首页 | 本学科首页   官方微博 | 高级检索  
文章检索
  按 检索   检索词:      
出版年份:   被引次数:   他引次数: 提示:输入*表示无穷大
  收费全文   138篇
  免费   2篇
  国内免费   3篇
测绘学   3篇
大气科学   20篇
地球物理   29篇
地质学   74篇
海洋学   5篇
天文学   11篇
自然地理   1篇
  2018年   2篇
  2017年   4篇
  2016年   5篇
  2013年   4篇
  2012年   3篇
  2011年   8篇
  2010年   4篇
  2009年   5篇
  2008年   3篇
  2007年   5篇
  2005年   3篇
  2004年   6篇
  2003年   4篇
  2002年   3篇
  2001年   4篇
  2000年   3篇
  1997年   2篇
  1996年   2篇
  1994年   1篇
  1993年   1篇
  1991年   1篇
  1990年   2篇
  1987年   2篇
  1986年   3篇
  1985年   1篇
  1984年   5篇
  1983年   1篇
  1982年   2篇
  1981年   4篇
  1980年   4篇
  1979年   2篇
  1977年   1篇
  1976年   5篇
  1975年   2篇
  1974年   1篇
  1973年   1篇
  1972年   2篇
  1971年   4篇
  1970年   3篇
  1969年   7篇
  1968年   2篇
  1965年   1篇
  1964年   2篇
  1961年   1篇
  1960年   1篇
  1956年   1篇
  1955年   1篇
  1954年   1篇
  1953年   2篇
  1951年   1篇
排序方式: 共有143条查询结果,搜索用时 31 毫秒
1.
Three different methods are presented to subtract thermal drifts and low-frequency noise from the signal of infrared array. The first is dead pixels with open Indium bumps, the second is reference output as implemented on the Hawaii2 multiplexer, and the third is dark pixels to emulate reference cells having a capacity connected to the gate of the unit cell field-effect transistor (FET). The third method is the most effective and yields a reduction in readout noise from15.4–9.4 erms. A novel method will be described to extend this readout technique to the Aladdin 1 K × 1 K InSb array. This revised version was published online in July 2006 with corrections to the Cover Date.  相似文献   
2.
Tritium data were collected between 1985 and 1987 on several cruises of the German research icebreaker “Polarstern” to the Weddell Sea. Maximum tritium concentrations in the surface waters are of the order of 200 mTU. The minimum values observed in the Weddell Sea Deep Water at about 1000 m depth are about 15–40 mTU. The bottom waters show tritium concentrations of about 70–100 mTU in the central gyre, increasing to about 120 mTU in the northwestern corner of the Weddell Sea. The overflowing Ice Shelf Water observed on the continental slope west of the Filchner Depression has tritium concentrations close to those of the surface waters, indicating rapid renewal of this water mass. The data reflect the rapid renewal of the bottom waters in the northwestern corner of the Weddell Sea and the mixing of bottom water from this boundary current into the bottom waters of the central Weddell Gyre.  相似文献   
3.
Transient tracer data (tritium, CFC11 and CFC12) from the southern, central and northwestern Weddell Sea collected during Polarstern cruises ANT III-3, ANT V-2/3/4 and during Andenes cruise NARE 85 are presented and discussed in the context of hydrographic observations. A kinematic, time-dependent, multi-box model is used to estimate mean residence times and formation rates of several water masses observed in the Weddell Sea.Ice Shelf Water is marked by higher tritium and lower CFC concentrations compared to surface waters. The tracer signature of Ice Shelf Water can only be explained by assuming that its source water mass, Western Shelf Water, has characteristics different from those of surface waters. Using the transient nature of tritium and the CFCs, the mean residence time of Western Shelf Water on the shelf is estimated to be approximately 5 years. Ice Shelf Water is renewed on a time scale of about 14 years from Western Shelf Water by interaction of this water mass with glacial ice underneath the Filchner-Ronne Ice shelf. The Ice Shelf Water signature can be traced across the sill of the Filchner Depression and down the continental slope of the southern Weddell Sea. On the continental slope, new Weddell Sea Bottom Water is formed by entrainment of Weddell Deep Water and Weddell Sea Deep Water into the Ice Shelf Water plume. In the northwestern Weddell Sea, new Weddell Sea Bottom Water is observed in two narrow, deep boundary currents flowing along the base of the continental slope. Classically defined Weddell Sea Bottom Water (θ ≤ −0.7°C) and Weddell Sea Deep Water (−0.7°C ≤ θ ≤ 0°C) are ventilated from the deeper of these boundary currents by lateral spreading and mixing. Model-based estimates yield a total formation rate of 3.5Sv for new Weddell Sea Bottom Water (θ = −1.0°C) and a formation rate of at least 11Sv for Antarctic Bottom Water (θ = −0.5°C).  相似文献   
4.
