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Deformable part models for object detection in medical images
BioMedical Engineering OnLine volumeÂ 13, ArticleÂ number:Â S1 (2014)
Abstract
Background
Object detection in 3D medical images is often necessary for constraining a segmentation or registration task. It may be a task in its own right as well, when instances of a structure, e.g. the lymph nodes, are searched. Problems from occlusion, illumination and projection do not arise, making the problem simpler than object detection in photographies. However, objects of interest are often not well contrasted against the background. Influence from noise and other artifacts is much stronger and shape and appearance may vary substantially within a class.
Methods
Deformable models capture the characteristic shape of an anatomic object and use constrained deformation for hypothesing object boundaries in image regions of low or nonexisting contrast. Learning these constraints requires a large sample data base. We show that training may be replaced by readily available user knowledge defining a prototypical deformable part model. If structures have a strong partrelationship, or if they may be found based on spatially related guiding structures, or if the deformation is rather restricted, the supporting data information suffices for solving the detection task. We use a finite element model to represent anatomic variation by elastic deformation. Complex shape variation may be represented by a hierarchical model with simpler part variation. The hierarchy may be represented explicitly as a hierarchy of subshapes, or implicitly by a single integrated model. Data support and model deformation of the complete model can be represented by an energy term, serving as qualityoffit function for object detection.
Results
The model was applied to detection and segmentation tasks in various medical applications in 2 and 3D scenes. It has been shown that model fitting and object detection can be carried out efficiently by a combination of a local and global search strategy using models that are parameterized for the different tasks.
Conclusions
A partbased elastic model represents complex withinclass object variation without training. The hierarchy of parts may specify relationship to neighboring anatomical objects in object detection or a partdecomposition of a complex anatomic structure. The intuitive way to incorporate domain knowledge has a high potential to serve as easily adaptable method to a wide range of different detection tasks in medical image analysis.
Background
Motivation
Although medical images provide insight into patientspecific human anatomy otherwise not accessible, their interpretation still requires extensive expert knowledge to fill the semantic gap between image data and depicted anatomy and/or function. Image characteristics of the objectofinterest may be known but are often not unique. Furthermore, noise, imaging or reconstruction artifacts alter the depicted content to a much greater extent than for pictures such as photos. Anatomical objects are not always contrasted well against each other and neighboring structures have similar appearance. However, most of the data is 3D. Change of shape and appearance due to projection has not to be dealt with.
Still, detection and segmentation is possible if a suitable model completes missing information and corrects measurement errors in the data. The premier effect of such deficient information would be an incorrect delineation of the object's boundary. Hence, shape is the most important supplementary model information. Context information about adjacent structures, as well as information about object and background appearance may be added for discriminating among similar objects.
Developing a different method for each new detection or segmentation task is inefficient. Thus, a major challenge is to find a parameterizable representation that can be adapted efficiently for finding different objects.
Object shape can be represented by sampling points on its boundary. If such model is fitted to the data, boundary points of a model instance are registered with likely boundary locations in the image (e.g., high gradient strength locations). If artifacts or low contrast cause some model points not to have counter parts in the image, the model instance predicts the local course of the boundary there. Visible shape parts have to be sufficiently characteristic so that this prediction does not result in inacceptable errors.
Several problems have to be dealt with:

The model has to include withinclass variation of the structure of interest, while inhibiting influences from betweenclass variation.

A weight for combining data and model needs to be set appropriately.

