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enh: move BIDS' spec references below the section's title
Co-authored-by: Mathias Goncalves <[email protected]>
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docs/methods.rst

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@@ -56,18 +56,29 @@ we obtain the nonzero component of the associated displacements field
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Direct B0 mapping sequences
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~~~~~~~~~~~~~~~~~~~~~~~~~~~
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.. admonition:: BIDS Specification
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See `this section of the BIDS specification
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<https://bids-specification.readthedocs.io/en/latest/04-modality-specific-files/01-magnetic-resonance-imaging-data.html#case-3-direct-field-mapping>`__.
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Some MR schemes such as :abbr:`SEI (spiral-echo imaging)` can directly
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reconstruct an estimate of *the fieldmap in Hz*, :math:`V(i,j,k)`.
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These *fieldmaps* are described with more detail `here
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<https://cni.stanford.edu/wiki/GE_Processing#Fieldmaps>`__.
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This corresponds to `this section of the BIDS specification
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<https://bids-specification.readthedocs.io/en/latest/04-modality-specific-files/01-magnetic-resonance-imaging-data.html#case-3-direct-field-mapping>`__.
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.. _sdc_phasediff :
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Phase-difference B0 estimation
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~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
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.. admonition:: BIDS Specification
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See `this section of the BIDS specification
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<https://bids-specification.readthedocs.io/en/latest/04-modality-specific-files/01-magnetic-resonance-imaging-data.html#case-2-two-phase-maps-and-two-magnitude-images>`__.
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Some scanners produce one ``phasediff`` map, where the drift between the two echos has
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already been calculated, see `the corresponding section of BIDS
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<https://bids-specification.readthedocs.io/en/latest/04-modality-specific-files/01-magnetic-resonance-imaging-data.html#case-1-phase-difference-map-and-at-least-one-magnitude-image>`__.
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The fieldmap variation in T, :math:`\Delta B_0 (i, j, k)`, that is necessary to obtain
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:math:`\Delta_\text{PE} (i, j, k)` in Eq. :math:`\eqref{eq:fieldmap-1}` can be
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calculated from two subsequient :abbr:`GRE (Gradient-Recalled Echo)` echoes,
@@ -97,23 +108,20 @@ the range :math:`[0 \dotsb 2\pi )`.
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It is necessary to find the integer number of offsets that make a region
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continuously smooth with its neighbors (*phase-unwrapping*, [Jenkinson2003]_).
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This corresponds to `this section of the BIDS specification
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<https://bids-specification.readthedocs.io/en/latest/04-modality-specific-files/01-magnetic-resonance-imaging-data.html#case-2-two-phase-maps-and-two-magnitude-images>`__.
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Some scanners produce one ``phasediff`` map, where the drift between the two echos has
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already been calculated (see `the corresponding section of BIDS
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<https://bids-specification.readthedocs.io/en/latest/04-modality-specific-files/01-magnetic-resonance-imaging-data.html#case-1-phase-difference-map-and-at-least-one-magnitude-image>`__).
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.. _sdc_pepolar :
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:abbr:`PEPOLAR (Phase Encoding POLARity)` techniques
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~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
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.. admonition:: BIDS Specification
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See `this section of the BIDS specification
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<https://bids-specification.readthedocs.io/en/stable/04-modality-specific-files/01-magnetic-resonance-imaging-data.html#case-4-multiple-phase-encoded-directions-pepolar>`__.
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Alternatively, it is possible to estimate the field by exploiting the symmetry of the
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distortion when the PE polarity is reversed.
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*SDCFlows* integrates two implementations based on FSL ``topup`` [Andersson2003]_,
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and AFNI ``3dQwarp`` [Cox1997]_.
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This corresponds to `this section of the BIDS specification
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<https://bids-specification.readthedocs.io/en/stable/04-modality-specific-files/01-magnetic-resonance-imaging-data.html#case-4-multiple-phase-encoded-directions-pepolar>`__.
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By default, FSL ``topup`` will be used.
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.. _sdc_fieldmapless :
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