|  | 
|  | 1 | +Methods and implementation | 
|  | 2 | +========================== | 
|  | 3 | +*SDCFlows* defines a clear :abbr:`API (application programming interface)` that divides | 
|  | 4 | +the problem of susceptibility distortions (SD) into two stages: | 
|  | 5 | + | 
|  | 6 | +#. **Estimation**: | 
|  | 7 | +   the MRI acquisitions in the protocol for :abbr:`SD (susceptibility distortions)` are | 
|  | 8 | +   discovered and preprocessed to estimate a map of B\ :sub:`0` non-uniformity in Hz (:math:`\Delta B_0`). | 
|  | 9 | +   The theory behind these distortions is well described in the literature ([Jezzard1995]_, [Hutton2002]_), | 
|  | 10 | +   and further discussed below (see a summary in :numref:`fig-1`). | 
|  | 11 | +   *SDCFlows* builds on freely-available software to implement three major strategies for estimating | 
|  | 12 | +   :math:`\Delta B_0` (Eq. :math:`\eqref{eq:fieldmap-1}`). | 
|  | 13 | +   These strategies are described below, and implemented within :py:mod:`sdcflows.workflows.fit`\ . | 
|  | 14 | + | 
|  | 15 | +#. **Application**: | 
|  | 16 | +   the B-Spline basis coefficients used to represent the estimated :math:`\Delta B_0` map mapped into the | 
|  | 17 | +   target :abbr:`EPI (echo-planar imaging)` scan to be corrected, and a displacement field in NIfTI | 
|  | 18 | +   format that is compatible with ANTs is interpolated from the B-Spline basis. | 
|  | 19 | +   The voxel location error along the :abbr:`PE (phase-encoding)` will be proportional to :math:`\Delta B_0 \cdot T_\text{ro}`, | 
|  | 20 | +   where :math:`T_\text{ro}` is the *total readout time* of the target :abbr:`EPI (echo-planar imaging)` (:numref:`fig-1`). | 
|  | 21 | +   The implementation of these workflows is found in the submodule :py:mod:`sdcflows.workflows.apply`\ . | 
|  | 22 | + | 
|  | 23 | +.. _fig-1: | 
|  | 24 | + | 
|  | 25 | +.. figure:: _static/sdcflows-OHBM21-fig1.png | 
|  | 26 | +   :width: 100% | 
|  | 27 | +   :align: center | 
|  | 28 | + | 
|  | 29 | +   Susceptibility distortions in a nutshell | 
|  | 30 | + | 
|  | 31 | +.. admonition:: BIDS Specification | 
|  | 32 | + | 
|  | 33 | +    See the section `Echo-planar imaging and *B0* mapping | 
|  | 34 | +    <https://bids-specification.readthedocs.io/en/latest/04-modality-specific-files/01-magnetic-resonance-imaging-data.html#echo-planar-imaging-and-b0-mapping>`__. | 
|  | 35 | + | 
|  | 36 | +Fieldmap estimation: theory and methods | 
|  | 37 | +--------------------------------------- | 
|  | 38 | +The displacement suffered by every voxel along the :abbr:`PE (phase-encoding)` direction | 
|  | 39 | +can be derived from Eq. (2) of [Hutton2002]_: | 
|  | 40 | + | 
|  | 41 | +.. math:: | 
|  | 42 | +
 | 
|  | 43 | +    \Delta_\text{PE} (i, j, k) = \gamma \cdot \Delta B_0 (i, j, k) \cdot T_\text{ro}, | 
|  | 44 | +    \label{eq:fieldmap-1}\tag{1} | 
|  | 45 | +
 | 
|  | 46 | +where | 
|  | 47 | +:math:`\Delta_\text{PE} (i, j, k)` is the *voxel-shift map* (VSM) along the :abbr:`PE (phase-encoding)` direction, | 
|  | 48 | +:math:`\gamma` is the gyromagnetic ratio of the H proton in Hz/T | 
|  | 49 | +(:math:`\gamma = 42.576 \cdot 10^6 \, \text{Hz} \cdot \text{T}^\text{-1}`), | 
|  | 50 | +:math:`\Delta B_0 (i, j, k)` is the *fieldmap variation* in T (Tesla), and | 
|  | 51 | +:math:`T_\text{ro}` is the readout time of one slice of the :abbr:`EPI (echo-planar imaging)` dataset | 
|  | 52 | +we want to correct for distortions. | 
|  | 53 | + | 
