"4141655"^^ . . "O estado W \u00E9 um estado qu\u00E2ntico emaranhado de tr\u00EAs qubits que tem a seguinte forma: . \u00C9 not\u00E1vel por representar um tipo espec\u00EDfico de e por ocorrer em v\u00E1rias aplica\u00E7\u00F5es na teoria da informa\u00E7\u00E3o qu\u00E2ntica. As part\u00EDculas preparadas nesse estado reproduzem as propriedades do teorema de Bell, que afirma que nenhuma teoria cl\u00E1ssica de vari\u00E1veis ocultas locais pode produzir as previs\u00F5es da mec\u00E2nica qu\u00E2ntica. Foi relatado pela primeira vez por W. D\u00FCr, G. Vidal e J. I. Cirac."@pt . "W-\u0441\u0442\u0430\u043D \u2014 \u0446\u0435 \u0437\u0430\u043F\u043B\u0443\u0442\u0430\u043D\u0438\u0439 \u043A\u0432\u0430\u043D\u0442\u043E\u0432\u0438\u0439 \u0441\u0442\u0430\u043D \u0442\u0440\u044C\u043E\u0445 \u043A\u0443\u0431\u0456\u0442\u0456\u0432, \u0449\u043E \u043C\u0430\u0454 \u0432\u0438\u0433\u043B\u044F\u0434: \u0442\u0430 \u0432\u0456\u0434\u0456\u0433\u0440\u0430\u0454 \u0432\u0430\u0436\u043B\u0438\u0432\u0443 \u0440\u043E\u043B\u044C \u0432 \u043E\u043F\u0438\u0441\u0456 \u0442\u0430 \u0434\u0435\u044F\u043A\u0438\u0445 \u0456\u043D\u0448\u0438\u0445 \u0437\u0430\u0441\u0442\u043E\u0441\u0443\u0432\u0430\u043D\u043D\u044F\u0445 ."@uk . . . "The W state is an entangled quantum state of three qubits which in the bra-ket notation has the following shape and which is remarkable for representing a specific type of multipartite entanglement and for occurring in several applications in quantum information theory. Particles prepared in this state reproduce the properties of Bell's theorem, which states that no classical theory of local hidden variables can produce the predictions of quantum mechanics. The state is named after Wolfgang D\u00FCr, who first reported the state together with Guifr\u00E9 Vidal, and Ignacio Cirac in 2002."@en . . . . . . . . . "The W state is an entangled quantum state of three qubits which in the bra-ket notation has the following shape and which is remarkable for representing a specific type of multipartite entanglement and for occurring in several applications in quantum information theory. Particles prepared in this state reproduce the properties of Bell's theorem, which states that no classical theory of local hidden variables can produce the predictions of quantum mechanics. The state is named after Wolfgang D\u00FCr, who first reported the state together with Guifr\u00E9 Vidal, and Ignacio Cirac in 2002."@en . . "1120382767"^^ . . . "W-\u0441\u0442\u0430\u043D \u2014 \u0446\u0435 \u0437\u0430\u043F\u043B\u0443\u0442\u0430\u043D\u0438\u0439 \u043A\u0432\u0430\u043D\u0442\u043E\u0432\u0438\u0439 \u0441\u0442\u0430\u043D \u0442\u0440\u044C\u043E\u0445 \u043A\u0443\u0431\u0456\u0442\u0456\u0432, \u0449\u043E \u043C\u0430\u0454 \u0432\u0438\u0433\u043B\u044F\u0434: \u0442\u0430 \u0432\u0456\u0434\u0456\u0433\u0440\u0430\u0454 \u0432\u0430\u0436\u043B\u0438\u0432\u0443 \u0440\u043E\u043B\u044C \u0432 \u043E\u043F\u0438\u0441\u0456 \u0442\u0430 \u0434\u0435\u044F\u043A\u0438\u0445 \u0456\u043D\u0448\u0438\u0445 \u0437\u0430\u0441\u0442\u043E\u0441\u0443\u0432\u0430\u043D\u043D\u044F\u0445 ."@uk . . . . "Estado W"@pt . . "En mec\u00E1nica cu\u00E1ntica, el estado W es consiste en una configuraci\u00F3n de tres c\u00FAbits, que se escribe y representa un tipo espec\u00EDfico de entrelazamiento cu\u00E1ntico a varios cuerpos. Este estado tiene varias aplicaciones en computaci\u00F3n cu\u00E1ntica, sistemas en este estado verifican las desigualdades de Bell, y por lo tanto demuestran que no existe una teor\u00EDa cl\u00E1sica de variables ocultas que reproduzca las predicciones de la mec\u00E1nica cu\u00E1ntica. El estado debe su nombre a Wolfgang D\u00FCr,\u200B qui\u00E9n report\u00F3 por primera vez sus propiedades en colaboraci\u00F3n con Guifr\u00E9 Vidal, e Ignacio Cirac en 2002.\u200B"@es . . "5903"^^ . . . . "En mec\u00E1nica cu\u00E1ntica, el estado W es consiste en una configuraci\u00F3n de tres c\u00FAbits, que se escribe y representa un tipo espec\u00EDfico de entrelazamiento cu\u00E1ntico a varios cuerpos. Este estado tiene varias aplicaciones en computaci\u00F3n cu\u00E1ntica, sistemas en este estado verifican las desigualdades de Bell, y por lo tanto demuestran que no existe una teor\u00EDa cl\u00E1sica de variables ocultas que reproduzca las predicciones de la mec\u00E1nica cu\u00E1ntica. El estado debe su nombre a Wolfgang D\u00FCr,\u200B qui\u00E9n report\u00F3 por primera vez sus propiedades en colaboraci\u00F3n con Guifr\u00E9 Vidal, e Ignacio Cirac en 2002.\u200B"@es . . . . "Estado W"@es . . "O estado W \u00E9 um estado qu\u00E2ntico emaranhado de tr\u00EAs qubits que tem a seguinte forma: . \u00C9 not\u00E1vel por representar um tipo espec\u00EDfico de e por ocorrer em v\u00E1rias aplica\u00E7\u00F5es na teoria da informa\u00E7\u00E3o qu\u00E2ntica. As part\u00EDculas preparadas nesse estado reproduzem as propriedades do teorema de Bell, que afirma que nenhuma teoria cl\u00E1ssica de vari\u00E1veis ocultas locais pode produzir as previs\u00F5es da mec\u00E2nica qu\u00E2ntica. Foi relatado pela primeira vez por W. D\u00FCr, G. Vidal e J. I. Cirac."@pt . . "W state"@en . "W-\u0441\u0442\u0430\u043D"@uk . . .