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Physica B: Condensed Matter
Volume 269, Issue 1 , July 1999, Pages 79-94

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doi:10.1016/S0921-4526(99)00048-4    How to Cite or Link Using DOI (Opens New Window)  
Copyright © 1999 Elsevier Science B.V. All rights reserved.

Polarized neutron reflectometry with phase analysis

N. K. PleshanovCorresponding Author Contact Information, E-mail The Corresponding Author

Petersburg Nuclear Physics Institute, PNPI, 188350, Gatchina, St. Petersburg, Russia

Received 21 March 1997; revised 20 November 1998. Available online 7 July 2000.


Abstract

A novel technique, polarized neutron reflectometry with phase analysis (PNRPA), is suggested, in which not only the moduli of reflection matrix elements but also up to three phase differences are measured. It is realized in the scheme with two flippers and an analyzer, by reflection of neutrons with the spin, in succession, parallel and antiparallel to two inclined axes fixed to the sample. More detailed information about magnetic layered structures can be thus obtained. An adequate mathematical formalism is given.

Author Keywords: Polarized neutrons; Reflectometry; Neutron optics; Magnetic films

PACS classification codes: 61.12.Ha


Article Outline

1. Introduction
2. Full neutron reflectometry
3. Scheme with one analyzing axis
4. Scheme with two analyzing axes
5. Magnetically collinear layered structures
6. Summary
Acknowledgements
References



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Fig. 1. Geometrical representation of the spin states of the incident and reflected neutrons in terms of polarization vectors, respectively, P0 (small xi, Greek and small delta, Greek are its polar and axial angles) and Pr (the corresponding angles are small eta, Greek and small zeta, Greek) for an arbitrary quantization (Z) axis. The (X, Y, Z) reference frame is generally independent of the system of coordinates (x, y, z) related to the sample. Due to precession in the guide field, the phase difference of the opposite spin components small delta, Greek (and, consequently, small eta, Greek and small zeta, Greek) is, generally, a function of the surface coordinates (x, y). The orientation of the polarization vector Pr at the sample surface is defined by interference of each pair (NSF and SF) of beams reflected in the same spin state and superposition of the two resultant coherent beams of neutrons in opposite spin states.

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Fig. 2. A structure model (three layers on a glass substrate). The z-axis is normal to the sample surface. Parameters of the model (i stands "for the ith layer"): d1=z1z0=50 nm, d2=z2z1=4 nm, d3=d1 (di is the thickness), V1=V3=100 neV, V2=80 neV (Vi is the nuclear potential), M1,in=M3,in=10 kG, M2=0 (Mi and Mi,in are the total and in-plane magnetization, respectively), small gamma, Greek1=small gamma, Greek3=small pi, Greek/6, (small gamma, Greeki is the angle between Mi,in and the (y, z)-plane).

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Fig. 3. Reflectivities R++, R+−, R−+, R−− (left), the phases curly or open small phi, Greek++, curly or open small phi, Greek+−, curly or open small phi, Greek−+, curly or open small phi, Greek−− of the reflection matrix elements (center) and the phase differences Δ+curly or open small phi, Greek−+curly or open small phi, Greek++, Δcurly or open small phi, Greek−−curly or open small phi, Greek+−, ΔNSFcurly or open small phi, Greek−−curly or open small phi, Greek++, ΔSFcurly or open small phi, Greek−+curly or open small phi, Greek+− (right) are given as a function of the wave vector component normal to the sample surface, kz. Since all reflectivities approach unity at small kz, one can easily guess their absolute magnitudes (the curves are shifted to each other by an integer number of orders). Calculations (a, b, c) are for the structure model shown in Fig. 2. Calculations (d, e) are for the same structure, but when the magnetization in the third layer is parallel to that in the first layer. The quantization axis is always along the applied field which is either along the x-axis (a, e) or along the z-axis (b, c, d) (the coordinate system is defined in Fig. 2). The magnitude of the applied field H is assumed to be vanishing except for the case (c) when it is 0.2 T. The magnetic induction vector in the i-th layer is Bi=Mi,in+H (i=1, 2, 3).

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Fig. 4. The incident neutrons polarized ‘up’ the guide field (P0||H) are assumed to be reflected in a state with the spins non-collinear to H. Since the spins of the reflected neutrons start precessing at different points of the sample surface, they are oriented identically (Pr=const) only in the beam cross sections parallel to the sample surface.

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Fig. 5. All magnetic fields (B) inside a stratified structure are assumed to be collinear. The unit vector b specifies one of the two opposite directions of B.

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Corresponding Author Contact Information Corresponding author. Tel.: +7-812-71-46973; Fax: +7-81271-39053; email: pnk@hep486.pnpi.spb.zu



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Physica B: Condensed Matter
Volume 269, Issue 1 , July 1999, Pages 79-94


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