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Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields

Publisher’s Note: On observation of neutron quantum states in the Earth’s gravitational field [Phys. Rev. D81, 052008 (2010)]

Anatoli Vankov

Published Apr 9, 2010• 1 citation
Publisher

Abstract

with errors in the text on pages 4 and 10. On page 4, left-hand column, the third line should read as ''driven by an external field (the QB, a particle in infinite well), and those driven by an internal field (the quantum. . .).'' On page 10, left-hand column, in the second paragraph, the sixth line should read as ''Airy equation and a neutron guide problem [23]. . . .'' ..

DOI
10.1103/physrevd.81.079901

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Comment On "On observation of neutron quantum states in the Earth's gravitational field"

V. K. Ignatovich

It is shown that criticism in the paper: "On observation of neutron quantum states in the Earth's gravitational field." Phys.Rev.D {\bf 81} 052008 (2010) of the experiment with neutrons to observe bound levels in gravity field is not correct.

arXiv:1101.0888•Jan 5, 2011•0 citations

On observation of neutron quantum states in the Earth’s gravitational field

Anatoli Vankov

Observation of neutron gravitational quantum states ${E}_{n}=mg{z}_{n}$ in the peV energy range (${z}_{1}$ is about $10\text{ }\text{ }\ensuremath{\mu}\mathrm{m}$ in the vertical direction) in the experiment conducted at Laue-Langevin Institute, Grenoble, with ultracold neutrons was recently reported in a series of publications. The purpose of the present work is to analyze the experiment. The experimental apparatus is designed to measure a transmission function $T({z}_{a})$, namely, a horizontal flux of relatively fast neutrons ($k\ensuremath{\gg}{k}_{z}$ in wavelength terms) passing through a slit of variable height ${z}_{a}$ of upper absorbing wall. The quantum states in question are defined by the so-called Airy functions, which are solutions to the stationary 1D equation for a neutron ``bouncing'' above the perfect mirror in a linear potential field. The Airy functions describe the quantum bouncer (QB), the concept of which is subject to theoretical study of toy 1D models of gravitationally bound particles in nonrelativistic quantum mechanics (QM). This is essentially different from the 3D nonstationary QM object, ``the running QB,'' investigated in the experiment. The authors assume that there is a connection between $T({z}_{a})$ and the probability density distribution $P(z,{z}_{a})$ for QB states. They devised the ``phenomenological model,'' in which the quantum pattern should be visible in the transmission curve. We argue, however, that the measured curve $T({z}_{a})$ is not sensitive to QB states. Instead, it is sensitive to dynamics of neutron horizontal transport inside the absorbing slit for neutrons of energy values about ${10}^{5}$ times greater than eigenvalues ${E}_{n}$. The latter are related to the neutron transverse mode ${k}_{z}$ and cannot be termed ``energies of neutron gravitational quantum states.'' We conclude that the experiment setup and real conditions are not adequate to the claimed objective, and the methodology of measured data treatment is flawed. The authors' claim that ``neutron gravitational quantum states are observed'' is neither theoretically nor experimentally substantiated. Final, statistically significant results of the experiment are consistent with our physical reasoning that the experiment is not sensitive to ``neutron gravitational quantum states'' (in terms of Airy mode) and does not prove even their existence in rigorous quantum-mechanical terms.

Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields•Mar 24, 2010•1 citation

Comment on “Measurement of quantum states of neutrons in the Earth’s gravitational field”

Johan Hansson, David Olevik, C. Türk +1 more

In the paper by Nesvizhevsky et al. [Phys. Rev. D 67, 102002 (2003)], it is argued that the lowest quantum state of neutrons in the Earth's gravitational field has been experimentally identified. While this is most likely correct, it is imperative to investigate all alternative explanations of the result in order to close all loopholes, as it is the first experiment ever claimed to have observed gravitational quantum states. Here we show that geometrical effects in the experimental setup can mimic the results attributed to gravity. Modifications of the experimental setup to close these possible loopholes are suggested.

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Reply to “Comment on ‘Measurement of quantum states of neutrons in the Earth’s gravitational field’ ”

Валерий Викторович Несвижевский, A. Petoukhov, H. G. Börner +6 more

Possible false effects in the experiment on the measurement of quantum states of neutrons in the Earth's gravitational field are discussed. It is shown that the measured quantum states are defined mainly by a mirror and the gravitational field.

