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The sampling locations are ranked in order of descending amount of total leaching (defined as the cumulative leaching from an individual compartment at the end of the experiment), thus collapsing both spatial axes of the sampling plane into one.
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θ is the angle between the magnetic field direction and the sample plane.
The angle between the magnetic field and the sample plane was 12.5°.
In addition, lateral dispersion at the sample plane can be avoided by making the deflection fields symmetric.
For this purpose, a bright and isolated fluorescent particle can be placed at the sample plane of interest.
This results in experimentally observed well-defined orientation dependence of the ρ value in the sample plane.
A permanent magnet was used to generate magnetic field which can be along arbitrary direction in the sample plane.
The resulting helical trajectories of the electrons at the sample plane mean that it is not possible to make a beam that is parallel at the sample.
The BM radiation, collected with 12 toroidal mirrors and collimated with paraboloidal mirrors, illuminates a spot of 60×40 μm2 at the sample plane of a commercial IR microscope.
The magnetic properties of the samples were measured using vibrating sample magnetism (PPMS-VSM) and an applied magnetic field parallel to the sample plane.
The focal spot at the sample plane was ∼1.5μ m in diameter, delivering ∼40 mW of laser power to the sample.
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