|  | 54 | +Let :math:`V` represent the *fieldmap* in Hz (or equivalently, | 
|  | 55 | +*voxel-shift-velocity map*, as Hz are equivalent to voxels/s), with | 
|  | 56 | +:math:`V(i,j,k) = \gamma \cdot \Delta B_0 (i, j, k)`, then, introducing | 
|  | 57 | +the voxel zoom along the phase-encoding direction, :math:`s_\text{PE}`, | 
|  | 58 | +we obtain the nonzero component of the associated displacements field | 
|  | 59 | +:math:`\Delta D_\text{PE} (i, j, k)` that unwarps the target :abbr:`EPI (echo-planar imaging)` dataset: | 
|  | 60 | + | 
|  | 61 | +.. math:: | 
|  | 62 | +
 | 
|  | 63 | +    \Delta D_\text{PE} (i, j, k) = V(i, j, k) \cdot T_\text{ro} \cdot s_\text{PE}. | 
|  | 64 | +    \label{eq:fieldmap-2}\tag{2} | 
|  | 65 | +
 | 
|  | 66 | +.. _sdc_direct_b0 : | 
|  | 67 | + | 
|  | 68 | +Direct B0 mapping sequences | 
|  | 69 | +~~~~~~~~~~~~~~~~~~~~~~~~~~~ | 
|  | 70 | +.. admonition:: BIDS Specification | 
|  | 71 | + | 
|  | 72 | +    See the section `Types of fieldmaps - Case 3: Direct field mapping | 
|  | 73 | +    <https://bids-specification.readthedocs.io/en/latest/04-modality-specific-files/01-magnetic-resonance-imaging-data.html#case-3-direct-field-mapping>`__ | 
|  | 74 | +    in the BIDS specification. | 
|  | 75 | + | 
|  | 76 | +Some MR schemes such as :abbr:`SEI (spiral-echo imaging)` can directly | 
|  | 77 | +reconstruct an estimate of *the fieldmap in Hz*, :math:`V(i,j,k)`. | 
|  | 78 | +These *fieldmaps* are described with more detail `here | 
|  | 79 | +<https://cni.stanford.edu/wiki/GE_Processing#Fieldmaps>`__. | 
|  | 80 | + | 
|  | 81 | +.. _sdc_phasediff : | 
|  | 82 | + | 
|  | 83 | +Phase-difference B0 estimation | 
|  | 84 | +~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ | 
|  | 85 | +.. admonition:: BIDS Specification | 
|  | 86 | + | 
|  | 87 | +    See the section `Types of fieldmaps - Case 2: Two phase maps and two magnitude images | 
|  | 88 | +    <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>`__ | 
|  | 89 | +    in the BIDS specification. | 
|  | 90 | + | 
|  | 91 | +    Some scanners produce one ``phasediff`` map, where the drift between the two echos has | 
|  | 92 | +    already been calculated, see the section | 
|  | 93 | +    `Types of fieldmaps - Case 1: Phase-difference map and at least one magnitude image | 
|  | 94 | +    <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>`__. | 
|  | 95 | + | 
|  | 96 | +The fieldmap variation in T, :math:`\Delta B_0 (i, j, k)`, that is necessary to obtain | 
|  | 97 | +:math:`\Delta_\text{PE} (i, j, k)` in Eq. :math:`\eqref{eq:fieldmap-1}` can be | 
|  | 98 | +calculated from two subsequent :abbr:`GRE (Gradient-Recalled Echo)` echoes, | 
|  | 99 | +via Eq. (1) of [Hutton2002]_: | 
|  | 100 | + | 
|  | 101 | +.. math:: | 
|  | 102 | +
 | 
|  | 103 | +    \Delta B_0 (i, j, k) = \frac{\Delta \Theta (i, j, k)}{2\pi \cdot \gamma \, \Delta\text{TE}}, | 
|  | 104 | +    \label{eq:fieldmap-3}\tag{3} | 
|  | 105 | +
 | 
|  | 106 | +where | 
|  | 107 | +:math:`\Delta \Theta (i, j, k)` is the phase-difference map in radians, | 
|  | 108 | +and :math:`\Delta\text{TE}` is the elapsed time between the two GRE echoes. | 
|  | 109 | + | 
|  | 110 | +For simplicity, the «*voxel-shift-velocity map*» :math:`V(i,j,k)`, which we | 
|  | 111 | +can introduce in Eq. :math:`\eqref{eq:fieldmap-2}` to directly obtain | 
|  | 112 | +the displacements field, can be obtained as: | 
|  | 113 | + | 
|  | 114 | +.. math:: | 
|  | 115 | +
 | 
