Skip to main content
  • Original article
  • Open access
  • Published:

Assessment of a novel 32-channel phased array for cardiovascular hybrid PET/MRI imaging: MRI performance



Cardiovascular imaging using hybrid positron emission tomography (PET) and magnetic resonance imaging (MRI) requires a radio frequency phased array resonator capable of high acceleration factors in order to achieve the shortest breath-holds while maintaining optimal MRI signal-to-noise ratio (SNR) and minimum PET photon attenuation. To our knowledge, the only two arrays used today for hybrid PET/MRI cardiovascular imaging are either incapable of achieving high acceleration or affect the PET photon count greatly.


This study is focused on the evaluation of the MRI performance of a novel third-party prototype 32-channel phased array designed for simultaneous PET/MRI cardiovascular imaging. The study compares the quality parameters of MRI parallel imaging, such as g-factor, noise correlation coefficients, and SNR, to the conventional arrays (mMR 12-channel and MRI-only 32-channel) currently used with hybrid PET/MRI systems. The quality parameters of parallel imaging were estimated for multiple acceleration factors on a phantom and three healthy volunteers. Using a Germanium-68 (Ge-68) phantom, preliminary measurements of PET photon attenuation caused by the novel array were briefly compared to the photon counts produced from no-array measurements.


The global mean of the g-factor and SNRg produced by the novel 32-channel PET/MRI array were better than those produced by the MRI-only 32-channel array by 5% or more. The novel array has resulted in MRI SNR improvements of > 30% at all acceleration factors, in comparison to the mMR12-channel array. Preliminary evaluation of PET transparency showed less than 5% photon attenuation caused by both anterior and posterior parts of the novel array.


The MRI performance of the novel PET/MRI 32-channel array qualifies it to be a viable alternative to the conventional arrays for cardiovascular hybrid PET/MRI. A detailed evaluation of the novel array’s PET performance remains to be conducted, but cursory assessment promises significantly reduced attenuation.


Hybrid imaging systems combining positron emission tomography (PET) and magnetic resonance imaging (MRI), namely PET/MRI scanners, are unique in providing both functional and intrinsically registered anatomical information from both PET and MRI simultaneously. PET/MRI systems are therefore highly advantageous for multimodality studies, which can improve the characterization and grading of metabolically active tumors using18F-fluoro-deoxy-glucose (FDG) (Catana et al. 2012; Camici et al. 2008), while superimposing such activity on anatomical images with the superior soft-tissue contrast of MRI to identify active inflammation (White et al. 2013). In addition, by combining perfusion tracers such as 13N-labeled-Ammonia (13NH3) with FDG, the PET/MRI has also been shown to be successful in cardiovascular imaging where left/right ventricular function and myocardial perfusion and blood flow in surrounding vessels of the heart can be quantified (Camici et al. 2008; Nensa et al. 2018; Nensa et al. 2014).

Since the emergence of whole-body PET/MRI systems, several technical challenges have been identified and commonly reported around the accurate quantification of the 511 keV annihilation photons detected in PET images (Pichler et al. 2008a; Pichler et al. 2008b; Rausch et al. 2017; Wagenknecht et al. 2013). The greatest challenge, apart from respiratory and cardiac motion, is the accurate correction of PET counts due to attenuation within materials located between the radioactive source and the PET detectors. Attenuation of 511 keV photons is caused by the presence of the patient body (tissues, air cavities, blood, and bones) and the scanner hardware in the PET field-of-view (FOV). Hardware, such as the patient bed, audio communication system, and radio frequency (RF) resonators, have the most attenuating effect and cause scattering or simply block the gamma rays from reaching the PET detectors (Kartmann et al. 2013; MacDonald et al. 2011; Tellmann et al. 2011). However, RF phased arrays are crucial for MRI parallel imaging as they achieve the shortest scan time with the highest spatial and temporal resolutions, and their use, particularly for cardiovascular MRI, is an essential part of the standard of care. The advantage of parallel imaging with high acceleration factor up to 4 in one-dimension for cardiac MRI was proven to be beneficial for imaging (Wintersperger et al. 2006). Therefore, a phased array with 32-channels is highly desired. Although a few dedicated PET/MRI RF phased arrays have been developed for brain (Anazodo et al. 2016 ; Sander et al. 2014) and breast (Dregely et al. 2014) imaging, no phased array, to our knowledge, has been developed for PET/MRI cardiovascular imaging. Currently, MRI-only research systems offer phased arrays with up to 128-channels for cardiovascular imaging (Schmitt et al. 2008), while clinical PET/MRI systems offer up to 12-channels. Although commercially available, PET/MRI arrays are typically restricted to a lower number of channels to reduce attenuation of gamma rays. Nevertheless, PET/MRI arrays have been reported to cause variation of the standardized uptake value (SUV) ranging from 18 to 60% closer to the array, if the attenuation correction (AC) is not included during the PET image reconstruction (Fürst et al. 2012; Ouyang et al. 2014; Paulus et al. 2012).