The search for object instances in the data has to deal with many local minima of the corresponding optimization criterion.
Fusing shape model and image data requires a qualityoffit (QoF) function where supporting information from the data are represented by a term {E}_{external}, which is regularized by a term {E}_{internal}, representing, in this case, deviation from the prototypical shape model:
This expression is found in many formulations of segmentation and detection tasks. It may be interpreted as an energy balance where external influences from a potential field generated by the data are counteracted by internal forces that represent domain knowledge such as the shape of an object or just the smoothness of its boundary. The parameter Î» weighs the reliability of these two kinds of information. The equation can also be interpreted as logarithm of the conditional probability given by a normaldistributed likelihood function based on {E}_{external} and a normaldistributed a priori probability depending on {E}_{internal}. Here, Î» represents the ratio of variances of the two distributions.
Equation (1) may be optimized by gradient descent. It requires that the model instance is initialized sufficiently close to the optimum searched for. For global optimization, stochastic search techniques, e.g., the method by [1] may be used, which draws randomly distributed initializations and selects the best fitting candidates based on (1).
With this paper, we present an elastically deformable model as representation for shape and appearance. We argue that this model may be used efficiently for object detection as it does represent shape variation and expected appearance for an object class without requiring training (although training may improve performance). The main reason for this lies in the fact that model information is represented by integrating simple deformable shapes in a partbased model that, depending on the task, either represents object parts or guiding structures. We show that this model can be applied to solve different detection and segmentation tasks in medical image analysis.
The remainder of the paper is structured as follows. We first present previous work on models in object detection for medical images. We then present our elastic model, its application to object detection and its extension to a partbased model. We conclude with a number of examples that show the different capabilities of applying the model to detection and segmentation tasks.
Previous work
Extracting an objectofinterest from the image contradicts the usual assumption for segmentation that segment characteristics are part of the data information. Extracting, e.g., a liver from CT images may require separating it from gall bladder, stomach, and feeding vessel. Depending on imaging modality and protocol the appearance of these structures may be very similar and insufficient for separation.
Extraction may be simple for a human observer with necessary knowledge about shape, appearance and location of the organ. In a computerguided solution, a detection task has to be solved first, which supports the subsequent boundary delineation task. The two tasks may be solved in parallel or sequentially. In the latter case, the detection result constrains the subsequent segmentation. In the former case, a model instance is expected to deform into the object that is searched for.
The information that is needed for detection and segmentation can be quite complex. Necessary domain knowledge may be introduced at several stages of the process and the "intelligence" of the solution lies in the construction of the process from its subtasks (e.g., the kidney detection and segmentation scheme of [2]). Alternatively, a model can be built that contains information of all aspects about the object necessary for identification in the data including possible dependencies between different types of information. Detection is then fitting a model to measured data (e.g., the application of a shape and appearance model for detecting the left ventricle of the heart in MRI [3]). We prefer the latter approach as it separates model description from the search for model instances and may be adapted easier to a new detection task.
If detection precedes delineation, it localizes the objectofinterest. In this case, the result locally constrains boundary delineation if the object is not sufficiently contrasted against adjacent structures. Localization may be interactive (e.g., seed points for region growing [4], closed active contours [5], or starting points for live wire delineation [6]). In this case, the detection result often includes little information with respect to object boundary, since interaction costs are usually kept to a minimum. Hence, interactive localization is most suitable if the boundary itself is well defined by the data and interaction is used to find the object among different structures with similar appearance. Small artifacts such as noise can be accommodated by requiring smooth and closed boundaries. If substantial parts of the boundary cannot be derived from data information, they need to be added by interactive delineation of boundary parts.
Localization by matched filter methods such as vesselness filters [7], blobness [8], template matching [9] and Hough transform [10] does not require interaction, except possibly for specification of a relevancy threshold for a successful detection. These methods are capable of finding multiple instances of an object. The filters predict the (average) object shape and appearance which may then be used as prior for datadriven segmentation, e.g., by graph cuts [11â€“13] or level sets [14, 15]. The methods operate with few parameters which usually can be found easily. Of course, it restricts shape representation either to variable, but simple shapes (e.g., the vesselness filter) for which intraclass variation can be described by few parameters, or to a representation by a single average shape (e.g., the generalized Hough transform).
Representing acceptable shape variation of complex object shape is more difficult. Unconstrained shape variation will cause the model to fit almost everywhere in the image while an overly constrained shape will not fit well to the data. Active Shape Models (ASM) and its many variants have found widespread use since their introduction in [16]. Shape is represented by coordinates of a set of labeled points. If appearance variation shall be represented as well, it is given by intensity or texture variation at these points. Variation is trained from correspondingly labeled test data. Influence from rotation, translation and sometimes scaling has to be removed by Procrustes analysis [17]. Variation is assumed to be normaldistributed and highly correlated. Hence, principal component analysis is used for decorrelation and information is reduced to a few eigenmodes (modes of variation). The model enables a potentially arbitrarily exact fitting of the missing boundary, as long as the visible part of the boundary sufficiently constrains the variation of the missing part.
Training of such a point distribution model (PDM) can serve two purposes. It estimates shape (and appearance) variation of the class of objects to be delineated and it restricts shape variation. The success of PDMs for modelguided segmentation has been shown in numerous publications (e.g., [5, 18, 19]). Often only few training samples  considering the degrees of freedom of the untrained model  are needed for segmentation. The reason is probably twofold. Firstly, withinclass shape variation has much fewer degrees of freedom than the model so that the true covariance can be estimated from few samples. Secondly, boundary delineation does not require exact estimates of intraclass variation anyway as long as incorrectly estimated shape variation is corrected from boundary information in the data.
Besides PDM, the Hough transform may be extended into a probabilistic shape model as well [20]. However, compared to a PDM, its versatility is restricted since appearance information is not part of the model and it is unclear how the trained information may be used for subsequent boundary delineation.
Since a shape model has not to be very accurate for boundary delineation, prototypical variation has also been used for shapesupported boundary delineation. If detection is not necessary (e.g. when tracking a heart shape in a 3d+time sequence), the necessary shape information are properties such as closedness, smoothness and similarity of the boundary between time frames. This has been used, e.g., in tracking the heart beat from CT using an active surface based on a finite element model (FEM) to restrict boundary variation between time steps [21]. This concept has been extended to an elastically deforming shape model (e.g., the massspring model [22] or an FEM [23]). Such model restricts organ variation to elastic deformation of a prototypical shape. This is particularly simple for a homogeneous, linearelastic FEM since only few parameters regulate its stiffness. Defining such a prototype solves part of the optimization problem in detection as well, since  similar to active contour models  rather basic image information can be embedded by forces acting on a model instance, locally attracting it to the objectofinterest.
However, an elastic model provides just an approximation of intraclass shape variation. To some extent, either the delineation goal or the detection goal has to be sacrificed if the shape of the object itself or its variability is complex. If stiffness overestimates true shape variation, the model instance may adapt to the object boundary given sufficiently reliable image information, but shape deformation may not be used for object detection. If the shape variation is overconstrained it may be used for object detection but will result in a poor segmentation of the object.
Instead of training complex shape variation, some of this variation can be efficiently represented using partbased models. A shape is decomposed into simpler parts. Variation is then that of the parts and that of partrelationships. In other applications, partbased models have been successfully used for articulated object detection (e.g., detection of faces and people [24], or pedestrian recognition [25]). Although partrelationships may be learnt [26], an advantage is that the qualitative knowledge of a decomposition of an object into parts is often readily available (e.g. the decomposition of the spine into a sequence of vertebrae separated by disks). We successfully applied a combination of deformable models with a partbased representation for several object detection and boundary delineation tasks in medical image analysis.
With this paper we describe how to use our partbased deformable model for object detection and segmentation and illustrate the applicability to different tasks in medical image analysis.
Methods
As stated above, variation represented by deformable models often does not have to be exact. However, if it is to be specified by the user instead of being trained from samples, parameterization of the model should be intuitive. Representing the object as an elastically deformable material meets this condition since most users have an understanding of how elasticity influences shape variability. Elastic models have been used in medical image applications for quite some time (e.g., [27] for elastic registration), although not often to restrict shape variation for detection tasks. We use this concept to replace trained shape variation. It should be noted that we do not want to simulate deformation behavior of an object (e.g., the deformation of the heart ventricles over time). Elastic deformation is solely used to replace distribution estimates to restrict shape variation among objects of the same class. Since describing complex shape variation by few elasticity parameters may be too simple, we use deformable objects as components of a partbased model. Relationships between parts are modeled by an elastic superstructure.
Object detection consists of a local and a global part. Localized delineation lets a model instance be attracted and deformed by image features. The global search is realized by repeatedly generating random initializations of model instances and selecting the best fitting candidates. Fitting is defined according to equation (1) by a data term that is regularized by shape deformation.
Finite Element Models (FEM)
We use FEMs to represent the deformable shape. A finite element model represents linearelastic deformation of a 2D or 3D object based on a discretization of the object domain into finite elements e. Elements are generated from node locations that sample the object domain. The number of nodes depends on the accuracy with which an object is described. For a given object, the FEM is generated from a 2D or 3D representation of the object's shape, either based on a priori knowledge, e.g., about the shape of a vertebra, or from an example segmentation. If segmented data is used, it should reflect a representative object example. It may also be helpful to smooth the segmentation in order to remove irrelevant detail from the model instance before generating the FEM. The FEM may be generated by triangulating the segment, e.g., by computing a Delaunay triangulation.
For a single element, external forces {f}^{\left(e\right)} at element nodes cause node displacement {u}^{\left(e\right)}. Their relation is governed by a stiffness matrix {K}^{\left(e\right)}
The displacement depends on applied forces, the elasticity and geometry of the element, as well as on the interpolation functions used to compute continuous material deformation within the element. When linear interpolation is sufficient  which is true for our applications  element shape and elasticity parameters are the only influences that define the deformation behavior.
The different elements e of the FEM are assembled according to the decomposition of the object domain (for details see [28]). It results in an aggregated stiffness matrix K which gives the following relation between forces f and displacement u via
Elementwise assemblage happens in two steps (see Figure 1). First, nodes of all elements are relabeled so that nodes of two different elements have the same label only if this node is common to the two elements. Then, expanded matrices {K}_{exp}^{\left(e\right)} and force vectors {f}_{exp}^{\left(e\right)} are created for each element e having a size that depends on the total number of nodes of the FEM. Locations in {K}_{exp}^{\left(e\right)} and {f}_{exp}^{\left(e\right)} that represent labels not occurring in e are filled with 0's. Assemblage is then simply summing expanded matrices and vectors.
The FEM approximates the mean shape and possible physicsbased deformation of the objectofinterest. Shape variation among different exemplars from the object class is given by the FEM decomposition and few material parameters. Assuming that the model consists of isotropic, linear elastic material, the elasticity of the elements can be described by Poisson's ratio and the elastic modulus [29]. The Poisson's ratio p is the ratio between deformation in the direction of an incident force and deformation orthogonal to it (see Figure 2a). For most materials, 0 â‰¥ p > 1, since compression in one direction causes expansion in the orthogonal direction. For object detection, it may be useful to define a positive Poisson ratio. This would cause contraction in all directions if forces in some direction cause compression. Scale invariance can be implemented (to a small extent) using this parameterization.
The elastic modulus, given the isotropic material assumptions above, may be described by Young's modulus. It tells how an isotropic material resists deformation due to opposing forces (see Figure 2b). Changing Young's modulus controls the amount of deformation due to external forces, e.g., imagederived forces.
Given element geometry, interpolation functions, Poisson's ratio and Young's modulus, the stiffness matrix can be computed for each element and assembled into global stiffness matrix K. Hence, the FEM, created from an exemplary segmentation or from a priori knowledge, represents a deformable shape by very few parameters that are intuitive in a sense that a user does not have to understand the underlying numerical concepts of the FEM method.
Dynamic optimization and object detection
Using the FEM for object detection requires localizing and deforming the model based on imagederived forces. The extension of the FEM to a dynamic model has the practical advantage that parts of the localization tasks can be solved as a timedependent attraction of a model instance to local image features. It requires extension of the governing equation by a mass matrix M, which represents resistance to forces based on the current acceleration Ã¼(t) at time t, and by a damping matrix D that represents transfer of kinetic energy dependent on current speed \stackrel{\xcb\u2122}{u}\left(t\right):
Specifying masses in M is necessary if a moving model instance should resist force changes from the image in order to let it move over spurious image details from noise or artifacts. If this is not necessary, mass may be omitted, leading to a damped gradient descent.
For practical reasons, we use Raleigh damping, which defines D as linear combination of M and K:
If the system is massfree, we may set D = I + Î² K, where I is the identity matrix.
External forces acting on FEM nodes may be defined separately and differently for every node. It is, however, practical to define node groups and let each node group be attracted by the same kind of image forces. Examples are the following:

