A diffuse scattering model of ultracold neutrons on wavy surfaces

Metal tubes plated with nickel-phosphorus are used in many fundamental physics experiments using ultracold neutrons (UCN) because of their ease of fabrication. These tubes are usually polished to a average roughness of 25-150 nm. However, there is no scattering model that accurately describes UCN scattering on such a rough guide surface with a mean-square roughness larger than 5 nm. We therefore developed a scattering model for UCN in which scattering from random surface waviness with a size larger than the UCN wavelength is described by a microfacet Bidirectional Reflectance Distribution Function model (mf-BRDF model), and scattering from smaller structures by the Lambert's cosine law (Lambert model). For the surface waviness, we used the statistical distribution of surface slope measured by an atomic force microscope on a sample piece of guide tube as input of the model. This model was used to describe UCN transmission experiments conducted at the pulsed UCN source at J-PARC. In these experiments, a UCN beam collimated to a divergence angle smaller than $\pm 6^{\circ}$ was directed into a guide tube with a mean-square roughness of 6.4 nm to 17 nm at an oblique angle, and the UCN transport performance and its time-of-flight distribution were measured while changing the angle of incidence. The mf-BRDF model combined with the Lambert model with scattering probability $p_{L} = 0.039\pm0.003$ reproduced the experimental results well. We have thus established a procedure to evaluate the characteristics of UCN guide tubes with a surface roughness of approximately 10 nm.

[1]  T. Okamura,et al.  Estimated performance of the TRIUMF ultracold neutron source and electric dipole moment apparatus , 2022, EPJ Web of Conferences.

[2]  C. Gibson,et al.  Characterization of electroless nickel-phosphorus plating for ultracold-neutron storage , 2022, Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment.

[3]  Paul Scherrer Institut,et al.  Ultracold neutron storage and transport at the PSI UCN source , 2021, The European Physical Journal A.

[4]  J. Martin,et al.  Current status of neutron electric dipole moment experiments , 2020, Journal of Physics: Conference Series.

[5]  M. Burghoff,et al.  Measurement of the Permanent Electric Dipole Moment of the Neutron. , 2020, Physical review letters.

[6]  T. Kikawa,et al.  Optimizing neutron moderators for a spallation-driven ultracold-neutron source at TRIUMF , 2019, Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment.

[7]  M.Daum,et al.  Neutron optics of the PSI ultracold-neutron source: characterization and simulation , 2019, The European Physical Journal A.

[8]  P. Schmidt,et al.  Proof of principle for Ramsey-type gravity resonance spectroscopy with qBounce , 2019, EPJ Web of Conferences.

[9]  E. Pierre Toward the First Ultracold-Neutron Production at TRIUMF , 2018, Proceedings of the International Conference on Neutron Optics (NOP2017).

[10]  H. Shimizu,et al.  First ultracold neutrons produced at TRIUMF , 2018, Physical Review C.

[11]  P. Geltenbort,et al.  Neutron lifetime measurements with a large gravitational trap for ultracold neutrons , 2017, Physical Review C.

[12]  Romain Pacanowski,et al.  A two-scale microfacet reflectance model combining reflection and diffraction , 2017, ACM Trans. Graph..

[13]  C. Y. Liu,et al.  Evaluation of commercial nickel-phosphorus coating for ultracold neutron guides using a pinhole bottling method , 2017, 1703.00508.

[14]  L. Pastewka,et al.  Quantitative characterization of surface topography using spectral analysis , 2016, 1607.03040.

[15]  Carsten Dachsbacher,et al.  Multiple-scattering microfacet BSDFs with the Smith model , 2016, ACM Trans. Graph..

[16]  Jonathan Dupuy,et al.  Photorealistic Surface Rendering with Microfacet Theory , 2015 .

[17]  N. Yamada,et al.  The ion beam sputtering facility at KURRI: Coatings for advanced neutron optical devices , 2015 .

[18]  S. N. Ivanov,et al.  Revised experimental upper limit on the electric dipole moment of the neutron , 2015, 1509.04411.

