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Ultracold neutrons (UCN) are free neutrons which can be stored in traps made from certain materials. The storage is based on the reflection of UCN by such materials under any angle of incidence.

Properties

The reflection is caused by the coherent strong interaction of the neutron with atomic nuclei. It can be quantum-mechanically described by an effective potential which is commonly referred to as the Fermi pseudo potential or the neutron optical potential. The corresponding velocity is called the critical velocity of a material. Neutrons are reflected from a surface if the velocity component normal to the reflecting surface is less or equal the critical velocity.

As the neutron optical potential of most materials is below 300 neV, the kinetic energy of incident neutrons must not be higher than this value to be reflected under any angle of incidence, especially for normal incidence. The kinetic energy of 300 neV corresponds to a maximum velocity of 7.6 m/s or a minimum wavelength of 52 nm. As their density is usually very small, UCN can also be described as a very thin ideal gas with a temperature of 3.5 mK.

Due to the small kinetic energy of an UCN, the influence of gravitation is significant. Thus, the trajectories are parabolic. Kinetic energy of an UCN is transformed into potential (height) energy with ~102 neV/m.

The magnetic moment of the neutron, produced by its spin, interacts with magnetic fields. The total energy changes with ~60 neV/T.

History

It was Enrico Fermi who realized first that the coherent scattering of slow neutrons would result in an effective interaction potential for neutrons traveling through matter, which would be positive for most materials. The consequence of such a potential would be the total reflection of neutrons slow enough and incident on a surface at a glancing angle. This effect was experimentally demonstrated by Fermi and Walter Henry Zinn and Fermi and Leona Marshall. The storage of neutrons with very low kinetic energies was predicted by Yakov Borisovich Zel'dovich and experimentally realized simultaneously by groups at Dubna and Munich.

Reflecting materials

Material:	VF	vC	η (10−4)
Beryllium	252 neV	6.89 m/s	2.0-8.5
BeO	261 neV	6.99 m/s
Nickel	252 neV	6.84 m/s	5.1
Diamond	304 neV	7.65 m/s
Graphite	180 neV	5.47 m/s
Iron	210 neV	6.10 m/s	1.7-28
Copper	168 neV	5.66 m/s	2.1-16
Aluminium	54 neV	3.24 m/s	2.9-10

Any material with a positive neutron optical potential can reflect UCN. The table on the right gives an (incomplete) list of UCN reflecting materials including the height of the neutron optical potential (V_F) and the corresponding critical velocity (v_C). The height of the neutron optical potential is isotope-specific. The highest known value of V_F is measured for ⁵⁸Ni: 335 neV (v_C=8.14 m/s). It defines the upper limit of the kinetic energy range of UCN.

The most widely used materials for UCN wall coatings are Beryllium, Beryllium oxide, Nickel (including ⁵⁸Ni) and more recently also diamond-like carbon (DLC).

Non-magnetic materials such as DLC are usually preferred for the use with polarized neutrons. Magnetic centers in e.g. Ni can lead to de-polarization of such neutrons upon reflection. If a material is magnetized, the neutron optical potential is different for the two polarizations, caused by

$V_F(pol.)=V_F(unpol.)\pm {\mu }_N\cdot B$

where ${\mu }_N$ is the magnetic moment of the neutron and $B={\mu }_0\cdot M$ the magnetic field created on the surface by the magnetization.

Each material has a specific loss probability per reflection,

$\mu (E,\theta )=2\eta \sqrt{\frac{E{\cos }^2\theta }{V_F-E{\cos }^2\theta }}$

which depends on the kinetic energy of the incident UCN (E) and the angle of incidence (θ). It is caused by absorption and thermal upscattering. The loss coefficient η is energy-independent and typically of the order of 10⁻⁴ to 10⁻³.

Experiments with UCN

The production, transportation and storage of UCN is currently motivated by their usefulness as a tool to determine properties of the neutron and to study fundamental physical interactions. Storage experiments have improved the accuracy or the upper limit of some neutron related physical values.

Measurement of the neutron lifetime

Today's world average value for the neutron lifetime is $885.7\pm 0.8s$, to which the experiment of Arzumanov et al. contributes strongest. Ref. measured ${\tau }_n=885.4\pm 0.9_{\mathrm{s}\mathrm{t}\mathrm{a}\mathrm{t}}\pm 0.4_{\mathrm{s}\mathrm{y}\mathrm{s}\mathrm{t}}s$ by storage of UCN in a material bottle covered with Fomblin oil. Using traps with different surface to volume ratios allowed them to separate storage decay time and neutron lifetime from each other. There is another result, with even smaller uncertainty, but which is not included in the World average. It was obtained by Serebrov et al., who found $878.5\pm 0.7_{\mathrm{s}\mathrm{t}\mathrm{a}\mathrm{t}}\pm 0.4_{\mathrm{s}\mathrm{y}\mathrm{s}\mathrm{t}}s$. Thus, the two most precisely measured values deviate by 5.6σ

Measurement of the neutron electric dipole moment

Mining Engineer (Excluding Oil ) Truman from Alma, loves to spend time knotting, largest property developers in singapore developers in singapore and stamp collecting. Recently had a family visit to Urnes Stave Church. The neutron electric dipole moment (nEDM) is a measure for the distribution of positive and negative charge inside the neutron. No nEDM has been found until now (May 2008). Today's lowest value for the upper limit of the nEDM was measured with stored UCN (see main article).

Observation of the gravitational interactions of the neutron

Physicists have observed quantized states of matter under the influence of gravity for the first time. Valery Nesvizhevsky of the Institute Laue-Langevin and colleagues found that cold neutrons moving in a gravitational field do not move smoothly but jump from one height to another, as predicted by quantum theory. The finding could be used to probe fundamental physics such as the equivalence principle, which states that different masses accelerate at the same rate in a gravitational field (V Nesvizhevsky et al. 2001 Nature 415 297).

Measurement of the A-coefficient of the neutron beta decay correlation

The only reported measurement of the beta-asymmety is from the Los Alamos group. Here's the first paper using UCN to complete a measurement of A using UCN was a 4.5% measurement reported in http://prl.aps.org/abstract/PRL/v102/i1/e012301 the next result from the LANSCE group is also a PRL first authored by Jianglai Liu in 2010 which was roughly 1.5% and a new result will be out in the coming year.