Most of previous models suggest that the Central Asia Orogenic Belt grew southward in the Phanerozoic. However, in the Bayanhongor region in west-central Mongolia, volcanic arc, accretionary prism, ophiolite, and passive margin complexes accreted northeastward away from the Baydrag micro-continent, and hence the region constitutes the southwestern part of a crustal-scale syntaxis close to the west. The syntaxis should be original, because presumably reorientation due to strike-slip faulting can be ignored. It is reconfirmed that the Baydrag eventually collided with another micro-continent (the Hangai) to the northeast. A thick sedimentary basin developed along the southern passive margin of the Hangai micro-continent. This region is also characterized by an exhumed metamorphosed accretionary complex and a passive margin complex, which are both bounded by detachment faults as well as basal reverse faults which formed simultaneously as extrusion wedges. This part of the Central Asia Orogenic Belt lacks exhumed crystalline rocks as observed in the Himalayas and other major collisional orogenic belts. In addition, we identified two phases of deformation, which occurred at each phase of zonal accretion as D1 through Cambrian and Devonian, and a synchronous phase of final micro-continental collision of Devonian as D2. The pre-collisional ocean was wide enough to be characterized by a mid-ocean ridge and ocean islands. Two different structural trends of D1 and D2 are observed in accretionary complexes formed to the southwest of the late Cambrian mid-ocean ridge. That is, the relative plate motions on both sides of the mid-ocean ridge were different. Accretionary complexes and passive margin sediments to the northeast of the mid-ocean ridge also experienced two periods of deformation but show the same structural trend. Unmetamorphosed cover sediments on the accretionary prism and on the Hangai micro-continent experienced only the D2 event due to micro-continental collision. These unmetamorphosed sediments form the hanging walls of the detachment faults. Moreover, they were at least partly derived from an active volcanic arc formed at the margin of the Baydrag micro-continent.  相似文献   
5.
The computer operating system of the Gregory Coudé Telescope (GCT) at Observatorio del Teide is described. The GRECOS command language provides the user with a flexible means of operating both telescope and spectrograph, to execute complex measuring sequences, and to handle and display his observational data.Paper presented at the 11th European Regional Astronomical Meetings of the IAU on New Windows to the Universe, held 3–8 July, 1989, Tenerife, Canary Islands, Spain.  相似文献   
6.
Minor granulites (believed to be pre-Triassic), surrounded by abundant amphibolite-facies orthogneiss, occur in the same region as the well-documented Triassic high- and ultrahigh-pressure (HP and UHP) eclogites in the Dabie–Sulu terranes, eastern China. Moreover, some eclogites and garnet clinopyroxenites have been metamorphosed at granulite- to amphibolite-facies conditions during exhumation. Granulitized HP eclogites/garnet clinopyroxenites at Huangweihe and Baizhangyan record estimated eclogite-facies metamorphic conditions of 775–805 °C and ≥15 kbar, followed by granulite- to amphibolite-facies overprint of ca. 750–800 °C and 6–11 kbar. The presence of (Na, Ca, Ba, Sr)-feldspars in garnet and omphacite corresponds to amphibolite-facies conditions. Metamorphic mineral assemblages and PT estimates for felsic granulite at Huangtuling and mafic granulite at Huilanshan indicate peak conditions of 850 °C and 12 kbar for the granulite-facies metamorphism and 700 °C and 6 kbar for amphibolite-facies retrograde metamorphism. Cordierite–orthopyroxene and ferropargasite–plagioclase coronas and symplectites around garnet record a strong, rapid decompression, possibly contemporaneous with the uplift of neighbouring HP/UHP eclogites.

