565 resultados para fission
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In the framework of the generalized liquid drop model (GLDM) and improved Royer's formula, we investigate the branching ratios and half-lives of alpha-decay to the members of the ground-state rotational bands of heavy even-even Fm and No isotopes. The calculated results are in good agreement with the available experimental data and some useful predictions are provided for future experiments.
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新核素的合成及衰变性质的研究一直是核物理科学的前沿领域,它对于人类拓广对原子核运动规律的认识有着十分重要的意义。本文首先概述了新核素合成的意义、方法,并简要阐述了一种奇异的衰变方式—β~-延发裂变,为实验部分的论述提供理论基础。在实验部分,本文阐述了用放射化学方法研究了钍、钡、镭等复杂反应产物的化学分离。通过在Th的分离中引用PMBP萃取和反萃体系,并采用氧化还原体系有效地去除了绝大多数杂质元素,特别是非常好的去除了碘和溴离子的沾污,较好地完成了Th与其它反应产物的分离。对Ba、Ra的分离主要采用快速的阳离子交换流程,达到了满意的分离效果。对用中能~(18)O离子束照射铀、钍的反应产物进行分离,对分离出的钍、钡、镭样品进行了γ(X)单谱和时间序列谱测量。并对记录下来的样品的谱图进行了分析。使用上述方法,我们在兰州重离子加速器(HIRFL)上用~(18)O离子照射重铀酸铵靶,通过多核子转移反应,首次合成并鉴别了新核素不相识~(238)Th。 同时通过不同的反应道产生~(237)Th,并对~(237)Th的半衰期进行了测定;在HIRFL上用~(18)O离子照射氧化钍靶对~(230)Ra的子体~(230)Ac的β~-延发裂变现象进行了观测,在被Ra样品爆光的云母径迹探测器上观察到了两个裂变径迹,从ThO_2靶中用三次BaCl_2沉淀法分离出钡、使用γ谱学这技术测定了十多个Ba的放射性同位素的截面。
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第一部分:β延发裂变(βDF)是一种稀有的核衰变模式,它在天体物理学和研究中具有重要价值;为研究远离β稳定线核素提供了可能性,是研究新核素合成的新台阶.第二部分:采用放射化学分离法从中能<'18>O离子辐照过的天然铀靶以及钍靶中分离出放射性Ba同位素,用高分辨的HPGe探测器测量Ba部分的γ射线谱,对测得的时间累计谱进行分析,用常规的计算产额生成截面的方法得到了Ba同位素的生成截面,并对其中的一些截面数据进行了讨论.第三部分:在中子发生器上用14-15MeV的中子轰击天然白金箔,通过<'198>Pt(n,2p)反应产生<'197>Os.使用两台HPGe探测器做γ(X)单谱和X-γ-t符合测量.对测得的数据进行了分析,结果显示我们合成并鉴定了新丰中子同位素<'197>Os,确定它的半衰期为2.8±0.5min.第四部分:用<'133>Ba作示踪剂对Ba在不锈钢片上的分子镀进行了研究.对在异丙醇溶液中的影响Ba分子镀的因素:电镀时间和电流密度等做了条件实验.在电流密度为4.0~6.0mA/cm<'2>,沉积时间30min的实验条件下,可在不锈钢片上获得厚度为0.5~1.0mg/cm<'2>的Ba镀层,也确定了Ba的电镀效率.
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本文基于改进的同位旋相关的量子分子动力学(ImIQMD)[1]模型对于反应系统48Ca+208Pb准裂变机制进行了研究。通过计算俘获截面、准裂变碎片质量分布等,并与实验结果进行了比较,我们认为ImIQMD模型对低能重系统准裂变反应的描述基本是合理的。 并合模型是判定碎片的经典模型,但是应用这个模型来判定核子集团会遇到一些困难,因为碎片之间往往相互离得较远,而核子集团之间相互距离相比之下很近。本文第四章对此给出了详细的讨论,提出了对原算法的改进,以及新的算法。 微观动力学模型的发展使得我们可以更细致地了解物理过程之中核子的运动,但是对于重系统而言,直接在核子尺度上来讨论具体的物理问题是十分繁杂的,因为不但核子数众多,而且核子间还存在强烈的相互作用。在这种情况下,根据研究需要定义核子集团的判定标准,而后得到核子集团分布,不但可以使“新的组成”数目减少,而且相互之间的作用强度也会下降,这就降低了处理的繁杂程度,并且与实验现象可以更接近。本文在第四章之中基于这个思想讨论了一些问题
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对品字型、拉长双脖型及级联三分裂的位势进行了计算。发现在有限温度下,品字型三分裂与级联三分裂、拉长双脖子三分裂相比,形变位能上并不是最优的。实验测量结果表明热核的能级密度参数是核温度的函数并与核大小有关,或激发能形式的变化。在25MeV/u Ar+Au的对心碰撞中,激发能已接近多重碎裂的“准相变区”
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本文首先回顾了重离子物理学的发展简史,并介绍了当前的一些关于重离子反应的理论方法,同时对于现在核物理的研究热点,热核的特性进行了概括性的叙述.由于裂变是作者工作的重点,因此在文章中,对裂变反应的理论也进行了介绍.为了能够清楚全面的说明我们的工作,本文对于实验装置和探测器也给出了详细的描述.最后,文章对25 MeVu Ar+Bi反应中的裂变进行了讨论.在这些讨论中,我们分析了反应中与裂变相关的数据,得到了碎片的质量,动能分布。同时运用与碎片相关联的4He粒子能谱提取了核温度和裂前裂后的4He粒子多重性,并利用这一数据计算了不同初始激发能下的裂点激发能和裂变时标.
