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通过水培试验,比较研究了硒在不同浓度下对小麦和水稻种子萌发及幼苗生长的生态毒理效应。结果表明,硒在适量范围内(<0.5 mg.L-1)对种子萌发过程中各生理指标有促进作用,高剂量(>5 mg.L-1)时,对种子活力、α-淀粉酶及幼苗和根生长具有胁迫效应。硒对小麦种子发芽各指标抑制率大于水稻,硒对种子根伸长的抑制率远远大于发芽抑制率。对硒浓度与种子发芽各项指标抑制率相关分析,呈显著正相关。应用小麦根伸长抑制率可作为化学物质生态风险评价的一项生物标志物。

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Wild-type Anabaena sp. strain PCC 7120, a filamentous nitrogen-fixing cyanobacterium, produces single heterocysts at semi-regular intervals. asr0100 (patU5) and alr0101 (patU3) are homologous to the 5' and 3' portions of patU of Nostoc punctiforme. alr0099 (hetZ) overlaps the 5' end of patU5. hetZ, patU5 and patU3 were all upregulated, or expressed specifically, in proheterocysts and heterocysts. Mutants of hetZ showed delayed or no heterocyst differentiation. In contrast, a patU3 mutation produced a multiple contiguous heterocyst (Mch) phenotype and restored the formation of otherwise lost intercalary heterocysts in a patA background. Decreasing the expression of patU3 greatly increased the frequency of heterocysts in a mini-patS strain. Two promoter regions and two principal, corresponding transcripts were detected in the hetZ-patU5-patU3 region. Transcription of hetZ was upregulated in a hetZ mutant and downregulated in a patU3 mutant. When mutants hetZ::C.K2 and hetZ::Tn5-1087b were nitrogen-deprived, P-hetC-gfp was very weakly expressed, and in hetZ::Tn5-1087b, P-hetR-gfp was relatively strongly expressed in cells that had neither a regular pattern nor altered morphology. We conclude that the hetZ-patU5-patU3 cluster plays an important role in co-ordination of heterocyst differentiation and pattern formation. The presence of homologous clusters in filamentous genera without heterocysts is suggestive of a more general role.