Carbonic fluid (CO2-rich) inclusions are predominant in both HP granulites and granulitized HP/UHP eclogites/garnet clinopyroxenites. They have low densities, having been reset during decompression. Minor amounts of CH4 and/or N2 as well as carbonate are present. In the granulitized HP/UHP eclogites/garnet clinopyroxenites, early fluids are high-salinity brines with minor N2, whereas low-salinity fluids formed during retrogression. Syn-granulite-facies carbonic fluid inclusions occur either in quartz rods in clinopyroxene (granulitized HP garnet clinopyxeronite) or in quartz blebs in garnet and quartz matrices (UHP eclogite). For HP granulites, a limited number of primary CO2 and mixed H2O–CO2(liquid) inclusions have also been observed in undeformed quartz inclusions within garnet, orthopyroxene, and plagioclase which contain abundant, low-density CO2±carbonate inclusions. It is suggested that the primary fluid in the HP granulites was high-density CO2, mixed with a significant quantity of water. The water was consumed by retrograde metamorphic mineral reactions and may also have been responsible for metasomatic reactions (“giant myrmekites”) occurring at quartz–feldspar boundaries. Compared with the UHP eclogites in this region, the granulites were exhumed in the presence of massive, externally derived carbonic fluids and subsequently limited low-salinity aqueous fluids, probably derived from the surrounding gneisses.  相似文献   

7.
New pseudosection modelling was applied to better constrain the P–T conditions and evolution of glaucophane‐bearing rocks in the Tamayen block of the Yuli belt, recognized as the world's youngest known blueschist complex. Based on the predominant clinoamphibole, textural relationships, and mineral compositions, these glaucophane‐bearing high‐P rocks can be divided into four types. We focused on the three containing garnet. The chief phase assemblages are (in decreasing mode): amphibole + quartz + epidote + garnet + chlorite + rutile/titanite (Type‐I), phengite + amphibole + quartz + garnet + chlorite + epidote + titanite + biotite + magnetite (Type‐II), and amphibole + quartz + albite + epidote + garnet + rutile + hematite + titanite (Type‐III). Amphibole exhibits compositional zoning from core to rim as follows: glaucophane → pargasitic amphibole → actinolite (Type‐I), barroisite → Mg‐katophorite/taramite → Fe‐glaucophane (Type‐II), glaucophane → winchite (Type‐III). Using petrographic data, mineral compositions and Perple_X modelling (pseudosections and superimposed isopleths), peak P–T conditions were determined as 13 ± 1 kbar and 550 ± 40 °C for Type‐I, 10.5 ± 0.5 kbar and 560 ± 30 °C for Type‐II (thermal peak) and 11 ± 1 kbar and 530 ± 30 °C for Type‐III. The calculations yield higher pressures and temperatures than previously thought; the difference is ~1–6 kbar and 50–200 °C. The three rock types record similar P–T retrograde paths with clockwise trajectories; all rocks followed trajectories with substantial pressure decrease under near‐isothermal conditions (Type‐I and Type‐III), with the probable exception of Type‐II where decompression followed colder geotherms. The P–T paths suggest a tectonic environment in which the rocks were exhumed from maximum depths of ~45 km within a subduction channel along a relative cold geothermal gradient of ~11–14 °C km?1.  相似文献   
8.
9.