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In this study, varieties of lipid bilayer-protected gold nanoparticles (AuNPs) were synthesized through a simple wet chemical method, and then the effect of freeze-thawing on the as-prepared AuNPs was investigated. The freeze-thawing process induced fusion or fission of lipid bilayers tethered on the AuNPs. The UV-vis spectra and transmission electron microscopy experiments revealed that the disruption of lipid bilayer structures on the nanoparticles led to the fusion or aggregation of AuNPs.
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Firstly, established sequence stratigraphy of Sinian System-Middle Triassic Series framework in Sichuan basin,be divided into 21 second-level sequence stratigraphy and 105 third-level sequence stratigraphy.From many aspects,discussed sequence stratigraphy characteristic. On the foundation of structure unconformity and fission track analysis, on the ground of An county-Shuinin county regional seismic section, using the positive evolution equilibrium principle technology, comprehensivly be mapped structure evolution of Sichuan basin. It can be divided into seven stages, that is :Pre-Sinian basement stage, cratonic depression basin(Z1-S)stage, cratonic rifted basin(D-T2)stage, passive continental margin(T3x1-3)stage, foreland basin(T3x4-6)stage, depression basin (Jurassic Period-Miocene Epoch) stage, formed basin (Holocene Epoch) stage. Analysis on structure evolution history,burial history,source rocks thermal evolution history, Maoba changxing formation gas pool forming process can be classified into four stages: ancient lithological oil pool stages in Indosinian-early Yanshanian period(T-J1-2), ancient structure- lithological gas pool stages in middle Yanshanian period(J3-K1), structure- lithological gas pool setting stages in last Yanshanian period(K2), structure- lithological gas pool adjusting and transformation stages in Himalayan period(R-Q). Maoba feixianguan formation gas pool forming process can be classified into two stages: second structure gas pool stages in last Yanshanian period(K2),second structure gas pool physical adjusting and transformation stages in Himalayan period(R-Q),and summarize reservoir formation model. On the base of newest exploration achievement and petroleum geologic comprehensive research , demonstrate how structure controls hydrocarbon accumulation. Structure controlling source rocks behaves structure controlling main source rocks’sedimentary facies, medium-large pools mainly located at center or margin of hydrocarbon generation. Structure controlling palaeo-karst reservoirs ,reef and beach facies reservoirs, fault and fracture reservoirs. Structure controlling palaeo-uplift, and palaeo-uplift controlling hydrocarbon migration, active reservoirs’forming, palaeo-structure traps forming. Structure controls distribution of mudstone and gypsolith, controls preservation. Structure controls hydrocarbon conducting, structure traps forming and hydrocarbon accumulation. Whether or no, Structure controls total process of basin forming-source rocks’generation- hydrocarbon accumulation. It is direct effect results of structure movements that large traps’ conditions, conducting migration conditions, high quality preservation. source rocks’condition and reservoirs’ condition are the indirect effect results. In the last analysis, “source rock controlling theory”, “high quality reservoir mainly controlling theory”, “palaeo-uplift controlling theory” and “current structure deciding theory” are structure controlling hydrocarbon accumulation. There are high variability and complex mechanisms in Sichuan basin , but the regional hydrocarbon accumulation conditions are very well, such as abundant source rocks, matching process of hydrocarbon accumulation and many exploration areas. By means of integrated analysis, put forward hydrocarbon exploration direction and large-middle targets of China Petroleum and Chemical Corporation .Thus, more and more hydrocarbon proved reserve and output in Sichuan basin will be contributed to China energy industry in a long future time.
