元阳铁陨石的矿物岩石学和微量元素地球化学研究

元阳铁陨石是2010年在云南省元阳县山区发现的,其内部的主要矿物为铁纹石和镍纹石,铁纹石的含量很高(约占80%),镍纹石的含量较低.铁纹石中Ni含量为4.88–6.21wt%,镍纹石中Ni含量为26.13–50.27 wt%.副矿物有陨磷铁镍石、闪锌矿和氮铬矿.陨磷铁镍石存在大、小两种颗粒,具有颗粒越大Ni含量越低的特点.元阳铁陨石中没有发现硅酸盐包体.由于经受了地表风化蚀变作用,样品边缘以及铁纹石裂隙间都发生了氧化.元阳铁陨石中铁纹石的条带宽度较粗,属于粗粒八面体结构.中子活化分析结果显示:元阳铁陨石的Ni(7 wt%)和Au(1.565 ppm)的含量都相对较低,和IAB-MG(IAB-Main group)群的铁陨石在化学成分上具有相似性,属于IAB-MG群.相对于其他IAB-MG群铁陨石,元阳铁陨石的Ir(1.00 ppm)含量偏低,这可能是由于其母体中富含Ir的矿相在冲击作用下并没有完全熔融.     

东乌珠穆沁旗中铁陨石

石铁陨石是由几乎相等的硅酸盐和铁镍金属组成的,其矿物组成、结构构造、化学成分和演化历史等,都兼有石陨石和铁陨石的特征,对探讨陨石的成因具有特殊的意义。石铁陨石分为两类:中铁陨石(Mesosiderite)和橄榄陨     

乌希里克铁陨石的组织结构、冷却历史和定量预测模型

铁陨石记录了陨石母体所经历的熔融、分异和冷却的热历史, 研究铁陨石内部的组织结构对理解陨石母体的热历史和内部圈层结构有重要的指导意义. 分析阿勒泰铁陨石个体-乌希里克(Wuxilike)铁陨石中铁纹石和镍纹石所构造的维斯台登(Widmanstatten)纹、梳状合纹石以及云状区等组织结构来探究其各自的形成过程. 通过热动力学计算软件和数据库, 建立了Widmanstatten经过取向校正的冷却速率计算模型, 并据此计算了该陨石在695℃–400℃区间内的冷却速率; 通过研究梳状合纹石内部铁、镍纹石中Ni元素的成分分布及其位相关系, 推理得到梳状合纹石的低温马氏体分解形成机制; 通过研究云状区域中颗粒大小和局部Ni含量的关系, 得出形成云状区域所对应的铁陨石在350℃下的冷却速率. 据此模拟计算出该铁陨石在695℃–200℃范围内形成Widmanstatten纹、各类合纹石和云状区的整个热历史. 基于固态相变所建立的定量模型可望为分析铁陨石的冷却历史提供更为准确的分析手段.     

云南西双版纳(曼桂)目击陨石的热变质和冲击变质研究

曼桂陨石是新近(2018年6月1日)陨落在云南西双版纳地区的目击球粒陨石,其中的主要矿物为橄榄石(Fa_(24.3±0.6))、斜方辉石(Fs_(20.6±0.5)Wo_(0.4±0.2))、长石(An_(11-12)Or_(2-4))、铁镍金属和陨硫铁,次要矿物为铬铁矿、白磷钙矿等.橄榄石和辉石的化学成分表明曼桂陨石属于L型普通球粒陨石.陨石中球粒很少且轮廓不清晰,基质矿物普遍经历过重结晶,重结晶矿物颗粒粒径较大,高钙辉石粒径25–30μm,长石颗粒大多超过50μm,说明该陨石属于6型岩石类型.橄榄石和辉石颗粒中发育有波状消光、嵌晶块状消光现象、平面裂隙和面状变形构造,长石熔长石化并不完全,陨石中观察到宽度不等且纵横交错的冲击熔融脉,表明曼桂普通球粒陨石受到的冲击变质作用可以达到S5级以上.通过熔融脉中的矿物组合推断出熔融脉中矿物经历的压力在15–16 GPa左右.     

