濒危植物秦岭冷杉的种实特性和幼苗适应性

　　秦岭冷杉(Abies chensiensis)是松科冷杉属常绿乔木，我国国家二级濒危植物，主要分布在我国的秦岭。迄今为止，国内外有关秦岭冷杉的研究鲜有报道。本文研究了核心分布区和边缘区秦岭冷杉的结实特性、球果和种子的形态变异、种子萌发特性及幼苗的最初生长和适应状况，并通过与同属非濒危物种巴山冷杉相关特性的比较研究，初步探讨了秦岭冷杉的繁殖生物生态学特性, 为全面揭示秦岭冷杉濒危机制奠定基础。 　　与冷杉属其他种相比，核心区秦岭冷杉种子较大，出种量也较高，但空粒率很高，达到88%以上;边缘分布区的空粒率更达到95%以上，反映出极高的败育率。秦岭地区秦岭冷杉结实量和结实率随海拔高度升高而减少;同时，两个海拔高度的对比表明，低海拔秦岭冷杉具有较大的球果和种子，饱满度高。表明在其垂直分布范围内，低海拔地段更适合秦岭冷杉的生长和发育。 　　核心区（即秦岭地区）的秦岭冷杉球果和种子的绝大部分指标均值显著大于边缘区（即神农架地区）。相同海拔条件下，秦岭冷杉绝大部分球果和种子形态指标在地区间、地区内种群间、种群内部均有显著差异，约85%的变异来自地区内个体间和个体内，说明秦岭冷杉的球果和种子形态特征变化受遗传控制更显著。人工林与天然林相比，大部分人工林球果和种子指标均值和变异幅度大于天然林，表明通过人为经营可以改善秦岭冷杉的一些生殖性状。 　　秦岭冷杉具有浅休眠，除经典的冷层积方法可以打破休眠外，适当的物理、化学方法处理，如流动水冲洗、适宜浓度硝酸钾、赤霉酸浸种也可以起到相似的作用。各种促进萌发的方法所得到的最大萌发率间没有显著差异。核心区种子萌发率显著高于边缘区;此外，核心区种子在萌发速度和进程上也要显著高于边缘区，这也表明核心区秦岭冷杉活力更高。同样，由于巴山冷杉较高的饱满度，同等条件下，巴山冷杉种子萌发率约三倍于秦岭冷杉种子。 　　野外幼苗的适应性研究主要通过播种后观测出苗率及幼苗在各种环境条件下的存活率、生长状况来进行。通过一年的观测发现，秦岭冷杉野外种子出苗率平均只有16.9%，一年后幼苗死亡率高于50%。 林窗中、土壤覆盖厚度2~3cm的苗床中种子出苗率最高;较深土壤厚度出苗率低说明秦岭冷杉土壤种子库对更新贡献较小。层积30天种子出苗率高于未处理的种子，但对生长率没有影响。林外苗床中幼苗生长率较高。矿质土壤基质上幼苗生长率明显高于林地中。

神农架巴山冷杉种子雨及种实特性研究

巴山冷杉主要分布于秦巴山地，是湖北神农架地区暗针叶林的建群种，构成了当地的优势群落，对神农架地区的植被景观具有决定意义。研究巴山冷杉的结实特性，种子雨时空格局，种子萌发能力和活力劣变过程，有利于进一步认识和分析这一物种的生活史特征，群落组成结构和更新动态。对这一重要物种的合理保护和有效利用具有促进作用。 在湖北神农架自然保护区选择巴山冷杉－箭竹、巴山冷杉－茵芋和巴山冷杉－陕甘花楸群落设置样地，通过布设种子收集器结合室内实验分析，对巴山冷杉种子雨的时空格局进行研究。待巴山冷杉球果成熟时，人工采集球果和种子，测量和比较巴山冷杉的结实特征，利用发芽实验研究巴山冷杉的萌发特性，并通过人工加速老化实验探讨巴山冷杉种子的劣变过程。 巴山冷杉种子雨始于10月初，持续超过2个月，不同类型的巴山冷杉种群表现出不同的种子雨时空格局。巴山冷杉－箭竹群落中巴山冷杉种子雨平均强度167.93±111.14粒/m2，有活力种子比例占22.31%，落种高峰期集中于10月27日到11月2日间，种子雨在种群中呈现聚集分布。巴山冷杉－茵芋群落种子雨强度在三个样地中最小，只有16.41±14.41粒/m2，有活力种子仅占3.05%。巴山冷杉－陕甘花楸群落，种子雨落种高峰为10月15日至10月21日，林冠内种子雨数量占到了收集总数的87.95%。扩散的种子数量与离开中心母树的距离间的关系近似正态分布。 对巴山冷杉的结实特性的分析结果表明，巴山冷杉球果近圆柱形，球果平均长5.37±0.75cm;平均宽3.01±0.32cm;重量介于5.9g～41.3g。巴山冷杉种子长1.08～8.68mm，种子宽1.16～6.42mm，种子厚0.66～3.48mm，种子千粒重7.30g。球果单果出种量在不同种群的频数分布格局不同，巴山冷杉球果和种子的各项指标在种群间和种群内存在显著差异。球果大小、出种量及单粒种子的质量间存在着极显著的正相关关系。此外，种子生活力水平在母树间差异较大，不同母树的种子发芽率和发芽势不等且随时间的萌发进程也不相同，相同种源的巴山冷杉种子在不同的培养条件下萌发能力不同，室温条件下具有最高的发芽率但在25℃，8h光照，恒温培养时的萌发最为整齐。 高温高湿条件能够加速巴山冷杉种子的老化进程，使巴山冷杉种子的含水量发生变化，种子的活力水平随着老化时间的延长而降低，40℃，100% 相对湿度处理6天后种子基本丧失活力。

