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標題: Titlebook: An Introduction to Hilbert Space and Quantum Logic; David W. Cohen Textbook 1989 Springer-Verlag New York Inc. 1989 Functionals.algebra.de [打印本頁]

作者: 馬用    時間: 2025-3-21 17:33
書目名稱An Introduction to Hilbert Space and Quantum Logic影響因子(影響力)




書目名稱An Introduction to Hilbert Space and Quantum Logic影響因子(影響力)學科排名




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書目名稱An Introduction to Hilbert Space and Quantum Logic被引頻次學科排名




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書目名稱An Introduction to Hilbert Space and Quantum Logic讀者反饋




書目名稱An Introduction to Hilbert Space and Quantum Logic讀者反饋學科排名





作者: Asperity    時間: 2025-3-21 21:43
Textbook 1989y strict prerequisites are calculus and linear algebra, but the level of mathematical sophistication assumes at least one or two intermediate courses, for example in mathematical analysis or advanced calculus. No background in physics is assumed.
作者: 分開    時間: 2025-3-22 02:30

作者: 殺子女者    時間: 2025-3-22 08:25

作者: Alienated    時間: 2025-3-22 09:01
https://doi.org/10.1007/978-3-642-65598-2 quantum mechanics. In Part B we outline a set of working hypotheses for quantum mechanics. In Part C we discuss a philosophical dilemma arising from these hypotheses and articulated in a famous paper written in 1935 by Einstein, Podolsky, and Rosen.
作者: Ruptured-Disk    時間: 2025-3-22 16:32
0941-3502 ns known as "quantum mechanics". The equations and their philosophical underpinnings were then collected into a model based on the mathematics of Hilbert space. From the Hilbert space model came the abstaction of "quantum logics". This book explores all three stages, but not in historical order. Ins
作者: 慌張    時間: 2025-3-22 20:55

作者: 貨物    時間: 2025-3-22 23:21
https://doi.org/10.1007/978-3-642-50181-4nts whose outcome sets are more general than the finite subsets of ? we saw in Chapter 1. We shall be guided by Lemma 1B.10, however, when we define the expected value of an observable as the integral of the identity function on ? with respect to a measure determined by a state on the logic.
作者: POLYP    時間: 2025-3-23 01:30
Subspaces in Hilbert Space,ing particle usually means obtaining an outcome from an infinite number of possibilities. In this chapter we shall learn about infinite dimensional Hilbert spaces. In particular, we shall consider the subspace structure of infinite dimensional Hilbert spaces. These provide the logics for orthodox quantum physics.
作者: BIPED    時間: 2025-3-23 09:00
,State Space and Gleason’s Theorem,nts whose outcome sets are more general than the finite subsets of ? we saw in Chapter 1. We shall be guided by Lemma 1B.10, however, when we define the expected value of an observable as the integral of the identity function on ? with respect to a measure determined by a state on the logic.
作者: 冒號    時間: 2025-3-23 13:01
Textbook 1989s "quantum mechanics". The equations and their philosophical underpinnings were then collected into a model based on the mathematics of Hilbert space. From the Hilbert space model came the abstaction of "quantum logics". This book explores all three stages, but not in historical order. Instead, in a
作者: 相符    時間: 2025-3-23 14:09
Experiments, Measure and Integration,ng it takes a marble to drop from a certain height. Then we record what happens after we do it—the coin comes up heads, we get burned, the marble takes 6 seconds to drop. What we record is called an outcome of the experiment. We identify an experiment by its outcome set, so we can write . = (heads,
作者: osculate    時間: 2025-3-23 19:51

作者: 縮減了    時間: 2025-3-24 02:06
Subspaces in Hilbert Space,-up and spin-down. Of course, many physical experiments have outcome sets that are not finite. A measurement of energy, position, or momentum of a moving particle usually means obtaining an outcome from an infinite number of possibilities. In this chapter we shall learn about infinite dimensional Hi
作者: congenial    時間: 2025-3-24 04:00