Boundary nodes are attracted by boundary features in the image

Inner nodes are attracted by image features according to the specific appearance of the object to be detected
Different kinds of boundary or appearance nodes can be defined if the expected edge strength or appearance varies in an objectspecific fashion.
External forces can be computed based on the current location and displacement of nodes with respect to image features in the model's vicinity. This may become necessary if the data is unreliable and current node locations and displacement are used to select image regions evaluated for force computation. An example will be demonstrated in Application 2 described below.
If data quality permits, external forces can be precomputed as gradient of a potential field derived from the image. Potential fields may be defined separately for each node group (see Figure 3). Nodes of the FEM are pulled to a minimum in the potential. In order to attract an FEM instance over some distance, the potential field is convolved with an influence function, i.e., a low pass filter that is decreasing with distance from the kernel center. Local features for boundary nodes are edges or edge features such as gradient length. Local features for appearance nodes depend on expected intensity or texture. The influence function is a Gaussian of which the variance determines the influence radius.
It should be noted that, while boundary nodes relate visible object boundary in the image directly to model nodes, appearance nodes typically do not. Since expected appearance (e.g., brightness) may or may not be constant over the object it may not help to move and deform an FEM instance into its proper place. Appearance nodes are useful nonetheless:

A single or several appearance nodes may help to determine whether the boundary nodes  which are only sampling the boundary  sit on the correct object boundary.

