標(biāo)題: Titlebook: GRMS or Graphical Representation of Model Spaces; Vol. 1 Basics W. Duch Book 1986 Springer-Verlag Berlin Heidelberg 1986 RMS.classification [打印本頁(yè)] 作者: 并排一起 時(shí)間: 2025-3-21 17:34
書(shū)目名稱(chēng)GRMS or Graphical Representation of Model Spaces影響因子(影響力)
書(shū)目名稱(chēng)GRMS or Graphical Representation of Model Spaces影響因子(影響力)學(xué)科排名
書(shū)目名稱(chēng)GRMS or Graphical Representation of Model Spaces網(wǎng)絡(luò)公開(kāi)度
書(shū)目名稱(chēng)GRMS or Graphical Representation of Model Spaces網(wǎng)絡(luò)公開(kāi)度學(xué)科排名
書(shū)目名稱(chēng)GRMS or Graphical Representation of Model Spaces被引頻次
書(shū)目名稱(chēng)GRMS or Graphical Representation of Model Spaces被引頻次學(xué)科排名
書(shū)目名稱(chēng)GRMS or Graphical Representation of Model Spaces年度引用
書(shū)目名稱(chēng)GRMS or Graphical Representation of Model Spaces年度引用學(xué)科排名
書(shū)目名稱(chēng)GRMS or Graphical Representation of Model Spaces讀者反饋
書(shū)目名稱(chēng)GRMS or Graphical Representation of Model Spaces讀者反饋學(xué)科排名
作者: Brain-Imaging 時(shí)間: 2025-3-22 00:05
Book 1986and seeing have much in common - we say "I see" meaning "I understand" , for example. Most of us prefer to have a picture of an abstract object. The remarkable popularity of the Feynman diagrams, and other diagrammatic approaches to many-body problem derived thereof, may be partially due to this pre作者: extinct 時(shí)間: 2025-3-22 03:25 作者: Urgency 時(shí)間: 2025-3-22 07:15
A Just Society for Ireland? 1964-1987 graph is simpler if we regard vertices and arcs of these larger graphs as ‘virtually present’: existing, but giving a null contribution to the real graph. The fixed-slope graphs, by virtue of this embedding property, admit a natural ordering of paths.作者: Bureaucracy 時(shí)間: 2025-3-22 11:43
The Collective Unconscious and Beyond in ,c molecule in Born-Oppenheimer approximation requires such states when a strong spin-orbit interaction is present. Graphical representation of the states that do not posses any symmetry other that being antisymmetric (corresponding to determinants) is particularly simple.作者: 嬉耍 時(shí)間: 2025-3-22 16:29
Sharon Wilson,Surita Mogan,Kiran Kaurmpty arc is most frequently set to zero making the arc vertical. The difference . — hm. should be choosen in such a way that . is always different from the slope of an empty arc and that each vertex is uniquely labeled by (., .) values.作者: 嬉耍 時(shí)間: 2025-3-22 18:12 作者: 領(lǐng)導(dǎo)權(quán) 時(shí)間: 2025-3-22 23:43
L?z—adapted graphsmpty arc is most frequently set to zero making the arc vertical. The difference . — hm. should be choosen in such a way that . is always different from the slope of an empty arc and that each vertex is uniquely labeled by (., .) values.作者: genesis 時(shí)間: 2025-3-23 05:08
https://doi.org/10.1007/978-3-319-41510-9e second group at the bottom levels of a graph. In this way two subgraphs, the first describing the space of s. particles in ∣.〉 basis and the second representing the space of s. particles in ∣.〉 basis, are obtained (Fig 4). The two subgraphs are joined by one vertex.作者: 語(yǔ)源學(xué) 時(shí)間: 2025-3-23 08:55
https://doi.org/10.1007/978-1-349-00178-1 is not how to construct spin eigenfunctions, but how to find proper graphical labels for them. In the second part of this work I will show how the information contained in the labels or in the structure of graphs may be used to calculate arbitrary matrix elements.作者: 事情 時(shí)間: 2025-3-23 10:39
?z—adapted graphs in different formse second group at the bottom levels of a graph. In this way two subgraphs, the first describing the space of s. particles in ∣.〉 basis and the second representing the space of s. particles in ∣.〉 basis, are obtained (Fig 4). The two subgraphs are joined by one vertex.作者: 呼吸 時(shí)間: 2025-3-23 17:10
?2—adapted graphs is not how to construct spin eigenfunctions, but how to find proper graphical labels for them. In the second part of this work I will show how the information contained in the labels or in the structure of graphs may be used to calculate arbitrary matrix elements.作者: fructose 時(shí)間: 2025-3-23 18:01