寺巷口普通球粒陨石的热变质和冲击变质历史研究

寺巷口陨石是一块经历强冲击变质的普通球粒陨石.系统研究陨石主体和冲击熔融脉的岩相学和矿物学.该陨石中球粒较少且轮廓和内部结构均模糊不清,基质重结晶程度高,橄榄石和辉石的成分非常均一.单斜辉石-斜方辉石矿物对计算得到的平衡温度峰值为891 4-36°C.说明寺巷口陨石的热变质程度与6型一致.陨石主体中的橄榄石具有明显的波状消光和面状变形裂隙,熔长石广泛存在,在冲击熔融脉中含有粗粒的林伍德石和镁铁榴石以及细粒的高压矿物组合,这些特征预示了寺巷口陨石经历了S6级的冲击变质作用且形成冲击脉的峰期压力可能在20 GPa-24 GPa左右,而温度可能高于2000°C.冲击熔融脉中自磷钙矿和铬铁矿的存在可能是因为经历了较长的退火时间,导致其高压矿物的回退.     

国内18块普通球粒陨石的岩石矿物学研究

描述了国内收集的18块普通球粒陨石的岩石矿物学特征,其中13块为新疆罗布泊地区的发现型陨石,1块为新疆库姆塔格地区的发现型陨石(Kumtag),1块为新疆阿克赛钦地区的发现型陨石(.Aksai Chin),另外3块分别为降落于青海省西宁市(Xining)、湖北省随州市(Fuhe)以及浙江省东阳市(Dongyang)内的降落型陨石.18块陨石均属于平衡型普通球粒陨石,其中H群8块(全部为H5),L群10块(1块L4,7块L5,2块L6).18块陨石所受冲击变质作用较弱,以S2、S3程度居多.大多数罗布泊陨石经历了较强的风化作用,仅有2块风化程度较低,分别为W1和W2,Kumtag与Aksai Chin陨石风化程度均为W2.在新疆塔克拉玛干沙漠东部的戈壁荒漠区发现的大量陨石表明该区域可能是欧亚地区重要的陨石富集区.     

NWA 13943(CK5型)碳质球粒陨石的矿物岩石学和稳定同位素组成研究

CK型陨石是一类高度氧化的碳质球粒陨石, 金属/磁铁矿的比值接近零. 与其它类型的碳质球粒陨石(岩石类型: 1-3)不同, 大多数CK型陨石在母体上经历了强烈的热变质过程(550--1270K), 以4-6型为主. 多项证据表明, CK和CV3型陨石具有成因联系. 但是, 两者在岩相结构和化学组成方面仍存在微小差异. 因此, 精细地区分和比较两者的地球化学特征对于验证CK-CV单一母体假说非常重要. Northwest Africa (NWA) 13943是一块新发现的陨石, 经历过较强烈的热变质作用. 利用扫描电子显微镜和电子探针, 确定了NWA 13943的岩石类型. 并运用质谱分析技术, 重点测定了NWA 13943陨石的全岩氧同位素和铬同位素组成. 综合岩石结构、矿物化学成分、氧同位素异常(△¹⁷O,△代表同位素分馏值)和铬同位素异常(ε⁵⁴Cr, ε表示样品中的同位素比值与标样中的同位素比值的相对偏差的10⁴倍),CK和CV型陨石的母体可能形成于原行星盘中两个相似但不同的化学源区.     

银河系化学元素的丰度特征和合成图像(Ⅱ):太阳系原始同位素丰度异常及其解释

太阳系原始同位素组成是研究太阳系起源和演化的基础。评述了太阳星云的原始放射性核素丰度特征及解释此丰度特征的分子云自增丰模型、AGB星污染模型和散裂反应模型。陨石包体中前太阳矿物颗粒的同位素组成异常表明,前太阳颗粒中低密度石墨、X型碳硅石可能来源于超新星爆发,而AGB星或红巨星被认为是尖晶石和碳硅石的最可能的恒星来源。太阳系中比较特殊的氖和氙的同位素组成异常也与超新星爆发密切相关。     

