土壤扩蓄增容肥对土壤养分含量及小麦产量影响的试验研究

本研究采用大田试验,分析了秸秆配方和废料配方两种土壤扩蓄增容肥对冬小麦生育期土壤有机质、主要速效养分和产量的影响。试验采用4因素(品种A、秸秆配方B、建筑垃圾配方C、灌水D)3水平正交试验设计。结果表明:施加土壤扩蓄增容肥可以有效提高土壤有机质含量达3.84g/kg;在节水条件下,能明显提高土壤速效养分的含量,增加了小麦对养分的吸收量,并优化了小麦对氮、磷、钾养分的吸收比例;并且施加土壤扩蓄增容肥较对照产量提高15%,且秸秆配方在各方面的效果均优于废料配方。

用侧向外延生长法降低立方相GaN中的层错密度

尝试用侧向外延（ELOG）方法来降低立方相GaN中的层错密度。侧向外延是在SiO_2/GaN/GaAs图像形底上进行的，对生长所得的立方相GaN外延层用扫描电子显微镜（SEM）和透射电子显微镜（TEM）进行了观察和分析，TEM的平面像表明经过ELOG方法生长后，立方相GaN外延层中的层错密度由侧向外延生长前的5 * 10~9cm~(-2)降低至生长后的6 * 10~8cm~(-2)。双晶X射线衍射（DCXRD）测量给出侧向外延前后外延层ω扫描（002）衍射摇摆曲线的半高宽（FWHM）分别为33’和17.8’，表明晶体质量有了较大改善。对立方相GaN侧向外延过程中层错减少的机制进行了讨论。

铕离子注入氧化硅膜光发射的研究

采用铕离子注入热生长SiO_2薄膜的方法，获得掺杂剂量为10~(14) cm~(-2)及10~(15)cm~(-2)的SiO_2:Eu~(3+)硅基复合膜，研究了该薄膜的光致发光退火特性。经1000℃退火后观察到Eu~(3+)的红光发射。在1200℃下氮气中退火观察到Eu~(2+)450 nm的强光发射。讨论了Eu~(3+)向Eu~(2+)的转变。

不同温度下氦离子辐照316L不锈钢氦泡形成的研究

本工作用2.5MeV的~4He~+分别在室温、500 ℃和600 ℃对经过固溶和冷扎处理的316L不锈钢进行了辐照，辐照剂量为2.7 × 10~(17)ions／cm~2，剂量率在3.6 × 10~(11) - 2.6 × 10~(12)ions／cm~2·s之间。用扫描电镜（SEM）观察样品表面形貌的变化，发现600 ℃时，辐照样品的表面出现许多形状不规则的小坑和类似颗粒的东西。用透射电镜（TEM）结合横截面制样技术观察样品内部氦泡的特征，发现室温和500 ℃下氦泡呈圆形，在600 ℃下氦泡呈多面体形状。温度由室温上升到500 ℃，氦泡的大小、数密度的变化比较小，当温度上升到600 ℃，氦泡直径迅速增大、数密度减小，估计在500 ℃和600 ℃之间存在一个氦泡演变转折点。对室温和600 ℃辐照样品中氦泡大小、数密度随深度的变化做定量测量，发现室温下氦泡的形核、长大主要依赖于氦原子的沉积浓度，而600 ℃下氦泡的形核、长大主要依赖于氦引进过程中产生的离位损伤（dpa）。另外，不同晶界处氦泡的特征也不同，大角晶界处氦泡优先生长；小角晶界处不存在氦泡的优先生长。在同一温度下，CW样品中氦泡的数密度比SA样品中氦泡的数密度大、直径小，对应氦泡产生的肿胀比SA样品的小

盘式吸渗仪测定土壤导水率的两种新方法

应用盘式吸渗仪测定田间土壤导水率具有快速简单的优点,但是测定结果的计算处理比较繁琐,寻求简单的计算方法是广泛应用盘式吸渗仪的关键问题。该文改变盘式吸渗仪测定土壤导水率的三维入渗过程为一维入渗过程,简化了测定结果的计算处理。结果显示:两种不同的一维入渗过程达到的稳定入渗率和导水率之间有很好的线性关系,但是三维过程计算的导水率大于一维过程。双套盘吸渗仪一维过程计算导水率与稳定入渗率一致性较好,但是和三维稳态、瞬态方法计算结果之间差异明显,因此在应用这些方法时需要适当调整参数,建议使用双套盘吸渗仪快速测定田间土壤导水率。