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The West Shandong Uplift and its adjacent basins, with same evolutional history before Mesozoic, are an important basin-orogenic systems in North China. After late Mesozoic, tectonic differentiation between basin and orogenic belt gradually displayed in the study area. The Boxing sag is a part of Jiyang Depression near to West Shandong Uplift, in which the whole Mesozoic and Cenozoic strata are preserved. Based on the analysis of sedimentary records in the Boxing sag, the Cenozoic structural and sedimentary evolutions in Boxing Sag and its response to Western Shandong uplift are discussed in this dissertation. The main conclusions in this research are presented as follows. Based on Seismic and well logging profile interpretation, fault growth index, thickness difference between bottom wall and top wall and fault activity rate from Eocene to Pliocene are studied. Boxing sag had three main faults, NE, NW and NEE trending faults. Research shows that the activity of the NW trending fault in the Boxing sag became weaken from E1-2S4 to N2m gradually. The evolution of NE and the NEE trending fault can be divided into three episodes, from E1-2k to E2s4, from E2s3 to E3s1, from N2m to E3d. The analysis of Paleogene samples of heavy mineral assemblages shows that metamorphic rocks represented by garnet, intermediate-acid igneous rocks represented by the assemblage of apatite, zircon and tourmaline became less from E1-2k to N2g, and sedimentary rocks represented by the assemblage of pyrite, barite and limonite also became less. Intermediate-basic igneous rocks represented by the assemblage of leucoxene, rutile and ilmenite and metamorphic rocks represented by epidote became more and more. Electronic microprobe analysis shows that glaucophane and barroisite are existed in Kongdian Formation and the 4th member of Shahejie Formation, and they demonstrate that Western Shandong and Eastern Shandong are all the source regions of the Boxing Sag, and they also indicate that oceanic crust existed before the collision between the Yangtze and North China continent. The fact that Eastern Shandong is the source region of Boxing Sag also indicates that Western Shandong was not high enough to prevent sediment from Eastern Shandong at E1-2k and E2s4. The results of the dating of five detrital zircons of Boxing Sag show Kongdian Formation and the 4th member of Shahejie Formation have the age peaks of 2800Ma and 700-800. It means that Eastern Shandong is the source region of Boxing Sag at early Paleogene and Western Shandong is not high enough to prevent the sediment from Eastern Shandong. The ages of 160-180 and 220-260 Ma, which exist in the Guantao Formation and Paleogene, are common in Eastern Shandong and rare in Western Shandong,and it implied that Western Shandong is a low uplift at 24Ma. The Paleogene strata have almost same age groups, while the Guantao Formation has significant variations of age groups, and this indicates that Boxing Sag and Western Shandong uplift had taken place tremendous changes. The results of apatite fission track in Boxing sag show that three times uplifts happened at the source region at 60 Ma, 45Ma and 15Ma respectively, and the Boxing sag experienced two subsidences at 60Ma, 45Ma and one uplift at 20Ma.
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The Eastern Himalayan Syntaxis (EHS) is one of the strongest deformation area along the Himalayan belt resulted from the collision between Indian plate and the Eurasian Plate since the 50~60Ma, and has sensitivity tracked and preserved the whole collisional processes. It should depend on the detail geological investigations to establish the deformational accommodate mode, and the uplift history, to elucidate the deep structure and the crust-mantle interaction of the Tibet Plateau of the EHS. The deep-seated (Main Mantle Thrusts) structures were exhumed in the EHS. The MMT juxtapose the Gangdese metamorphic basement and some relic of Gangdese mantle on the high Himalayan crystalline series. The Namjagbawa group which is 1200~1500Ma dated by U/Pb age of zircon and the Namla group which is 550Ma dated by U/Pb age of zircon is belong to High Himalayan crystalline series and Gangdese basement respectively. There is some ophiolitic relic along the MMT, such as metamorphic ocean mantle peridotite and metamorphic tholeiite of the upper part of ocean-crust. The metamorphic ocean mantle peridotites (spinel-orthopyroxene peridotite) show U type REE patterns. The ~(87)Sr/~(86)Sr ratios were, 0.709314~0.720788, and the ~(143)Nd/~(144)Nd ratios were 0.512073~0.512395, plotting in the forth quadrant on the ~(87)Sr/~(86)Sr-~(143)Nd/~(144)Nd isotope diagram. Some metamorphic basalt (garnet amphibolite) enclosures have been found in the HP garnet-kynite granulite. The garnet amphibolites can be divided two groups, the first group is deplete of LREE, and the second group is flat or rich LREE, and their ~(87)Sr/~(86)Sr, ~(143)Nd/~(144)Nd ratios were 0.70563~0.705381 and 0.512468~0.51263 respectively. Trace element and isotopic characteristics of the garnet amphibolites display that they formed in the E-MORB environment. Some phlogolite amphibole harzburgites, which exhibit extensive replacement by Phl, Amp, Tc and Dol etc, were exhumed along the MMT. The Phl-Amp harzburgites are rich in LREE and LILE, such as Rb, K etc, and depletes Eu (Eu~* = 0.36 ~ 0.68) and HFSE, such as Nb, Ta, Zr, Hf, P, Ti etc. The