火星陨石NWA 8716的岩矿学特征及粗粒橄榄石斑晶的来源

火星陨石可以为研究火星岩浆演化过程提供直接证据并限制其源区特征.通常认为含粗粒橄榄石斑晶辉玻无球粒陨石携带有火星原始地幔的信息,因此选取该类样品Northwest Africa (NWA) 8716为研究对象,进行岩相结构及矿物成分分析. NWA8716由橄榄石、辉石、填隙状熔长石以及其他次要矿物组成.其中橄榄石颗粒有两种级别的粒径,长轴分别约为0.5–1.8 mm和50–400μm.较小橄榄石斑晶内部的熔体包裹体和NWA 8716全岩成分(计算值)均显示明显的轻稀土元素亏损([La/Yb]CI值为0.06–0.1),说明NWA 8716源于一个亏损的火星岩浆池.粗粒橄榄石斑晶的来源对衡量该样品是否能够代表原始熔体成分非常重要.对橄榄石晶体的粒径统计分析发现,粗粒橄榄石斑晶应为堆晶.进一步对铁-镁以及稀土元素分配特征的计算表明NWA 8716并非形成于一个封闭系统,但是计算所得原始熔体成分与全岩成分差异不大,因此粗粒橄榄石斑晶应当来源于与母岩浆成分相似的熔体.总的看来, NWA 8716应当来源于亏损型火星幔源区且演化程度较低.     

ALH84001一块著名的火星陨石

1984年12月27日,美国宇航局、美国国家科学基金会和史密森学会联合组成的南极陨石搜寻计划小组在南极洲艾伦丘陵的冰层中发现了一块陨石,后将其命名为名为“艾伦-希尔斯84001”（简称ALH84001）。     

Radiative association of C and P, and Si and P atoms

The rate coefficients for the formation of carbon monophosphide (CP) and silicon monophosphide (SiP) by radiative association are estimated for temperatures ranging from 300 to 14 100 K. In this temperature range, the radiative association rate coefficients are found to vary from  1.14 × 10⁻¹⁸  to  1.62 × 10⁻¹⁸ cm³ s⁻¹  and from  3.73 × 10⁻²⁰  to  7.03 × 10⁻²⁰ cm³ s⁻¹  for CP and SiP, respectively. In both cases, rate coefficients increase slowly with the increase in temperature.     

DDO photometry and metallic abundances of E and SO galaxies and globular clusters of the LMC and SMC

Metallicity of 8 E and SO galaxies as well as that of red globulars of the LMC and SMC were obtained by means of DDO integrated photometry calibrated with galactic globular clusters (Bica and Pastoriza, 1983; hereafter referred to as Paper I). A correction was obtained in order to reduce the colors of the galaxies to zero redshift. The relation metallicity vsM _V for the galaxies is analyzed (adding to our sample the observations of McClure and Van den Bergh, 1968; and Faber, 1973a). For the Magellanic Clouds we found metallicity ranging from intermediate to poor.     

Substructure and the cusp and fold relations

Gravitational lensing of a background source by a foreground galaxy lens occasionally produces four images of the source. The cusp and the fold relations impose conditions on the ratios of magnifications of these four-image lenses. In this theoretical investigation, we explore the sensitivity of these relations to the presence of substructure in the lens. Starting with a smooth lens potential, we add varying amounts of substructure, while keeping the source position fixed, and find that the fold relation is a more robust indicator of substructure than the cusp relation for the images. This robustness is independent of the detailed spatial distribution of the substructure, as well as of the ellipticity of the lensing potential and the presence of external shear.     

Gravity and Topography of Moon and Planets

Planetology serves the understanding on the one hand of the solar system and on the other hand, for investigating similarities and differences, of our own planet. While observational evidence about the outer planets is very limited, substantial datasets exist for the terrestrial planets. Radar and optical images and detailed models of gravity and topography give an impressive insight into the history, composition and dynamics of moon and planets. However, there exists still significant lack of data. It is therefore recommended to equip all future satellite missions to the moon and to planets with full tensor gravity gradiometers and radar altimeters.     

