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  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Generation of a Smooth Ostium Surface for Aneurysm Surface Models</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Mathias Neugebauer</string-name>
          <email>mathias.neugebauer@ovgu.de</email>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Bernhard Preim</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Department of Simulation and Graphics, Otto-von-Guericke Universita ̈t Magdeburg</institution>
        </aff>
      </contrib-group>
      <fpage>399</fpage>
      <lpage>403</lpage>
      <abstract>
        <p>The exploration of the complex flow patterns within cerebral aneurysms is crucial for risk assessment, therapy planning and medical research. In order to support visual exploration, geometric descriptors are necessary to decompose the complex flow data. An important descriptor is the ostium, the area of inflow into the aneurysm, since other descriptors can be derived from it. We describe an interpolation-based approach to generate a smooth ostium surface that was successfully applied to seven different aneurysm surface models.</p>
      </abstract>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>Introduction</title>
      <p>
        A cerebral aneurysm is a pathological artery dilatation and forms an area with a
high risk of rupture. Insight into intravascular flow characteristics is important
for risk assessment, therapy planning and comparison of treatment options (e.g.
different stents and their placement) as well as the development of new, minimal
invasive treatment techniques. A way to retrieve this kind of data is a CFD
simulation, based on 3D reconstructions of the affected vessel. The resulting
flow data is complex and a subdivision into functional unities supports the visual
exploration. Since blood flow is mainly influenced by the surrounding vascular
geometry [
        <xref ref-type="bibr" rid="ref1">1</xref>
        ], this subdivision should be derived from geometric landmarks. An
important landmark is the ostium, the area of inflow into the aneurysm. Based
on this landmark, the aneurysm can be separated from the unaffected parts of
the parent vessel. Additional geometric descriptors (dome, central axis, axes of
minimal and maximum extent, etc.) can be calculated if the ostium is known.
They are important for quantification and characterization of the corresponding
parts of the flow field and for a general support of the visual exploration (adapted
visualization, viewpoint selection, meaningfully restricted degrees of freedom
during navigation, etc.).
      </p>
      <p>
        In [
        <xref ref-type="bibr" rid="ref2">2</xref>
        ] the angle between the parent vessel bifurcation and the aneurysm neck
plane was quantified. However, they did not explicitly reconstruct the ostium.
Karmonik et al. [
        <xref ref-type="bibr" rid="ref3">3</xref>
        ] applied an image-based approach by fitting circles to the cross
section of the parent vessel. This approach is error-prone, if the vessel strongly
deviates from a tubular shape, which is often the case close to the aneurysm.
To avoid this problem, our approach to generate a surface representation of the
ostium is based on landmarks that were derived from the aneurysm surface,
rather than from within the parent vessel.
      </p>
    </sec>
    <sec id="sec-2">
      <title>Methods</title>
      <p>The generation of the ostium surface is a two step approach: Shape features
are generated which subsequently form the input for a smooth sampling of the
ostium surface by means of interpolation. Some of the shape features are created
during the pre-processing whereas others are explicitly computed to meet the
requirements of the final ostium surface shape.
2.1</p>
      <sec id="sec-2-1">
        <title>Input Data</title>
        <p>
          Anatomically the ostium describes the area of inflow into the aneurysm. In
most of the cases, flow data is calculated on a CFD-compliant volume-mesh.
We derive the ostium surface from this mesh as well. A detailed description of
the segmentation process, that is necessary to derive a volume mesh from the
image data, is beyond the scope of this work. We refer to [
          <xref ref-type="bibr" rid="ref4">4</xref>
          ] who segment
cerebral aneurysms from phase contrast magnetic resonance angiography (PCMRA)
data utilizing multi range filters and local variances and to [
          <xref ref-type="bibr" rid="ref5">5</xref>
          ] who apply
geometric deformable models to computed tomography angiography (CTA) and 3D
rotational angiography (3DRA) data.
        </p>
        <p>
          Besides the surface of the volume mesh we need two more inputs: the parent
vessel centerline and a contour that describes the location of the ostium with
respect to the surface (Fig. 1a). The parent vessel centerline is also derived from
the surface of the volume mesh, utilizing its Voronoi diagram. A robust
implementation is given as part of the Vascular Modeling Toolkit (VMTK) [
          <xref ref-type="bibr" rid="ref2">2</xref>
          ]. The
ostium contour (CO) is constructed geometrically as a result of an iterative
process that utilizes the parent vessel centerline and the surface as input. Starting
from an estimated dome point of the aneurysm four control points are shifted
towards the parent vessel. Model assumptions (the ostium is bent around the
parent vessel, it is always oriented towards the aneurysm [
          <xref ref-type="bibr" rid="ref6">6</xref>
          ]) need to be satisfied
during this process. Finally, two of the control points (P1, P2) are placed on the
parent vessel, at the transition zone between parent vessel an aneurysm. The
remaining control points (P3, P4) lie in between them and describe the bending.
The smooth ostium contour is formed by a closed spline going through all control
points (P1 - P4). In [
          <xref ref-type="bibr" rid="ref6">6</xref>
          ] this process is described in detail.