trace element indicate that the Phl-Amp harzburgites have island arc signature. Their ~(87)Sr/~(86)Sr are varied from 0.708912 to 0.879839, ~(143)Nd/~(144)Nd from 0.511993 to 0.512164, ε Nd from- 9.2 to - 12.6. Rb/Sr isochrone age of the phlogolite amphibole harzburgite shows the metasomatism took place at 41Ma, and the Amp ~(40)Ar/~(39)Ar cooling age indcate the Phl-Amp harzburgite raising at 16Ma. There is an intense crust shortening resulted from the thrust faults and folds in the Cayu block which is shortened more 120km than that of the Lasha block in 35~90Ma. With the NE corner of the India plate squash into the Gangdese arc, the sinistral Pai shear fault and the dextral Aniqiao shear fault on the both sides of the Great bent of Yalun Zangbu river come into active in 21~26Ma. On the other hand, the right-lateral Gongrigabu strike-slip faults come into activity at the same period, a lower age bound for the Gongrigabu strike-slip fault is estimated to be 23~24Ma from zircon of ion-probe U/Pb thermochronology. The Gongrigabu strike-slip faults connect with the Lhari strike-slip fault in the northwestern direction and with the Saganing strike-slip at the southeastern direction. Another important structure in the EHS is the Gangdese detachment fault system (GDS) which occurs between the sedimental cover and the metamorphic basement. The lower age of the GDS is to be 16Ma from the preliminary 40Ar/39Ar thermochronology of white mica. The GDS is thought to be related to the reverse of the subducted Indian crust and the fast uplift of the EHS. Structural and thermochronology investigation of the EHS suggest that the eastern Tibet and the western Yunnan rotated clockwise around the EHS in the period of 35~60Ma. Later, the large-scale strike-slip faults (RRD, Gaoligong and Saganing fault) prolongate into the EHS, and connect with the Guyu fault and Gongrigabu fault, which suggest that the Indianchia block escape along these faults. Two kind of magmatic rocks in the EHS have been investigated, one is the mantle-derived amphibole gabbro, dioposide diorite and amphibole diorite, another is crust origin biotit-garnet adamellite, biotit-garnet granodiorite and garnet-amphibole-biotite granite. The amphibole gabbro dioposite diorite and amphibole diorite are rich in LREE, and LILE, such as Ba, Rb, Th, K, Sr etc, depleted in HFSE, such as Nb, Ta, Zr, Hf, Ti etc. The ratio of ~(87)Sr/~(86)Sr are from 0.7044 to 0.7048, ~(143)Nd/~(144)Nd are from 0.5126 to 0.5127. The age of the mantle origin magamatic rocks, which result from the partial melt of the raising and decompression anthenosphere, is 8Ma by ~(40)Ar/~(39)Ar dating of amphibole from the diorite. The later crust origin biotite-garnet adamellite, biotite-garnet granodiorite and garnet-amphibole-biotite granite are characterized by aboudance in LREE, and strong depletion of Eu. The ratios of ~(87)Sr-~(86)Sr are from 0.795035 to 0.812028, ~(143)Nd/~(144)Nd from 0.51187 to 0.511901. The ~(40)Ar/~(39)Ar plateau age of the amphibole from the garnet-amphibole-biotite granite is 17.5±0.3Ma, and the isochrone age is 16.8±0.6Ma. Their geochemical characteristics show that the crust-derived magmatic rocks formed from partial melting of the lower curst in the post-collisional environment. A group of high-pressure kaynite-garnet granulites and enclave of high-pressure garnet-clinopyroxene grnulites and calc-silicate grnulites are outcroped along the MMT. The peak metamorphic condition of the high-pressure granulites yields T=800~960 ℃, P=1.4~1.8Gpa, corresponding the condition of 60km depth. The retrograde assemblages of the high-pressure grnulites occur at the condition of T=772.3~803.3 ℃, P=0.63~0.64Gpa. The age of the peak metamorphic assemblages are 45 ~ 69Ma indicated by the zircon U/Pb ion-plobe thermochronology, and the retrograde assemblage ages are 13~26Ma by U/Pb, ~(40)Ar/~(39)Ar thermochronology. The ITD paths of the high-pressure granulites show that they were generated during the tectonic thickening and more rapid tectonic exhumation caused by the subducting of the Indian plate and subsequent break-off of the subducted slab. A great deal of apatite, zircon and sphene fission-track ages, isotopic thermochronology of the rocks in the EHS show that its rapid raising processes of the EHS can be divided into three main periods. There are 35~60Ma, 13~25Ma, 0~3Ma. 3Ma is a turn in the course of raising in the EHS which is characterized by abruptly acceleration of uplifting. The uplift ratios are lower than 1mm .a~(-1) before 3Ma, and higher than 1mm .a~(-1) with a maximum ratio of 30mm .a~(-1) since 3Ma. The bottom (knick point) of the partial anneal belt is 3.8km above sea level in the EHS, and correspond to age of 3Ma determined by fission-track age of apatite. The average uplift ratio is about 1.4 mm .a~(-1) below the knick point. The EHS has raised 4.3km from the surface of 2.36km above sea level since 3Ma estimated by the fossil partial anneal belt of the EHS. We propose a two-stage subduction model (B+A model) basing on Structural, thermochronological, magmatical, metamorphic and geophysical investigations of the EHS. The first stage is the subduction of the Indian continental margin following after the subduction of the Tethys Ocean crust and subsequent collision with the Gangdese arc, and the second stage is the Indian crust injecting into the lower crust and upper mantle of the Tibet plateau. Slab break-off seems to be occurred between these two stages.
