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International Journal of Theoretical Physics

Difference Posets in the Quantum StructuresBackground

Ferdinand Chovanec, Františk Kôpka

Published Mar 1, 2000• 9 citations
Publisher
DOI
10.1023/a:1003625401906

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QUANTUM THEORY BASED ON FUZZY SETS

Ferdinand Chovanec, Mária Jurečkova

A new probability model based on the theory of fuzzy sets is presented. In thismodel, a difference of comparable fuzzy sets is the primary operation. The idea ofa difference of fuzzy sets (fuzzy events) is simple: If we have two comparable eventsa and b ( a ≤ b ), then our knowledge on a and b entails the complete knowledge ofthe complement of a in b , i. e., b ⊖ a .The new algebraic structure of fuzzy sets is called a difference poset (a D-poset) offuzzy sets. Some properties of a lattice ordered D-poset of fuzzy sets (a D-lattice offuzzy sets) are studied. An MV-algebra of fuzzy sets (a Bold algebra) is characterizedin the D-poset of fuzzy sets set-up. The sufficient and necessary conditions for a Dlatticeof fuzzy sets to be a Bold algebra are given. The basic notions of the quantumlogic theory - a state and an observable are defined in D-posets of fuzzy sets.

The International Conference on Mathematics and Engineering Physics/The International Conference on Mathematics and Engineering Physics•May 1, 2006•0 citations

On Bounded Posets Arising from Quantum Mechanical Measurements

Dietmar W. Dorninger, Helmut Länger

Let S be a set of states of a physical system. The probabilities p ( s ) of the occurrence of an event when the system is in different states s ∈ S define a function from S to [0, 1] called a numerical event or, more precisely, an S - probability . If one orders a set P of S -probabilities in respect to the order of functions, further includes the constant functions 0 and 1 and defines p ′ = 1 − p for every p ∈ P , then one obtains a bounded poset of S -probabilities with an antitone involution. We study these posets in respect to various conditions about the existence of the sum of certain functions within the posets and derive properties from these conditions. In particular, questions of relations between different classes of S -probabilities arising this way are settled, algebraic representations are provided and the property that two S -probabilities commute is characterized which is essential for recognizing a classical physical system.

International Journal of Theoretical Physics•Jun 22, 2016•3 citations
A new probability model based on the theory of fuzzy sets is presented. In thismodel, a difference of comparable fuzzy sets is the primary operation. The idea ofa difference of fuzzy sets (fuzzy events) is simple: If we have two comparable eventsa and b ( a ≤ b ), then our knowledge on a and b entails the complete knowledge ofthe complement of a in b , i. e., b ⊖ a .The new algebraic structure of fuzzy sets is called a difference poset (a D-poset) offuzzy sets. Some properties of a lattice ordered D-poset of fuzzy sets (a D-lattice offuzzy sets) are studied. An MV-algebra of fuzzy sets (a Bold algebra) is characterizedin the D-poset of fuzzy sets set-up. The sufficient and necessary conditions for a Dlatticeof fuzzy sets to be a Bold algebra are given. The basic notions of the quantumlogic theory - a state and an observable are defined in D-posets of fuzzy sets.
Let S be a set of states of a physical system. The probabilities p ( s ) of the occurrence of an event when the system is in different states s ∈ S define a function from S to [0, 1] called a numerical event or, more precisely, an S - probability . If one orders a set P of S -probabilities in respect to the order of functions, further includes the constant functions 0 and 1 and defines p ′ = 1 − p for every p ∈ P , then one obtains a bounded poset of S -probabilities with an antitone involution. We study these posets in respect to various conditions about the existence of the sum of certain functions within the posets and derive properties from these conditions. In particular, questions of relations between different classes of S -probabilities arising this way are settled, algebraic representations are provided and the property that two S -probabilities commute is characterized which is essential for recognizing a classical physical system.