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3
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0000611294
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E. Findeisen, R. Feidenhans’l, M.E. Vigild, K.N. Clausen, J. Bindslev Hansen, M. Bentzon and J.P. Goff, J. Appl. Phys., 76, 4636 (1994).
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(1994)
J. Appl. Phys.
, vol.76
, pp. 4636
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Findeisen, E.1
Feidenhans’l, R.2
Vigild, M.E.3
Clausen, K.N.4
Bindslev Hansen, J.5
Bentzon, M.6
Goff, J.P.7
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4
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3643132790
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M.E. Vigild, E. Findeisen, R. Feidenhans’l, K.N. Clausen, C. Barholm-Hansen, M. Bentzon and J.B. Hansen, J. Appl. Phys., 79, 4050-4056 (1996).
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(1996)
J. Appl. Phys.
, vol.79
, pp. 4050-4056
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Vigild, M.E.1
Findeisen, E.2
Feidenhans’l, R.3
Clausen, K.N.4
Barholm-Hansen, C.5
Bentzon, M.6
Hansen, J.B.7
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7
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85013610316
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x-ray reflectometry one can usually do further fine tuning by using the absorption of x-rays by the sample: First one sets the spectrometer to detect the direct through going beam. Then the sample is translated until it blocks half of the direct beam. Subsequently, the sample is rotated to have a minimum blockage, corresponding to a position parallel to the direct beam. These last two steps are repeated until they converge. This procedure works only if the sample strongly absorbs the beam, which is usually not the case with neutrons, for which many samples are transparent
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In x-ray reflectometry one can usually do further fine tuning by using the absorption of x-rays by the sample: First one sets the spectrometer to detect the direct through going beam. Then the sample is translated until it blocks half of the direct beam. Subsequently, the sample is rotated to have a minimum blockage, corresponding to a position parallel to the direct beam. These last two steps are repeated until they converge. This procedure works only if the sample strongly absorbs the beam, which is usually not the case with neutrons, for which many samples are transparent.
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8
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85013612396
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arm = 537 mm will be used in the following
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arm = 537 mm will be used in the following.
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11
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85013622469
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This is equivalent to dividing the refractive indices by the refractive index of the first medium, since the refractive indices are close to one
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This is equivalent to dividing the refractive indices by the refractive index of the first medium, since the refractive indices are close to one.
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