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Based on the temperature data from 196 wells and thermal conductivity measurements of 90 rock samples, altogether 35 heat flow data are obtained. The results show that the Junggar basin is a relatively "cold basin" at present. The thermal gradients vary between 11.6 and 26.5 ℃/km, and the thermal conductivity change from 0.17 to 3.6 W/mK. Heat flow ranges from 23.4 to 53.7 mW/m~2 with a mean of 42.3 ± 7.7 mW/m~2. The heat flow pattern shows that heat flow is higher on the uplifts and lower on the depressions. The overall low present-day heat flow in the Junggar Basin reflects its stable cratonic basement and Cenozoic tectonothermal evolution characterized by lithospheric thickening, thrust and fault at shallow crust as well as consequently quick subsidence during the Late Cenozoic. The study of the basin thermal history, which is one of the important content of the basin analysis, reveals not only the process of the basin's tectonothermal evolution, but also the thermal evolution of the source rocks based on the hydrocarbon generation models. The latter is very helpful for petroleum exploration. The thermal history of the Junggar basin has been reconstructed through the heat flow based method using the VR and Fission track data. The thermal evolutions of main source rocks (Permian and Jurassic) and the formations of the Permian and the Jurassic petroleum systems as well as the influences of thermal fields to petroleum system also have been discussed in this paper. Thermal history reconstruction derived from vitrinite reflectance data indicates that the Paleozoic formations experienced their maximum paleotemperature during Permian to Triassic with the higher paleoheat flow of around 70-85 mW/m~2 and the basin cooled down to the present low heat flow. The thermal evolution put a quite important effect on the formation and evolution of the petroleum system. The Jurassic petroleum system in the Junggar basin is quite limited in space and the source rocks of Middle-Lower Jurassic entered oli-window only along the foreland region of the North Tianshan belt, where the Jurassic is buried to the depth of 5-7 km. By contrast, the Middle-Lower Permian source rocks have initiated oil and gas generation in latter Permian to Triassic, and the major petroleum systems, like Mahu-West Pen 1 Well, was formed prior to Triassic when later Paleozoic formation reached the maximum paleotemperature.
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As an important part of petroleum exploration areas in the west of China, the north part of Qaidam basin is very promising in making great progress for petroleum discovery. But there are still many obstacles to overcome in understanding the process of petroleum formation and evaluation of oil & gas potential because of the complexity of geological evolution in the study area. Based upon the petroleum system theory, the process of petroleum formation is analyzed and the potential of oil & gas is evaluated in different petroleum systems by means of the modeling approach. The geological background for the formation of petroleum systems and the consisting elements of petroleum systems are described in detail. The thickness of strata eroded is estimated by means of vitrinite reflectance modeling, compaction parameter calculating and thickness extrapolating. The buried histories are reconstructed using the transient compaction model, which combines of forward and reverse modeling. The geo-history evolution consists of four stages - sedimentation in different rates with different areas and slow subsidence during Jurassic, uplifting and erosion during Cretaceous, fast subsidence during the early and middle periods of Tertiary, subsidence and uplifting in alternation during the late period of Tertiary and Quaternary. The thermal gradients in the study area are from 2.0 ℃/100m to 2.6 ℃/100m, and the average of heat flow is 50.6 mW/m~2. From the vitrinite reflectance and apatite fission track data, a new approach based up Adaptive Genetic Algorithms for thermal history reconstruction is presented and used to estimate the plaeo-heat flow. The results of modeling show that the heat flow decreased and the basin got cooler from Jurassic to now. Oil generation from kerogens, gas generation from kerogens and gas cracked from oil are modeled by kinetic models. The kinetic parameters are calculated from the data obtained from laboratory experiments. The evolution of source rock maturation is modeled by means of Easy %Ro method. With the reconstruction of geo-histories and thermal histories and hydrocarbon generation, the oil and gas generation intensities for lower and middle Jurassic source rocks in different time are calculated. The results suggest that the source rocks got into maturation during the time of Xiaganchaigou sedimentation. The oil & gas generation centers for lower Jurassic source rocks locate in Yikeyawuru sag, Kunteyi sag and Eboliang area. The centers of generation for middle