Meanwhile, developing a dedicated PET/MRI phased array with a higher number of channels is technically challenging, leading researchers to focus on the approach of correcting the attenuation of the currently available MRI arrays (Eldib et al. 2015; Ferguson et al. 2014; Frohwein et al. 2018; Kartmann et al. 2013). The common approach to correct for attenuation of an RF phased array is to generate a hardware AC map, also known as a μ-map, produced from a CT scan at a specific tube voltage (Carney et al. 2006; Patrick et al. 2017). The process of generating a hardware-AC map is normally conducted by the scanner manufacturers for all vendor-provided hardware, prior to delivery of the scanner. AC maps are accurately included during PET image reconstruction for fixed rigid hardware, such as the patient table and rigid RF arrays. For more accurate AC of flexible RF arrays, fiducial markers can be added to guide the registration of the hardware AC map with the PET image (Kartmann et al. 2013).

Although, RF arrays with a lower number of channels are adequate for most oncologic applications, simultaneous PET/MRI for cardiovascular imaging can still benefit from faster parallel imaging using a dedicated PET/MRI RF 32-channel phased array prospectively designed for minimal PET attenuation. It is, therefore, important to investigate alternative approaches to minimize the attenuation caused by a high-density phased array for cardiovascular PET/MRI imaging. In this work, we evaluate a third-party dedicated 32-channel phased array optimized for parallel imaging of the heart with PET/MRI. The quality parameters for parallel imaging, such as the geometry factor (g-factor), SNR, and noise correlation coefficients, are compared to the two commercially available and currently used, MRI-only 32-channel and the PET/MRI 12-channel arrays.

The reduction in PET signal due to attenuation caused by the candidate array was briefly examined and reported. Although this work focusses on the MRI performance of the array, the equally important PET performance of the candidate array will be compared in detail to the existing arrays and will be reported in a separate manuscript. Only a cursory evaluation of PET performance will be reported herein. We hypothesize that if the MRI quality parameters of the PET/MRI 32-channel array are similar with those produced by MRI-only 32-channel array, and if global gamma ray attenuation of the PET/MRI 32-channel array is less than that of the mMR 12-channel array, the MRI performance of the PET/MRI 32-channel array would be acceptable for hybrid/simultaneous PET/MRI cardiovascular imaging.

Materials and methods

Description of the arrays

The PET/MRI phased array consists of two parts; a posterior and an anterior, allowing the patient to be scanned in head-first, supine position. The RF elements were arranged to cover the entire heart region and can be connected to the scanner at four ports. The ports are arranged, with two ports for the anterior array, and two ports for the posterior array, allowing each part of the array to be used independently. The anterior and posterior part of the 32-channel arrays has 16 elements each, arranged in a 4 × 4 fashion to maximize acceleration factor in directions within the coronal plane. The flexible body mMR 6-channel array (Siemens Healthcare Limited, Erlangen, Germany) elements are arranged in 3 × 2 fashion, which is similar in arrangement to the spine matrix array (Siemens Healthcare Limited, Erlangen, Germany). Therefore, the flexible body mMR 6-channel array was combined with six elements from the posterior spine matrix mMR array formulating a set of mMR 12-channel array used in this work.

In this study, a commercially available cardiac MRI-only 32-channel array (In-Vivo Corporation, Gainesville, FL, USA) was used, while the prototype novel PET/MRI 32-channel (developed in 2016) was provided for assessment by a local company (Ceresensa. Inc., Canada).

MRI phantom imaging

For this study, a balanced steady-state free precession (balanced-SSFP or TrueFISP in vendor’s nomenclature) pulse technique was selected due to its ability to acquire sub-second scan time per slice and its sensitivity to high fluid-tissue contrast (Haacke et al. 1990). All MRI acquisitions were performed on a 3.0T PET/MRI system (Biograph mMR Software Version VE11P, Siemens Healthineers, Erlangen, Germany).

All three arrays operated with posterior and anterior parts, making the condition of the measurements identical as seen in Fig. 1. Phantom imaging data were acquired using a standard cylindrical acrylic container (OD = 28 cm) filled with a solution of both NiSO4·6(H2O) and NaCl in distilled water. To mimic the location of the heart in a patient, the distance between the anterior and posterior array elements were kept to approximately 27 cm and the 12 cm high cylindrical phantom was centered between them, leaving the elements approximately 7.5 cm away from the surface of the phantom. To examine the parallel imaging capabilities of each array, a single 2D-slice at the center of the phantom in the coronal plane was acquired using the manufacturer’s 2D TrueFISP sequence. Multiple acquisitions were performed with phase encoding in left-right (LR) direction, for different acceleration factors ranging from R = 1 to R = 6. A second set of acquisitions similar to the above was performed, changing the phase encoding into the foot-head (FH) direction, for the same number of acceleration factors. The image reconstruction utilized the generalized autocalibration partially parallel acquisitions (GRAPPA) technique (Griswold et al. 2002), with 64 reference lines for all accelerations. The 2D TrueFISP-GRAPPA parameters for the LR and FH encoding were BW = 440 Hz/pixel, FOV = 253 × 253 mm, spatial resolution of 1.3 × 1.3 × 8.0 mm3, flip angle = 50°, and TE/TR = 2.40/4.79 ms. For each acceleration factor R, noise data was also acquired with the same parameters except the RF amplitude was set to zero. The above two sets of coronal acquisitions were repeated two times on the phantom for each array, with a total of 64 acquisitions for each array.