Roberto Filippini,Cipriano Forzaowski and Malinowski 1980; Jeziorski . 1984). Notwithstanding their hopes the majority votes for one-particle approximation, because it is fundamental to our intuitions and capable of high accuracy (cf Handy 1978).作者: Excitotoxin 時(shí)間: 2025-3-24 01:58 作者: 要求比…更好 時(shí)間: 2025-3-24 04:26 作者: 神刊 時(shí)間: 2025-3-24 06:59 作者: 影響深遠(yuǎn) 時(shí)間: 2025-3-24 14:16
Book 1986 take a global view from the perspective of the whole many-particle space. But how to visualize the space of all many-particle states ? Methods of such visualization or graphical representation of the ,spaces of interest to physicists and chemists are the main topic of this work.作者: integrated 時(shí)間: 2025-3-24 16:43
0342-4901 ods of such visualization or graphical representation of the ,spaces of interest to physicists and chemists are the main topic of this work.978-3-540-17169-0978-3-642-93347-9Series ISSN 0342-4901 Series E-ISSN 2192-6603 作者: 吸氣 時(shí)間: 2025-3-24 19:05 作者: 陳腐思想 時(shí)間: 2025-3-25 02:07
(L?z,?z)—adapted graphstal orderings. Although it is not possible to find a planar graph representing this space the graph of Fig ., with orbitals grouped according to their . values, is more legible than the graphs corresponding to other orbital orderings. In Fig . more complicated case, with 3., 3. and 3. orbital basis,作者: 圍裙 時(shí)間: 2025-3-25 04:24 作者: 職業(yè)拳擊手 時(shí)間: 2025-3-25 10:39 作者: 討人喜歡 時(shí)間: 2025-3-25 13:59 作者: 山崩 時(shí)間: 2025-3-25 19:24 作者: CRACY 時(shí)間: 2025-3-25 20:18 作者: erythema 時(shí)間: 2025-3-26 01:51 作者: 變化無(wú)常 時(shí)間: 2025-3-26 05:55
Summary and open problemsture of such spaces. Spaces built from a large number of primitive states of the same type have particularly simple structures. The techniques of graphical evaluation of matrix elements are developed in Part . (abelian symmetries) and Part . (non-abelian symmetries). The insight that the graphs give作者: Ingest 時(shí)間: 2025-3-26 10:50 作者: syring 時(shí)間: 2025-3-26 15:28
,A Guide to Kipling’s Short Stories,tal orderings. Although it is not possible to find a planar graph representing this space the graph of Fig ., with orbitals grouped according to their . values, is more legible than the graphs corresponding to other orbital orderings. In Fig . more complicated case, with 3., 3. and 3. orbital basis,作者: deforestation 時(shí)間: 2025-3-26 19:23
https://doi.org/10.1007/978-3-319-05305-9 possibility of representing the (L?.,?.) and (L?., ?.)-adapted spaces with the help of a fagot graph is presented. The (L?., ?.)-adapted graphs are very convenient in calculations of atomic properties and in nuclear shell model calculations; bearing in mind the complexity of L?.-adapted states it i作者: 浪蕩子 時(shí)間: 2025-3-26 22:52 作者: 產(chǎn)生 時(shí)間: 2025-3-27 01:56 作者: grounded 時(shí)間: 2025-3-27 07:12
Christoph Thiele,Falk Fahrenholzs the independent-particle approximation works rather well and it is possible to choose the one-particle states in such a way, that among all many-particle symmetry-adapted states there is one state or a combination of a few states clearly dominating the exact solution. In such cases one may argue t作者: OWL 時(shí)間: 2025-3-27 11:52
Hanspeter Saluz,Jean-Pierre Jostred according to their symmetry species and certain vertices at the lowest levels of a given symmetry removed. Following Fig . graphs showing ., ., ., . symmetry configurations for water are presented (these graphs were produced on a normal line printer and are a part of output of a computer program作者: PLIC 時(shí)間: 2025-3-27 13:38
Peter Jackson,John T. Gallagherig . are equivalent the first is the most natural, because the contribution of each arc to the total . and . numbers is clearly visible and we may introduce a horizontal axis to measure ., . values. In the two other cases we have to label each arc with two weights, one for the number of electrons as作者: BUOY 時(shí)間: 2025-3-27 18:52 作者: 打折 時(shí)間: 2025-3-27 22:56
Prefaced seeing have much in common — we say “I see” meaning “I understand”, for example. Most of us prefer to have a picture of an abstract object. The remarkable popularity of the Feynman diagrams, and other diagrammatic approaches to many-body problem derived thereof, may be partially due to this prefer作者: languor 時(shí)間: 2025-3-28 02:56 作者: adj憂(yōu)郁的 時(shí)間: 2025-3-28 07:24 作者: 赤字 時(shí)間: 2025-3-28 13:05 作者: 身體萌芽 時(shí)間: 2025-3-28 18:15 作者: COM 時(shí)間: 2025-3-28 22:29
