@@ -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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+
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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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+
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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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-
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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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+
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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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+
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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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-
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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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+
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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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-
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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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