Estimating the flow rate capacity of an overturned rail carriage end exit in the presence of smoke

While incidents requiring the rapid egress of passengers from trains are infrequent, perhaps the most challenging scenario for passengers involves the evacuation from an overturned carriage subjected to fire. In this paper we attempt to estimate the flow rate capacity of an overturned rail carriage end exit. This was achieved through two full-scale evacuation experiments, in one of which the participants were subjected to non-toxic smoke. The experiments were conducted as part of a pilot study into evacuation from rail carriages. In reviewing the experimental results, it should be noted that only a single run of each trial was undertaken with a limited — though varied — population. As a result it is not possible to test the statistical significance of the evacuation times quoted and so the results should be treated as indicative rather than definitive. The carriage used in the experiments was a standard class Mark IID which, while an old carriage design, shares many features with those carriages commonly found on the British rail network. In the evacuation involving smoke, the carriage end exit was found to achieve an average flow rate capacity of approximately 5.0 persons/min. The average flow rate capacity of the exit without smoke was found to be approximately 9.2 persons/min. It was noted that the presence of smoke tended to reduce significantly the exit flow rate. Due to the nature of the experimental conditions, these flow rates are considered optimistic. Finally, the authors make several recommendations for improving survivability in rail accidents. Copyright © 2000 John Wiley & Sons, Ltd.

Time delay between singly and doubly ionizing wavepackets in laser-driven helium

We present calculations of the time delay between single and double ionization of helium, obtained from full-dimensionality numerical integrations of the helium-laser Schroedinger equation. The notion of a quantum mechanical time delay is defined in terms of the interval between correlated bursts of single and double ionization. Calculations are performed at 390 and 780 nm in laser intensities that range from 2 X 10^14 to 14 X 10^14 W /cm^2. We find results consistent with the rescattering model of double ionization but supporting its classical interpretation only at 780 nm.

Dynamic resonances and tunnelling in the multiphoton ionization of argon

We present results of wavepacket simulations for multiphoton ionization in argon. A single active electron model is applied to estimate the single-electron ionization rates and photoelectron energy distributions for lambda = 390 nm light with intensities up to I = 2 x 10(14) W cm(-2). The multiphoton ionization rates are compared with R-matrix Floquet calculations and found to be in very good agreement. The photoelectron energy distribution is used to study the nature of ionization at the higher intensities. Our results are consistent with recent calculations and experiments which show the imprint of the tunnelling process in the multiphoton regime. For few-cycle intense pulses, we find that the strong modulation of intensity and increased bandwidth leads to dynamic mixing of the 3d and 5s resonances.

Association between smoking and recurrence of venous thromboembolism and bleeding in elderly patients with past acute venous thromboembolism.

BACKGROUND: While the association between smoking and arterial cardiovascular events has been well established, the association between smoking and venous thromboembolism (VTE) remains controversial. OBJECTIVES: To assess the association between smoking and the risk of recurrent VTE and bleeding in patients who have experienced acute VTE. PATIENTS/METHODS: This study is part of a prospective Swiss multicenter cohort that included patients aged ≥65years with acute VTE. Three groups were defined according to smoking status: never, former and current smokers. The primary outcome was the time to a first symptomatic, objectively confirmed VTE recurrence. Secondary outcomes were the time to a first major and clinically relevant non-major bleeding. Associations between smoking status and outcomes were analysed using proportional hazard models for the subdistribution of a competing risk of death. RESULTS: Among 988 analysed patients, 509 (52%) had never smoked, 403 (41%) were former smokers, and 76 (8%) current smokers. After a median follow-up of 29.6months, we observed a VTE recurrence rate of 4.9 (95% confidence interval [CI] 3.7-6.4) per 100 patient-years for never smokers, 6.6 (95% CI 5.1-8.6) for former smokers, and 5.2 (95% CI 2.6-10.5) for current smokers. Compared to never smokers, we found no association between current smoking and VTE recurrence (adjusted sub-hazard ratio [SHR] 1.05, 95% CI 0.49-2.28), major bleeding (adjusted SHR 0.59, 95% CI 0.25-1.39), and clinically relevant non-major bleeding (adjusted SHR 1.21, 95% CI 0.73-2.02). CONCLUSIONS: In this multicentre prospective cohort study, we found no association between smoking status and VTE recurrence or bleeding in elderly patients with VTE.