Jurassic source rocks locate in Saishenteng faulted sag and Yuka faulted sag. With the evidence of bio-markers and isotopes of carbonates, the oil or gas in Lenghusihao, Lenghuwuhao, Nanbaxian and Mahai oilfields is from lower Jurassic source rocks, and the oil or gas in Yuka is from middle Jurassic source rocks. Based up the results of the modeling, the distribution of source rocks and occurrence of oil and gas, there should be two petroleum systems in the study area. The key moments for these two petroleum, J_1-R(!) and J_2-J_3, are at the stages of Xiaganchaigou-Shangyoushashan sedimentation and Xiayoushashan-Shizigou sedimentation. With the kinetic midels for oil generated from kerogen, gas generated from kerogen and oil cracked to gas, the amount of oil and gas generated at different time in the two petroleum systems is calculated. The cumulative amount of oil generated from kerogen, gas generated from kerogen and gas cracked from oil is 409.78 * 10~8t, 360518.40 * 10~8m~3, and 186.50 * 10~8t in J_1-R(!). The amount of oil and gas generated for accumulation is 223.28 * 10~8t and 606692.99 * 10~8m~3 in J_1-R(!). The cumulative amount of oil generated from kerogen, gas generated from kerogen and gas cracked from oil is 29.05 * 10~8t, 23025.29 * 10~8m~3 and 14.42 * 10~8t in J_2-J_3 (!). The amount of oil and gas generated for accumulation is 14.63 * 10~8t and 42055.44 * 10~8m~3 in J_2-J_3 (!). The total oil and gas potential is 9.52 * 10~8t and 1946.25 * 10~8m~3.
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East China Sea Shelf Basin (ECSSB), as a basin with prospect of oil & gas resource and due to its special geological location on the west margin of the west Pacific, attracts a lot of attention from many geologists in the world.Based on systematic temperature measurements, bottom hole temperature (BHT) and the oil temperature data, the geothermal gradients in the ECS SB are calculated and vary from 25 to 43°C/km, with a mean of 32.7°C/km. The geothermal gradient in Fuzhou Sag has the higher value(40.6°C/km) in Taibei Depression than that in others. The lower value (27.2 °C/km) occurs in in Xihu Depression. The middle values occurs in Jiaojiang and Lishui sags in Taibei Depression with a mean value of 34.8 °C/km. Incorporated with the measured thermal conductivity, heat flow values show that the ECSSB is characterized by present-day heat flow around 70.6mW/m2, varying between 55 and 88 mW/m2. No significant difference in heat flow is observed between the Xihu and the Taibei Depressions. These heat flow data suggest that the ECSSB is geothermally not a modem back-arc basin.Applying the paleogeothermal gradient based method, thermal history is reconstructed using vitrinite reflectance (VR) and apatite fission track (AFT) data. The results suggest that the thermal history was different in the Taibei and the Xihu depressions. Paleo-heat flow values when the pre-Tertiary formations experienced their maximum temperature at the end of the Paleocene reached a mean of 81 mW/m2 in the Taibei Depression, much higher than the present-day value. The lower Tertiary sediments in the Xihu Depression experienced maximum temperatures at the end of Oligocene and reached a mean paleo-heat flow value of 83.4 mW/m2. The time, when the paleo-heat flow reached the maximum value, suggests that the ECSSB rifted eastward.Tectonic subsidence analysis shows that the timing of the major rifting episode was different across the ECSSB. The rifting occurred from the Late Cretaceous to the early Eocene in the Taibei Depression, followed by thermal subsidence from the late Eocene to the end of Miocene. In contrast, in the Xihu Depression the initial subsidence lasted until the early Miocene and thermal subsidence to the end of Miocene. From Pliocene to the present, an accelerated subsidence took place all along the West Pacific margin of the east Asia.The thermal lithosphere thickness is determined by temperature profile in the lithosphere, the mantle adiabat or the dry basalt solidus. It indicates that the thermal lithosphere reached the thinnest thickness at the end of Eocene in the Taibei Depression and the end of Oligocene in the Xihu Depression, respectively, corresponding with a value of 57-66km and 56-64km. In Taibei Depression, the lithosphere thickness decreased 16-22km from the end of Mesozoic to Paleocene. After Paleocene, the thickness increased 13-16km and reached 71-79 km at present-day. In Xihu Depression, From the end of Oligocene to present-day, the thickness increased 10-13km and reached 69-76km at present-day. The evolution of the lithosphere thickness is associated closely with the lithosphere stretching.Combining the reconstructed thermal history and the burial history, the maturation of the Jurassic oil-source rock shows that the main hydrocarbon generation phase was in the mid-Jurassic and a secondary hydrocarbon generation occurred at the end of Paleocene. The secondary generation was controlled mainly by the tectono-thermal background during the Paleocene.
