Contest details

In the last few years a multitude of new reconstruction approaches have been proposed in diffusion MRI, each group testing the performances of their proposed algorithms with their own synthetic data and evaluation criteria. When proposing a new approach, then, it can be really hard to compare the performances against the state-of-the-art techniques.

The diffusion MRI reconstruction contest is organized with the aim to provide all researchers in this field with a common framework to test their own algorithms on given synthetic datasets and fairly compare their results against other approaches, thus paving the way for a common way to assess the performances and evaluate the results of each method.

How to register

The registration procedure is very simple: just send an email to the organizers with the following details:

  • name of the team (can be either the real name of the group or a name of fantasy);
  • location and institution;
  • contact person and e-mail used for correspondence (NB: this e-mail will never appear on this website);
  • brief description of the method used during the contest (1-2 lines briefly describing the proposed approach).

The registration is open to everyone.

Call for papers

Each team participating to the contest will be requested to write a 1-page abstract describing the approach undertaken. All papers will be gathered to form the workshop proceedings. These proceedings will be published on this website and on the official IEEE International Symposium on Biomedical Imaging (ISBI 2012) website.

Please refer to this template for typesetting your abstract. Since the results will be unknown at the time of submission of the abstract, only a technical description of the method is indeed requested.

Details about the contest

The purpose of the contest is to compare different reconstruction approaches on the same synthetic data and under controlled conditions. To do this, some training data will be released prior of the contest itself, thus allowing the contestants to practice with the data format and test their methods on it. To draw the final ranking, however, another dataset will be used, but this time the ground-truth will be unknown to the contestants.

Note

Contest details might be subjected to changes before the release of the testing dataset. We are receiving some very valuable comments and suggestions about the framework of the contest and we have reserved ourselves the rights to include them for the final contest in order to be as fair as possible. However, the final rules will be published before the testing data is released and will not be modified any further.

Training data

As mentioned above, before the real contest we will release a training data phantom to permit the participants to practice and test their methods with the same kind of data they will be evaluated later on for the final ranking of the contest. This data can be download from the (download section). The ground-truth of this synthetic dataset will be disclosed, meaning that the fibers configuration in each voxel will be revealed to the contestants.

The data will be accompanied with the MATLAB code to simulate the signal at any position in q-space. The participants can simulate the signal corresponding to whatever acquisition scheme they need, without limitations on the number or positions of the samples. They can do whatever they want on this data, there are no limitation on the number of samples to simulate, the experiments they can perform or the algorithms they use. Basically, there are no rules here!

Testing data

Concerning the testing data, which is the synthetic phantom used to evaluate each method and to draw the final ranking of the contest, the ground-truth will be, of course, unknown to the participants. The fibers configuration in each voxel of this dataset will be disclosed only when the final ranking of the contest are published. The format of the data is the same as for the testing data; only the configuration of the fiber compartments in each voxel changes.

Important

The ground-truth of the testing data will be unknown to the contestants! The actual fibers configuration in each voxel of this dataset will be revealed when the final ranking is published.

In order to probe the signal, the contestants will submit to the organizers their acquisition scheme (i.e. one “gradient_list.txt” file) with the q-space positions to probe. Then, they will receive back a file with the signal simulated at each requested sampling point and with different level of noise. In particular, the performances of each method with data having an SNR of 10, 20 and 30 will be tested. At this point, each team can apply his proposed reconstruction method on these signal samples and will then submit to the organizers the estimated fibers configuration in each voxel.

The evaluations of the performances of each method and the final ranking will be published on this website together with the ground-truth of the testing dataset.

Important

Each participant can request the organizers only one acquisition scheme (i.e. “gradient_list.txt”) containing the q-space coordinates where to simulate the signal corresponding to the testing data phantom.

Isolated voxels and structured field

Every synthetic phantom used throughout the contest (both for training and testing) is actually made of two distinct voxel fields:

  1. Isolated voxels dataset.

    This dataset consists in a matrix where each voxel has no spatial relations with its neighbours, so they can be considered independent one another and there isn’t any structure in this dataset. Each voxel contains a random fibers configuration (i.e. the number of fibers can change, their orientations etc). In particular, the dataset will contain voxels with different combinations of:

    • number of fiber compartments;
    • directions of the main axis of each fiber compartment;
    • diffusivity profile (diffusivities).

    The purpose of this dataset is to assess the average performance of each reconstruction method in disentangling distinct fiber compartments under specific experimental conditions.

  2. Structured field dataset.

    This datasets aims to simulate more closely a “real” fibers configuration occuring in reality; several “fiber bundles” are generated having spatial coherence of diffusion properties across neighbouring voxels (see the following figure). The purpose of this dataset is to test the ability of each proposed method to exploit information from neighboring voxels during the reconstruction of the fiber configuration at a given position.