Appearance nodes that sample the appearance inside the object and in the background in the object's vicinity may serve as a complex boundary model in cases where the boundary is difficult to detect in the data using a local operation such as edge detection.
Since local features are not unique (otherwise, detection would be trivial), the influence radius, i.e., kernel width should be as large as possible in order to attract FEM instances from far away, but small enough to avoid overlapping influences, i.e., blurring from different local features.
Given particular potential fields, an FEM instance can be placed anywhere in the image and deforms under the fieldderived forces. The potential field is constant over time and may be precomputed. Forces f change with the displacement in the potential field and, therefore, with time. An instance has found its final destination when internal forces from deformation and external forces from the image balance each other. Computing adaptation of the deforming FEM instance to the image requires computation of the dynamic system described by equation (4).
Computation of this system of dependent differential equations can be done in several ways (see, e.g., [28]). We prefer a computation via decorrelation into independent modes. It does not only produce a stable solution to the problem but also allows selecting relevant deformation modes (similar to the selection of variation modes in ASM). This has been used for object classification [30], mapping between similar objects [31], and to provide a base for training an ASM, if training is desired and possible [32].
For optimization, a generalized eigenproblem is solved for mass matrix M and stiffness matrix K
where Î› is the diagonal matrix of eigenvalues, E is the column matrix of eigenvectors and I is the identity matrix. Mapping K and M onto E and assuming Raleigh damping according to equation (5) results in a new system
The new diagonalized system contains simple differential equations of the type
where e _{i} is the ith eigenvector of E and Î» _{i} is the ith eigenvalue. An analytical solution for such equations can be computed stably and fast. The approach is applicable for a massfree system as well.
Eigenvectors and eigenvalues carry semantics similar to ASM. An eigenvector is called a mode of vibration and represents a generalized symmetry axis of shape deformation. The overall deformation is a weighted sum of the generalized deformations due to the transformed forces E^{T} f(t). It is possible to reduce the number of modes in order to remove small information details and reduce computational costs. Eigenvalues characterize the amount of force necessary to cause displacement. Assuming ascending order of eigenvalues, the first n! eigenvalues of an ndimensional FEM will be zero and represent rigid transformation (rotation and translation). The following, intermediate eigenvalues are the most relevant modes representing shape deformation.
Rigid transformation is still part of the model, which is different to ASM where the trained model is normalized with respect to rotation and translation and where this information has to be incorporated into the fitting process by means of an additional registration step. This causes problems, however, since deformation constrained by the stiffness matrix K is defined as strain caused by a directed force on an infinitesimal line at this point. Since this line is defined in the given coordinate system, rotation of the FEM instance would make the stiffness matrix K dependent on the current rotation, hence dependent on time t. This is unwanted since it would require recomputation of K and of the vibration modes at every new iteration step. Neglecting it would cause some part of the rotation to be interpreted as deformation possibly leading to serious distortions (see Figure 4) [33]. This is only acceptable if we assume that local fitting of the model instance comprises only little rotation. Still, this would result in a loss of the benefit of including rotation into the optimization. Hence, we use warping techniques, presented, e.g., by [33, 34] to circumvent the problem.
The basic idea of warping is to include the current rotation into the representation. Therefore, forces are applied to the unrotated model and the result is rotated back. If warping is applied on the node level, the current rotation R _{ i } is computed for all nodes i. They are concatenated into an orthogonal matrix R of which its inverse is applied to the current displacement u(t) as well as to its derivatives. Deformation is then applied to these vectors and the result is rotated back (the impact of this correction can be seen in Figure 4). It can be shown that this can be applied in the spectral basis as well [33]. This essentially means that the current vibration modes are "rotated" versions of the original modes.
The current rotation can be computed by several methods. A fast way is to search for the rotation R _{ i } at node coordinates x _{ i } that optimally registers difference vectors d _{ ij } = x _{ i }  x _{ j } between x _{ i } and adjacent nodes x _{ j } relative to difference vectors d _{ ij 0}at t = 0. The resulting optimization problem
for each node can be computed fast using a method proposed by [35].
Dynamic optimization of an FEM instance as described above produces a locally optimal fit. For global optimization we use a stochastic initialization technique similar to the method that was suggested by [1]. FEM instances are initialized at different locations in the image and serve as detection candidates for the objectofinterest. After performing local optimization as described above the best candidates spawn new instances in their vicinity. The process ends when no further improvement can be reached.
Rating candidates requires definition of a QoF function. It is defined according to equation (1). Data quality {E}_{external} measures the value of the potential field at final node locations and the regularization term {E}_{internal} measures the deviation of the model from its initial shape based on the weights of the vibration modes.
Computational complexity of the process is O(N) where N is the number of nodes of the model instance. However, computation times depend on the convergence of the various iterative optimization schemes, namely the iterative deformation, the iterative computation of the singular value decomposition in [35] for computing the warping, and on the number of iterations in the stochastic search.
Hierarchical partbased model
The few parameters of the deformable model described in the previous section are sufficient for object detection as long as the object in question has a rather characteristic mean shape and appearance. If this is not the case, training of shape variation such as in ASMs would help. However, to reduce training effort (ideally up to a point where all parameters are userspecified based on domain knowledge), information has to be included in a qualitative rather than a quantitative way. Hence, we adopted the principle of partbased models for augmenting the descriptive power of our model.
Representation by a partbased model serves two different purposes:

The parts may be subobjects of the objectofinterest (such as the vertebrae of a spine model).