2.2
        </p>
      </sec>
      <sec id="sec-2-2">
        <title>Shape Features for the Ostium Surface</title>
        <p>The ostium contour CO and a part of the parent vessel centerline that is projected
into the ostium area are the shape features of the ostium surface. These features
enable us to generate a closed surface in between. The outer border of the
surface is already given by the ostium contour CO through P1 - P4 (Fig. 1a). The
projection of the centerline, going through P1 and P2, ensures that the ostium
surface adjusts to the location and the bending of the underlying parent-vessel
(Fig. 2a).
Centerline Correction Beneath the ostium the centerline tends to bulge into
the aneurysm (Fig. 2a), since the surface in this area deviates from the tubular
shape given in the parent vessel. This part of the parent vessel centerline needs
to be corrected. First we identify the last reliable parts of the centerline within
the parent vessel, before and after the aneurysm. Each of these parts is defined
by two points (a1, a2) on the centerline that have minimal distances to P1 and
P2 (b1, b2) respectively. These four points are used as control points for a cubic
Lagrange polynomial that will replace the unreliable part of the centerline. The
parameterization t for each point is t(a1) = 0:0, t(a2) = !, t(a3) = 1:0 − !,
t(a4) = 1:0 where ! is defined by</p>
        <p>The Lagrange approximation algorithm is used to sample the polynomial and
the original centerline points are replaced with the samples.</p>
        <p>Centerline Projection The corrected centerline is projected into to ostium
area by interpolating between the vectors −→v1 = P−−1→a2 and −→v2 = P−−2→b1 (Fig. 2a).
For each point pi of the n centerline points between a2 and b1 the projected
point p′i is defined by
p′i = pi +
(
1 − n
i )
→−v1 +
( i )
n
−→v2</p>
        <p>The projected centerline (CP ) starts from P1, resembles the shape of the
underlying parent-vessel centerline and ends at P2.
2.3</p>
      </sec>
      <sec id="sec-2-3">
        <title>Surface Generation</title>
        <p>The projected centerline CP divides the ostium surface, we want to generate, into
two parts. Without loss of generality we describe the surface generation process
(a) Input data
(b) Surface 1
(c) Surface 2
(2)
for only one of these parts, since it is a local approach that can be applied to
both parts separately.</p>
        <p>We subdivide the segment of ostium contour CO that is contained in the
chosen part into two segments Ca and Cb of equal geodesic length. The two
segments share the division point pd and are uniformly sampled with the same
number of samples k. The surface is generated by linear interpolation from Ca
to Cb. For this, we need a suitable interpolation path. This path is given by
linear segments L1 − Lj that are defined between the j points of the projected
centerline CP and pd. Each segment Li is sampled uniformly and has the same
number of samples k as the contour segments. For the first linear segment L1,
a set of vectors Va is defined by V−→ai = L−−1−iC−→ai, where L1i is the sample on L1
and Cai is the corresponding sample on Ca. The same is done for the last linear
segment Lj and Cb with the vector set Vb as result (Fig. 2b).</p>
        <p>We now have a set of vectors Va that is related to Ca and a set Vb that is
related to Ca respectively. The j linear segments with k samples each define
the sampling of our surface. For each sample point Lmn, with 0 ≤ m &lt; j and
0 ≤ n &lt; k, we define a displacement that includes the linear interpolation from
Va to Vb</p>
        <p>L′mn = Lmn +
(</p>
        <p>m ) V−−→an + ( m ) V−→bn
1 − j j
(3)
The regular j ×k structure of the sample point allows us to use simple, vertex
Idbased construction rules to define the topology based on the displaced sampling
points. The result is a mesh that smoothly interpolates the geometric constraints
given by CO (represented by Ca,Cb) and CP (represented by L1 − Lj ) (Fig. 1b).
(a) Centerline projection
(b) Interpolation scheme</p>
      </sec>
    </sec>
    <sec id="sec-3">
      <title>Results and Discussion</title>
      <p>
        We used MeVisLab 2.1 as prototyping environment, since it wraps the
Visualization Toolkit (VTK) whose mesh processing and visualization capabilities
form the basis of our implementation. As input data seven different polygonal
models were derived from different imaging devices (CTA/MRA) during
clinical standard procedures. The centerlines of the parent vessels were calculated
using VMTK and used as input for the generation of the ostium contours [
        <xref ref-type="bibr" rid="ref6">6</xref>
        ].
The ostium surface could be generated successfully for all ostium contours. On
a mid-class laptop the computation time for a high-resolution ostium surface
(4096 sample points) on different datasets was in between 0:8 and 1:1 sec with
a non-optimized, straightforward implementation. Besides a small overhead for
preprocessing (projection of the centerline, subdividing the contour into Ca, Cb)
the computation time depends linearly on the surface resolution.
      </p>
      <p>The resulting ostium surfaces are smooth and bend natural according to
the underlying parent vessel and the aneurysm-vessel transition area (Fig. 1b,c).
Medical experts found them to be plausible and correctly related to the particular
morphologic situation. Using this ostium surface, the next step is to generate an
aneurysm-specific coordinate system that includes the semantic decomposition
of the aneurysm (ostium, neck, dome) and special geometric landmarks and
axes. This coordinate system will form the basis for adaptable visualizations
and support the visual exploration process.</p>
      <p>Acknowledgement. This work has been funded by the federal state of
SaxonyAnhalt in the scope of the MOBESTAN project (5161AD/0308M).</p>
    </sec>
  </body>
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