Bird attributes, plant characteristics, and seed dispersal of Pera glabrata (Schott, 1858), (Euphorbiaceae) in a disturbed cerrado area

Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

Summer deficit irrigation strategies in hedgerow olive orchard cv. ‘Arbequina’: Effect on fruit characteristics and yield.

Maximum production in hedgerow olive orchards is likely not achieved with maximum evapotranspiration over the long-term. Thus, regulated deficit irrigation (RDI) should be considered as a management option. Four irrigation treatments were evaluated during the summer when olive is most drought resistant. Control (CON) was irrigated to maintain the rootzone close to field capacity. Severe water deficit was applied by irrigating 30% CON from end of fruit drop to end July (DI-J) and from end July until beginning of oil synthesis (DI-A). Less severe water deficit was applied during July and August (DI-JA) by irrigating 50% CON. Flowering, fruiting, abscission, fruit development, fresh and dry weight of fruits, and oil production were evaluated. There were not significant differences in number of buds initiated, number of fruits per inflorescence and fruit drop. Oil production was significantly different between irrigation treatments in all experimental years. CON produced more oil and fruit with higher oil% than DI-A and DI-JA. Oil production of DI-J was not significantly reduced compared to CON and oil% was greater. DI-J was the most effective RDI strategy; with 16% less applied water relative to CON average loss in oil production of 8% was not significantly different to CON. While DI-JA saved most water (27%), oil production was reduced by 15%. Greatest loss in oil production (21%) was observed in DI-A with water saving of 22%.

New dimeric supramolecular structure of mixed (phthalocyaninato)(porphyrinato)-europium(III) sandwiches : preparation and spectroscopic characteristics

The mixed double-decker Eu\[Pc(15C5)4](TPP) (1) was obtained by base-catalysed tetramerisation of 4,5-dicyanobenzo-15-crown-5 using the half-sandwich complex Eu(TPP)(acac) (acac = acetylacetonate), generated in situ, as the template. For comparative studies, the mixed triple-decker complexes Eu2\[Pc(15C5)4](TPP)2 (2) and Eu2\[Pc(15C5)4]2(TPP) (3) were also synthesised by the raise-by-one-story method. These mixed ring sandwich complexes were characterised by various spectroscopic methods. Up to four one-electron oxidations and two one-electron reductions were revealed by cyclic voltammetry (CV) and differential pulse voltammetry (DPV). As shown by electronic absorption and infrared spectroscopy, supramolecular dimers (SM1 and SM3) were formed from the corresponding double-decker 1 and triple-decker 3 in the presence of potassium ions in MeOH/CHCl3.

Vibrational spectroscopy of phthalocyanine and naphthalocyanine in sandwich-type (na)phthalocyaninato and porphyrinato rare earth complexes : (Part 10) The infrared and Raman characteristics of phthalocyanine in heteroleptic bis(phthalocyaninato) rare earth complexes with decreased molecular symmetry

The infrared (IR) spectroscopic data for a series of eleven heteroleptic bis(phthalocyaninato) rare earth complexes MIII(Pc)[Pc(α-OC5H11)4] (M = Sm–Lu, Y) [H2Pc = unsubstituted phthalocyanine, H2Pc(α-OC5H11)4 = 1,8,15,22-tetrakis(3-pentyloxy)phthalocyanine] have been collected with 2 cm−1 resolution. Raman spectroscopic properties in the range of 500–1800 cm−1 for these double-decker molecules have also been comparatively studied using laser excitation sources emitting at 632.8 and 785 nm. Both the IR and Raman spectra for M(Pc)[Pc(α-OC5H11)4] are more complicated than those of homoleptic bis(phthalocyaninato) rare earth analogues due to the decreased molecular symmetry of these double-decker compounds, namely C4. For this series, the IR Pc√− marker band appears as an intense absorption at 1309–1317 cm−1, attributed to the pyrrole stretching. With laser excitation at 632.8 nm, Raman vibrations derived from isoindole ring and aza stretchings in the range of 1300–1600 cm−1 are selectively intensified. In contrast, when excited with laser radiation of 785 nm, the ring radial vibrations of isoindole moieties and dihedral plane deformations between 500 and 1000 cm−1 for M(Pc)[Pc(α-OC5H11)4] intensify to become the strongest scatterings. Both techniques reveal that the frequencies of pyrrole stretching, isoindole breathing, isoindole stretchings, aza stretchings and coupling of pyrrole and aza stretchings depend on the rare earth ionic size, shifting to higher energy along with the lanthanide contraction due to the increased ring-ring interaction across the series. The assignments of the vibrational bands for these compounds have been made and discussed in relation to other unsubstituted and substituted bis(phthalocyaninato) rare earth analogues, such as M(Pc)2 and M(OOPc)2 [H2OOPc = 2,3,9,10,16,17,23,24-octakis(octyloxy)phthalocyanine].