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Jurong -Hai'an block of lower Yangtz area is one of the important petroleum exploration area among the residual marine basins in the south China. In the history of the basin's evolution, the strongly compressing, napping, folding and deforming during Indosinian to Yanshan epoch resulted in destruction of the early formed petroleum pool. Therefore, the strategy exploration of the secondary hydrocarbon generation and later formation of petroleum pool was brought forward for petroleum exploration and planning in the study area..On the basis of tectonic and sedimentary as well as present-day thermal regime evolution, using vitrinite reflectance and apatite fission track data and the paleo-heat flow based method, the basin's thermal history is reconstructed and hence the strata's temperature history are obtained. In addition, the maturation histories of the main four sets of marine hydrocarbon source rocks in the block are calculated. Furthermore, taking the maturity in the end of early Cretaceous as the original maturity and according to the formulas fitted by the secondary hydrocarbon generation model, the secondary hydrocarbon generation potential of the four sets of source rock is evaluated.The results of thermal history reconstruction show that Jurong-Hai'an block was under an uniform thermal setting during the Caledonian to Hercynian period and characterized by middle heat flow (52~57rnW/ m2). The uniform thermal setting was divided during and after Indosinian to Yanshan epoch. Wuwei area of southern Anhui province was under the high heat flow setting(~90 mW/m2)between 236Ma and 137Ma; Jurong area of southern Jiangsu ,Huangqiao area and Subei basin reached its maximum heat flow of 90,84 and 78-82 mW/m2 at 101Ma,157Ma and 56Ma respectivelyThe study of secondary hydrocarbon generation shows that the upper Paleozoic and Triassic source rocks have excellent secondary hydrocarbon generation potential. Silurian source rock posses some secondary hydrocarbon generation. Cambrian source rock, however, nearly has no secondary hydrocarbon generation. Overall there are no advantages of secondary hydrocarbon generation in the southern area of Jiansu. The intensity of secondary hydrocarbon generation in North Jiangsu basin is definitely better than that in the southern area of Jiangsu.
