This paper concentrates on considering the down/up crossing property of weighted Markov collision processes. The joint probability generating function of down crossing and up crossing numbers of weighted Markov collis...This paper concentrates on considering the down/up crossing property of weighted Markov collision processes. The joint probability generating function of down crossing and up crossing numbers of weighted Markov collision processes until its extinction are obtained by constructing and studying a related multi-dimensional Markov chain. Hence, the joint probability distribution of down crossing and up crossing numbers and the mean numbers are obtained.展开更多
Our study area covered the Eastern Himalayan Syntaxis (EHS) and its southern extension (Hengduan Mountain or western Sichuan and Yunnan (WSY)) which is located at the orthogonal and oblique collisional front between I...Our study area covered the Eastern Himalayan Syntaxis (EHS) and its southern extension (Hengduan Mountain or western Sichuan and Yunnan (WSY)) which is located at the orthogonal and oblique collisional front between Indian and Asian continents during Cenozoic.Based on geometric and kinematic mapping of the major boundary or regional faults (Dongjug—Mainling(1), Anigiao(2) and Jali(3), Guyu(4) faults in EHS, Ailaoshan—Red River(5), Lancangjiang(6), Gaoligong(7), Binlangjiang(8) and Magok(9) faults in WSY) (see Fig.1), especially on abundant geochronological dating of the mylonitic rocks along these faults, and coupled with magmato\|metamorphic sequences of this region, we try to deal with the temporal and spatial relationships of collisional process to answer questions such as: (1) when did collision start ? (2) is thrusting as a initial and dominant deformation mode to absorb the crustal shortening after suturing, or earlier thrusting usually followed by large\|scale strike\|slip faults? (3) are the two structural patterns coeval at times, or do they occur alternatively during deformation history? (4) are the collisional and associate uplift processes a continuous one or periodic? Insight into such questions is crucial for better understanding of the continental deformation and testing the models available or constraining a new one.展开更多
The single-and double-electron capture(SEC, DEC) processes of He^(2+) ions colliding with Ne atoms are studied by utilizing the full quantum-mechanical molecular-orbital close-coupling method. Total and state-selectiv...The single-and double-electron capture(SEC, DEC) processes of He^(2+) ions colliding with Ne atoms are studied by utilizing the full quantum-mechanical molecular-orbital close-coupling method. Total and state-selective SEC and DEC cross sections are presented in the energy region of 2 eV/u to 20 keV/u. Results show that the dominant reaction channel is Ne^(+)(2s2p^(6) ^(2)S) + He^(+)(1s) in the considered energy region due to strong couplings with the initial state Ne(2s^(2)2p^(6)^(1)S) + He^(2+) around the internuclear distance of 4.6 a.u. In our calculations, the SEC cross sections decrease initially and then increase whereby, the minimum point is around 0.38 keV/u with the increase of collision energies. After considering the effects of the electron translation factor(ETF), the SEC cross sections are increased by 15%–25% nearby the energy region of keV/u and agree better with the available results. The DEC cross sections are smaller than those of SEC because of the larger energy gaps and no strong couplings with the initial state. Due to the Demkov-type couplings between DEC channel Ne^(2+)(2s^(2)2p^(4)^(1)S) + He(1s^(2)) and the dominating SEC channel Ne^(+)(2s2p^(6) ^(2)S) + He^(+)(1s), the DEC cross sections increase with increasing impact energies. Good consistency can also be found between the present DEC and the experimental measurements in the overlapping energy region.展开更多
