[8ae8532] | 1 | .. currentmodule:: sasmodels |
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| 2 | .. Wim Bouwman, DUT, written at codecamp-V, Oct2016 |
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| 3 | |
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| 4 | .. _SESANS: |
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| 5 | |
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| 6 | SANS to SESANS conversion |
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| 7 | ========================= |
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| 8 | |
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| 9 | The conversion from SANS into SESANS in absolute units is a simple Hankel |
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| 10 | transformation when all the small-angle scattered neutrons are detected. |
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| 11 | First we calculate the Hankel transform including the absolute intensities by |
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| 12 | |
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| 13 | .. math:: G(\delta) = 2 \pi \int_0^{\infty} J_0(Q \delta) \frac{d \Sigma}{d \Omega} (Q) Q dQ \!, |
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| 14 | |
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| 15 | in which :math:`J_0` is the zeroth order Bessel function, :math:`\delta` |
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| 16 | the spin-echo length, :math:`Q` the wave vector transfer and :math:`\frac{d \Sigma}{d \Omega} (Q)` |
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[f0fc507] | 17 | the scattering cross section in absolute units. |
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| 18 | |
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| 19 | Out of necessity, a 1-dimensional numerical integral approximates the exact Hankel transform. |
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| 20 | The upper bound of the numerical integral is :math:`Q_{max}`, which is calculated from the wavelength and the instrument's maximum acceptance angle, both of which are included in the file. |
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| 21 | While the true Hankel transform has a lower bound of zero, most scattering models are undefined at :math: `Q=0`, so the integral requires an effective lower bound. |
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| 22 | The lower bound of the integral is :math:`Q_{min} = 0.1 \times 2 \pi / R_{max}`, in which :math:`R_{max}` is the maximum length scale probed by the instrument multiplied by the number of data points. |
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| 23 | This lower bound is the minimum expected Q value for the given length scale multiplied by a constant. |
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| 24 | The constant, 0.1, was chosen empirically by integrating multiple curves and finding where the value at which the integral was stable. |
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| 25 | A constant value of 0.3 gave numerical stability to the integral, so a factor of three safety margin was included to give the final value of 0.1. |
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| 26 | |
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| 27 | |
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| 28 | From the equation above we can calculate the polarisation that we measure in a SESANS experiment: |
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[8ae8532] | 29 | |
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| 30 | .. math:: P(\delta) = e^{t \left( \frac{ \lambda}{2 \pi} \right)^2 \left(G(\delta) - G(0) \right)} \!, |
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| 31 | |
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[f0fc507] | 32 | in which :math:`t` is the thickness of the sample and :math:`\lambda` is the wavelength of the neutrons. |
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