|  | 116 | +    V(i, j, k) = \frac{\Delta \Theta (i, j, k)}{2\pi \cdot \Delta\text{TE}}. | 
|  | 117 | +    \label{eq:fieldmap-4}\tag{4} | 
|  | 118 | +
 | 
|  | 119 | +This calculation is further complicated by the fact that :math:`\Theta_i` | 
|  | 120 | +(and therefore, :math:`\Delta \Theta`) are clipped (or *wrapped*) within | 
|  | 121 | +the range :math:`[0 \dotsb 2\pi )`. | 
|  | 122 | +It is necessary to find the integer number of offsets that make a region | 
|  | 123 | +continuously smooth with its neighbors (*phase-unwrapping*, [Jenkinson2003]_). | 
|  | 124 | + | 
|  | 125 | +.. _sdc_pepolar : | 
|  | 126 | + | 
|  | 127 | +:abbr:`PEPOLAR (Phase Encoding POLARity)` techniques | 
|  | 128 | +~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ | 
|  | 129 | +.. admonition:: BIDS Specification | 
|  | 130 | + | 
|  | 131 | +    See the section `Types of fieldmaps - Case 4: Multiple phase encoded directions ("pepolar") | 
|  | 132 | +    <https://bids-specification.readthedocs.io/en/latest/04-modality-specific-files/01-magnetic-resonance-imaging-data.html#case-4-multiple-phase-encoded-directions-pepolar>`__. | 
|  | 133 | + | 
|  | 134 | +Alternatively, it is possible to estimate the field by exploiting the symmetry of the | 
|  | 135 | +distortion when the :abbr:`PE (phase-encoding)` polarity is reversed. | 
|  | 136 | +*SDCFlows* integrates two implementations based on FSL ``topup`` [Andersson2003]_, | 
|  | 137 | +and AFNI ``3dQwarp`` [Cox1997]_. | 
|  | 138 | +By default, FSL ``topup`` will be used. | 
|  | 139 | + | 
|  | 140 | +.. _sdc_fieldmapless : | 
|  | 141 | + | 
|  | 142 | +Fieldmap-less approaches | 
|  | 143 | +~~~~~~~~~~~~~~~~~~~~~~~~ | 
|  | 144 | +Many studies acquired (especially with legacy MRI protocols) do not have any | 
|  | 145 | +information to estimate susceptibility-derived distortions. | 
|  | 146 | +In the absence of data with the specific purpose of estimating the :math:`B_0` | 
|  | 147 | +inhomogeneity map, researchers resort to nonlinear registration to an | 
|  | 148 | +«*anatomically correct*» map of the same individual (normally acquired with | 
|  | 149 | +:abbr:`T1w (T1-weighted)`, or :abbr:`T2w (T2-weighted)` sequences). | 
|  | 150 | +One of the most prominent proposals of this approach is found in [Studholme2000]_. | 
|  | 151 | + | 
|  | 152 | +*SDCFlows* includes an (experimental) procedure, based on nonlinear image registration | 
|  | 153 | +with ANTs' symmetric normalization (SyN) technique. | 
|  | 154 | +This workflow takes a skull-stripped :abbr:`T1w (T1-weighted)` image and | 
|  | 155 | +a reference :abbr:`EPI (Echo-Planar Imaging)` image, and estimates a field of nonlinear | 
|  | 156 | +displacements that accounts for susceptibility-derived distortions. | 
|  | 157 | +To more accurately estimate the warping on typically distorted regions, this | 
|  | 158 | +implementation uses an average :math:`B_0` mapping described in [Treiber2016]_. | 
|  | 159 | +The implementation is a variation on those developed in [Huntenburg2014]_ and | 
|  | 160 | +[Wang2017]_. | 
|  | 161 | + | 
|  | 162 | +The process is divided in two steps. | 
|  | 163 | +First, the two images to be aligned (anatomical and one or more :abbr:`EPI (echo-planar imaging)` sources) are prepared for | 
|  | 164 | +registration, including a linear pre-alignment of both, calculation of a 3D :abbr:`EPI (echo-planar imaging)` *reference* map, | 
|  | 165 | +intensity/histogram enhancement, and *deobliquing* (meaning, for images where the physical | 