The parts may relate the objectofinterest to surrounding objects that help to localize the object.
Additionally to the elastic deformation of the parts, division into parts, their relationship to each other, and potential mutual deformation are relevant for model specification.
A partbased model can be realized conveniently within a hierarchical FEM (HFEM) framework [36â€“38]. The shape is decomposed into parts based on user's specification. Each part is represented by an FEM. This constitutes the morphological layer of the complex object. Parts may have different material properties and different potential fields to accommodate their different semantics. Spatial relationships between parts are represented by a secondlevel FEM which constitutes the structural layer. Forces on the structural layer FEM are exerted from deformation and displacement on the morphological layer of the HFEM. They, in turn, impose constraints on the shape of its structural layer.
The HFEM may be realized explicitly by generating a set of morphological and structural FEM or implicitly by generating a single, heterogeneous FEM from the morphological and the structural FEM.
Explicit representation results in a set of independent morphological FEM that are coupled to the structural layer via virtual zerolengthsprings that connect nodes of the two layers [36] (see Figure 5). Relationships between subshapes are specified by the kind of connection between the layers. For instance, the following relationships can be defined for a 2D model using different numbers of nodes (see Figure 6):

A singleconnected shape may rotate independently but is restricted in distance to other subshapes via the structural layer.

A subshape that is connected via two nodes to the structural layer is further restricted in its rotation. Properties such as approximate orthogonality or parallelism of parts can be ensured by this kind of connection.

A subshape connected by more than two nodes shares some of its nonrigid deformations via the structural layer.
The influence of external forces between layers is then realized by a message passing algorithm [37]. Displacements due to deformation on the morphological layer act as external forces on the structural layer, while deformations on the structural layer cause forces on the morphological layer. Computation of the dynamic behavior, hence, requires solving the optimization problem presented in the previous section for each subshape on the morphological layer, passing the resulting forces to the structural layer, computing the resulting deformation and passing displacement back to the morphological layer.
In the hierarchical representation, each FEM is diagonalized separately resulting in its own vibration modes. It allows selecting vibration modes independently for each FEM. Hence, different requirements on precision, e.g., between structural and morphological layer, or for different substructures on the morphological layer can be accommodated.
When computing the quality of fit, equation (1) has to be computed first for energies E _{ j } of each subshape j on the morphological layer, resulting in a weighted sum of morphological fits
The weights w _{ j } may be used to account for a different importance of parts. If, for instance, some parts are just guiding structures to find the actual objectofinterest, their fit has not to be very precise.
Since the part relationship may be decisive for detecting the object, deformation and image support is then computed for the structural layer FEM as well. Deformation is measured in the same way as for the morphological layer. The external energy is now given by the state of the morphological subshapes. Hence, it is simply defined by the QoF from the subshapes of the layer below.
Alternatively to representing the part model as a hierarchy of homogeneous FEM it may also be represented as single heterogeneous FEM [38] (see Figure 7). Heterogeneity refers to the fact that it will be a combination of the different partFEMs, each of which possibly having different elasticity parameters.
Morphological and structural layer FEM are defined as above. However, instead of treating them as single FEM, which communicate through message passing, the FEM are assembled in the same way as elements were assembled to the FEM. Assemblage is guided by node connections between structural and morphological layer as before. Through the assemblage these nodes are treated as shared nodes between elements of the morphological and the structural layer.
Solving the partbased FEM optimization by assemblage in a single, heterogeneous FEM has different properties compared to the previous method:

Computation of vibration modes applies to the complete partbased object and optimization does not require message passing between deformable part models.

The qualityoffit is computable in the same way than for a single FEM based on deformation and input from the data.

Different potential fields and/or different material properties of the partFEM replace the weights in equation 10.