Zusammenfassung Die Arbeit bringt alle Erfahrungen über Föhn in luftelektrischer Hinsicht, die im Laufe von fünf Jahren durch Registrierungen, Messungen und Beobachtungen vor allem im Raum des Wettersteingebirges bei Garmisch-Partenkirchen gewonnen wurden. Es stand hierfür ein Netz von sieben ständig betriebenen Stationen zur Verfügung, zwei weitere Stationen wurden 1958 während einer zweimonatigen Exkursion auf dem Zugspitzplatt (2600 m NN) unterhalten. Diese neun Stationen lagen in einigermaßen gleichmäßiger Höhenstaffelung zwischen 675 und 2963 m NN. Ihre Basisentfernungen waren relativ gering. Alle neun Stationen registrierten den luftelektrischen Potentialgradienten, vier der sieben ständigen sowie eine der beiden vorübergehenden Stationen registrierten zusätzlich den luftelektrischen Leitungsstrom. Als weitere Elemente des Komplexes Luftelektrizität und Aerosol wurden registriert bzw. gemessen: positive und negative Kleinionen, positive und negative Luftleitfähigkeit, natürliche und künstliche Radioaktivität der Luft, Kondensationskerne (Aitkenkerne), Luftverunreinigung, Spitzenstrom und Atmospherics. Ein tragendes Grundprinzip der Arbeit ist die synoptische Verwertung der Daten des relativ dichten und auch in die Vertikale reichenden Stationsnetzes, mit dessen Hilfe ein dreidimensionaler Ausschnitt der Atmosphäre überschaubar wird. Die Einheitlichkeit der verwendeten Methoden sowohl in der räumlichen als auch in der über Jahre gehenden zeitlichen Erstreckung trägt zur Festigung der Ergebnisse und Schlüsse bei.Aus dem Beobachtungsmaterial wird abgeleitet, daß Föhnlagen sich nicht dadurch auszeichnen, daß sich bestimmte luftelektrische Einzelgrößen dabei besonders oder außergewöhnlich verhalten würden. Typisch für den Föhn ist vielmehr ein ganz bestimmter Akkord der luftelektrischen (und meteorologischen) Elemente, wobei sich innerhalb des Stationsnetzes wiederum typische Variationen bemerkbar machen.Luftelektrisch gesehen, konnten zwei Föhntypen unterschieden werden: Bei Typ I sind die Kurven des Potentialgradienten und des Leitungsstromes sehr glatt, der Potentialgradient ist anhaltend erniedrigt, die Werte des Leitungsstromes und der Kleinionendichte sind erhöht. Kennzeichnend für Föhntyp II ist ein extrem unruhiger Verlauf der Potentialgradient- und Leitungsstromkurven bei stark erhöhten Werten an den Talstationen; er ist immer mit dem Vorkommen von Schneefegen an den Gebirgskämmen mehr oder weniger weit südlich der Registrierstationen gekoppelt. Häufig besteht bei Föhntyp II eine Bodeninversion.Für beide Föhntypen werden repräsentative Einzelbeispiele gebracht. Außerdem wurde das gesamte Beobachtungsmaterial der Jahre 1955 bis 1958 statistisch verarbeitet, um für die sieben Stationen, d. i. im Schnitt durch die Atmosphäre bis rund 3000 m NN, das luftelektrische und meteorologische Bild eines mittleren Föhntages für beide Typen abzuleiten. Die bei Föhn gesammelten Ergebnisse sind übrigens nicht nur zur Erweiterung unserer Vorstellungen über den Föhn an sich von Bedeutung, sondern geben auch Hinweise zu anderen geophysikalischen Problemen, so etwa auf dem Gebiet der Wolkenphysik (z. B. durch die Erfahrungen hinsichtlich der Ladungstrennung beim Zusammenprall und Zerbrechen von Eiskristallen), zur Frage der atmosphärischen elektrischen und elektromagnetischen Wellenvorgänge (durch Registrierungen von Stationen, die sich gerade in der Grenzschicht zwischen Föhn und positiv geladener, schwingender Inversionsoberseite befinden) sowie zur Frage des Ionisationsgleichgewichtes und der Beziehungen zwischen Kleinionen- und Kondensationskerndichte, denn in der Föhnströmung sind ja die Kondensationskerndichten besonders niedrig und außerdem ist—in den Nordalpen—die natürliche Luftradioaktivität während des Föhns erhöht.Bioklimatische Gesichtspunkte werden lediglich angedeutet.