Fig. 1
figure 1

Phantom experiment setup for the three arrays PET/MRI 32-channel, MRI-only 32-channel, and mMR 12-channel. Position of isocenter were kept unchanged from one acquisition to the other

A reflected power test was performed to ensure that there is no undue change to the RF field transmitted by the integrated body resonator due to poor decoupling from the receiver array (Schmitt et al. 2008). A low percent difference in reference voltage between the “with-array” and “no-array” conditions indicates that no undue amount of transmitted energy is absorbed within the receiver array. The reference voltage was determined by the scanner’s automated RF calibration procedure and represents the voltage necessary to obtain a 180° flip angle using a 1 ms square RF pulse. This test was performed only on the PET/MRI 32-channel array, since it is not licensed or approved by a third-body regulator.

In-vivo imaging

For in-vivo imaging, acquisitions were performed on three healthy volunteers, recruited with written informed consent according to a research ethics protocol approved by the Research Ethics Board (protocol ID 6319). In addition to the same pulse sequences that were performed in the phantom acquisitions, ECG-triggered 2D TrueFISP cine images were acquired on a single breath-hold with axial double-oblique orientation and a four-chamber view of the heart. The imaging parameters of the cine MRI with activated GRAPPA for R = 2 (anterior-posterior phase encoding) were TE/TR = 1.58/36.3 ms, 25 segments, spatial resolution of 1.0 × 1.4 × 6.0 mm3, FOV = 253 × 300 mm, flip angle = 50°, and BW = 930 ± 16 Hz/pixel. For the three volunteers, the average beat-to-beat interval was 906 ± 50 ms. Each volunteer was fitted with MRI-compatible ECG electrodes, so that the data is retrospectively ECG-gated. Volunteers were imaged in the head-first supine position, with a total acquisition time of under 10 s in 13 heart beats. Each volunteer was imaged consecutively with all three arrays under the same conditions and using the same imaging parameters as described above. The full duration of an imaging session for one volunteer with the three arrays was under 60 min.

Data processing and analysis

For phased arrays, SNR is more likely to be overestimated if measured from the magnitude of the image, due to bias of the Rician-distributed noise in the image magnitude (Henkelman 1985; Pruessmann et al. 1999). The noise measured by a phased array is influenced by the overlapping of each element and cannot be treated as a single source of noise, i.e., a fraction of the noise observed by each element is correlated noise and must be accounted for via noise correlation coefficient to avoid overestimation. Notably, the mMR 12-channel array utilizes OEM-specified combiner chip, while both MRI-only and PET/MRI arrays do not. Therefore, using raw data (k-space) for signal and noise was necessary to perform appropriate and fair comparison and identical reconstruction. Two techniques were introduced (Pruessmann et al. 1999; Robson et al. 2008), by which SNR of phased arrays can be estimated in a pixel-by-pixel fashion. Both techniques have addressed the geometric overlapping of array elements (known as g-factor). In this work, the g-factor was computed from both the estimated noise covariance, which was computed from noise correlation coefficients of the array elements in Appendix A (Pruessmann et al. 1999), and sensitivity map (spatial element sensitivity) which was estimated off-line. The formulas used to compute sensitivity, g-factor, and SNR parameters are described by Eqs. (1), (2), and (3) in Pruessmann et al. (1999) and presented here for convenience.

$$ {S}_{pj}={S}_j\ast {r}_{\mathrm{p}} $$
$$ {\mathrm{g}}_p=\sqrt{{\left({\left({S}^H{\Psi}^{-1}\mathrm{S}\right)}^{-1}\right)}_{p,p}\ {\left({S}^H{\Psi}^{-1}S\right)}_{p,p}} $$

Where S is the complex sensitivity matrix, Ψ the noise correlation coefficient, r is the aliased p pixel position, and j is the array element number. The g-factor-based SNRg was estimated on a pixel-by-pixel fashion for multiple acceleration factors R = 2 to R = 6 from the fully sampled image SNR0, which was found by the difference method (Price et al. 1990).

$$ {\mathrm{SNR}}_{\mathrm{g}}=\frac{{\mathrm{SNR}}_0}{{\mathrm{g}}_p\sqrt{R}\ } $$

For the two phantom experiments, global mean, from masked images, and standard deviation (SD) of the SNR0, SNRg, and g-factor were calculated at each R value independently for both one-dimension (phase encoding LR or FH) and two-dimensions (phase encoding is in both LR and FH). The relationship between mean SNRg and inverse g-factor as functions of R were examined and compared for the three arrays. Mean and SD of the noise correlation coefficients were estimated excluding the self-correlated coefficients (diagonal values of the matrix). The percentage difference of the quality parameters for the MRI-only and PET/MRI 32-channel arrays were estimated using Eq. (4), where v1 is the PET/MRI array parameter value and v2 is the MRI-only array parameter value. For the interpretation of the percentage difference, a criterion was established in which the absolute function in the formula was ignored allowing directional estimates. Instead, the measured parameters for the MRI-only array were subtracted from those of the PET/MRI array. Hence, a negative percentage difference would indicate a better performance of the PET/MRI array for the g-factor parameter. All quality parameters of the parallel imaging and data analysis for each array were computed using Matlab 9.3.0 (The MathWorks, Natick, MA, USA).