If warping is used on the node level this applies to the complete FEM. Hence, singleconnected FEM do not allow independent rotation.
In general, the second solution is simpler regarding computation of dynamic deformation and stochastic optimization, but it also integrates parts tighter into the representation. Therefore, it depends on the application which of the two methods should be preferred. This will be discussed further in the next section where we will present different applications using the two approaches for different analysis goals in medical image analysis.
Results and discussion
In the following, we present a number of applications to illustrate how to parameterize and use a partbased deformable model for various tasks in medical image analysis. We will summarize performance and results for each application. Since we use the application to demonstrate the use of the model, we refer to the original publications [38â€“40] for details.
Indentifying Heschl's gyrus in flat maps of the human cortex
Experiments with functional magnetic resonance imaging (fMRI) attempt to localize and delineate particular brain regions, such as the human primary auditory cortex (pAC) and neighboring higherorder areas, in vivo. The pAC is known to be located on the first transverse temporal gyrus (i.e., Heschl's gyrus, HG). Since the region covered by the pAC is very small with respect to the spatial resolution of fMRI and the signal to noise ratio is rather poor, fMRI data of a population of subjects are combined to arrive at a representative functional map. The combination of individual data to a group map requires the mapping of corresponding regions across subjects. We solved this registration task by localizing macroanatomical landmarks (i.e., the lateral "Sylvian" fissure and superior temporal sulcus) that delineate the superior temporal lobe and enclose the highly variable Heschl's gyrus. The detection is performed using a deformable model of HG that is fitted to the cortical surface (i.e., a surface mesh that represents the greywhite matter interface, gwI) [36, 40]).
Input data for the deformable object detection task are 2dimensional flat maps of the gwI (details about cortex reconstruction and flattening can be found in [41]). The function value at each location in the flat map is the curvature of the folded cortex before flattening (see Figure 8). Hence, change from outward folds (gyri) to inward folds (sulci) is given by zero crossings in the flat map.
Identifying HG in a given flat map requires finding a specific Ushaped border at those zero crossings. This is difficult since the size, location, orientation and individual shape of HG vary substantially between subjects, while there are several gyri of similar shape in each cortical flat map. Experts identify the correct gyrus by means of its relation with two anatomical landmarks: the Sylvian fissure (SF) and sulcus temporalis superior (STS) are approximately parallel to each other and orthogonal to HG.
A partbased deformable model is well suited to represent anatomical descriptions such as Ushapedness and spatial relations between cortical gyri and sulci.
HG, STS and SF were modeled on the morphological layer of a twolevel model and combined on a structural layer that models the structural configurations of the macroanatomical landmarks. Since the gyri and sulci were simple 2D shapes, they were manually drawn based on example images. For HG, two different variants were created since some subjects may have a HG with a sulcus intermedius (SI).
Boundary nodes of the HG and the HG+SI models had access to smooth potential fields, whose minima represent zero crossing locations of the flat map. In practice, the filtering operations were approximated as follows. For a given surface mesh we computed a discrete, differenceofGaussian filtered version of the curvature mapping: We first applied an operator that separated convex regions (gyri) and concave regions (sulci), and then we used a discrete approximation of a heat diffusion kernel to smooth the resulting binary map. The low pass filter kernel widths of Ïƒ _{1} = 2 mm and Ïƒ _{2} = 2Ïƒ _{1} for the differenceofGaussian provided a good tradeoff between a large region of influence and blurring of adjacent zero crossings. During the model fit, we estimated for each model node the vector to the nearest salient vertex on the cortical surface mesh (with a local maximum filter response and within a given sampling distance) and used the weighted radial component of this vector as external force.
Internal nodes of the HG model responded to positive curvature (gyri) only, whereas the HG+SI model contained nodes responding to negative curvature (sulci) at the SI location as well. Again, the potential fields were in practice defined based on heat kernel smoothed versions of the binary curvature maps.
The shape and pose of HG, the exact relations between HG and the landmarks and also the shape of the landmarks SF and STS vary dramatically between subjects:

Since SF and STS primarily served as limits for restricting the cortex region to be searched for HG, it was important to robustly and correctly localize these landmarks, while only roughly matching their main branches. The STS and SF models were constructed as simple lineshaped structures, undersampled with FE nodes that responded only to appearance, i.e. curvature information. This sparse sampling allowed bridging gaps in the curvature maps, while sufficient similarity of the structure to a line was still ensured. (example images showing variability of SF, STS)

The model at the toplayer arranged HG (and HG+SI, resp.) as the central part of the AC folding pattern nearly orthogonal to the two surrounding parallel sulci. To set up a sparse top layer model, "link" nodes were identified for related subshapes and duplicated such that the resulting structural model consisted of these shared link nodes (see Figure 9). Four nodes represented the parallel arrangement of SF and STS in the 2D flat maps, and the internal node was linked with the HG model to position it "above STS" and "below SF". In the structural prior model HG+SI an additional node was linked with a simple SI model in a "contained in HG"relation.

The FE nodes are then subject to boundary conditions, such that any nodal displacement in the morphological coordinate frames (e.g., due to image forces) enforced displacements in the global model coordinate frame, while the resulting nodal displacements of the toplayer model acted as acrosslevel spring forces on the link nodes of the morphological shape models.

The search for the independent optimum pose parameters (of the structural model as well as HG and HG+SI, resp.) was based on a quasi stochastic sampling of an a priori constrained search space. To define the constraints, we used the Talairachtransformed flat map coordinate system [40, 42] and asked an expert to annotate an example and specify possible variations in the location, size and orientation of the anatomical structures. This information was encoded in terms of pose parameter distribution functions.

Young's modulus was 2.0, Poisson ratio was 0.4 and material density was set to 1.0 for all models.
At each iteration of the deformable model search, a population of 100 model instances was initialized with random affine parameterizations and fitted to the data. Randomness was introduced into this evolutionary process by employing a rank selection of fitted instances. Reproductive success varied with the relative "fitness", i.e. quality, of instances. Poor fitting results were deleted, and Gaussian noise was added to the pose parameters of the best fitting instances to simulate the "mutation" in the reproduction step and initialize new deformable model instances. This evolution process ends if no improvement in overall fitting quality was observed (typically after 3 steps).
Success of the deformable model search for HG was measured by determining the percentage of cases were the correct gyrus was identified by one or more model instances among the 2% of best rated candidate solutions. The method was applied to flat maps from 80 subjects. A detailed discussion of results can be taken from [36, 40]. In summary, we could show that

Using just the HG model without guiding structures and constraints on possible poses resulted in a 5% success. By constraining the search space, the correct gyrus was identified in about 50% of all cases.

Using the HG model together with SF and STS resulted in 80% success which can be improved to more than 90% if model parameters have been trained.

This partbased model could be directly used (1) to compute precise segmentations of HG with less than 3 mm error compared with manual segmentations of HG and (2) to classify the given cortical surfaces correctly with respect to the presence of a sulcus intermedius.

Using a singlelayer model that comprises HG, STS and SF instead of the multiple layer model led to a significant decrease in result quality which did not improve by training. This means that the relevant anatomical information was better captured by the structural decomposition and deformation parameters.