Hickman's fast nonadiabatic collision model for the ion-pair formation reaction A+BC→A^++BC^- was improved,where the classical trajectory has been represented by solution of motion equation UR=-dV(R)/dR, here V(R...Hickman's fast nonadiabatic collision model for the ion-pair formation reaction A+BC→A^++BC^- was improved,where the classical trajectory has been represented by solution of motion equation UR=-dV(R)/dR, here V(R)is Morse potential.Employing this model to the CS+O_2→CS^++O_2^-reaction,a satisfactory agreement with experimental data has been obtained.展开更多
Taking into account the effects of shadowing and jet quenching, the large transverse momentum distribution of K＋, π＋ and K＋/π＋ ratios at s = 200 GeV originating from resolved photoproduction processes is calcula...Taking into account the effects of shadowing and jet quenching, the large transverse momentum distribution of K＋, π＋ and K＋/π＋ ratios at s = 200 GeV originating from resolved photoproduction processes is calculated based on perturbative quantum chromodynamics. It is found that the contribution of K＋ and π＋ produced by photoproduction processes is evident. The K＋ /π＋ ratios in Au-Au collisions show an obvious enhancement compared with p p collisions. The numerical results indicate that the photoproduetion processes are good modification for kaon and pion production.展开更多
The semiclassical non-perturbative atomic orbital close-coupling approach has been employed to study the electron capture and excitation processes in He^(2+)-H(1s)and He^(2+)-H(2s)collision systems.In order to ensure ...The semiclassical non-perturbative atomic orbital close-coupling approach has been employed to study the electron capture and excitation processes in He^(2+)-H(1s)and He^(2+)-H(2s)collision systems.In order to ensure the accuracy of our calculated cross sections,a large number of high excited states and pseudostates are included in the expansion basis sets which are centered on the target and projectile,respectively.The total and partial charge transfer and excitation cross sections are obtained for a wide-energy domain ranging from 1 keV/amu to 200 keV/amu.The present calculations are also compared with the results from other theoretical methods.These cross section data are useful for the investigation of astrophysics and laboratory plasma.展开更多
北衙金多金属矿田是藏东-金沙江-哀牢山新生代富碱斑岩成矿带中南段的代表性矿床之一,发育一个与富碱斑岩密切相关的金多金属成矿系统。本文较为系统地分析了矿田内的成岩成矿作用特征及其演化过程,并探讨其与印-亚碰撞造山过程的响应...北衙金多金属矿田是藏东-金沙江-哀牢山新生代富碱斑岩成矿带中南段的代表性矿床之一,发育一个与富碱斑岩密切相关的金多金属成矿系统。本文较为系统地分析了矿田内的成岩成矿作用特征及其演化过程,并探讨其与印-亚碰撞造山过程的响应关系。富碱斑岩具有埃达克岩的地球化学亲合性,其源区是喜马拉雅期印-亚碰撞造山造成的软流圈向东挤出汇聚使大规模走滑断裂活化,诱发玄武质下地壳部分熔融的壳幔过渡层,成岩年龄可分为第一期(65～59Ma)、第二期(36～32Ma)、第三期(26～24Ma)和最晚期(3.8～3.6Ma)等4期,其中第二、三期与富碱岩带北段的两期岩浆集中活动时期基本吻合,形成的斑岩对金多金属成矿较为有利。区内金多金属矿床可划分为三个矿床类型和七个矿床亚类,即与喜马拉雅早—中期斑岩有关的金多金属矿床(Ⅰ),包括接触带夕卡岩型、斑岩型和热液充填型(及熔浆型)金多金属矿床;与喜马拉雅第三期斑岩有关的金多金属矿床(Ⅱ),包括爆破角砾岩型和叠加热液改造型金多金属矿床;以及与喜马拉雅期表生作用有关的风化堆积型金矿床(Ⅲ),包括古砂矿型和红色粘土型金矿床。Ⅰ、Ⅱ类型矿床受富碱斑岩及伴生的 NE 到 NNE 向断裂控制,赋存于富碱斑岩体内、内外接触带及其附近围岩的层间破碎带或构造裂隙带中,在成因和空间上与斑岩及隐爆角砾岩等密切有关。成矿物质和成矿流体主要来源于地幔,围岩地层只是提供了成矿的空间,不同类型的矿体之间呈"贯通式"的时间和空间关系,构成了一个统一的喜马拉雅期富碱斑岩-热液型金多金属成矿系统。先期形成矿床明显受后期岩浆热液的叠加改造,但矿化分布和成矿元素组合仍表现为以斑岩为中心,存在 CuAu(Mo)多金属→FeCuAuPbZn 多金属→AuPhZnAg 多金属的分带特征。从最早期含金铁矿床形成之后,原生金矿的次生富集和表生成矿作用就已开始,并形成不同成因类型的风化-堆积型金矿床。其中,古红色粘土型金矿床的成矿主要发生在始新世到渐新世,河-湖相古砂金矿床形成于23～5Ma 期间,红色粘土型(残坡积型)金矿床可从始新世一直延续至今。通过与区域斑岩成岩成矿演化时序的对比,提出与藏东-金沙江-哀牢山斑岩成矿带上的众多矿床一样,北衙矿田内的成岩成矿作也是喜马拉雅期印-亚陆陆碰撞造山带成岩成矿作用在东南缘构造转换带的远程效应,记录了印-亚大陆碰撞造山的详细过程。因而,该矿田深部及外围地区,仍存在巨大的找矿潜力。盐源-丽江断裂带可能也是一务与藏东-金沙江.哀牢山斑岩成矿带联系密切而又相对独立的富碱斑岩成矿带。展开更多
基金This work was substantially supported by the National Natural Science Foundation of China(Grant Nos.11771452,11971486)the Natural Science Foundation of Hunan(No.2020JJ4674).