L?z—adapted graphsumbers . of a single particle take many values . = 0,±1,±2… while for the spin only two values . = ±1/2 were possible. Orbitals (primitive states) with different . values should be represented by arcs of different slopes. There are two parameters demanding careful choice in order to make legible gra作者: 嚴(yán)厲批評(píng) 時(shí)間: 2025-3-29 01:42 作者: exercise 時(shí)間: 2025-3-29 03:14 作者: GLOSS 時(shí)間: 2025-3-29 07:49
(L?z,?2)—adapted graphsd by now. S-diagram is made from M-diagram by removing vertices corresponding to negative . values. The graph with α, . α… order of spin orbitals as well as four-slope graphs are a kind of extended M-diagrams: their paths, after doubly occupied orbitals are removed and dependence of arc slopes on . 作者: Autobiography 時(shí)間: 2025-3-29 12:00 作者: dialect 時(shí)間: 2025-3-29 16:32
(?2,T?2)—adapted graphslculation of the nuclear properties. Due to the nature of nuclear forces solutions of nuclear equations are sought in full many-particle spaces built from primitive functions, called in context of nuclear shell-model calulations’orbits’, that are almost always taken as harmonic oscillator functions 作者: 使殘廢 時(shí)間: 2025-3-29 22:10 作者: Resection 時(shí)間: 2025-3-30 01:20 作者: gnarled 時(shí)間: 2025-3-30 07:20 作者: Rejuvenate 時(shí)間: 2025-3-30 11:46
Mathematical remarks theory on one side, and group-theoretical methods to characterize these model spaces on the other. However, examining books on graph theory (cf Ore 1962; Harary 1969; Deo 1974; Beineke and Wilson 1978; Swamy and Thulasiraman 1981) I have found rather little relevant material. Although it is possibl作者: left-ventricle 時(shí)間: 2025-3-30 14:52
Summary and open problemsations was restricted to a minimum — as if pictures of buildings were presented without really entering into details of engineering problems — the multitude of spaces used in physics is responsible for this rather long presentation. I realize that many kinds of spaces were omitted and thus descripti作者: 捐助 時(shí)間: 2025-3-30 20:28
978-3-540-17169-0Springer-Verlag Berlin Heidelberg 1986作者: 沖擊力 時(shí)間: 2025-3-30 22:44 作者: 懶洋洋 時(shí)間: 2025-3-31 03:09 作者: 不要嚴(yán)酷 時(shí)間: 2025-3-31 08:44 作者: optional 時(shí)間: 2025-3-31 09:40
Graphs and computersThe last subject that I want to cover briefly is of more technical nature. For more information the reader is refered to the literature quoted in this section.作者: 表示問(wèn) 時(shí)間: 2025-3-31 17:16
https://doi.org/10.1007/978-3-030-47487-4d seeing have much in common — we say “I see” meaning “I understand”, for example. Most of us prefer to have a picture of an abstract object. The remarkable popularity of the Feynman diagrams, and other diagrammatic approaches to many-body problem derived thereof, may be partially due to this prefer作者: 捕鯨魚(yú)叉 時(shí)間: 2025-3-31 18:32 作者: GENRE 時(shí)間: 2025-3-31 23:13
The Collective Unconscious and Beyond in ,t space. For fermionic systems these basis states should be antisymmetric - a very strong requirement, immediately invoking the Pauli principle. Adding spin states |.) and |.) to each orbital state that belongs to V. we obtain 2. spin-orbital states. These spin-orbital states are ordered and identif作者: enterprise 時(shí)間: 2025-4-1 03:56 作者: 南極 時(shí)間: 2025-4-1 06:19 作者: Felicitous 時(shí)間: 2025-4-1 10:32
Sharon Wilson,Surita Mogan,Kiran Kaurumbers . of a single particle take many values . = 0,±1,±2… while for the spin only two values . = ±1/2 were possible. Orbitals (primitive states) with different . values should be represented by arcs of different slopes. There are two parameters demanding careful choice in order to make legible gra作者: Efflorescent 時(shí)間: 2025-4-1 16:58 作者: condescend 時(shí)間: 2025-4-1 21:29
https://doi.org/10.1007/978-1-349-00178-1tly the only useful symmetry of a physical system (this is true in particular for molecular systems). Moreover, the isospin operator T? of nucleons has the same formal properties as the total spin operator ?.. Construction and use of the spin eigenfunctions is therefore particularly important and wh