The method is very robust to changes in the parameterization.
This example shows that domain knowledge, such as the structural arrangement of landmark structures that predict the location of a highly variable object of interest within data that carry poor semantics, can be directly formulated in the form of efficient constraints of a hierarchical, deformable model. This is very interesting in that one could expect that such a model provides a better symbolic representation of the "true" object anatomy and anatomical variability than a model that is learnt from annotated training data. Moreover, the expert knowledge can be more efficiently improved by training (e.g., of correct poses) and expressed with less effort (e.g., by annotating a single example and "painting" connecting relations such as "parallel to" and "contained in" between the different structures, by accepting good solutions, applying interactive forces during the model fit or by correcting the deformed shape of poorly fitted model instances).
Segmenting the Substantia Nigra in transcranial sonography
Transcranial sonography (TCS) produces ultrasound images of the brain that are acquired by imaging through the temporal bone window. The mesencephalic brain stem, or midbrain, containing the substantia nigra (SN) is visible in TCS images, although image quality compared to regular ultrasound images is poor.
The echogenicity of the SN is a relevant feature in the diagnosis of Parkinson's disease [43]. Computerguided delineation of SN in TCS images has been the goal of the work presented in [39]. We observed that the butterflyshaped midbrain section imaged by TCS is fairly invariant across patients as is the SN location relative to the midbrain. Since image artifacts inhibit a direct segmentation of the SN on the basis of low level image features, such as intensity or gradients, we used an elastically deformable model for the detection of the midbrain. This is again a partbased model, but here we used a hierarchy of morphologies in a sequential fit (see Figure 10). The first layer consisted of two SN regions that were attached to a midbrain shape model on the second layer. The shape model is then used to constrain the final segementation (instead of using the shape itself for segmentation such as in [44]).
Since artifacts and noise severely distort the images, it was not possible to compute smooth and reliable potential functions by linear filtering. To set up external image forces, we used a regional classifier over image regions that are large enough to counteract this effect and provide object boundary information. Three different node potentials were defined to account for the nondeterministic image signal:

Appearance nodes of all parts have a similar potential function: SN nodes reacted on high echodensity, since the SN typically produces more reflections than surrounding midbrain tissue. The internal nodes of the SN models sample a Gaussian low pass filtered version I* = G _{ Ïƒ } âˆ— I of the image I (where Ïƒ = 2.0), and the intensity forces are f = Îºâˆ‡I*, with Îº > 0. For the echopoor midbrain, we expect low intensities in the interior and let Îº < 0.

The boundary FE nodes did not rely on intensity gradients since these were extremely unreliable. Instead, we computed at each iteration of the model fit a balloonforce f _{ b } = Îº _{ b } n in the model instances' current contour normal direction that pulls the nodes towards more robustly estimated intertissue boundaries. The magnitude and sign Îº _{ b } of the balloon force was defined using regional texture information. We dynamically computed an optimal discriminant between "object" and "background" based on statistics over image intensity samples taken from the inside of the model and from the background. The sampling regions were defined in the image in inward and outward normal directions at the boundary nodes of the model instance.