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本文用加拿大国立研究院(National Research Council of Canada) Fuhrer等人编制的FORTRAN语言程序(以下简称NRCC程序),对两个冠醚类化合物进行了简正坐标分析,这两个化合物分子是二氧六环(C_4H_8O_2)和12-冠-4(C_8H_(16)O_4)。作者用Synder和Zerbi提出的一般价力场,计算了二氧六环的36个简正振动频率,精化四次后的结果误差为14.04 cm~(-1),得到了二氧六环的精化力场和势能分析矩阵;做了12-冠-4-的中红外光谱(3200-5000cm~(-1))。远红外光谱(500-70cm~(-1))和拉曼光谱(3200-50 cm~(-1),从而归属出12-冠-4的78个简正振动频率实验值;利用二氧六环的精化力场作为初始力场,计算了12-冠-4的简正振动频率,对78个简正振动频率进行了精化计算,精化三次后的结果误差为13.99 cm~(-1),精化后得到12-冠-4的精化力场和势能分布矩阵;将NRCC程序以BASIC语言移至TRS-80微型机上,对二氧六环进行了计算,结果良好,首次给出二氧六环一般价力场的势能分布。一、对二氧六环的处理 二氧六环分子式C_4H_8O_2,合14个原子,有3N-6=36个简正振动频率。分子结构系由二个乙氧基(-CH_2-CH_2-O-)单元组成的含有四个碳,两个氧的六元环,平衡态分子为椅式构象,属于C_(2h)点群,36个简正振动频率分为四个对称类Ag、Au、Bg和Bu,分布是:Ag 10个,Bg 8个,Au 9个,Bu9个。二氧六环的分子结构及坐标示意图见28而图5,定义了14个伸缩内坐标,26个弯曲内坐标,6个扭曲内坐标,共46个,C-C键长1.54A,C-O键长1.41 A,C-H键长1.096A,键角都用109°28'。用CART程序(NRCC程序之一)计算二氧六环14个原子的笛卡尔坐标,用GMAT程序(NRCC程序之二)计算其B矩阵和G矩阵,用FPERT程序(NRCC程序之三)计算其简正振动频率、精化力场,计算用一般价力场,引入V矩阵对称化,将46个坐标化为46个(内)对称坐标,10个多余坐标在FPERT程序计算中除去。二、对12-冠-4的处理 12-冠-4分子式C_8H_(16)O_4,含28个原子,共3N-6=78个简正振动频率,分子结构为四个乙氧基(-CH_2-CH_2-O-)单元组成的含八个碳、四个氧的12元环,自由分子的12-冠-4属于C点群。结构数据引自Groth的X光衍射分数和坐标,自己编制了BASIC语言程度将分数坐标化为笛卡尔坐标,用GMAT程序计算B矩阵和G矩阵,FPERT程序计算78个简正振动频率、精化力场、计算势能分布矩阵,引入U矩阵将92个内坐标化为92个对称坐标,14个多余坐标在FPERT程序中自动除去。三、结果 势能分布矩阵给出分子的振动归属,对这两个冠醚类分子的3N-6个简正振动频率,可以划分为五个振动区域。1.C-H伸缩振动区(3000-2800 cm~(-1)) 在该区中,二氧六环有八个值:2974、2966、2854和2867 cm~(-1)各两个,12-冠-4有16个值:2935、2923、2915和2907 cm~(-1)各两个,2860 cm~(-1)8个,高于2900 cm~(-1)者为反对称伸缩振动,低于2900 cm~(-1)者为对称伸缩振动。2.亚甲基弯曲振动之一(1500-1400 cm~(-1)) 该区的主要振动是亚甲基剪式振动(Scissor),其它振动小于10%二氧六环在该区有四个频率:1443、1461、1451和1457 cm~(-1),12-冠-4有八个频率:1466、1450、1450和1405 cm~(-1)各两个。3.亚甲基弯曲振动区二(1400-1200 cm~(-1))该区的主要振动模式为亚甲基的颤动(wag)、卷曲(twist)和摆动(rock)振动,其它振动小于13%。二氧六环在该区有八个频率:1334、1303、1396、1216、1367、1264、1377和1296 cm~(-1),12-冠-4有十六个频率:1388、1363、……1229 cm~(-1)(其中1288、1307cm~(-1)非简并,其余皆两重简并)。4.环的骨架伸缩振动区(1200-600 cm~(-1))该区振动模式复杂,除环的骨架伸缩振动外,还有亚甲基的wag、twist、rock以及环的骨架弯曲振动,而且这些振动的势能分布值都不小。二氧六环在该区有十一个频率,从1127至610 cm~(-1),12-冠-4有二十个频率,从1135至184 cm~(-1)且大都是二重简并的。5.低频区(600-50cm~(-1))这两个分子在低频区的势能分布略有差别。二氧六环在该区有五个频率:503、486、427、276和224 cm~(-1),主要振动模式为骨架弯曲振动和扭曲振动,C-O、C-C的扭曲振动在三个最低频率中分布占10-30%。12-冠-4在该区有18个频率,除570和547cm~(-1)处,都是二重简并的,六个最低频率的振动模式完全属于C-O、C-C键的扭曲振动,其它振动小于10%,所以200 cm~(-1)以下可称为12-冠-4的扭曲振动区,在600-200cm~(-1)之间的12个频率主要是骨架的弯曲振动,也有一定量的亚甲基wag、twist、rock振动。12-冠-4的简正坐标分析尚未有人做过。二氧六环的计算结果与Snyder和Zerbi的分析相吻合,12-冠-4和二氧六环两分子势能分布的相对一致性证明了对12-冠-4的简正坐标分析基本是正确的。本文比较了二分子的力常数和振动频率,探讨了环的大小对振动光谱的影响。四、NRCC程序简介 NRCC程序由CART、GMAT和FPERT三个程序组成,即可联一起运用,亦可分开独立进行运算。该程序功能强,所占内存大,适于大、中型计算机使用。CART程序之名字取自Cartisian Co-or-dinates的前四个字母,功能系由分子结构参数(键长、键角)计算分子内各原子的笛卡尔坐标。GMAT程序之名字取自G matrix的前四个字母,功能系由分子内各原子的笛卡尔坐标,原子质量和内坐标定义计算分子内各原子的坐标交换矩阵B和Wilson振动动能矩阵G。FPERT程序之名字取自F Perturbation的前五个字母,功能系由分子振动功能矩阵G、势能常数即力常数矩阵F计算分子的简正振动频率和势能分布矩阵,再通过实验频率精化势能矩阵F。NRCC程序可对含30个原子、60个内坐标的分子进行简正坐标分析,扩充后容量增大一倍。该程序可选用一般价力场(General Valence Force Field, 简称GVFF)和UBS力场(Urey-Bradley-Shimanouchi Force Field),简称UBSFF或UBFF)。可选用对称化U矩阵,可自行决定力场精化次数和阻尼常数以限制精化结果的收敛性。五、NRCC程序在TRS-80微型机上移植试尝(该部分曾在第三届长春夏季化学讨论会上宣读)针对NRCC程序占内存空间大、难以在微型机上实现的情况,作者将NRCC程序改编为BASIC语言,改变程序的原来结构,形成一组BASIC语言程序:CART/BAS、GMAT/BAS和VIFR/BAS,改编后的BASIC程序在TRS-80微型机调试通过,TRS-80机字长8位,New Dos系统内存32K。改写后的程序只保持了原程序的基本原理,在内存,语句上改动很大,以适于微型机使用。数据在程序中直接嵌入,利于修改替换,且BASIC语言简单易学,便于操作。CART/BAS程序可计算含30个原子以内的分子的笛卡尔坐标,GMAT/BAS程序可计算含20个原子、45个内坐标的分子的G矩阵,VIFR/BAS程序可计算含15个原子的分子的简正振动频率。利用这组程序,作者以二氧六环分子为例做了一些试尝运算,误差14.4 cm~(-1),相对误差1.8%,结果较理想。