|  | 166 | +coordinates axes and the data array axes are not aligned, the physical coordinates are | 
|  | 167 | +rotated to align with the data array). | 
|  | 168 | +Such a preprocessing is implemented in | 
|  | 169 | +:py:func:`~sdcflows.workflows.fit.syn.init_syn_preprocessing_wf`. | 
|  | 170 | +Second, the outputs of the preprocessing workflow are fed into | 
|  | 171 | +:py:func:`~sdcflows.workflows.fit.syn.init_syn_sdc_wf`, | 
|  | 172 | +which executes the nonlinear, SyN registration. | 
|  | 173 | +To aid the *Mattes* mutual information cost function, the registration scheme is set up | 
|  | 174 | +in *multi-channel* mode, and laplacian-filtered derivatives of both anatomical and :abbr:`EPI (echo-planar imaging)` | 
|  | 175 | +reference are introduced as a second registration channel. | 
|  | 176 | +The optimization gradients of the registration process are weighted, so that deformations | 
|  | 177 | +effectively possible only along the :abbr:`PE (phase-encoding)` axis. | 
|  | 178 | +Given that ANTs' registration framework performs on physical coordinates, it is necessary | 
|  | 179 | +that input images are not *oblique*. | 
|  | 180 | +The anatomical image is used as *fixed image*, and therefore, the registration process | 
|  | 181 | +estimates the transformation function from *unwarped* (anatomically *correct*) coordinates | 
|  | 182 | +to *distorted* coordinates. | 
|  | 183 | +If fed into ``antsApplyTransforms``, the resulting transform will effectively *unwarp* a distorted | 
|  | 184 | +:abbr:`EPI (echo-planar imaging)` given as input into its *unwarped* mapping. | 
|  | 185 | +The estimated transform is then converted into a :math:`B_0` fieldmap in Hz, which can be | 
|  | 186 | +stored within the derivatives folder. | 
|  | 187 | + | 
|  | 188 | +.. danger :: | 
|  | 189 | +
 | 
|  | 190 | +    This procedure is experimental, and the outcomes should be scrutinized one-by-one | 
|  | 191 | +    and used with caution. | 
|  | 192 | +    Feedback will be enthusiastically received. | 
|  | 193 | +
 | 
|  | 194 | +Other (unsupported) approaches | 
|  | 195 | +~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ | 
|  | 196 | +There exist some alternative options to estimate the fieldmap, such as mapping the | 
|  | 197 | +point-spread-function [Zaitsev2004]_, or by means of nonlinear registration of brain | 
|  | 198 | +surfaces onto the distorted :abbr:`EPI (echo-planar imaging)` data [Esteban2016]_. | 
|  | 199 | + | 
|  | 200 | +Estimation tooling | 
|  | 201 | +~~~~~~~~~~~~~~~~~~ | 
|  | 202 | +The workflows provided by :py:mod:`sdcflows.workflows.fit` make use of several utilities. | 
|  | 203 | +The cornerstone of these tools is the fieldmap representation with B-Splines | 
|  | 204 | +(:py:mod:`sdcflows.interfaces.bspline`). | 
|  | 205 | +B-Splines are well-suited to plausibly smooth the fieldmap and provide a compact | 
|  | 206 | +representation of the field with fewer parameters. | 
|  | 207 | +This representation is also more accurate in the case the images that were used for estimation | 
|  | 208 | +are not aligned with the target images to be corrected because the fieldmap is not directly | 
|  | 209 | +interpolated in the projection, but rather, the position of the coefficients in space is | 
|  | 210 | +updated and then the fieldmap reconstructed. | 
|  | 211 | + | 
|  | 212 | +Unwarping the distorted data | 
|  | 213 | +---------------------------- | 