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我国西南地区分布有广阔的亚热带潮湿区岩溶,以贵州为中心,总面积达50万km2,是世界上连片分布面积最大的岩溶区。贵州高原地处青藏高原东南缘,云贵高原的东翼,是中国大陆“西高东低”地貌格局中重要的过渡区段,对其新生代地质、地貌演化进行研究无疑具有重要的意义,不仅是对贵州薄弱的新生代地质、地貌研究的补充,而且可以直接通过夷平面展开与青藏高原的对比,探讨青藏高原隆升对贵州高原的直接影响。风化壳作为夷平面的组成部分,在过去没有引起足够的重视,但随着成功实例的不断出现,人们逐渐开始认识到风化壳是夷平面识别和重建的重要依据,也是夷平面环境信息的重要载体。贵州作为碳酸盐岩集中分布区,碳酸盐岩风化壳剖面广泛存在,尤其在黔中、黔北等地区各级夷平面上均发育有红色风化壳,利用碳酸盐岩红色风化壳能为夷平面的识别和形成时代的确立提供可靠的证据,特别是风化壳形成年龄的确定对夷平面时标的建立更具有积极意义。有关贵州地区红色风化壳形成时代的确定,多年来已有一些学者对此展开了研究,但贵州红色风化壳形成时代的确定存在着很大争论。虽然存在其它原因的可能性,但造成这种争论的根本原因在于贵州红色风化壳形成时代是依据其它资料(如夷平面、气候事件等)推断出来的,而不是根据直接测年数据界定的。因此,风化壳直接测年才是解决问题的关键。 本文在前人工作研究的基础之上,利用扫描电镜手段对贵州碳酸盐岩地区上覆风化壳土层中的石英颗粒进行观察、统计、分析,为风化壳成土的物质来源寻找新的证据;同时,经地球化学分析、测试等手段,判断风化壳土层中的晶体石英颗粒为风化壳形成初期的新生矿物——次生石英颗粒,并利用裂变径迹测年法对这种次生石英颗粒进行测年,最终探讨贵州碳酸盐岩地区上覆风化壳土层的形成年代。主要取得了以下几点认识: 一、石英颗粒蚀刻条件的优选 由于石英颗粒裂变径迹的长度和数量与晶格、铀含量、年龄等因素有关,所以不同地区的石英颗粒样品的裂变径迹蚀刻条件也存在差别;目前国际上有关石英颗粒的裂变径迹测年应用的实例较少,还没有统一的有关石英颗粒蚀刻条件的国际标准;现有的石英颗粒蚀刻条件有多种,但是缺乏对这些方法的优缺点进行对比评价。因此,我们要进行反复的条件实验,对比不同石英蚀刻剂的蚀刻效率,找寻适合石英颗粒的最佳蚀刻剂。实验结果表明,40%的HF溶液为最佳蚀刻剂,最佳蚀刻时间:温度在4℃左右(冬季)时为40min;温度在29℃左右(夏季)时为30min。 二、石英的外形、表面机械作用特征及其指示意义 我们利用扫描电镜对石英颗粒外形特征进行观察、统计、分析,结果表明本次研究的石英颗粒形态类型主要有两种:棱状-次棱状石英颗粒以及圆状、次圆状石英颗粒,其中棱状-次棱状石英颗粒包含了一部分晶体形态较为完整的石英颗粒。 根据石英颗粒表面机械作用特征分析结果,结合剖面区域地质特征,可初步判断剖面中的石英颗粒有三种物质来源:碳酸盐岩中的原生碎屑石英,有长时间长距离搬运特征;燧石团块石英,有短距离搬运或原位沉积特征;晶形较完整的次生石英,无搬运特征。三种石英均具有原位特征,前两种类型的石英是直接对基岩的继承,第三种类型的石英是风化壳剖面的次生矿物。 三、石英颗粒表面的化学作用特征及其风化强度指示意义 我们通过对石英颗粒表面化学作用形态的观察,发现大兴剖面、新蒲剖面和官坝剖面的石英颗粒表面化学溶解作用和化学沉淀作用都非常强烈,这表明三个剖面均处于湿、热环境中,均处于强烈的化学风化阶段。而且大兴剖面中石英颗粒表面的化学作用最强烈,气候较其他两个剖面更湿热,剖面的风化强度也最大,即各剖面的风化强度由强到弱排序为:大兴、新蒲、官坝。这一结果与矿物组成分析、化学风化强度、硅铝、铝铁硅风化系数比以及相对风化强度等的地球化学分析指标相一致,这也再次证明了我们采用石英颗粒表面形态特征分析手段的可行性和可靠性。 四、石英颗粒的裂变径迹年龄 三种类型石英颗粒的裂变径迹测年数据表明:a、同一样点石英颗粒裂变径年龄呈现一定的规律:F.T.AGE圆状、次圆状>F.T.AGE不规则状(棱状、次棱状)>F.T.AGE标准晶形(次生石英)。b、不同剖面的不规则状石英颗粒形成于同一个时期;不同剖面的圆状、次圆状石英颗粒形成于同一个时期。这两种石英颗粒不适于贵州碳酸盐岩风化壳的测年研究。c、不同剖面的标准晶形石英颗粒形成于不同时期,形成于碳酸盐岩酸不溶物原地堆积过程中,即与风化壳剖面同期形成,可用于贵州碳酸盐岩风化壳的测年研究。这一测量结果与我们对石英颗粒表面形态特征的观察、统计、分析结果相一致。 五、风化壳物源的新证据 贵州碳酸盐岩风化壳中的石英颗粒表面形态的分析结果表明,贵州碳酸盐岩风化壳的物质来源于碳酸盐岩中酸不溶物原地风化残积的产物,与其下伏基岩有着明显的继承性。这一分析结果与王世杰等人的碳酸盐岩酸不溶物的提取实验、地球化学、矿物学、粒度特征及区域地质背景等多方面的分析结果相一致,为贵州碳酸盐岩风化壳的物质来源及成因提供新的、更细致的证据。 六、贵州晚新生代地质-环境研究历史轮廓初建 由于目前对贵州及周边地区的风化-气候研究相对缺乏,数据资料较稀少,还没有形成完整的系统,我们本次研究也是建立在对风化壳中次生英颗粒年代学研究的基础上,研究还不是很透彻,因此只能对地质-环境研究历史轮廓进行初建。本文根据本次研究剖面土层中晶体次生石英颗粒的裂变径迹年龄分布情况,结合前人已有资料,对贵州25Ma以来的地质-环境演化历史的轮廓进行初建。从次生石英裂变径迹年龄值来看,中新世以来贵州主要经历了如下构造-风化期:25-19Ma、16-13Ma、10-6.5Ma、5-2Ma、1.7-1Ma。