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Size modification of Au nanoparticles (NPs), deposited on the Au-thick film surface and irradiated by slow highly charged ions (SHCI) 40Arq+ (3 6 q 6 12) with fixed low dose of 4.3 1011 ions/cm2 and various energy ranging from 74.64 to 290.64 keV at room temperature (293.15 K), was investigated by atomic force microscopy (AFM) and transmission electron microscopy (TEM). The effect of projectile kinetic energy on the modified size of NPs was explored by an appropriate choice of the fixed process parameters such as ion flux, irradiation temperature, incident angle, irradiation time, etc. The morphological changes of NPs were interpreted by models involving collisional mixing, Ostwald ripening (OR) and inverse Ostwald ripening (IOR) of spherical NPs on a substrate. A critical kinetic energy as well as a critical potential energy of the projectile in the Au NPs size modification process were observed.

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This paper reports that the K x-ray spectra of the thin target 47Ag, 48Cd, 49In and 50Sn were measured by an HPGe semi-conductor detector in collisions with 84.5 MeV 6C4+ ions. Our experiment revealed the Kα x-ray energy shifts were not obvious and the Kβ1 x-ray energy shifts were about 90∼110 eV. The simple model of Burch et al has been previously used to calculate the K x-ray energy shifts due to an additional vacancy in 2p orbit. The present work extends the model of Burch to calculate the x-ray energy shifts of multiple ionized atoms induced by heavy ions with kinetic energy of MeV/u. In addition to our experimental results, many other experimental results are compared with the calculated values by using the model.