|  | 214 | +:py:mod:`sdcflows.workflows.apply` contains workflows to project fieldmaps represented by B-Spline | 
|  | 215 | +basis into the space of the target :abbr:`EPI (echo-planar imaging)` data. | 
|  | 216 | + | 
|  | 217 | +Discovering fieldmaps in a BIDS dataset | 
|  | 218 | +--------------------------------------- | 
|  | 219 | +To ease the implementation of higher-level pipelines integrating :abbr:`SDC (susceptibility distortion correction)`, | 
|  | 220 | +*SDCFlows* provides :py:func:`sdcflows.utils.wrangler.find_estimators`. | 
|  | 221 | + | 
|  | 222 | +Explicit specification with ``B0FieldIdentifier`` | 
|  | 223 | +~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ | 
|  | 224 | +.. admonition:: BIDS Specification | 
|  | 225 | + | 
|  | 226 | +    See the section `Expressing the MR protocol intent for fieldmaps - Using *B0FieldIdentifier* metadata | 
|  | 227 | +    <https://bids-specification.readthedocs.io/en/latest/04-modality-specific-files/01-magnetic-resonance-imaging-data.html#using-b0fieldidentifier-metadata>`__. | 
|  | 228 | + | 
|  | 229 | +If one or more ``B0FieldIdentifier``\ (s) are set within the input metadata (following BIDS' specifications), | 
|  | 230 | +then corresponding estimators will be built from the available input data. | 
|  | 231 | + | 
|  | 232 | +Implicit specification with ``IntendedFor`` | 
|  | 233 | +~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ | 
|  | 234 | +.. admonition:: BIDS Specification | 
|  | 235 | + | 
|  | 236 | +    See the section `Expressing the MR protocol intent for fieldmaps - Using *IntendedFor* metadata | 
|  | 237 | +    <https://bids-specification.readthedocs.io/en/latest/04-modality-specific-files/01-magnetic-resonance-imaging-data.html#using-intendedfor-metadata>`__. | 
|  | 238 | + | 
|  | 239 | +In the case no ``B0FieldIdentifier``\ (s) are defined, then *SDCFlows* will try to identify as many fieldmap | 
|  | 240 | +estimators as possible within the dataset following a set of heuristics. | 
|  | 241 | +Then, those estimators may be linked to target :abbr:`EPI (echo-planar imaging)` data by interpreting the | 
|  | 242 | +``IntendedFor`` field if available. | 
|  | 243 | + | 
|  | 244 | +Fieldmap-less by registration to a T1-weighted image | 
|  | 245 | +~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ | 
|  | 246 | +If none of the two previous options yielded any workable estimation strategy, and provided that | 
|  | 247 | +the argument ``fmapless`` is set to ``True``, then :py:func:`~sdcflows.utils.wrangler.find_estimators` | 
|  | 248 | +will attempt to find :abbr:`BOLD (blood-oxygen level-dependent)` or :abbr:`DWI (diffusion-weighted imaging)` | 
|  | 249 | +instances within single sessions that are consistent in :abbr:`PE (phase-encoding)` direction and | 
|  | 250 | +*total readout time*, assuming they have been acquired with the same shimming settings. | 
|  | 251 | + | 
|  | 252 | +If one or more anatomical images are found, and if the search for candidate | 
|  | 253 | +:abbr:`BOLD (blood-oxygen level-dependent)` or :abbr:`DWI (diffusion-weighted imaging)` data | 
|  | 254 | +yields results, then corresponding fieldmap-less estimators are set up. | 
|  | 255 | + | 
|  | 256 | +It is possible to force the fieldmap-less estimation by passing ``force_fmapless=True`` to the | 
|  | 257 | +:py:func:`~sdcflows.utils.wrangler.find_estimators` utility. | 
|  | 258 | + | 
|  | 259 | +References | 
|  | 260 | +---------- | 