[19]  M.Daum,et al.  A prestorage method to measure neutron transmission of ultracold neutron guides , 2015, 1508.06144.

[20]  H. Shimizu,et al.  Pulsed ultra-cold neutron production using a Doppler shifter at J-PARC , 2015, 1507.07223.

[21]  V. L. Ryabov,et al.  Measurement of the Neutron Lifetime with Ultracold Neutrons Stored in a Magneto-Gravitational Trap , 2014, JETP Letters.

[22]  J. Karch,et al.  Transmission of ultra-cold neutrons through guides coated with materials of high optical potential , 2014 .

[23]  E. Heitz Understanding the Masking-Shadowing Function in Microfacet-Based BRDFs , 2014 .

[24]  S. N. Ivanov,et al.  Apparatus for measurement of the electric dipole moment of the neutron using a cohabiting atomic-mercury magnetometer , 2013, 1305.7336.

[25]  M. Horisberger,et al.  Diffuse reflection of ultracold neutrons from low-roughness surfaces , 2010 .

[26]  S. Materne,et al.  PENeLOPE—on the way towards a new neutron lifetime experiment with magnetic storage of ultra-cold neutrons and proton extraction , 2009 .

[27]  P. Geltenbort,et al.  QuBounce: the dynamics of ultra-cold neutrons falling in the gravity potential of the Earth , 2009 .

[28]  Hiromi Sato,et al.  Design of neutron beamline for fundamental physics at J-PARC BL05 , 2009 .

[29]  K. Torrance,et al.  Microfacet Models for Refraction through Rough Surfaces , 2007, Rendering Techniques.

[30]  P. Fierlinger,et al.  Storage of ultracold neutrons in a volume coated with diamondlike carbon , 2006 .

[31]  S. Lamoreaux,et al.  Neutron electric-dipole moment, ultracold neutrons and polarized 3He , 1994 .

[32]  Donald P. Greenberg,et al.  A comprehensive physical model for light reflection , 1991, SIGGRAPH.

[33]  Sirota,et al.  X-ray and neutron scattering from rough surfaces. , 1988, Physical review. B, Condensed matter.

[34]  Robert L. Cook,et al.  A Reflectance Model for Computer Graphics , 1987, TOGS.

[35]  B. Mandelbrot,et al.  Fractal character of fracture surfaces of metals , 1984, Nature.

[36]  J. Robson Axial peaking of ultra-cold neutrons in a guide tube , 1976 .

[37]  T. Trowbridge,et al.  Average irregularity representation of a rough surface for ray reflection , 1975 .

[38]  R. Golub,et al.  Monte Carlo calculation of ultra cold neutron flow through long tubes with a realistic angular distribution of reflected neutrons , 1975 .

[39]  I. Berceanu,et al.  Molecular flow of ultracold neutrons through long tubes , 1973 .

[40]  K. Torrance,et al.  Theory for off-specular reflection from roughened surfaces , 1967 .

[41]  W. Hager,et al.  and s , 2019, Shallow Water Hydraulics.

[42]  Y. Iwashita,et al.  Production of ultra cold neutrons by a doppler shifter with pulsed neutrons at J-PARC , 2014 .

[43]  Y. Iwashita,et al.  Present status of neutron fundamental physics at J-PARC , 2012 .

[44]  K. Schreckenbach,et al.  Transmission measurements of guides for ultra-cold neutrons using UCN capture activation analysis of vanadium , 2010 .

[45]  F. Hartmann,et al.  A method for evaluating the transmission properties of ultracold-neutron guides , 2007 .

[46]  P. Iaydjiev,et al.  New experimental limit on the electric dipole moment of the neutron , 1999 .

[47]  N. Ramsey Electric-dipole moments of elementary particles , 1982 .

[48]  A. Steyerl Effect of surface roughness on the total reflexion and transmission of slow neutrons , 1972 .

[49]  D. Broadhurst THE NEUTRON ELECTRIC DIPOLE MOMENT ? , 1971 .