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quantum limit : ウィキペディア英語版
quantum limit
A quantum limit in physics is a limit on measurement accuracy at quantum scales.〔
〕 Depending on the context, the limit may be absolute (such as the Heisenberg limit), or it may only apply when the experiment is conducted with naturally occurring quantum states (e.g. the standard quantum limit in interferometry) and can be circumvented with advanced state preparation and measurement schemes.
The usage of term standard quantum limit or SQL is, however, broader than just interferometry. In principle, any linear measurement of a quantum mechanical observable of a system under study that does not commute with itself at different times leads to such limits. In short, it is the Heisenberg uncertainty principle that is the cause .
A more detailed explanation would be that any measurement in quantum mechanics involves at least two parties, an Object and a Meter. The former is the system which observable, say \hat x, we want to measure. The latter is the system we couple to the Object in order to infer the value of \hat x of the Object by recording some chosen observable, \hat}, conjugate to the readout observable \hat}, additive to and independent on the value of the measured quantity \hat x. This one is known as ''measurement imprecision'' or ''measurement noise''. Because of the Heisenberg uncertainty principle, this imprecision cannot be arbitrary and is linked to the back-action perturbation by the uncertainty relation:
:\Delta } \geqslant \hbar/2\,,
where \Delta a = \sqrt is a standard deviation of observable a and \langle\hat a\rangle stands for expectation value of a in whatever quantum state the system is. The equality is reached if the system is in a ''minimum uncertainty state''. The consequence for our case is that the more precise is our measurement, ''i.e'' the smaller is \Delta \mathcal, the larger will be perturbation the Meter exerts on the measured observable \hat x. Therefore, the readout of the meter will, in general, consist of three terms:
:\hat + \delta \hat()\,,
where \hat x_ is a value of \hat x that the Object would have, were it not coupled to the Meter, and \delta \hat }" TITLE="\hat}. The uncertainty of the latter is proportional to \Delta \mathcal\propto\Delta \mathcal^. Thus, there is a minimal value, or the limit to the precision one can get in such a measurement, provided that \delta\hat} are uncorrelated 〔

.
The terms "quantum limit" and "standard quantum limit" are sometimes used interchangeably. Usually, "quantum limit" is a general term which refers to ''any'' restriction on measurement due to quantum effects, while the "standard quantum limit" in any given context refers to a quantum limit which is ubiquitous in that context.
==Examples==


抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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