|  | 261 | +.. [Jezzard1995] Jezzard, P. & Balaban, R. S. (1995) Correction for geometric distortion in | 
|  | 262 | +    echo planar images from B0 field variations. Magn. Reson. Med. 34:65–73. | 
|  | 263 | +    doi:`10.1002/mrm.1910340111 <https://doi.org/10.1002/mrm.1910340111>`__. | 
|  | 264 | +.. [Hutton2002] Hutton et al., (2002) Image Distortion Correction in fMRI: A Quantitative | 
|  | 265 | +    Evaluation, NeuroImage 16(1):217-240. doi:`10.1006/nimg.2001.1054 | 
|  | 266 | +    <https://doi.org/10.1006/nimg.2001.1054>`__. | 
|  | 267 | +.. [Jenkinson2003] Jenkinson, M. (2003) Fast, automated, N-dimensional phase-unwrapping | 
|  | 268 | +    algorithm. MRM 49(1):193-197. doi:`10.1002/mrm.10354 | 
|  | 269 | +    <https://doi.org/10.1002/mrm.10354>`__. | 
|  | 270 | +.. [Andersson2003] Andersson, J. (2003) How to correct susceptibility distortions in spin-echo | 
|  | 271 | +    echo-planar images: application to diffusion tensor imaging. NeuroImage 20:870–888. | 
|  | 272 | +    doi:`10.1016/s1053-8119(03)00336-7 <https://doi.org/10.1016/s1053-8119(03)00336-7>`__. | 
|  | 273 | +.. [Cox1997] Cox, R. (1997) Software tools for analysis and visualization of fMRI data. NMR Biomed. | 
|  | 274 | +    10:171–178, doi:`10.1002/(sici)1099-1492(199706/08)10:4/5%3C171::aid-nbm453%3E3.0.co;2-l | 
|  | 275 | +    <https://doi.org/10.1002/(sici)1099-1492(199706/08)10:4/5%3C171::aid-nbm453%3E3.0.co;2-l>`__. | 
|  | 276 | +.. [Studholme2000] Studholme et al. (2000) Accurate alignment of functional EPI data to | 
|  | 277 | +    anatomical MRI using a physics-based distortion model, | 
|  | 278 | +    IEEE Trans Med Imag 19(11):1115-1127, 2000, doi: `10.1109/42.896788 | 
|  | 279 | +    <https://doi.org/10.1109/42.896788>`__. | 
|  | 280 | +.. [Treiber2016] Treiber, J. M. et al. (2016) Characterization and Correction | 
|  | 281 | +    of Geometric Distortions in 814 Diffusion Weighted Images, | 
|  | 282 | +    PLoS ONE 11(3): e0152472. doi:`10.1371/journal.pone.0152472 | 
|  | 283 | +    <https://doi.org/10.1371/journal.pone.0152472>`_. | 
|  | 284 | +.. [Wang2017] Wang S, et al. (2017) Evaluation of Field Map and Nonlinear | 
|  | 285 | +    Registration Methods for Correction of Susceptibility Artifacts | 
|  | 286 | +    in Diffusion MRI. Front. Neuroinform. 11:17. | 
|  | 287 | +    doi:`10.3389/fninf.2017.00017 | 
|  | 288 | +    <https://doi.org/10.3389/fninf.2017.00017>`_. | 
|  | 289 | +.. [Huntenburg2014] Huntenburg, J. M. (2014) `Evaluating Nonlinear | 
|  | 290 | +    Coregistration of BOLD EPI and T1w Images | 
|  | 291 | +    <http://pubman.mpdl.mpg.de/pubman/item/escidoc:2327525:5/component/escidoc:2327523/master_thesis_huntenburg_4686947.pdf>`__, | 
|  | 292 | +    Berlin: Master Thesis, Freie Universität. | 
|  | 293 | +.. [Zaitsev2004] Zaitsev, M. (2004) Point spread function mapping with parallel imaging techniques and | 
|  | 294 | +    high acceleration factors: Fast, robust, and flexible method for echo-planar imaging distortion correction, | 
|  | 295 | +    MRM 52(5):1156-1166. doi:`10.1002/mrm.20261 <https://doi.org/10.1002/mrm.20261>`__. | 
|  | 296 | +.. [Esteban2016] Esteban, O. (2016) Surface-driven registration method for the structure-informed segmentation | 
|  | 297 | +    of diffusion MR images. NeuroImage 139:450-461. | 
|  | 298 | +    doi:`10.1016/j.neuroimage.2016.05.011 <https://doi.org/10.1016/j.neuroimage.2016.05.011>`__. | 
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