$$ \%\mathrm{difference}=\frac{v_1-{v}_2}{\ 0.5\ \left({v}_1+{v}_2\right)}\ 100\% $$

PET activity test

To estimate PET photon attenuation, two-point Dixon acquisitions were performed prior to the PET acquisition, with and without the array, on the mMR Ge-68 daily quality control (QC) phantom (Siemens, Healthineers, Erlangen, Germany). The Dixon acquisition consisted of a 3D dual-echo spoiled gradient sequence with the following parameters: TE/TR = 1.23/3.96 ms, slice thickness = 3.1 mm, flip angle = 9°, and FOV = 312 × 500 mm. The phantom was mounted following the procedure used in the daily QC, where neither the patient table nor array were present in the bore of the PET/MRI system during the Dixon acquisition. An 8-min PET acquisition was carried out immediately after the Dixon while the array was placed around the phantom. Placing the array took no more than 2 min; therefore, only the last 6 min of the data were used for PET image reconstruction. The resultant data was labeled as “no-array, no-table” and was used as a base line to compare to PET/MRI array. The same acquisitions were repeated on the phantom but with the array’s anterior part placed on the top of the QC phantom, while the array’s posterior part was placed below the QC phantom. Mean of PET counts per seconds (CPS) from the acquisitions, without applying AC maps, were estimated from the central transaxial slice of the phantom for each PET acquisition.


The voltage recorded for 180° RF pulse with the volunteer in the scanner, but without the PET/MRI 32-channel array, was 562 V. It was 598 V with the volunteer loading the array in the scanner, resulting in only 6% difference. This percentage difference of the reference voltages is indicative of the decoupling inefficiency of the array and shows that the coupling between the array and the body resonator is minimal. In this case, the PET/MRI 32-channel array shows 94% decoupling efficiency.

MRI phantom imaging

Table 1 summarizes the MRI quality parameter means and SDs, such as SNR0, SNRg sensitivity-based g-factor, and inverse g-factor as estimated for all arrays at all acceleration factors, in 1D (LR or FH) and 2D. The table also includes the mean and SD of the noise correlation coefficients for all arrays. Noise correlation coefficient matrices representing between-channel coupling for the three arrays are graphically represented in Fig. 2. Each array produced a mean noise correlation coefficient of less than 0.2 (20% correlation). For example, noise correlation means at R = 2, excluding self-correlated elements (diagonal), were 10%, 11%, and 15% for the MRI-only 32-channel, PET/MRI 32-channel, and mMR 12-channel arrays, respectively.

Table 1 Mean ± SD of parallel imaging quality parameters (noise correlation coefficients, SNR0, SNRg, and 1/g) computed for the three arrays. The table lists the parameters for different phase encoding direction in 1D (LR or FH) and in 2D (LR and FH). Note the similar or better performance of the PET-MRI 32ch array compared to the MRI-only 32-channel array
Fig. 2
figure 2

Noise correlation coefficients matrix for each of the three arrays; PET/MRI 32-channel, MRI-only 32-channel, and mMR 12-channel. The scale of the color bar represents the correlation coefficients values, which could also be reported as correlation percentage. The average noise correlation coefficients (excluding the matrix diagonal) for the PET/MRI array was measured to be < 0.13 (< 13% correlation)

Figure 3 displays means and SDs of the noise correlation coefficients for the three arrays as a function of the acceleration factor, with the mMR 12-channel array producing the largest standard deviation (2.1%) of all three arrays.

Fig. 3
figure 3

Mean and SD of the noise correlation coefficients shown as a function of acceleration factor for the three arrays. Of note: the mMR 12-channel array mean noise correlation shows a drop at R = 2, with SD of 0.021 (2.1%). The MRI-only 32-channel shows the lowest values, yet noise correlation coefficients increases by 0.019 (1.9%) from R = 1 to R = 6, while the PET/MRI 32-channel array has shown an increase by 0.012 (1.2%)

Figure 4 presents measured inverse g-factors maps for 1D acceleration (phase encoding in LR and FH direction) for all arrays. The 1/g-factor maps of the PET/MRI 32-channel array are compared to the two commercial arrays for each acceleration factor and produced the lowest mean g-factor and, hence, the lowest noise amplification of the three arrays, as recorded in Table 1. For example, at acceleration factor R = 3 in the LR direction, the mMR array produced a mean g-factor of 2.10 compared to 1.32 for the MRI-only 32-channel array and 1.25 for the PET/MRI 32-channel array. A similar pattern of g-factor was also observed when estimated with encoding in the FH direction.