文摘This paper concentrates on considering the down/up crossing property of weighted Markov collision processes. The joint probability generating function of down crossing and up crossing numbers of weighted Markov collision processes until its extinction are obtained by constructing and studying a related multi-dimensional Markov chain. Hence, the joint probability distribution of down crossing and up crossing numbers and the mean numbers are obtained.
文摘Our study area covered the Eastern Himalayan Syntaxis (EHS) and its southern extension (Hengduan Mountain or western Sichuan and Yunnan (WSY)) which is located at the orthogonal and oblique collisional front between Indian and Asian continents during Cenozoic.Based on geometric and kinematic mapping of the major boundary or regional faults (Dongjug—Mainling(1), Anigiao(2) and Jali(3), Guyu(4) faults in EHS, Ailaoshan—Red River(5), Lancangjiang(6), Gaoligong(7), Binlangjiang(8) and Magok(9) faults in WSY) (see Fig.1), especially on abundant geochronological dating of the mylonitic rocks along these faults, and coupled with magmato\|metamorphic sequences of this region, we try to deal with the temporal and spatial relationships of collisional process to answer questions such as: (1) when did collision start ? (2) is thrusting as a initial and dominant deformation mode to absorb the crustal shortening after suturing, or earlier thrusting usually followed by large\|scale strike\|slip faults? (3) are the two structural patterns coeval at times, or do they occur alternatively during deformation history? (4) are the collisional and associate uplift processes a continuous one or periodic? Insight into such questions is crucial for better understanding of the continental deformation and testing the models available or constraining a new one.
基金Supported by the National Natural Science Foundation of China (Grant Nos. 11774344 and 11474033)the National Key Research and Development Program of China (Grant No. 2017YFA0402300)。
文摘The single-and double-electron capture(SEC, DEC) processes of He^(2+) ions colliding with Ne atoms are studied by utilizing the full quantum-mechanical molecular-orbital close-coupling method. Total and state-selective SEC and DEC cross sections are presented in the energy region of 2 eV/u to 20 keV/u. Results show that the dominant reaction channel is Ne^(+)(2s2p^(6) ^(2)S) + He^(+)(1s) in the considered energy region due to strong couplings with the initial state Ne(2s^(2)2p^(6)^(1)S) + He^(2+) around the internuclear distance of 4.6 a.u. In our calculations, the SEC cross sections decrease initially and then increase whereby, the minimum point is around 0.38 keV/u with the increase of collision energies. After considering the effects of the electron translation factor(ETF), the SEC cross sections are increased by 15%–25% nearby the energy region of keV/u and agree better with the available results. The DEC cross sections are smaller than those of SEC because of the larger energy gaps and no strong couplings with the initial state. Due to the Demkov-type couplings between DEC channel Ne^(2+)(2s^(2)2p^(4)^(1)S) + He(1s^(2)) and the dominating SEC channel Ne^(+)(2s2p^(6) ^(2)S) + He^(+)(1s), the DEC cross sections increase with increasing impact energies. Good consistency can also be found between the present DEC and the experimental measurements in the overlapping energy region.
文摘Hickman's fast nonadiabatic collision model for the ion-pair formation reaction A+BC→A^++BC^- was improved,where the classical trajectory has been represented by solution of motion equation UR=-dV(R)/dR, here V(R)is Morse potential.Employing this model to the CS+O_2→CS^++O_2^-reaction,a satisfactory agreement with experimental data has been obtained.
