Hanna Frantz1 and Volker Rasche1
1Department of Internal Medicine II, Ulm University Medical Center, Ulm, Germany
Synopsis
Keywords: Data Acquisition, New Trajectories & Spatial Encoding Methods
Motivation: Major limitation of lung MRI is respiratory motion which can be overcome by retrospective self-gating approaches.
Goal(s): Achieving sufficient SNR values in the parenchyma is crucial for clinical evaluations and the assessment of physiological parameters.
Approach: This abstract presents a single-petal rosette UTE trajectory that is evaluated for k-space-, as well as image-based, retrospective self-gated lung imaging in comparison to the radial UTE trajectory.
Results: Higher SNR values and sharpness are obtained when using the SPR trajectory, compared to radial UTE sampling approaches at constant temporal resolution.
Impact: This
abstract presents a single-petal rosette UTE trajectory (SPR) for 2D self-gated
lung imaging, yielding higher SNR and sharpness in comparison to radial UTE
sampling approaches.
Purpose
Ultrashort T2* relaxation times, found e.g. in lung
tissue1 require MR imaging approaches with short echo times (TE). Ultrashort
echo time (UTE) sequences enable data acquisition with minimization of TE by acquisition
of the data during ramping of the read-out gradient as opposed to only sampling
when the gradient plateau is reached.
To eliminate respiratory motion, retrospective gating
techniques are frequently applied to lung imaging, overcoming the highly limited
maximum scan duration for a breath-hold acquisition of a few seconds.
In this contribution, we applied a single petal rosette
trajectory (SPR), which more efficiently covers k-space by additional data
sampling during the required rephrasing of a UTE acquisition. The performance
of the suggested trajectory and variants thereof for self-gated free-breathing
acquisitions is investigated in volunteers and compared to radial UTE imaging.Methods
The suggested approach was tested in 5 healthy volunteers with no reported
respiratory disorders, who provided informed written consent prior to the MR
examination. Images were acquired during a single breath-hold, each for
inspiration and expiration, as well as during a free breathing scan of
2-3 minutes at a 3 T whole-body clinical imaging system (Ingenia
3.0T CX, Philips Healthcare, Best, The Netherlands) using a 32 (16 anterior, 16 posterior) torso coil (dStream Torso, Philips
Healthcare). All data were acquired in coronal slice orientation centred
at the bifurcation of the trachea.
The SPR trajectory2 is parametrized by
$$k(t) = k_{\text{max}}
\sin(\omega t) \text{e}^{it} ,$$
with k being
the position in k-space, kmax the outmost position of sampling
k-space and $$$\omega$$$ the angular frequency, which was chosen as 5/3. The radial
UTE acquisition followed the radial UTE center-out sampling pattern3.
In both approaches, an angular increment following the tiny golden angle
sampling scheme ($$$\varphi_7$$$ = 23.6281°)4 was used. The number of
readouts for both approaches was determined to Nyquist sample k-space for the radial
UTE sequence. All relevant scan parameters are listed in table 1.
For image reconstruction, an in-house
built reconstruction framework, implemented in MATLAB (The MathWorks, Natick, Massachusetts, USA) was used.
The k-space density functions for the SPR trajectory were calculated using a
Voronoi tessellation5.
The gating was performed using a k0-based
self-gating approach (SGksp) (SG signal derived from temporal
evolution of DC-signal, subsequently bandpass filtered and combined with
principal component analysis to get the respiratory navigator signal), as well
as two image-based approaches (SGimg) (navigator signal derived from
high-temporal resolution images by gradient analysis of the lung-liver
interface (LLI), respiratory stages were determined by a histogram-based
approach (SGimg,hist), as well as an absolute value-based approach
(SGimg,abs)). The self-gating reconstructions are described in
further detail in Metze et al.6 A temporal resolution of 100 ms was
chosen for all self-gated reconstructions.
The parenchyma was segmented semi-automatically and
SNR was calculated according to
$$\text{SNR} = \sqrt{2-\frac{\pi}{2} } \frac{\text{SI}_{\text{ROI}}}{\omega_{\text{BG}}},$$
with SIROI being the signal intensity of a
region of interest (ROI) and $$$\omega_{\text{BG}}$$$ the standard deviation of
background noise. Additionally, image sharpness was assessed by a standard
metric7, identifying the positions of pixels corresponding to 25 and
75% of the maximum signal intensity of an intensity profile, chosen across the LLI.Results
Data acquisition could be completed for all
volunteers.
SNR improved by 20% for breath-hold acquisitions when
comparing SPR and radial UTE images. For the self-gated reconstructions, the
SNR in the lung parenchyma increased between 33% and 41% as can be appreciated
in figure 2.
Figure 3 shows the line profile placed over the LLI
for breath-hold and self-gated images of one volunteer for both radial UTE and
SPR trajectory, for inspiration and expiration, respectively.
While sharpness
for images reconstructed using SGksp only differs by less than 20%,
the image based self-gating approaches increase sharpness by up to 270% for the
expiratory phase, as can be seen in figure 4.Discussion and Conclusion
The SPR trajectories cover more k-space data without
increasing repetition time or total scan duration, since each petal ends in k0,
thus removing the necessity of a rephasing gradient applied prior to spoiling.
The resulting oversampling of k-space yields improved SNR compared to radial UTE
sampling.
The higher sampling density of k-space per interleave
decreases aliasing artifacts in the high-temporal resolution images, thus
increasing performance of especially image-based self-gating approaches, which
can be appreciated in the sharpness analysis.
Considering the previously outlined compatibility of
the SPR trajectory with image-based self-gating approaches, suitability of the
SPR trajectory with the nuSG algorithm7 suggests itself to be
further evaluated. Additionally, an implementation for 3D imaging within the
framework of stack-of-stars might be worth pursuing.Acknowledgements
The authors
thank the Ulm University Center for Translational Imaging MoMAN for its support.
This work was supported by the German Research Foundation funding agreement
465599659. Technical support from Philips Healthcare is gratefully
acknowledged.
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