Fig. 4
figure 4

1/g factor maps for the three arrays with R = 2 to R = 6 in both LR and FH phase encoding direction. Notice a substantial noise amplification beyond R = 2 for the mMR 12-channel array in comparison to the two 32-channel arrays

Using percentage difference formula number [4] with parameters in Table 1, one can compare any parameters of one array to another. Beyond acceleration factor of R = 2 in either encoding directions, the PET/MRI 32-channel array shows more than 30% improvement in g-factor and SNRg compared to the mMR array. The PET/MRI 32-channel array mean g-factor for R = 3 in the FH encoding direction was improved relative to the LR phase encoding direction by 7%, while the MRI-only 32-channel array showed no changes in mean g-factors at R = 3 according to phase encoding direction.

Figure 5 presents the 1/g-factor maps for selected 2D acceleration factors RLR × RFH = 2 × 2, 2 × 3, 2 × 4, 3 × 3, and 3 × 4. In Fig. 5 and Table 1, the 2D acceleration is shown to be possible with the PET/MRI 32-channel for up to 3 × 3 with only a SNR loss of less than half of that of the mMR 12-channel array, and 8% better than the MRI-only 32-channel array. Table 2 focuses on the percentage differences of the parallel imaging quality parameters between the two 32-channel arrays for the case of L-R encoding direction. The percentage difference between the non-accelerated (R = 1) SNR0 for both arrays was 10.3%, while the SNR0 measured from the PET/MRI array at R = 2 was better than the MRI-only array by approximately 19%. The percentage differences in the case of mean g-factor for R = 1 and R = 2 were found to be negligible, while for accelerations factors R > 2, the mean g-factor of the PET/MRI array was more than 5% over that measured from the MRI-only array, as seen in Table 2. The mean and SD of SNRg, as a function of acceleration factor for the three arrays, are displayed in Fig. 6.

Fig. 5
figure 5

1/g factor maps in the case of 2D acceleration with RR = 2 × 2 to RR = 3 × 4. The PET/MRI 32-channel array achieves the least noise amplification with max of 0.97 at RR = 3 × 3 in comparison to 0.88 for the MRI-only array, while the mMR 12-channel array produced the maximum noise amplification of 0.83

Table 2 The percent difference of parallel imaging quality parameters (left-to-right encoding direction) comparing both 32-channel arrays
Fig. 6
figure 6

Estimated SNRg as a function of acceleration factors from R = 1 to R = 6, with GRAPPA reconstruction. The estimated SNRg shown here follows the theory and is in agreement with expected profile as first proposed by (Griswold et al. 2002)

MRI in vivo imaging

The SNRg pixel-by-pixel maps from in vivo acquisitions (single centre-slice 2D TrueFISP, cine disabled), at 1D acceleration factor R = 3 and R = 4, were derived by utilizing elements sensitivity and are presented in Fig. 7. At the mid-ventricular level and up to the apex, the effect of the noise amplifications at R = 3 (and higher) are comparable for the 32-channel arrays and they outperform the mMR 12-channel array. A higher SNRg from the in vivo acquisitions (2D TrueFISP cine 4-chamber view) on a male volunteer was achieved using the PET/MRI 32-channel array (Fig. 8). The line profile of the SNRg across the center of a four-chamber view of the heart was approximately 15% higher for the PET/MRI 32-channel array over the two other conventional arrays (Fig. 9).

Fig. 7
figure 7

In vivo maps of SNRg (i.e., including noise amplification considerations) comparison of the three arrays, using a single center-slice 2D TrueFISP image acquired at R = 3 and R = 4, with left-right encoding. The SNR maps show greater degradation of the SNR for the mMR 12-channel compared to the 32ch arrays at higher acceleration factors

Fig. 8
figure 8

The first of 25 four-chamber view images acquired with a 2D TrueFISP cine sequence on a male volunteer with acceleration factor of 2 (R = 2)

Fig. 9
figure 9

A centre line (dashed line in Fig. 8) profile of the heart showing SNRg generated by the three arrays using a 2D TrueFISP cine four-chamber view. The scanning plane/orientation is not identical, and the line had to be centered in the heart as much as possible for each acquisition above. The SNRg profile of the PET/MRI array (solid line) is higher than the other arrays

PET imaging

Figure 10 compares center-slice of the PET activities acquired on the Ge-68 phantom for the three arrays and the “no-array, no-table” measurement. The estimated global mean of the PET counts per second (CPS), from the circled region contouring the phantom, were found to be 557CPS, 534CPS, 436CPS, and 395CPS, for “no-table no-array,” PET/MRI 32-channel array, MRI-only 32-channel array, and mMR 12-channel array respectively. The difference between the PET CPS from “no-table, no-array” to PET/MRI 32-channel array was 4.1%.

Fig. 10
figure 10

PET counts per second (CPS) map of the middle slice of the Ge-68 phantom for each array separately and reference (“no-array, no-table”). The global mean count per seconds was measured from the region contoured by the red circle. The figure is windowed to accentuate the hardware attenuation artifacts visible immediately outside the phantom. All images used identical windowing

Discussion and conclusion

Overall, the MRI performance assessed by the percentage differences of noise correlation, g-factor, and SNR between the two 32-channel arrays is found to be similar and favored the PET/MRI array greatly at acceleration of R = 4 and R = 6. The design of this dedicated PET/MRI array has provided superior (> 30%) in all the results over the mMR 12-channel array for acceleration factors greater than 2, theoretically allowing for use of shorter breath-holds, which is often critical in cardiac imaging.