    _images/PHANTOM_demo.png

    Screenshots of a possible synthetic dataset used during the contest. On the left panel, the directions of the fiber compartments in each voxel are reported; as usual, they are color-coded depending on their direction (RED: x-axis, GREEN: y-axis, BLUE: z-axis). On the right panel, instead, the ODFs are plotted for each voxel; ODFs are analytically computed from the model.

Contest rules

In the training phase there are actually no rules! Every participant can probe the signal corresponding to the training data for an unlimited number of times and for every combination of sampling schemes. The structure of this synthetic phantom (i.e. number of fiber compartments in each voxel, orientation etc) will be known to the teams.

Concerning the testing phase some rules apply; here it is a brief summary:

  1. Any signal processing technique, algorithm, available software is allowed, but the outcomes of the proposed method must be reproducible.
  2. The ground-truth of the synthetic phantom will be unknown to the participants, of course! It will be revealed when the final ranking is published.
  3. For the evaluation of the performances of their method, participants will submit to the organizers one (and only one) acquisition scheme (i.e. “gradient_list.txt” file) containing the coordinates in q-space where to probe the signal. They will receive back the signal probed at every position requested.
  4. The maximum number of q-space samples which is possible to probe is fixed to 257, corresponding to the number of samples of a standard DSI acquisition on a hemisphere, assuming central symmetry.
  5. The minimum number of q-space samples is fixed to 6, corresponding to the number of samples of a standard DTI acquisition.
  6. There are no restrictions, however, on the q-space position of the samples.
  7. If a group wishes to participate with different methods, they just need to subscribe the different methods as separate teams (e.g. EPFL01 and EPFL02). They will be treated as independent participants. However, it is strictly forbidded to share the signal samples received for each separate method.

Evaluation criteria

Two main criteria will be considered for determining the final ranking: the reconstruction quality and the number of samples probed. As a general rule, the method achieving the best reconstruction quality with the smallest number of samples will win the contest. Of course the balance among these two criteria is very challenging. We are putting all our might in order to come up with a “fair” trade-off, but we are very open to suggestions in this respect.

At the voxel level, a score will be attributed to each reconstruction method accounting for the following metrics:

  • Correct estimation of the number of fiber compartments, expressed by means of the probability of false fibre detection:

    \frac{ | M_{true} - M_{estimated} | }{ M_{true}}

    where M_{true} and M_{estimated} are, respectively, the real and estimated number of fiber compartments inside the voxel.

  • Angular precision of the estimated fiber compartments, assessed by means of the angular error (in degrees) between the estimated fiber directions and the true ones inside the voxel:

    \arccos( \vec{d}_{true} \cdot \vec{d}_{estimated}) \, \frac{180}{\pi}

    where \vec{d}_{true} is a true direction inside the voxel and \vec{d}_{estimated} is its closest estimate. The final value will be the average of the angular errors computed for all the true fiber compartments. Missing and additional fiber compartments will be penalyzed proportionally to the corresponding volume fraction.

  • Accuracy in the estimation of the ODF, computed as the normalized mean squared error between the estimated ODF, \text{ODF}_{estimated}, and the one analytically computed from the model used for the simulations, \text{ODF}_{true}:

    \frac{ || \text{ODF}_{true} - \text{ODF}_{estimated} ||_2^2 }{ || \text{ODF}_{true} ||_2^2 }

Distinct rankings will be created for every metric, different levels of noise and given specific conditions (i.e. crossing angles). Points will be assigned to each method based on the position of each standing (e.g. 10 points to the 1st, 6 to the 2nd etc.) The reconstruction method accumulating the highest number of points will win the contest!

Note

More details about the exact evaluation of the performances of each reconstruction method (i.e. exact computation of the scores and final ranking) will be published only after the results have been submitted. We do no want to force groups to “tweak” and “tune” their methods depending on the exact evaluation criteria. We would like to fairly compare the methods with the standard metrics used in the literature (e.g. ([Michailovic2011], [Landman2011])). However, as usual, we are open to suggestions and discussions. Should you have any comments, please do not hesitate to contact us by due time!

