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measurement problem : ウィキペディア英語版 | measurement problem The measurement problem in quantum mechanics is the problem of how (or ''whether'') wavefunction collapse occurs. The inability to observe this process directly has given rise to different interpretations of quantum mechanics, and poses a key set of questions that each interpretation must answer. The wavefunction in quantum mechanics evolves deterministically according to the Schrödinger equation as a linear superposition of different states, but actual measurements always find the physical system in a definite state. Any future evolution is based on the state the system was discovered to be in when the measurement was made, meaning that the measurement "did something" to the system that is not obviously a consequence of Schrödinger evolution. To express matters differently (to paraphrase Steven Weinberg〔(Steven Weinberg: ''Einstein's Mistakes'' ) in Physics Today (2005); see subsection "Contra quantum mechanics"〕), the Schrödinger wave equation determines the wavefunction at any later time. If observers and their measuring apparatus are themselves described by a deterministic wave function, why can we not predict precise results for measurements, but only probabilities? As a general question: How can one establish a correspondence between quantum and classical reality?〔Wojciech Hubert Zurek ''Decoherence, einselection, and the quantum origins of the classical'' (Reviews of Modern Physics, Vol. 75, July 2003 )〕 ==Schrödinger's cat== The best known example is the "paradox" of the Schrödinger's cat. A mechanism is arranged to kill a cat if a quantum event, such as the decay of a radioactive atom, occurs. Thus the fate of a large scale object, the cat, is entangled with the fate of a quantum object, the atom. Prior to observation, according to the Schrödinger equation, the cat is apparently evolving into a linear combination of states that can be characterized as an "alive cat" and states that can be characterized as a "dead cat". Each of these possibilities is associated with a specific nonzero probability amplitude; the cat seems to be in some kind of "combination" state called a "quantum superposition". However, a ''single, particular observation'' of the cat does not measure the probabilities: it always finds either a living cat, or a dead cat. After the measurement the cat is definitively alive or dead. The question is: ''How are the probabilities converted into an actual, sharply well-defined outcome?''
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