium-saturated, neutral aqueous solutions of indole, in the absence and in the presence of the solutes NaBr, BaCl2*2H20 and CdSCV Fluorescence spectra and fluorescence lifetimes have also been obtained in the absence and in the presence of the above solutes, The hydrated electron is produced monophotonically and biphotonically at an apparent maximum rate which is increased by BaCl2*2H20 and decreased by NaBr and CdSOif. The neutral indolyl radical may be produced monophotonically and biphotonically or strictly monophotonically at an apparent maximum rate which is increased by NaBr and CdSO^ and is unaffected by BaCl2*2H20. The indole triplet state is produced monophotonically at a maximum rate which is increased by all solutes. The hydrated electron decays by pseudo first order processes, the neutral indolyl radical decays by second order recombination and the indole triplet state decays by combined first and second order processes. Hydrated electrons are shown to react with H , H2O, indole, Na and Cd"*""1"". No evidence has been found for the reaction of hydrated electrons with Ba . The specific rate of second order neutral indolyl radical recombination is unaffected by NaBr and BaCl2*2H20, and is increased by CdSO^. Specific rates for both first and second order triplet state decay processes are increased by all solutes. While NaBr greatly reduced the fluorescence lifetime and emission band intensity, BaCl2*2H20 and CdSO^ had no effect on these parameters. It is suggested that in solute-free solutions and in those containing BaCl2*2H20 and CdSO^, direct excitation occurs to CTTS states as well as to first excited singlet states. It is further suggested that in solutions containing NaBr, direct excitation to first excited singlet states predominates. This difference serves to explain increased indole triplet state production (by ISC from CTTS states) and unchanged fluorescence lifetimes and emission band intensities in the presence of BaCl2*2H20 and CdSOt^., and increased indole triplet state production (by ISC from S^ states) and decreased fluorescence lifetime and emission band intensity in the presence of NaBr. Evidence is presented for (a) very rapid (tx ^ 1 us) processes involving reactions of the hydrated electron with Na and Cd which compete with the reformation of indole by hydrated electron-indole radical cation recombination, and (b) first and second order indole triplet decay processes involving the conversion of first excited triplet states to vibrationally excited ground singlet states.

Fluorescence Studies of Photosystem II Fluorescence Quenching During Desiccation

Poikilohydric organisms have developed mechanisms to protect their photosynthetic machinery during times of desiccation. In hydrated conditions nonphotochemical quenching (NPQ) mechanisms are able to safely dissipate excess excitation energy as heat, but mechanisms of NPQ associated with desiccation tolerance are still largely unclear. In the lichen Parmelia sulcata, photosystem protection has been associated with an energy quenching energetically coupled to PSII and characterized by a fast-fluorescence decay lifetime, and long-wavelength emission. The present study compares the relative ability of green algae and lichens to recover photosynthetic activity after periods of desiccation using steady state fluorescence emission spectroscopy, and picosecond time-resolved fluorescence decay measurements. It was determined that desiccation induced quenching involves an antenna quenching mechanism with similar characteristics appearing in both P. sulcata and green algae. Algae isolated from lichens suggest symbiosis in the lichen appears to enhance this naturally occurring phenomenon and provide greater protection during desiccation.

Pulsed Photoacoustic Determination of Absolute Fluorescent Quantum Yield of the Laser Dye Rhodamine B

Pulsed photoacoustic technique which is found to be a very convenient and accurate method, is used for the determination of absolute fluorescence quantum yield of laser dye rhodamine B. Concentration and power dependence of quantum yield of rhodamine B in methanol for excitation at 532 nm is reported here. Results show that a rapid decrease in quantum yield as the concentration is increased and finally it reaches the limit corresponding to fluorescence quenching.

Double-autoionization decay of resonantly excited single-electron states

Perturbation theory in the lowest non-vanishing order in interelectron interaction has been applied to the theoretical investigation of double-ionization decays of resonantly excited single-electron states. The formulae for the transition probabilities were derived in the LS coupling scheme, and the orbital angular momentum and spin selection rules were obtained. In addition to the formulae, which are exact in this order, three approximate expressions, which correspond to illustrative model mechanisms of the transition, were derived as limiting cases of the exact ones. Numerical results were obtained for the decay of the resonantly excited Kr 1 3d^{-1}5p[^1P] state which demonstrated quite clearly the important role of the interelectron interaction in double-ionization processes. On the other hand, the results obtained show that low-energy electrons can appear in the photoelectron spectrum below the ionization threshold of the 3d shell. As a function of the photon frequency, the yield of these low-energy electrons is strongly amplified by the resonant transition of the 3d electron to 5p (or to other discrete levels), acting as an intermediate state, when the photon frequency approaches that of the transition.

The use of pulse amplitude modulated fluorescence techniques for metal toxicity assessment in fluvial biofilms

Metal pollution in rivers is in great concern with human activities in the fluvial watershed. This thesis aims to investigate the potential use of chl-a fluorescence parameters as biomarkers of metal toxicity, and to find cause-effect relationships between metal exposures, other environmental factor (i.e. light), and functional and structural biofilm responses. This thesis demonstrates that the use of chl-a fluorescence parameters allows detect early effects on biofilms caused by zinc toxicity, both in the laboratory as in polluted rivers. In microcosm experiments, the use of chl-a fluorescence parameters allows evaluates structural changes on photosynthetic apparatus and in algal groups’ composition of biofilms long-term exposed to zinc. In order to evaluate the effects of chronic metal pollution in rivers, it is recommended the use of biofilm translocation experiments and the use of a multi-biomarker approach.