Fragmentation and hydration of tektites and microtektites

Abstract— An examination of data collected over the last 30 years indicates that the percent of glass fragments vs. whole splash forms in the Cenozoic microtektite strewn fields increases towards the source crater (or source region). We propose that this is due to thermal stress produced when tektites and larger microtektites fall into water near the source crater while still relatively hot (>1150 °C). We also find evidence (low major oxide totals, frothing when melted) for hydration of most of the North American tektite fragments and microtektites found in marine sediments. High-temperature mass spectrometry indicates that these tektite fragments and microtektites contain up to 3.8 wt% H₂O. The H₂O-release behavior during the high-temperature mass-spectrometric analysis, plus high CI abundances (0.05 wt%), indicate that the North American tektite fragments and microtektites were hydrated in the marine environment (i.e., the H₂O was not trapped solely on quenching from a melt). The younger Ivory Coast and Australasian microtektites do not exhibit much evidence of hydration (at least not in excess of 0.5 wt% H₂O); this suggests that the degree of hydration increases with age. In addition, we find that some glass spherules (with <65 wt% SiO₂) from the upper Eocene clinopyroxene-bearing spherule layer in the Indian Ocean have palagonitized rims. These spherules appear to have been altered in a similar fashion to the splash form K/T boundary spherules. Thus, our data indicate that tektites and microtektites that generally contain >65 wt% SiO₂ can undergo simple hydration in the marine environment, while impact glasses (with <65 wt% SiO₂) can also undergo palagonitization.     

Radii and Albedos of four Trojan asteroids and Jovian satellites 6 and 7

Thermal radiation has been detected from four asteroids of the Trojan group, and J6 and J7, the brightest of the outer satellites of Jupiter. The six objects all have exceedingly low geometric albedos of 0.02 or 0.03 according to calculations based on their known visual brightness and the measured thermal fluxes. 624 Hektor, the largest object studied here, has a radius of 110 ± 20 km, though the exact shape of this body is in question. While the sample observed in this work is small (the total number of Trojans larger than 0.25 km in radius is about 1000), the fact that all four studied have similarly low albedos suggests that this property is characterisic of the Trojans and at least two of the outer members of Jupiter's retinue of satellites. The low surface albedo of the Trojans may preclude the proposed origin of the Jovian group of comets among these bodies according to E. Rabe. Updated tables of the dimensions of all the Jovian satellites are given.     

Uranus and Neptune: Shape and rotation

Both Uranus and Neptune are thought to have strong zonal winds with velocities of several 100 m s⁻¹. These wind velocities, however, assume solid-body rotation periods based on Voyager 2 measurements of periodic variations in the planets’ radio signals and of fits to the planets’ magnetic fields; 17.24 h and 16.11 h for Uranus and Neptune, respectively. The realization that the radio period of Saturn does not represent the planet’s deep interior rotation and the complexity of the magnetic fields of Uranus and Neptune raise the possibility that the Voyager 2 radio and magnetic periods might not represent the deep interior rotation periods of the ice giants. Moreover, if there is deep differential rotation within Uranus and Neptune no single solid-body rotation period could characterize the bulk rotation of the planets. We use wind and shape data to investigate the rotation of Uranus and Neptune. The shapes (flattening) of the ice giants are not measured, but only inferred from atmospheric wind speeds and radio occultation measurements at a single latitude. The inferred oblateness values of Uranus and Neptune do not correspond to bodies rotating with the Voyager rotation periods. Minimization of wind velocities or dynamic heights of the 1 bar isosurfaces, constrained by the single occultation radii and gravitational coefficients of the planets, leads to solid-body rotation periods of ∼16.58 h for Uranus and ∼17.46 h for Neptune. Uranus might be rotating faster and Neptune slower than Voyager rotation speeds. We derive shapes for the planets based on these rotation rates. Wind velocities with respect to these rotation periods are essentially identical on Uranus and Neptune and wind speeds are slower than previously thought. Alternatively, if we interpret wind measurements in terms of differential rotation on cylinders there are essentially no residual atmospheric winds.     

On universal elements,and conversion procedures to and from position and velocity

An element set is advocated that is familiar (in traditional terms), and yet applicable to every type of conic-section orbit without loss of accuracy. It is not free of singularity, but this is not a serious deficiency. Conversion procedures, to and from position and velocity, are outlined, with Fortran-77 listings appended. Tests have indicated that the errors in the pair of procedures are minimal, accuracy being limited only by computer precision and the (fixed) number of iterations used in the Kepler-equation solutions.