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Quantum states of neutron in Earth’s gravitional field: A challenge from the 36th international physics olympaid

Vijay A. Singh, Praveen Pathak, K. Krishna Chaitanya

Resonance•Aug 1, 2006•1 citation

Study of the neutron quantum states in the Earth's gravitational field

Валерий Викторович Несвижевский, Hans G. Börner, T.A. Baranova +6 more

We studied the neutron quantum states in the potential well formed by the Earth's gravitational field and a horizontal mirror. The estimated characteristic sizes of the neutron wave functions in two lowest quantum states correspond to their expectations with an accuracy of ~25%. A spatial density distribution in a standing neutron wave above a mirror was measured for a set of a few lowest quantum states. A position-sensitive neutron detector with an extra high spatial resolution of 1-2 mu m was developed and tested for this particular task. Although this experiment was not designed or optimized to search for an additional short-range force, nevertheless it allowed us to slightly improve the published boundary in the nanometer range of characteristic distances. We studied systematical uncertainties in the chosen "flow-through" method as well as the feasibility to improve further the accuracy in this experiment

•May 25, 2005•0 citations
with errors in the text on pages 4 and 10. On page 4, left-hand column, the third line should read as ''driven by an external field (the QB, a particle in infinite well), and those driven by an internal field (the quantum. . .).'' On page 10, left-hand column, in the second paragraph, the sixth line should read as ''Airy equation and a neutron guide problem [23]. . . .'' ..
Observation of neutron gravitational quantum states En=mgzn{E}_{n}=mg{z}_{n}En​=mgzn​ in the peV energy range (z1{z}_{1}z1​ is about $10\text{ }\text{ }\ensuremath{\mu}\mathrm{m}$ in the vertical direction) in the experiment conducted at Laue-Langevin Institute, Grenoble, with ultracold neutrons was recently reported in a series of publications. The purpose of the present work is to analyze the experiment. The experimental apparatus is designed to measure a transmission function T(za)T({z}_{a})T(za​), namely, a horizontal flux of relatively fast neutrons ($k\ensuremath{\gg}{k}_{z}$ in wavelength terms) passing through a slit of variable height za{z}_{a}za​ of upper absorbing wall. The quantum states in question are defined by the so-called Airy functions, which are solutions to the stationary 1D equation for a neutron ``bouncing'' above the perfect mirror in a linear potential field. The Airy functions describe the quantum bouncer (QB), the concept of which is subject to theoretical study of toy 1D models of gravitationally bound particles in nonrelativistic quantum mechanics (QM). This is essentially different from the 3D nonstationary QM object, ``the running QB,'' investigated in the experiment. The authors assume that there is a connection between T(za)T({z}_{a})T(za​) and the probability density distribution P(z,za)P(z,{z}_{a})P(z,za​) for QB states. They devised the ``phenomenological model,'' in which the quantum pattern should be visible in the transmission curve. We argue, however, that the measured curve T(za)T({z}_{a})T(za​) is not sensitive to QB states. Instead, it is sensitive to dynamics of neutron horizontal transport inside the absorbing slit for neutrons of energy values about 105{10}^{5}105 times greater than eigenvalues En{E}_{n}En​. The latter are related to the neutron transverse mode kz{k}_{z}kz​ and cannot be termed ``energies of neutron gravitational quantum states.'' We conclude that the experiment setup and real conditions are not adequate to the claimed objective, and the methodology of measured data treatment is flawed. The authors' claim that ``neutron gravitational quantum states are observed'' is neither theoretically nor experimentally substantiated. Final, statistically significant results of the experiment are consistent with our physical reasoning that the experiment is not sensitive to ``neutron gravitational quantum states'' (in terms of Airy mode) and does not prove even their existence in rigorous quantum-mechanical terms.
In the paper by Nesvizhevsky et al. [Phys. Rev. D 67, 102002 (2003)], it is argued that the lowest quantum state of neutrons in the Earth's gravitational field has been experimentally identified. While this is most likely correct, it is imperative to investigate all alternative explanations of the result in order to close all loopholes, as it is the first experiment ever claimed to have observed gravitational quantum states. Here we show that geometrical effects in the experimental setup can mimic the results attributed to gravity. Modifications of the experimental setup to close these possible loopholes are suggested.
We studied the neutron quantum states in the potential well formed by the Earth's gravitational field and a horizontal mirror. The estimated characteristic sizes of the neutron wave functions in two lowest quantum states correspond to their expectations with an accuracy of ~25%. A spatial density distribution in a standing neutron wave above a mirror was measured for a set of a few lowest quantum states. A position-sensitive neutron detector with an extra high spatial resolution of 1-2 mu m was developed and tested for this particular task. Although this experiment was not designed or optimized to search for an additional short-range force, nevertheless it allowed us to slightly improve the published boundary in the nanometer range of characteristic distances. We studied systematical uncertainties in the chosen "flow-through" method as well as the feasibility to improve further the accuracy in this experiment