The method used in this work to assess the MRI quality parameters for parallel imaging are commonly used by researchers as reported in Meise et al. (2010), Reeder et al. (2005), Schmitt et al. (2008), Wiggins et al. (2006), and Wintersperger et al. (2006). This work has combined the use of both parallel imaging techniques with high-density arrays to shorten the breath-hold during acquisition which is necessary for cardiovascular imaging. At R = 4 using TrueFISP imaging, the shortest breath-hold that could be achieved was approximately 9 s producing 25 images of a single slice.

Unlike the two currently used arrays, the anterior portion of the PET/MRI array is very light and thin and as such does not conform to the subject’s chest under its own weight. This was resolved by using straps to achieve adequate conformity and proximity to the subject’s body. With this design, its elements have the highest proximity to the heart of the three arrays, which benefits penetration depth and results into a better SNR far from the array as demonstrated by Fig. 9.

We recorded lower noise correlation SDs (0.5%) for both 32-channel arrays compared to the mMR 12-channel array, as seen in Fig. 3, which indicates greater stability of the arrays’ noise correlation coefficients as a function of acceleration factor during parallel imaging. One element of the PET/MRI 32-channel array produced a noise coefficient of 61%, and this may have caused the high mean of the coefficients. This could be due to off-resonance tuning of the element which introduced excess noise to the neighboring ones.

We have demonstrated with the phantom results in Figs. 4 and 5 that the 32-channel PET/MRI array produces higher SNR than the other two arrays for 1D and 2D acceleration, which confirms that the array is a strong candidate for use as the MRI receiver array in hybrid PET/MRI cardiovascular imaging. As seen in Table 1, at almost all R values, the mean g-factor of the PET/MRI 32-channel array showed better results than those of the other two arrays. The SNR behavior from phantom and in vivo measurements matches those reported in Griswold et al. (2002) regarding parallel imaging theories compared to the effect of acceleration on SNR measured with phased arrays. It was noticed that the estimated SNRg of the MRI-only 32-channel array at R = 4 is 17% less than the PET/MRI array, yet it produced the smallest noise correlation coefficient. The reason for this behavior could be due to smaller element size and geometry differences from one array to the other, or alternative reasons may be a suboptimal output gain adjustment or imperfect signal pre-amplification. The parallel imaging quality parameters of the prospectively designed PET/MRI 32-channel array are comparable to the MRI-only array confirming its ability to be employed for 1D acceleration up to R = 6, and 2D parallel imaging up to acceleration of 3 × 3.

In conclusion, the PET/MRI 32-channel array prospectively designed for simultaneous PET and MRI demonstrated competitive MRI performance compared to both the 32-channel MRI-only array and the 12-channel PET/MRI array. PET photon attenuation caused by the PET/MRI 32-channel array was measured to be < 5% compared to the no-array PET photon activities. The PET performance will be studied in detail and will be presented in a separate manuscript.

We therefore conclude that the PET/MRI 32-channel array studied here is a viable alternative for simultaneous cardiovascular PET/MRI using parallel imaging. The PET/MRI array can surpass currently used arrays, particularly for high parallel imaging acceleration applications.

Availability of data and materials

The data that support the findings of this study are available from Lawson Health Research, but restrictions apply to the availability of these data, which were used under license for the current study, and so are not publicly available. Data are however available from the authors upon reasonable request and with permission of Lawson Health Research.



Attenuation correction








Generalized autocalibration partially parallel acquisitions


Linear attenuation coefficients




Magnetic resonance imaging


Positron emission tomography


Quality control


Radio frequency


Standard deviation


Signal-to-noise ratio


Standardized uptake value


Steady-state free precession


Ultra-short echo time


  • Anazodo UC, Farag A, Théberg J, Teuho J, Thompson RT, Teräs M, Taylor R, Butler J, Finger EC, Prato FS, Thiessen JD. (2016) Assessment of PET performance of a 32-Channel MR Brain Array Head Coil Compatible with PET for Integrated PET-MRI. Preceding PSMR conference Cologne, Germany.

  • Camici PG, Prasad SK, Rimoldi OE (2008) Stunning, hibernation, and assessment of myocardial viability. Circulation 117(1):103–114

    Article  Google Scholar 

  • Carney JP, Townsend DW, Rappoport V, Bendriem B (2006) Method for transforming CT images for attenuation correction in PET/CT imaging. Am Assoc Phys Med 33(4):976–983

    Google Scholar 

  • Catana C, Drzezga A, Heiss WD, Rosen BR (2012) PET/MRI for neurologic applications. J Nucl Med 53:1916–1925

    Article  Google Scholar 

  • Dregely I, Lanz T, Metz S, Mueller MF, Kuschan M, Nimbalkar M, Bundschuh RA, Ziegler SI, Haase A, Nekolla SG (2014) A 16-channel MR coil for simultaneous PET/MR imaging in breast cancer. Eur Soc Radiol 25:1154–1161

    Article  Google Scholar 

  • Eldib M, Bini J, Robson P, Calcagno C, Faul D, Tsoumpas C, Fayad ZA (2015) Markerless attenuation correction for carotid MRI surface receiver coils in combined PET/MR imaging. Phys Med Biol 60(12):4705