Methane cross-validation between three Fourier Transform Spectrometers: SCISAT ACE-FTS, GOSAT TANSO-FTS, and ground-based FTS measurements in the Canadian high Arctic

We present cross-validation of remote sensing measurements of methane profiles in the Canadian high Arctic. Accurate and precise measurements of methane are essential to understand quantitatively its role in the climate system and in global change. Here, we show a cross-validation between three datasets: two from spaceborne instruments and one from a ground-based instrument. All are Fourier Transform Spectrometers (FTSs). We consider the Canadian SCISAT Atmospheric Chemistry Experiment (ACE)-FTS, a solar occultation infrared spectrometer operating since 2004, and the thermal infrared band of the Japanese Greenhouse Gases Observing Satellite (GOSAT) Thermal And Near infrared Sensor for carbon Observation (TANSO)-FTS, a nadir/off-nadir scanning FTS instrument operating at solar and terrestrial infrared wavelengths, since 2009. The ground-based instrument is a Bruker 125HR Fourier Transform Infrared (FTIR) spectrometer, measuring mid-infrared solar absorption spectra at the Polar Environment Atmospheric Research Laboratory (PEARL) Ridge Lab at Eureka, Nunavut (80° N, 86° W) since 2006. For each pair of instruments, measurements are collocated within 500 km and 24 h. An additional criterion based on potential vorticity values was found not to significantly affect differences between measurements. Profiles are regridded to a common vertical grid for each comparison set. To account for differing vertical resolutions, ACE-FTS measurements are smoothed to the resolution of either PEARL-FTS or TANSO-FTS, and PEARL-FTS measurements are smoothed to the TANSO-FTS resolution. Differences for each pair are examined in terms of profile and partial columns. During the period considered, the number of collocations for each pair is large enough to obtain a good sample size (from several hundred to tens of thousands depending on pair and configuration). Considering full profiles, the degrees of freedom for signal (DOFS) are between 0.2 and 0.7 for TANSO-FTS and between 1.5 and 3 for PEARL-FTS, while ACE-FTS has considerably more information (roughly 1° of freedom per altitude level). We take partial columns between roughly 5 and 30 km for the ACE-FTS–PEARL-FTS comparison, and between 5 and 10 km for the other pairs. The DOFS for the partial columns are between 1.2 and 2 for PEARL-FTS collocated with ACE-FTS, between 0.1 and 0.5 for PEARL-FTS collocated with TANSO-FTS or for TANSO-FTS collocated with either other instrument, while ACE-FTS has much higher information content. For all pairs, the partial column differences are within ± 3 × 1022 molecules cm−2. Expressed as median ± median absolute deviation (expressed in absolute or relative terms), these differences are 0.11 ± 9.60 × 10^20 molecules cm−2 (0.012 ± 1.018 %) for TANSO-FTS–PEARL-FTS, −2.6 ± 2.6 × 10^21 molecules cm−2 (−1.6 ± 1.6 %) for ACE-FTS–PEARL-FTS, and 7.4 ± 6.0 × 10^20 molecules cm−2 (0.78 ± 0.64 %) for TANSO-FTS–ACE-FTS. The differences for ACE-FTS–PEARL-FTS and TANSO-FTS–PEARL-FTS partial columns decrease significantly as a function of PEARL partial columns, whereas the range of partial column values for TANSO-FTS–ACE-FTS collocations is too small to draw any conclusion on its dependence on ACE-FTS partial columns.