VGP角离散与地磁场低阶非轴向偶极子分量

虚地磁极（VGP）的角离散携带着地磁场低阶非轴向偶极子分量空间变化的重要信息．重申地球主磁场定解问题的适定性,指出McFadden等模型G存在重复计入轴向偶极子分量的内在矛盾;作为模型G基础的VGP角离散的偶极族-四极族分解仅具有数据拟合意义．证明,如果地磁场的非轴向偶极子分量相对轴向偶极子分量为小量,那么VGP角离散的纬度变化主要由轴向偶极子Gauss系数约化的低阶Gauss系数的平方和决定．因此作出估计,在过去5Ma中,赤道偶极子和赤道四极子的Gauss系数的幅度大致相当,约为轴向偶极子Gauss系数的10％．     

1950—1980年中国地区主磁场模型的建立及分析

本文根据丰富的地磁资料,用泰勒多项式方法推算出1950.0、1960.0、1970.0和1980.0年中国地区的主磁场模型,绘制出各个年代地磁要素的等值线图,分析研究了局部地区地磁场泰勒多项式模型的特点.     

地磁暴与电离层骚扰的关系

一、引言 太阳活动区喷发出的粒子流引起太阳风对地球磁场和电离层作用,从而发生地磁暴和电离层骚扰,所以它们的发生是与太阳活动有着密切的关系。但是,在地磁暴期间常常伴随着电离层F_2层骚扰,即峰值电子密度相对于中值有大的减少或增加。     

贺兰山群层序及主变形期褶皱构造探讨

本文对贺兰山群由下到上划分为阿楞呼都格变粒岩组、柳树沟片麻岩组和秃鲁根钙硅酸粒岩－大理岩组。主变形期的构造事件为在南倾的北东东向倒转复式褶皱上发育着与其平行的区域性轴面面理、线理和逆冲型同变质韧性剪切带，其中又以塔什沟－柳树沟复背形和秃鲁根向形最具代表性。     

持续光照下光强对北极海域芬迪亚历山大藻生长及产毒的影响

以格陵兰岛西部、冰岛沿海和楚科奇海的芬迪亚历山大藻为受试对象,并以缅因湾的芬迪亚历山大藻藻株做为参照,从沉积物或海水中的休眠孢囊或营养细胞中分离到12株目标藻种,并在实验室建立纯培养系。然后对这些地域的藻种在不同光照下生长特性的比较、对毒素含量进行研究,发现芬迪亚历山大藻在持续光照条件下最适的生长光强范围是38—91μmol×m~(–2)×s~(–1)。另外,在所有分离到的12株藻细胞中均未检测到脱氨甲酰基膝沟藻毒素2(dc GTX2),大部分藻细胞都在光强较强时,即生长速率低时表现出更高的细胞毒素含量和毒性。     

1945—1995年国际参考地磁场

本文回顾了国际参考地磁场(IGRF)的建立和修改过程;介绍了最新的IGRF模型,即第六代国际参考地磁场;综述了国际参考地磁场在地磁学中的应用,并指出了在使用过程中需要注意的一些问题.     

1950-1980年中国地区主磁场模型的建立及分析

本文根据丰富的地磁资料,用泰勒多项式方法推算出1950.0、1960.0、1970.0和1980.0年中国地区的主磁场模型,绘制出各个年代地磁要素的等值线图,分析研究了局部地区地磁场泰勒多项式模型的特点.     

Fabric controls on strain accommodation in naturally deformed mylonites: The influence of interconnected micaceous layers

We present microstructural analyses demonstrating how the geometrical distribution and interconnectivity of mica influences quartz crystallographic preferred orientation (CPO) development in naturally deformed rocks. We use a polymineralic (Qtz + Pl + Kfs + Bt + Ms ± Grt ± Tur) mylonite from the Zanskar Shear Zone, a section of the South Tibetan Detachment (NW Himalaya), to demonstrate how quartz CPO intensity decreases from quartz-dominated domains to micaceous domains, independently of whether or not quartz grains are pinned by mica grains. We then use a bimineralic (Qtz + Ms) mylonite from the Main Central Thrust (NW Himalaya) to show how increasing mica grain connectivity is concomitant with a systematic weakening of quartz CPO. Our results draw distinctions between CPO weakening due to: (i) second phase drag, leading to ineffective recovery in quartz; and (ii) increased transmission and localisation of strain between interconnected mica grains. In the latter case, well-connected micaceous layers take up most of the strain, weakening the rock and preventing straining of the stronger quartz matrix. Our findings suggest that rock weakening in quartz-rich crustal rocks is influenced not only by the presence of mica-rich layers but also the degree of mica grain connectivity, which allows for more effective strain localization through the entire rock mass.     

饲料中主要能量物质对大菱鲆幼鱼生长的影响

于1999年6－8月，采用正交设计统计方法，对主要能量物质蛋白质、脂肪和糖类对大菱Ping幼鱼生长的影响进行研究。利用L16（4^3）正交设计了16组大菱Ping幼鱼饲料，在各级饲料中，蛋白质、脂肪和糖类的含量范围分别为36％－45％、8％－20％和0％－6％，共进行了60d的喂养实验，并对饲料及鱼体成分进行分析测定。结果表明，各主要能量物质对鱼体增重和配合饲料转化率的影响顺序为蛋白质＞糖类＞脂肪，且蛋白质的变化对增重率的影响极显著，对饲料转化率的影响显著。     

Metamorphic P–T profile and P–T path discontinuity across the far‐eastern Nepal Himalaya: investigation of channel flow models

Thermobarometric data and compositional zoning of garnet show the discontinuities of both metamorphic pressure conditions at peak‐T and P–T paths across the Main Central Thrust (MCT), which juxtaposes the high‐grade Higher Himalayan Crystalline Sequences (HHCS) over the low‐grade Lesser Himalaya Sequences (LHS) in far‐eastern Nepal. Maximum recorded pressure conditions occur just above the MCT (～11 kbar), and decrease southward to ～6 kbar in the garnet zone and northward to ～7 kbar in the kyanite ± staurolite zone. The inferred nearly isothermal loading path for the LHS in the staurolite zone may have resulted from the underthrusting of the LHS beneath the HHCS. In contrast, the increasing temperature path during both loading and decompression (i.e. clockwise path) from the lowermost HHCS in the staurolite to kyanite ± staurolite transitional zone indicates that the rocks were fairly rapidly buried and exhumed. Exhumation of the lowermost HHCS from deeper crustal depths than the flanking regions, recording a high field pressure gradient (～1.2–1.6 kbar km^?1) near the MCT, is perhaps caused by ductile extrusion along the MCT, not the emplacement along a single thrust, resulting in the P–T path discontinuities. These observations are consistent with the overall scheme of the model of channel flow, in which the outward flowing ‘HHCS’ and inward flowing ‘LHS’ are juxtaposed against each other and are rapidly extruded together along the ‘MCT’. A rapid exhumation by channel flow in this area is also suggested by a nearly isothermal decompression path inferred from cordierite corona surrounding garnet in gneiss of the upper HHCS. However, peak metamorphic temperatures show a progressive increase of temperature structurally upward (～570–740 °C) near the MCT and roughly isothermal conditions (～710–810 °C) in the upper structural levels of the HHCS. The observed field temperature gradient is much lower than those predicted in channel flow models. However, the discrepancy could be resolved by taking into account heat advection by melt and/or fluid migration, as these can produce low or nearly no field temperature gradient in the exhumed midcrust, as observed in nature.