Vibrational spectroscopy of phthalocyanine and naphthalocyanine in sandwich-type (na)phthalocyaninato and porphyrinato rare earth complexes: Part 14. The infrared and Raman characteristics of phthalocyanine in “pinwheel-like” homoleptic bis[1,8,15,22-tetrakis(3-pentyloxy)phthalocyaninato] rare earth(III) double-decker complexes

The infrared (IR) spectroscopic data and Raman spectroscopic properties for a series of 13 “pinwheel-like” homoleptic bis(phthalocyaninato) rare earth complexes M[Pc(α-OC5H11)4]2 [M = Y and Pr–Lu except Pm; H2Pc(α-OC5H11)4 = 1,8,15,22-tetrakis(3-pentyloxy)phthalocyanine] have been collected and comparatively studied. Both the IR and Raman spectra for M[Pc(α-OC5H11)4]2 are more complicated than those of homoleptic bis(phthalocyaninato) rare earth analogues, namely M(Pc)2 and M[Pc(OC8H17)8]2, but resemble (for IR) or are a bit more complicated (for Raman) than those of heteroleptic counterparts M(Pc)[Pc(α-OC5H11)4], revealing the decreased molecular symmetry of these double-decker compounds, namely S8. Except for the obvious splitting of the isoindole breathing band at 1110–1123 cm−1, the IR spectra of M[Pc(α-OC5H11)4]2 are quite similar to those of corresponding M(Pc)[Pc(α-OC5H11)4] and therefore are similarly assigned. With laser excitation at 633 nm, Raman bands derived from isoindole ring and aza stretchings in the range of 1300–1600 cm−1 are selectively intensified. The IR spectra reveal that the frequencies of pyrrole stretching and pyrrole stretching coupled with the symmetrical CH bending of –CH3 groups are sensitive to the rare earth ionic size, while the Raman technique shows that the bands due to the isoindole stretchings and the coupled pyrrole and aza stretchings are similarly affected. Nevertheless, the phthalocyanine monoanion radical Pc′− IR marker band of bis(phthalocyaninato) complexes involving the same rare earth ion is found to shift to lower energy in the order M(Pc)2 > M(Pc)[Pc(α-OC5H11)4] > M[Pc(α-OC5H11)4]2, revealing the weakened π–π interaction between the two phthalocyanine rings in the same order.

Raman spectroscopic characteristics of phthalocyanine and naphthalocyanine in sandwich-type phthalocyaninato and porphyrinato rare earth complexes Part 5. – Raman spectroscopic characteristics of naphthalocyanine in mixed [tetrakis(4-tert-butylphenyl)porphyrinato]-(naphthalocyaninato) rare earth double-deckers

Raman spectra were recorded in the range 400–1800 cm−1 for a series of 15 mixed \[tetrakis(4-tert-butylphenyl)porphyrinato](2,3-naphthalocyaninato) rare earth double-deckers M(TBPP)(Nc) (M = Y; La–Lu except Pm) using laser excitation at 632.8 and 785 nm. Comparisons with bis(naphthalocyaninato) rare earth counterparts reveal that the vibrations of the metallonaphthalocyanine M(Nc) fragment dominate the Raman features of M(TBPP)(Nc). When excited with radiation of 632.8 nm, the most intense vibration appears at about 1595 cm−1, due to the naphthalene stretching. These complexes exhibit the marker Raman band for Nc•− as a medium-intense band in the range 1496–1507 cm−1, attributed to the coupling of pyrrole and aza stretching, while the marker Raman band of Nc2− in intermediate-valence Ce(TBPP)(Nc) appears as a strong band at 1493 cm−1 and is due to the isoindole stretchings. By contrast, when excited with radiation of 785 nm that is in close resonance with the main Q absorption band of the naphthalocyanine ligand, the ring radial vibrations at ca 680 and 735 cm−1 for MIII(TBPP)(Nc) are selectively intensified and are the most intense bands. For the cerium double-decker, the most intense vibration also acting as the marker Raman band of Nc2− appears at 1497 cm−1 with contributions from both pyrrole CC and aza CN stretches. The same vibrational modes show weak to medium intensity scattering at 1506–1509 cm−1 for MIII(TBPP)(Nc) and this is the marker Raman band of Nc•− when thus excited. The scatterings due to the Nc breathings, ring radial vibration, aza group stretchings, naphthalene stretchings, benzoisoindole stretchings and the coupling of pyrrole CC and aza CN stretchings in MIII(TBPP)(Nc) are all slightly blue shifted along with the decrease in rare earth ionic radius, confirming the effects of increased ring–ring interactions on the Raman characteristics of naphthalocyanine in the mixed ring double-deckers.