基金Supported by the National Natural Science Foundation of China under Grant Nos 11065010 and 11465021
文摘Taking into account the effects of shadowing and jet quenching, the large transverse momentum distribution of K＋, π＋ and K＋/π＋ ratios at s = 200 GeV originating from resolved photoproduction processes is calculated based on perturbative quantum chromodynamics. It is found that the contribution of K＋ and π＋ produced by photoproduction processes is evident. The K＋ /π＋ ratios in Au-Au collisions show an obvious enhancement compared with p p collisions. The numerical results indicate that the photoproduetion processes are good modification for kaon and pion production.
基金supported by the National Key Research and Development Program of China (Grant No.2022YFA 1602500)the National Natural Science Foundation of China (Grant Nos.11934004 and 12241410).
文摘The semiclassical non-perturbative atomic orbital close-coupling approach has been employed to study the electron capture and excitation processes in He^(2+)-H(1s)and He^(2+)-H(2s)collision systems.In order to ensure the accuracy of our calculated cross sections,a large number of high excited states and pseudostates are included in the expansion basis sets which are centered on the target and projectile,respectively.The total and partial charge transfer and excitation cross sections are obtained for a wide-energy domain ranging from 1 keV/amu to 200 keV/amu.The present calculations are also compared with the results from other theoretical methods.These cross section data are useful for the investigation of astrophysics and laboratory plasma.
文摘北衙金多金属矿田是藏东-金沙江-哀牢山新生代富碱斑岩成矿带中南段的代表性矿床之一,发育一个与富碱斑岩密切相关的金多金属成矿系统。本文较为系统地分析了矿田内的成岩成矿作用特征及其演化过程,并探讨其与印-亚碰撞造山过程的响应关系。富碱斑岩具有埃达克岩的地球化学亲合性,其源区是喜马拉雅期印-亚碰撞造山造成的软流圈向东挤出汇聚使大规模走滑断裂活化,诱发玄武质下地壳部分熔融的壳幔过渡层,成岩年龄可分为第一期(65～59Ma)、第二期(36～32Ma)、第三期(26～24Ma)和最晚期(3.8～3.6Ma)等4期,其中第二、三期与富碱岩带北段的两期岩浆集中活动时期基本吻合,形成的斑岩对金多金属成矿较为有利。区内金多金属矿床可划分为三个矿床类型和七个矿床亚类,即与喜马拉雅早—中期斑岩有关的金多金属矿床(Ⅰ),包括接触带夕卡岩型、斑岩型和热液充填型(及熔浆型)金多金属矿床;与喜马拉雅第三期斑岩有关的金多金属矿床(Ⅱ),包括爆破角砾岩型和叠加热液改造型金多金属矿床;以及与喜马拉雅期表生作用有关的风化堆积型金矿床(Ⅲ),包括古砂矿型和红色粘土型金矿床。Ⅰ、Ⅱ类型矿床受富碱斑岩及伴生的 NE 到 NNE 向断裂控制,赋存于富碱斑岩体内、内外接触带及其附近围岩的层间破碎带或构造裂隙带中,在成因和空间上与斑岩及隐爆角砾岩等密切有关。成矿物质和成矿流体主要来源于地幔,围岩地层只是提供了成矿的空间,不同类型的矿体之间呈"贯通式"的时间和空间关系,构成了一个统一的喜马拉雅期富碱斑岩-热液型金多金属成矿系统。先期形成矿床明显受后期岩浆热液的叠加改造,但矿化分布和成矿元素组合仍表现为以斑岩为中心,存在 CuAu(Mo)多金属→FeCuAuPbZn 多金属→AuPhZnAg 多金属的分带特征。从最早期含金铁矿床形成之后,原生金矿的次生富集和表生成矿作用就已开始,并形成不同成因类型的风化-堆积型金矿床。其中,古红色粘土型金矿床的成矿主要发生在始新世到渐新世,河-湖相古砂金矿床形成于23～5Ma 期间,红色粘土型(残坡积型)金矿床可从始新世一直延续至今。通过与区域斑岩成岩成矿演化时序的对比,提出与藏东-金沙江-哀牢山斑岩成矿带上的众多矿床一样,北衙矿田内的成岩成矿作也是喜马拉雅期印-亚陆陆碰撞造山带成岩成矿作用在东南缘构造转换带的远程效应,记录了印-亚大陆碰撞造山的详细过程。因而,该矿田深部及外围地区,仍存在巨大的找矿潜力。盐源-丽江断裂带可能也是一务与藏东-金沙江.哀牢山斑岩成矿带联系密切而又相对独立的富碱斑岩成矿带。