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以工业用原淀粉为基体,醋酸酐为酯化剂,与酸进行酯化反应,制得取代度为2.90的醋酸酯淀粉。以制得的醋酸酯淀粉为主料研制肥料包膜用膜溶液,并制备包膜尿素。结果表明,此包膜材料具有很强的成膜性和柔韧性,成膜质的细腻光滑、致密,膜与尿素表面接合紧密,能很好地适应尿素颗粒表面的外形轮廓而将其紧密覆盖。包膜尿素后,对尿素态氮的释放有明显的控释作用。

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Surface-tethered oppositely charged weak polyelectrolyte block copolymer brushes composed of poly(2-vinyl pyridine) (P2VP) and poly(acrylic acid) (PAA) were grown from the Si wafer by atom-transfer radical polymerization. The P2VP-b-PAA brushes were prepared through hydrolysis of the second PtBA block to the corresponding acrylic acid. The P2VP-b-PAA brushes with different PAA block length were obtained. The P2VP-b-PAA brushes revealed a unique reversible wetting behavior with pH. The difference between the solubility parameters for P2VP and PAA, the changes of surface chemical composition and surface roughness, and the reversible wetting behavior illustrated that the surface rearrangement occurred during treatment of the P2VP-b-PAA brushes by aqueous solution with different pH value. The reversible properties of the P2VP-b-PAA brushes can be used to regulate the adsorption of the sulfonated PS nanoparticles.

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This paper reports on a successful application of the concept of nanoreactors to effectively controlling the selectivity of the free radical grafting of maleic anhydride (MAH) onto polypropylene (PP) in the melt, an industrially relevant process. More specifically, a free radical initiator of type ROOR was first confined into (or encapsulated by) the galleries of an organically modified montmorillonite (o-MMT) whose interdistance was 2.4 nm. Primary free radicals (RO center dot) formed inside the o-MMT galleries had to diffuse out before they could react with the PP backbone. The controlled release of the primary free radicals significantly increased the grafting degree of MAH onto PP and greatly reduced the level of the chain scission of the latter. Those results were better understood by electron spin resonance studies on model systems and by Monte Carlo simulations.

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Multi-color LLP phenomenon was observed in Mn2+-doped ZnO-B2O3-SiO2 glassceramics after the irradiation of a UV lamp at room temperature. Transparent ZnO-B2O3-SiO2 glass emitted reddish LLP while opaque glass-ceramics prepared by the glass sample after heat treatment emitted yellowish or greenish LLP. The change of the phosphorescence is due to the alteration of co-ordination state of Mn2+. The phosphorescence of the samples was seen in the dark with naked eyes even 12 h after the irradiation with a UV lamp (lambda(max) = 254 nm) for 30 min. Based on the approximative t(-1) decay law of the phosphorescence, we suggest that the LLP is attributed to the thermally assisted electron-hole recombination.

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The chlorophyll fluorescence in soybean leaves was observed by a portable fluorometer CF-1000 under field conditions. On clear days, F-0 increased while F, and F-v/F-m decreased gradually in the morning. At midday F-O reached its maximum while F-v and F-v/F-m reached their minimum. The reverse changes occurred in the afternoon. At dusk these parameters could return to levels near those at dawn. Following exposure to a strong sunlight for more than 3 h, the dark-recovery process displayed three phases: (1) slow increases in F-0, F-v and F-v/F-m within the first hour; (2) a faster decrease in F-0 and faster increases in F-v and F-v/F-m within subsequent two hours; (3) a slow decrease in F-0 and slow increases in F-v and F-v/F-m within the fourth hour. In comparison with darkness, weak irradiance had no stimulating effect on the recovery from photoinhibition. Hence the photoinhibition in soybean leaves is mainly the reflection of reversible inactivation of some photosystem 2 reaction centres, but not the result of D1 protein loss.