    Article  Google Scholar 

  • Ferguson A, McConathy J, Su Y, Hewing D, Laforest R (2014) Attenuation effects of MR headphones during brain PET/MR studies. J Nucl Med Technol 42:93–100

    Article  Google Scholar 

  • Frohwein LJ, Heß M, Schlicher D, Bolwin K, Büther F, Jiang X, Schäfers K (2018) PET attenuation correction for flexible MRI surface coils in hybrid PET/MRI using a 3D depth camera. Phys Med Biol 63(2):025033

    Article  Google Scholar 

  • Fürst S, Souvatzoglou M, Martinez-Möller A, Nekolla S, Schwaiger M, Ziegler S. (2012). Impact of MRI surface coils on quantification in integrated PET/MR. The Journal of Nuclear Medicine 53(supplement 1), 436.

  • Griswold MA, Jakob PM, Heidemann RM, Nittka M, Jellus V, Wang J, Kiefer B, Haase A (2002) Generalized autocalibrating partially parallel acquisitions (GRAPPA). Magn Reson Med 47(6):1202–1210

    Article  Google Scholar 

  • Haacke EM, Wielopolski PA, Tkach JA & Modic MT. (1990). Steady-state free precession imaging in the presence of motion: application for improved visualization of the cerebrospinal fluid. Radiology 175(2):545–552.

  • Henkelman RM (1985). Measurement of signal intensities in the presence of noise in MR images. Medical Physics 12(2):232–233.

    Article  CAS  Google Scholar 

  • Kartmann R, Paulus DH, Braun H, Aklan B, Ziegler S, Navalpakkam BK, Lentschig M, Quick HH (2013) Integrated PET/MR imaging: automatic attenuation correction of flexible RF coils. Med Phys 40(8):082301

    Article  Google Scholar 

  • MacDonald LR, Kohlmyer S, Liu C, Lewellen TK, Kinahan PE (2011) Effects of MR surface coils on PET quantification. Med Phys 38(6):2948–2956

    Article  Google Scholar 

  • Meise FM, Rivoire J, Terekhov M, Wiggins GC, Keil B, Karpuk S, Salhi Z, Wald LL, Schreiber LM (2010) Design and evaluation of a 32-channel phased-array coil for lung imaging with hyperpolarized 3-helium. Magn Reson Med 63(2):456–464

    Article  Google Scholar 

  • Nensa F, Bamberg F, Rischpler C, Menezes L, Poeppel TD, Fougère CL, Beitzke D, Rasul S, Loewe C, Nikolaou K, Bucerius J, Kjaer A, Gutberlet M, Prakken NH, Vliegenthart R, Slart RHJA, Nekolla SG, Lassen ML, Pichler BJ, Schlosser T, Jacquier A, Quick HH, Schäfers M, Hacker M, Francone M, Bremerich J, Natale L, Wildberger J, Sinitsyn V, Hyafil F, Verberne HJ, Sciagrà R, Gimelli A, Übleis C, Lindner O, On Behalf of the European Society of Cardiovascular, R. & The European Association of Nuclear Medicine Cardiovascular, C (2018) Hybrid cardiac imaging using PET/MRI: a joint position statement by the European Society of Cardiovascular Radiology (ESCR) and the European Association of Nuclear Medicine (EANM). Eur J Hybrid Imaging 2(1):14

    Article  Google Scholar 

  • Nensa F, Beiderwellen K, Heusch P, Wetter A (2014) Clinical applications of PET/MRI: current status and future perspectives. Diagn Interv Radiol 20(5):438–447

    Article  Google Scholar 

  • Ouyang J, Petibon Y, Huang C, Reese TG, Kolnick AL, Fakhri GE (2014) Quantitative simultaneous positron emission tomography and magnetic resonance imaging. J Med Imaging 1(3):1-7, 7.

    Article  Google Scholar 

  • Patrick JC, Terry Thompson R, So A, Butler J, Faul D, Stodilka RZ, Yartsev S, Prato FS, Gaede S (2017) Technical note: comparison of megavoltage, dual-energy, and single-energy CT-based μ-maps for a four-channel breast coil in PET/MRI. Med Phys 44(9):4758–4765

    Article  Google Scholar 

  • Paulus DH, Braun H, Aklan B, Quick HH (2012) Simultaneous PET/MR imaging: MR-based attenuation correction of local radiofrequency surface coils. Med Phys 39(7):4306–4315

    Article  Google Scholar 

  • Pichler B, Judenhofer M, Wehrl H (2008a) PET/MRI hybrid imaging: devices and initial results. Eur Radiol 18(6):1077–1086

    Article  Google Scholar 

  • Pichler BJ, Wehrl HF, Kolb A, Judenhofer MS (2008b) Positron emission tomography/magnetic resonance imaging: the next generation of multimodality imaging? Semin Nucl Med 38(3):199–208

    Article  Google Scholar 

  • Price RR, Axel L, Morgan T, Newman R, Perman W, Schneiders N, Selikson M, Wood M, Thomas SR (1990) Quality assurance methods and phantoms for magnetic resonance imaging: Medical Physics, report of AAPM nuclear magnetic resonance Task Group No. 1. 17(2):287–295.