Summary In this paper the author summarizes data, results of evaluations, and experiences in the field of atmospheric electricity, as far as connected with foehn situations. The observations were mainly made in the region of Garmisch-Partenkirchen (Wetterstein Mountains, Northern Alps) and cover a period of five years. Seven recording stations with heights between 675 and 2963 m above sea-level were operated permanently, two further stations were operated on the Zugspitzplatt (2600 m) during two months in 1958. All the nine stations have relatively small distances from each other. At each of the nine stations the atmospheric electrical potential gradient was recorded, at four of the permanent stations and at one of the temporary stations the air-earth current was recorded, too. Further there were recorded or measured positive and negative small ions, positive and negative conductivity, natural and artificial radioactivity of the air, condensation nuclei, air pollution, point discharge current, and sferics. A characteristic of this investigation is that a dense network of stations extending also in the vertical direction yields a synopsis of a small three-dimensional portion of the atmosphere, and that uniformly without interruptions through years.It is pointed out that a foehn situation is not distinguished by a special or extraordinary behaviour of single atmospheric electrical elements, but by a typical accord of the atmospheric electrical and meteorological elements, with typical spatial variations of them within the network.From the point of view of atmospheric electricity two main types of foehn were found: Type I shows lowered and smooth potential gradient curves at all stations, further increased and smooth curves of conduction current, increased concentrations of small ions, etc. Foehn of Type II, amongst other characteristics, shows increased and extremely agitated curves of potential gradient and conduction current at the valley stations. Type II is observed when there is drifting snow at the mountain ridges south of the recording stations and mainly in cases where the foehn current does not reach the bottom of the valley.Both types are illustrated here by examples. Beyond this, the data obtained at the seven permanent stations during four years were reduced to average foehn days of both types. The observations made during foehn, however, have interest not only for our knowledge of this weather situation itself but give results which are also important for studies on cloud physics (experience on charge separations caused by breaking and impact in drifting snow), on atmospheric electric and electromagnetic waves (records of stations just being in the boundary layer between foehn current and positively charged upper surface of an inversion), for the investigation of the ionization equilibrium and of the relations between the concentrations of small ions and condensation nuclei (there are special conditions because of the low concentrations of condensation nuclei in the foehn current and because of the increased natural radioactivity of air during foehn in our region), etc.Bioclimatological points of view are mentioned, only.

Résumé La présente étude groupe les résultats obtenus depuis cinq ans au sujet de l'aspect électrique du foehn grâce à des mesures faites dans la région du Wetterstein près de Garmisch-Partenkirchen où se trouvait un réseau de 7 stations fixes ainsi que 2 stations installées pendant une excursion de deux mois au Zugspitzplatt (2600 m.). Ces 9 postes étaient répartis entre 675 et 2693 m. et se trouvaient peu éloignés les uns des autres; tous enregistraient le gradient de potentiel, 5 le courant de conductibilité en sus. En outre on enregistrait ou mesurait: les petits ions positifs et négatifs, la conductibilité positive et négative, la radioactivité naturelle et artificielle de l'air, les noyaux de condensation, la pollution et les parasites. Le principe de base est l'utilisation des données du point de vue synoptique. L'uniformité des méthodes et leur application à longue échéance donne du poids aux résultats.On constate que les situations de foehn ne se distinguent pas par des valeurs extraordinaires des différentes grandeurs de l'électricité de l'air. Les éléments électriques et météorologiques présentent entre eux, par foehn, un accord caractéristique, tandis qu'à l'intérieur du réseau il y a des variations typiques. On peut distinguer deux types de foehn. Type I avec courbe lisse du gradient de potentiel et du courant de conductibilité; le gradient de potentiel est anormalement faible, le courant de conductibilité est accru ainsi que la densité des petits ions. Type II avec marche très agitée du gradient de potentiel et du courant (valeurs accrues aux stations basses); le foehn de type II est toujours accompagné de chasse-neige sur les crêtes au Sud; il y a souvent inversion au sol.Exemples des deux types de foehn. En outre tout le matériel d'observation des années 1955 à 1958 a été traité de façon à obtenir une image de l'état moyen de l'atmosphère jusqu'à 3000 m. pour les deux types. Les résultats trouvent également leur application à d'autres problèmes tels que la rupture de charge par heurts et bris de cristaux, les phénomènes concernant les ondes électromagnétiques, l'équilibre d'ionisation, la relation entre les petits ions et la densité des noyaux de condensation. Les points de vue biologiques ne sont qu'esquissés.


Mit 23 Textabbildungen

The research reported in this document has been sponsored in part by the Geophysics Research Directorate of the Air Force Cambridge Research Center, Air Research and Development Command, United States Air Force, under Contract AF 61 (514)-732-C, AF 61 (514)-949 and AF 61 (052)-55, through the European Office, ARDC.Die Auswertungen der Schönwetter-Registrierungen wurden durch Sachbeihilfen seitens der Deutschen Forschungsgemeinschaft möglich gemacht.Die Luftradioaktivitätsmessungen wurden aus Zuschüssen des Bundesministeriums für Atomkernenergie und Wasserwirtschaft an das Institut für Gesteinskunde der Universität München bestritten.  相似文献   
10.
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号