TY - GEN
T1 - Weak value measurement with an incoherent measuring device
AU - Cho, Young Wook
AU - Cho, Hyang Tag
AU - Ra, Young Sik
AU - Kim, Yoon Ho
PY - 2010
Y1 - 2010
N2 - In the Aharonov-Albert-Vaidman (AAV) weak measurement, it is assumed that the measuring device or the pointer is in a quantum mechanical pure state. In reality, however, it is often not the case. In this paper, we generalize the AAV weak measurement scheme to include more generalized situations in which the measuring device is in a mixed state. We also report an optical implementation of the weak value measurement in which the incoherent pointer is realized with the pseudo-thermal light. The theoretical and experimental results show that the measuring device under the influence of partial decoherence could still be used for amplified detection of minute physical changes and are applicable for implementing the weak value measurement for massive particles.
AB - In the Aharonov-Albert-Vaidman (AAV) weak measurement, it is assumed that the measuring device or the pointer is in a quantum mechanical pure state. In reality, however, it is often not the case. In this paper, we generalize the AAV weak measurement scheme to include more generalized situations in which the measuring device is in a mixed state. We also report an optical implementation of the weak value measurement in which the incoherent pointer is realized with the pseudo-thermal light. The theoretical and experimental results show that the measuring device under the influence of partial decoherence could still be used for amplified detection of minute physical changes and are applicable for implementing the weak value measurement for massive particles.
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M3 - Conference contribution
AN - SCOPUS:84897730905
SN - 9781557528896
T3 - Optics InfoBase Conference Papers
BT - Quantum Electronics and Laser Science Conference, QELS 2010
T2 - Quantum Electronics and Laser Science Conference, QELS 2010
Y2 - 16 May 2010 through 21 May 2010
ER -