Young's modulus was 0.9, Poisson ratio was 0.25 and material density was set to 0.9 for all models
As in the previous section, a deformable shape search computed the best fitting shape by simultaneous optimization of multiple twolayer model instances. In this application, however, the search was performed sequentially on the global (midbrain localization) and local context (detection and segmentation of the SN). After finding the best fitting instance of the midbrain model, multiple instances with different parameterizations of the SN models were aligned to it and matched to the data to detect the hyperintense SN regions. This sequential process was necessary because the SN appears as a stripelike structure on both branches of midbrain, but regularly exhibits the same echotexture as the adjacent brain tissue. That is, the midbrain serves as "guiding structure" for the contained SN, but for a given TCS image it is neither known in advance whether the SN is clearly visible, nor how much an echodense pattern of the SN extends. The fit of SN models should not influence the deformation of the midbrain model instance.
Successful detection means that the true boundary of the SN will be in the vicinity of the boundary estimate by the SN subshapes. A final segmentation should make use of this information (e.g., shapedriven level sets [15] or graph cuts [12]). In the last step of our algorithm, the boundaries of the two deformed SN templates were taken as initial placement of Active Contour Models, which are then locally deformed to precisely adapt to the SN boundaries in the TCS image. The template contours were resampled to increase the sampling density and flexibility of the contour models. Internal forces and external balloon forces were set up as described in [45] and above (see [39] for details).
The model was applied to 10 data sets, for which expert segmentations were available, and it was found that in all cases the echogenic patterns of the midbrain and SN were correctly localized (Figure 11 shows an example). Small values of 1.03 Â± 0.44 mm boundary error at a pixel size of 0.1482 mm showed that the region boundaries were also outlined with high precision. This example application shows how to combine a model search with a constrained segmentation without training based on qualitative a priori knowledge about the appearance of the object. It also shows that the model is able to overcome problems from serious distortions in the image by replacing gradient information by a more elaborate boundary model.
Detection of human vertebrae in MRI
Investigation of normal variation of the anatomy of the spine and its vertebrae is one of the research questions within SHIP (Study of Health in Pommerania, [46]). We use MRI from SHIP to detect the course of vertebrae of the lower back. More than 40 different MRI image sequences have been acquired within SHIP from several thousands of subjects in Pommerania. Two of the sequences  a T_{1}weighted and a T_{2}weighted sequence  showing spine and vertebrae were used for the detection task using our modelbased approach. Although vertebrae detection and segmentation focuses on radiographs and CT images, MRIbased analysis has been the subject of research in medical image analysis as well [47]. The domain knowledge in existing methods is often represented by a specific combination of processing modules where model information is inserted at several stages. Our goal was to investigate whether this can be replaced by our deformable part model. The advantage would be that adapting the detection to some other application would solely relate to model generation without having to change modules of the search process.
Global optimization was not used since initialization is simple for the given data. The user places the model instance in a sagittal view on the middle slice of the image sequence. Optimization then takes place by model deformation based on local image attributes.
The model was constructed according to the appearance of vertebrae and spine in a sample image sequence. Main attractor is the spine which is clearly visible in all images. Hence, the model consisted of a twolevel hierarchy where vertebrae subshapes were connected with a spine subshape by a structural model on the second level (see Figure 12). Vertebrae subshapes were constructed all equal since no substantial variation is expected between different vertebrae of the lower back. The spine model supported proper localization of the vertebrae. Since its most discriminate aspect was the cylindrical shape, it was represented by a deformable, straight cylinder consisting of appearance nodes only. Appearance nodes represent the vertebra shape, since the relatively low and varying signal of the gradient allows only for small values of Ïƒ in the smoothing function if boundary nodes were chosen. This strategy bears some similarity to the boundary model that was employed in the previous example for localizing the midbrain in TCS.
For each of the two shape models, the vertebra and the spine, a weighted combination of the T_{1}weighted and the T_{2}weighted image was computed as appearance input (Figure 3 shows computation of the vertebra potential function). Weights for each of the two models were determined a priori and produced a clearly recognizable local minimum for vertebra and spine appearance, respectively.
We used a single heterogeneous model, since the subshapes formed a common unit (the spine model) for which, e.g., vibration modes are computed and selected. The restriction that subshapes cannot rotate independently around a single connection was not critical. It was even a desired attribute since it very well reflected anatomical relations between subshapes. Young's modulus was 1.0, Poisson ratio was 0.0 and material density was set to 0.1 for all models.
Model generation from the sample shape was by Delauney triangulation from evenly distributed sample nodes. It produces a set of "wellshaped" tetrahedrons. Computing the rotation using node warping was solved by minimizing equation 9. Total computation time until convergence on a standard quadcore CPU was between 1.1 and 2.6 seconds per case with an average computation time of 1.5 seconds.
We evaluated the method on 49 data sets from SHIP. Detection was declared successful if the center of each vertebra subshape was in the corresponding vertebra in the image data. Examples of results can be seen in Figure 13. Vertebrae were detected correctly in all but one case. In further 3 cases, minor misorientations happened. E = 1 provided an almost stationary behavior with respect to detection for parameter changes of more than 10% for the other parameters. Further details on results can be taken from [38].
Since one of the analysis goals is to investigate whether variants exist in a normal population, we also clustered shape information of the spinal canal [48]. We currently also investigate clustering on the entire model using the weight vectors of the fitted model instances for analysis of the shape of the spinal cord. This is future work, of course, since detection is not yet followed by segmentation. However, first results are promising, since clustering weight vectors into five clusters using kmeans clustering revealed four shape variants that seem to be anatomically meaningful (see Figure 14). Cluster variance, however, is relatively high compared to intercluster distances (see Table 1)
Conclusion
We presented a partbased deformable model that can be used for directly and efficiently representing domain knowledge necessary for detection of objects in medical images. Different examples demonstrate its application to contextbased detection, modelbased segmentation, and to shape analysis.
Establishing and applying such model requires readily available methods for generating a triangulated shape and appearance models from a segmentation as well as methods for local and global optimization. Domain knowledge of our partbased deformable model resides almost completely in the model and not in the sequence of processes to fit the model to the data. The model does not require training, since the few parameters (stiffness, decomposition into parts, node potentials, pose parameters) can be set a priori and adapted intuitively. However, experience about setting up the model will speed up the design process. A number of decisions have to be made:

Structural decomposition of the model depends on partrelationships that can be derived from knowledge about the anatomy or arrangement objects to be detected. In medical applications, parts are typically anatomic substructures or a group of neighboring landmark structures that are necessary to determine an object's position.

Elasticity parameters describe the variability between shape instances and  on the structural level  variability of spatial relations between subshapes.

External forces are set depending on the expected appearance of the object in the image. While gradientbased potential forces often allow for exact determination of the object boundary, they may be supplemented by intensity or texturebased forces if gradient information is unreliable.
In future we will investigate the potential for parameter training of the model. Training of the few parameters in the data and the model terms should be much simpler requiring less training data than training of a PDM. An alternative to adapt parameters would be to take the detection result as an initialization for the search of an optimal potential field given the converged model instance instead of trying to improve the overall performance of the model. This may also enhance the potential of the model to guide datadriven segmentation schemes such as level set segmentation or graph cuts. It will also be worthwhile to take a second look at the analysis of shape parameters for the detection of shape classes using adapted model parameters.
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Acknowledgements
We thank the Leibniz Institute for Neurobiology Magdeburg, Ludwig Niehaus, formely of the Clinic for Neurology of the University Hospital Magdeburg, and the Study of Health in Pomerania (SHIP) for providing the image data used in the experiments.
Declarations
Funding for this article came from the DFG priority program 1335: Scalable Visual Analytics (grant TO 166/132).
This article has been published as part of BioMedical Engineering OnLine Volume 13 Supplement 1, 2014: Selected articles from the 35th Annual International Conference of the IEEE Engineering in Medicine and Biology Society: Workshop on Current Challenging Image Analysis and Information Processing in Life Sciences. The full contents of the supplement are available online at http://www.biomedicalengineeringonline.com/supplements/13/S1
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KDT supervised the work of MR and KE and conceived of the paper, MR developed and investigated the 3D integrated FEM, KE developed and investigated the hierarchical FEM, all authors contributed to the draft of the manuscript, all authors read and approved the final manuscript.
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Toennies, K., Rak, M. & Engel, K. Deformable part models for object detection in medical images. BioMed Eng OnLine 13 (Suppl 1), S1 (2014). https://doi.org/10.1186/1475925X13S1S1
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DOI: https://doi.org/10.1186/1475925X13S1S1