Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Weak measurements and negative probabilities

Klaus Mølmer

Published Jan 1, 2000• 0 citations
OpenAlex

Related papers

Negative probabilities and information gain in weak measurements

Xuanmin Zhu, Qun Wei, Quanhui Liu +1 more

arXiv:1212.6324•Physics Letters A•Jul 19, 2013•5 citations

Weak measurements, non-classicality and negative probability

Sooryansh Asthana, V. Ravishankar

arXiv:2006.12436•Quantum Information Processing•Oct 1, 2021•2 citations

How "negative probabilities" emerge in weak measurements?

Xuanmin Zhu, Qun Wei, Quanhui Liu +1 more

We study the outcomes in a general measurement with postselection, and derive upper bounds for the pointer readings in weak measurement. Using the idea of weak measurement, we study Hardy's gedanken experiment and show how the negative probabilities emerge in weak measurement. By calculating the information gain of the measuring device about which path the particles pass through, we show that the negative probabilities only emerge for cases when the information gain is little due to very weak coupling between the measuring device and the particles. When the coupling strength increases, we can unambiguously determine whether a particle passes through a given path every time, hence the average shifts always represent true probabilities, and the strange negatives probabilities disappear.

•Dec 27, 2012•1 citation

Weak measurements measure probability amplitudes (and very little else)

D. Sokolovski

arXiv:1511.04241•Physics Letters A•Mar 2, 2016•34 citations

When a negative weak value −1 plays the counterpart of a probability 1

Kazuhiro Yokota, Nobuyuki Imoto

When the weak value of a projector is 1, a quantum system behaves as in that eigenstate with probability 1. By definition, however, the weak value may take an anomalous value lying outside the range of probability like −1. From the viewpoint of a physical effect, we show that such a negative weak value of −1 can be regarded as the counterpart of the ordinary value of 1. Using photons, we experimentally verify it as the symmetrical shift in polarization depending on the weak value given by pre-postselection of the path state. Unlike observation of a weak value as an ensemble average via weak measurements, the effect of a weak value is definitely confirmed in Hong–Ou–Mandel effect: the symmetrical shift corresponding to the weak value can be directly observed as the rotation angle of a half wave plate.

arXiv:1607.08039•New Journal of Physics•Dec 2, 2016•6 citations

Negative probabilities and measurement disturbance

Lars M. Johansen

Bulletin of the American Physical Society•Mar 10, 2008•0 citations
We study the outcomes in a general measurement with postselection, and derive upper bounds for the pointer readings in weak measurement. Using the idea of weak measurement, we study Hardy's gedanken experiment and show how the negative probabilities emerge in weak measurement. By calculating the information gain of the measuring device about which path the particles pass through, we show that the negative probabilities only emerge for cases when the information gain is little due to very weak coupling between the measuring device and the particles. When the coupling strength increases, we can unambiguously determine whether a particle passes through a given path every time, hence the average shifts always represent true probabilities, and the strange negatives probabilities disappear.
When the weak value of a projector is 1, a quantum system behaves as in that eigenstate with probability 1. By definition, however, the weak value may take an anomalous value lying outside the range of probability like −1. From the viewpoint of a physical effect, we show that such a negative weak value of −1 can be regarded as the counterpart of the ordinary value of 1. Using photons, we experimentally verify it as the symmetrical shift in polarization depending on the weak value given by pre-postselection of the path state. Unlike observation of a weak value as an ensemble average via weak measurements, the effect of a weak value is definitely confirmed in Hong–Ou–Mandel effect: the symmetrical shift corresponding to the weak value can be directly observed as the rotation angle of a half wave plate.