Teams participating

In this page we list all the registered teams:

Team Members Method
Tocororo01

Erick Jorge Canales-Rodríguez, Lester Melie-García, Yasser Iturria-Medina, Yasser Alemán-Gómez

CIBERSAM and FIDMAG Hermanas Hospitalarias Benito Menni CASM (Barcelona, Spain), Cuban Neuroscience Center (Havana, Cuba), Department of Experimental Medicine and Surgery, Hospital General Universitario Gregorio Marañón (Madrid, Spain)

Reconstruction method described in (E.J. Canales-Rodríguez, C.P. Lin, Y. Iturria-Medina, C.H. Yeh, K.H. Cho and L. Melie-García, “Diffusion orientation transform revisited”, Neuroimage, Jan 15;49(2):1326-39, 2010)
Tocororo02

Erick Jorge Canales-Rodríguez, Lester Melie-García, Yasser Iturria-Medina, Yasser Alemán-Gómez

CIBERSAM and FIDMAG Hermanas Hospitalarias Benito Menni CASM (Barcelona, Spain), Cuban Neuroscience Center (Havana, Cuba), Department of Experimental Medicine and Surgery, Hospital General Universitario Gregorio Marañón (Madrid, Spain)

Reconstruction method described in (E.J. Canales-Rodríguez, Y. Iturria-Medina, Y. Alemán-Gómez and L. Melie-García, “Deconvolution in diffusion spectrum imaging”, Neuroimage, Mar;50(1):136-49, 2010)
The HARDY

Farshid Sepehrband, Jayran Chupan, Quang Tieng, Viktor Vegh, Steven Yang

Centre for Advanced Imaging, The University of Queensland (Brisbane, Australia)

Iterative scheme that employs super-resolution techniques similar to track-density imaging to create tractography at higher anatomical resolution, which in turn is used as prior knowledge to regularize the HARDI reconstruction
The HOT gang

Yaniv Gur

SCI Institute, University of Utah (Salt Lake City, USA)

Low-rank approximations of Higher Order Tensors (HOT)
MrSCIL

Michael Paquette, Maxime Descoteaux

Sherbrooke Connectivty Imaging Lab, Sherbrooke University (Sherbrooke, Quebec, Canada)

Method under development
MrSS

Maxime Descoteaux, Arnaud Boré

Sherbrooke Connectivty Imaging Lab, Sherbrooke University (Sherbrooke, Quebec, Canada)

Single-shell HARDI reconstruction method
NIPG

Ying-Chia Lin, Gloria Menegaz

University of Verona (Verona, Italy)

Multi-resolution denoising approach
Athena

Emmanuel Caruyer, Sylvain Merlet, Aurobrata Ghosh, Rachid Deriche

Inria (Sophia-Antipolis Méditerranée, France)

Method under development
Frogs

Alonso Ramirez-Manzanares, Angel Ramon Aranda Campos, Mariano Rivera Meraz

University of Guanajuato (Guanajuato, Mexico), Research Center on Mathematics, CIMAT, A.C., (Guanajuato, Mexico)

Improved version of the Diffusion Basis Functions Method (A. Ramírez-Manzanares, M. Rivera, et al, “Diffusion basis functions decomposition for estimating white matter intravoxel fiber geometry”, IEEE TMI, 26(8), 2007)
Hawks

Merry Mani, Mathews Jacob, Jianhui Zhong

University of Rochester (Rochester, USA), University of Iowa (Iowa City, USA)

Method under development
The Diffusiontamers

Paulo Rodrigues, Vesna Prčkovska

Universitat de Barcelona (Barcelona, Spain), IDIBAPS (Barcelona, Spain)

Method under development
Tyranny

Eleftherios Garyfallidis

University of Cambridge (Cambridge, United Kingdom)

The Equatorial Inversion Transform
Frunik

Marco Reisert, Valerij Kiselev, Henrik Skibbe

Department of Radiology, University Medical Center (Freiburg, Germany)

L1-based deconvolution with spatial regularization


Results and ranking

This section reports the results of the preliminary analysis performed at the time of the challenge. Please note that some results are missing (not available at the time ot the submission) or corrupted (issues in the data format like orientation problem etc).

Please refer to the latest analysis for more recent and detailed results.

Teams’ performance

This section reports the individual performace of each team.

Final ranking

As discussed during the workshop, finding the proper trade-off between the quality a methoid achieves and the number of samples it uses was very though, if not impossible at all to estimate since it depends a lot on the question one wants to answer.

Anyway, for the scope of this contest, three different weighting functions f(\epsilon,n) have been proposed:

  • f_1(\epsilon,n) = \epsilon
  • f_2(\epsilon,n) = \epsilon \cdot \exp{(n/257)}
  • f_3(\epsilon,n) = \epsilon \cdot \sqrt{n}

where \epsilon and n are, respectively, the value of one of the given error metrics and the number of samples used.

Of course, increasing the weighting degree has the effect of favoring methods with less points. The weighting function has been democratically selected among the participants by email before revealing the comparison results. The function f_2(\epsilon,n) was the chosen one.

In the following, we report the three separate standings created by using the three aforementioned weighting functions.

References

[Michailovic2011]Michailovic et al. Spatially regularized compressed sensing for high angular resolution diffusion imaging. IEEE TMI, 30: 1100-1115 (2011)
[Landman2011]Landman et al. Resolution of crossing fibers with constrained compressed sensing using diffusion tensor MRI. Neuroimage, In press (2011)

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