作者: 好開玩笑    時間: 2025-3-24 06:53
,State Space and Gleason’s Theorem,otions of pure states, mixtures of states, and physical properties. Next we define an observable on a logic, allowing us to consider physical experiments whose outcome sets are more general than the finite subsets of ? we saw in Chapter 1. We shall be guided by Lemma 1B.10, however, when we define t
作者: 無法取消    時間: 2025-3-24 10:51
Spectrality, with a Hilbert space . and its projection logic, we defined an observable as a logic-valued function on the real Borel sets. Then through expected values every observable was shown to be associated with a member of . (H), and then every member of . (.) was associated with a Hermitian operator on .
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作者: 史前    時間: 2025-3-24 21:57
Carl Zeiss,P. Culmann,E. Wanderslebng it takes a marble to drop from a certain height. Then we record what happens after we do it—the coin comes up heads, we get burned, the marble takes 6 seconds to drop. What we record is called an outcome of the experiment. We identify an experiment by its outcome set, so we can write . = (heads,
作者: 捏造    時間: 2025-3-24 23:58

作者: 宣稱    時間: 2025-3-25 04:01

作者: 純樸    時間: 2025-3-25 11:02
,Einführung in die Matrizenrechnung,es of the structure. Besides mathematical interest, the functions on Hilbert space that we study in this chapter provide a crucial link to the notion of an “observable physical quantity” in the Hilbert space formulation of quantum mechanics.
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作者: audiologist    時間: 2025-3-25 21:10
https://doi.org/10.1007/978-3-642-65598-2 of dealing with a physical universe behaving in contradiction to classical Newtonian physics, whereas “quantum mechanics” means a specific set of working hypotheses about the physical universe. Up to now we have been exploring quantum physics in general. Part A of this chapter is a brief history of
作者: 制定    時間: 2025-3-26 03:10
An Introduction to Hilbert Space and Quantum Logic978-1-4613-8841-8Series ISSN 0941-3502 Series E-ISSN 2197-8506
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作者: 移動    時間: 2025-3-26 20:48

作者: 污穢    時間: 2025-3-27 00:26
Experiments, Measure and Integration,ng it takes a marble to drop from a certain height. Then we record what happens after we do it—the coin comes up heads, we get burned, the marble takes 6 seconds to drop. What we record is called an outcome of the experiment. We identify an experiment by its outcome set, so we can write . = (heads, tails) to denote the coin flip experiment.
作者: defibrillator    時間: 2025-3-27 02:27
Hilbert Space Basics,uct” between vectors in a vector space and using the inner product to consider angles between vectors. A ‘Hilbert space’ is a vector space with an inner product. We begin by defining an inner product space.
作者: Ceramic    時間: 2025-3-27 07:00
Maps on Hilbert Spaces,es of the structure. Besides mathematical interest, the functions on Hilbert space that we study in this chapter provide a crucial link to the notion of an “observable physical quantity” in the Hilbert space formulation of quantum mechanics.
作者: HAUNT    時間: 2025-3-27 10:36
Spectrality, with a Hilbert space . and its projection logic, we defined an observable as a logic-valued function on the real Borel sets. Then through expected values every observable was shown to be associated with a member of . (H), and then every member of . (.) was associated with a Hermitian operator on . by Gleason’s theorem and the spectral theorem.
作者: 反復拉緊    時間: 2025-3-27 17:11
Problem Books in Mathematicshttp://image.papertrans.cn/a/image/155281.jpg
作者: chlorosis    時間: 2025-3-27 19:34
https://doi.org/10.1007/978-1-4613-8841-8Functionals; algebra; development; eigenvalue; experiment; geometry; influence; mathematics; mechanics; momen
作者: Engulf    時間: 2025-3-27 23:21
978-1-4613-8843-2Springer-Verlag New York Inc. 1989
作者: 狂熱文化    時間: 2025-3-28 04:00

作者: 值得尊敬    時間: 2025-3-28 06:48
The Logic of Nonclassical Physics,In this chapter we introduce a mathematical formulation for the foundations of quantum physics.
作者: 不容置疑    時間: 2025-3-28 13:51

作者: 無價值    時間: 2025-3-28 18:21
Experimental Investigation of Flames,n expect this growing trend to continue. However, in spite of the increasing level of sophistication of the numerical simulations, guidance from experiment is still necessary. Such guidance is needed for several reasons:




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