  • Pruessmann KP, Weiger M, Scheidegger MB, Boesiger P (1999) SENSE: Sensitivity encoding for fast MRI. Magnetic Resonance in Medicine 42(5):952–962.

    Article  CAS  Google Scholar 

  • Rausch I, Quick HH, Cal-Gonzalez J, Sattler B, Boellaard R, Beyer T (2017) Technical and instrumentational foundations of PET/MRI. Eur J Radiol 94:A3–A13

    Article  Google Scholar 

  • Reeder SB, Wintersperger BJ, Dietrich O, Lanz T, Greiser A, Reiser MF, Glazer GM, Schoenberg SO (2005) Practical approaches to the evaluation of signal-to-noise ratio performance with parallel imaging: application with cardiac imaging and a 32-channel cardiac coil. Magn Reson Med 54(3):748–754

    Article  Google Scholar 

  • Robson PM, Grant AK, Madhuranthakam AJ, Lattanzi R, Sodickson DK, Mckenzie CA (2008) Comprehensive quantification of signal-to-noise ratio and g-factor for image-based and k-space-based parallel imaging reconstructions. Magn Reson Med 60:895–907

    Article  Google Scholar 

  • Sander CY, Keil B, Chonde DB, Rosen BR, Catana C, Wald LL (2014) A 31-channel MR brain array coil compatible with positron emission tomography. Magn Reson Med 73(6):2363–2375

    Article  Google Scholar 

  • Schmitt M, Potthast A, Sosnovik DE, Polimeni JR, Wiggins GC, Triantafyllou C, Wald LL (2008) A 128-channel receive-only cardiac coil for highly accelerated cardiac MRI at 3 Tesla. Magn Reson Med 59(6):1431–1439

    Article  Google Scholar 

  • Tellmann L, Quick H, Bockisch A, Herzog H, Beyer T (2011) The effect of MR surface coils on PET quantification in whole-body PET/MR: results from a pseudo-PET/MR phantom study. Med Phys 38(5):2795–2805

    Article  CAS  Google Scholar 

  • Wagenknecht G, Kaiser H-J, Mottaghy FM, Herzog H (2013) MRI for attenuation correction in PET: methods and challenges. MAGMA 26(1):99–113

    Article  Google Scholar 

  • White JA, Rajchl M, Butler J, Thompson RT, Prato FS, Wisenberg G (2013) Active cardiac sarcoidosis first clinical experience of simultaneous positron emission tomography–magnetic resonance imaging for the diagnosis of cardiac disease. Circulation 127(22):e639–e641

    Article  Google Scholar 

  • Wiggins G, Triantafyllou C, Potthast A, Reykowski A, Nittka M, Wald L (2006) 32-channel 3 tesla receive-only phased-array head coil with soccer-ball element geometry. Magn Reson Med 56(1):216–223

    Article  CAS  Google Scholar 

  • Wintersperger BJ, Reeder SB, Nikolaou K, Dietrich O, Huber A, greiser A, LANZ T, Reiser MF, Schoenberg SO (2006) Cardiac CINE MR imaging with a 32-channel cardiac coil and parallel imaging: impact of acceleration factors on image quality and volumetric accuracy. J Magn Reson Imaging 23(2):222–227

    Article  Google Scholar 

Download references


The authors gratefully acknowledge funding from MITACS (Application Ref. IT12869) (to JThé), an industry-sponsored internship (to AF) in collaboration with Multi Magnetics Inc. (London, Ontario, Canada). Partial salary support of AF by NSERC Discovery Grant (No. RGPIN-2016-05055) (to JThé), infrastructure support by Ontario Research Fund (RE07-021) (to FSP) and by Canada Foundation for Innovation Grant (11358) (to FSP).


MITACS (Application Ref. IT12869) and NSERC Discovery Grant (No. RGPIN-2016-05055).

Author information

Authors and Affiliations



AF: Experiment design, data acquisition, data analysis, and writing manuscript. RTT: data visualizing, editing manuscript. JDT: data examination, editing manuscript. JB: data acquisition, editing manuscript. FSP: data examination, editing manuscript. JT: Experiment supervision, data examination, editing manuscript. All authors read and approved the final manuscript.

Corresponding author

Correspondence to Adam Farag.

Ethics declarations

Ethics approval and consent to participate

Data acquisitions from human involved in this study followed the procedures in accordance with a research ethics protocol approved by Western University Research Ethics Board (protocol ID 6319).

Consent for publication

Written informed consent was obtained from volunteers and individual involved in this study.

Competing interests

The first author declares that he owns limited number of shares in Ceresesna Inc.

Publisher’s Note

Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Rights and permissions

Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (, which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.

Reprints and permissions

About this article

Check for updates. Verify currency and authenticity via CrossMark

Cite this article

Farag, A., Thompson, R.T., Thiessen, J.D. et al. Assessment of a novel 32-channel phased array for cardiovascular hybrid PET/MRI imaging: MRI performance. European J Hybrid Imaging 3, 13 (2019).

Download citation

  • Received:

  • Accepted:

  • Published:

  • DOI: