Elton Tadeu Montrazi1, Ricardo Martinho1, Qingjia Bao2, Keren Sasson1, Lilach Agemy1, Avigdor Scherz1, and Lucio Frydman1
1Weizmann Institute of Science, Rehovot, Israel, 2Chinese Academy of Sciences, Wuhan, China
Synopsis
Deuterium metabolic
imaging (DMI) is a promising approach to study tumor metabolism. Still, DMI’s
signal-to-noise ratio (SNR) is limited because of 2H’s low Larmor
frequency, coupled to the low concentrations of DMI’s targets. We recently proposed
a multi-echo balanced steady-state free precession (ME-bSSFP) method increasing
DMI’s SNR, but still find it lacking in some aspects. This work assesses simple
apodization, Compressed Sensing Multiplicative (CoSeM) and Block-matching/3D
filtering (BM3D) denoising methods for improving DMI’s results. The ability of the
latter denoising methods to enhance sensitivity without blurring resolution, is
evidenced by pancreatic cancer studies carried at 15.2T.
Introduction
DMI is a promising tool
for tumor prognosis and diagnosis, based on the injection of deuterated precursors.1,2
[6,6’-2H2]-glucose for instance is uptaken by tumors, leading
to tge formation of [3,3’-2H2]-lactate.3,4 [2H]-water
(HDO) is also formed as per other pathways. Chemical shift imaging (CSI) can be
used to spectrally-resolve these species, thereby assessing their uptake and kinetics.
CSI’s SNR, however, is limited by 2H’s low gyromagnetic ratio –
ca. 6.5 times that of 1Hs. Short T1s partly compensate
for this; yet low concentrations compound back the problem. We have recently
demonstrated that ME-bSSFP increases DMI’s SNR ca. 3x over CSI.4 Important
metabolic aspects such as glucose’s rim uptake effects and lactate in small
tumors/metastases, however, are still in the limit of what ME-bSSFP can detect.
Further improvements in image quality could arise from denoising methods5
The present work assesses a widely-used denoising method, BM3D6; in
addition, we explore CoSeM, a method developed by us which removes
instability-related multiplicative noise.7 The outcomes of these
methods are also evaluated against simple apodization. Methods
All experiments were
approved by the Weizmann Institute IACUC. C57 black mice were implanted with
KPC rodent pancreatic ductal adenocarcinoma (PDAC).8 For the DMI, ~4 g/kg body weight of [6,6’-2H2]-glucose
in PBS were injected via a tail-vein line, and 2H spectroscopic
images were acquired on a 15.2T Bruker scanner, using surface coils tuned to
650 MHz (1H) and 100 MHz (2H). A 2D ME-bSSFP sequence was
optimized for the analyses as follows: TR =11.48 ms, five TEs with 2.1 ms echo
spacings, 60° flip angle excitations, ~6 min signal averaging per image, 32x32
matrix sizes, field-of-view FOV = 40x40mm, ≈10 mm slices accommodating the full
tumors’ thicknesses. Accompanying 1H coronal images were collected
using TurboRARE: 10 slices, 0.8 mm slice thickness, 0.2 mm slice gaps, same
FOVs as ME-bSSFP, 512x512 encoding matrix. 1H B0 maps
were obtained by 3D double gradient echo, with same FOVs as for ME-bSSFP and 64x64x8
encoding matrices. ME-bSSFP data were reconstructed using 2D FT after zero-filling
each echo to 64x64; images arising from these separated echoes were processed
using IDEAL,4,9 to isolate images for the individual chemical shifts. The 1H-based magnetic field maps
were used as initial guesses for IDEAL’s magnetic field, in order to avoid “swaps”
otherwise observed upon processing.10 Isolated chemical shifts images were then
subject to BM3D (magnitude images) and CoSeM (complex images) algorithms –or to
apodization– for denoising. To translate the intensities into metabolic
concentrations, 2H’s natural abundance (~10 mM concentration prior
to injection in liquid-containing spaces), together with ME-bSSFP’s signal attenuations
as expected from the scanning parameters and the T1/T2 for
each species,3 were used.
For BM3D, a
pseudorandom noise kernel known (the Dirac delta; 'gw' in the script) was used,
resulting in white uncorrelated noise.6 The inputs to this algorithm were
the magnitude images, and a noise variance = 0.02. As for CoSeM: this method
quantifies and discards phase-encoded scans that may have been strongly
influenced by multiplicative noise; the fact that data are missing is then
overcome by relying on compressed sensing reconstructions, thereby attenuating/suppressing
multiplicative noise and delivering images with increased SNR. The inputs for
CoSeM were the complex images, 2000 renditions, lambda = 0.4, threshold = 0.05.
Apodization involved a 5mm FWHH Gaussian smoothing.Results & Discussion
Figure 1 shows a 1H
image acquired prior to DMI, on a PDAC-implanted mouse. Also shown are DMI
images arising ≈1 hour after [6,6’-2H2]-glucose
injection, collected using ME-bSSFP and then separated for HDO, glucose and
lactate. At this time the lactate is
maximal and, although glucose has largely washed out from the kidney, it is still
present in this organ as well as in the tumor region. Lactate is only present in
the tumor, while HDO is relatively diffuse throughout the body –even if it is visible
with major intensity in the tumor position.
Figure 2 compares the
DMI images of Figure 1, with denoised versions. All methods improve the SNR; for
a ROI containing the tumor, these SNR increases in the 2H images are
as per Table 1. Still, blurring effects brought about by the sensitivity
enhancement are also noticeable.
The changes in SNR and
resolution are more clearly highlighted in Figure 3, which plots the transverse
and longitudinal cross sections shown by colored lines in Figure 2. From these traces
one can appreciate how all denoising methods smooth out obvious noise features;
apodization, however, clearly smooths out fine image structures as well –foremost
among them details of glucose’s tumor rim uptake. No significant differences can be appreciated
between the resolutions and sensitivities of BM3D and CoSeM.Conclusion
DMI denoising methods were
tested on a KPC model of PDAC. All increased SNR, but only CoSeM and BM3D did
so without excessive smearing. Chances are that when SNR is at premium, e.g.
lactate’s detection, this blurring is not important; but it may be so if trying
to define subtler features and physiologically meaningful heterogeneities.Acknowledgements
This work was supported by the Thompson Family,
the Minerva and the Israel Cancer Research Foundations. LF heads the Clore
Institute for High-Field Magnetic Resonance Imaging and Spectroscopy, whose
support is also acknowledged.References
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