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

Bulletin of the American Physical Society

The weak measurement process and the weak value of spin for metastable helium $2^{3}S_{1}$

Vincenzo Monachello, P. F. Barker, R. L. Flack, Basil J. Hiley

Published May 24, 2016• 0 citations
OpenAlex

Related papers

The Two-Photon Transition Probabilities from the Metastable 2 ~S1 State in the Helium Like Series

Oleg Bely, P. Faucher

Astronomy and Astrophysics•Jan 1, 1969•0 citations

The De-Excitation of Helium Metastable Atoms in Helium

E. H. S. Burhop

Proceedings of the Physical Society Section A•Mar 1, 1954•14 citations

A method for measuring the real part of the weak value of spin using non-zero rest mass particles

Vincenzo Monachello, R. L. Flack, Basil J. Hiley +1 more

A method for measuring the real part of the weak (local) value of spin is presented using a variant on the original Stern-Gerlach apparatus. The experiment utilises metastable helium in the $\rm 2^{3}S_{1}$ state. A full simulation using the impulsive approximation has been carried out and it predicts a displacement of the beam by $\rm Δ_{w} = 17 - 33\,μm$. This is on the limit of our detector resolution and we will discuss ways of increasing $\rm Δ_{w}$. The simulation also indicates how we might observe the imaginary part of the weak value.

arXiv:1701.04808•Jan 17, 2017•0 citations

A Method for Measuring the Weak Value of Spin for Metastable Atoms

R. Flack, Vincenzo Monachello, Basil J. Hiley +1 more

A method for measuring the weak value of spin for atoms is proposed using a variant of the original Stern-Gerlach apparatus. A full simulation of an experiment for observing the real part of the weak value using the impulsive approximation has been carried out. Our predictions show a displacement of the beam of helium atoms in the metastable 23S1 state, Δw, that is within the resolution of conventional microchannel plate detectors indicating that this type of experiment is feasible. Our analysis also determines the experimental parameters that will give an accurate determination of the weak value of spin. Preliminary experimental results are shown for helium, neon and argon in the 23S1 and 3P2 metastable states, respectively.

Entropy•Jul 30, 2018•4 citations

The Magnetic Moment of Helium in the TRIPLET-S(1) Metastable State.

C. W. Drake

•Jan 1, 1958•0 citations

The weak value of spin for atomic systems

Vincenzo Monachello, R. L. Flack

A system is being designed and constructed in order to measure the weak value of spin for atomic systems. The experiment utilises spin-1 metastable helium atoms in the 2 3 S 1 state. This paper outlines the experiment and its features.

Journal of Physics Conference Series•Mar 1, 2016•3 citations
The weak measurement process and the weak value of spin for metastable helium 23S12^{3}S_{1}23S1​
A method for measuring the real part of the weak (local) value of spin is presented using a variant on the original Stern-Gerlach apparatus. The experiment utilises metastable helium in the 23S1\rm 2^{3}S_{1}23S1​ state. A full simulation using the impulsive approximation has been carried out and it predicts a displacement of the beam by Δw=17−33 μm\rm Δ_{w} = 17 - 33\,μmΔw​=17−33μm. This is on the limit of our detector resolution and we will discuss ways of increasing Δw\rm Δ_{w}Δw​. The simulation also indicates how we might observe the imaginary part of the weak value.
A method for measuring the weak value of spin for atoms is proposed using a variant of the original Stern-Gerlach apparatus. A full simulation of an experiment for observing the real part of the weak value using the impulsive approximation has been carried out. Our predictions show a displacement of the beam of helium atoms in the metastable 23S1 state, Δw, that is within the resolution of conventional microchannel plate detectors indicating that this type of experiment is feasible. Our analysis also determines the experimental parameters that will give an accurate determination of the weak value of spin. Preliminary experimental results are shown for helium, neon and argon in the 23S1 and 3P2 metastable states, respectively.