1. Introduction
The invasive assessment of coronary microvascular dysfunction (CMD) is a growing field, particularly following the success of the CorMiCa trial (Coronary Microvascular Angina trial, NCT: NCT03193294), showing that an invasive diagnostic procedural approach resulted in improved symptoms and quality of life for patients with angina with non-obstructive coronary artery disease (ANOCA) [1]. Additionally, a recent randomised control trial by Sinha et al., showed that ANOCA patients with a reduced coronary flow reserve (CFR) benefit from anti-ischaemic therapy [2]. Moreover, a meta-analysis and systematic review by Kelshiker et al. has shown that CFR holds significant prognostic value across a wide range of cardiac pathologies [3].
In contemporary practice, several methodologies for the invasive evaluation of CMD exist [4], namely, Doppler [5,6], Bolus Thermodilution [7,8], Continuous Thermodilution [9,10], and angiogram-derived [11,12,13]. The various benefits, pitfalls, and differences between them have been the subject matter of several notable publications [14,15,16,17,18].
Continuous Thermodilution is a novel method in the invasive assessment of coronary microvascular dysfunction (CMD) which allows the volumetric quantification of absolute coronary flow (Q) in mL/min from which subsequent microvascular indices can be derived. It has been demonstrated to be safe and operator independent in multiple studies [19,20]. Additionally, it has demonstrated good correlations with invasive Doppler assessment [21], as well as non-invasive 15O-H2O-PET assessment [17]. Furthermore, it has superior reproducibility to the other widely utilised method of bolus thermodilution [15].
However, it is not without pitfalls. During the continuous thermodilution procedure, temperature is measured continuously during the intracoronary saline infusion at a sampling rate of 100 Hz allowing the quantification of Q throughout the cardiac cycle. By default, the proprietary analysis software “Coroflow” (Version 3.4, Coroventis, Uppsala, Sweden), applies a 2 s moving average filter to the temperature trace to average out the significant variation in flow throughout the cardiac cycle. The moving average filter can also be increased to 4 or 6 s from within the software settings. This, however, can be ineffective in the presence of irregular heart rates, ventricular extrasystoles, and deep inspiration, resulting in unsteady traces, ambiguity regarding the placement of markers denoting distal mixed temperature (T) and infusate temperature (Ti), and a theoretical under or over estimation of Q.
This study aims to investigate whether using a longer moving average filter will result in improved reproducibility whilst maintaining diagnostic agreements and accuracy (Scheme 1). Additionally, whether a longer filter will adequately smoothen the data, in order to improve interpretability.
2. Methods
2.1. Study Design
This is a sub-analysis of a previously reported study [15]. Patients with angina and non-obstructive coronary artery disease (ANOCA) were prospectively enrolled from January 2021 to January 2022. The study protocol was approved by the institutional review board (IRB of the Onze-Lieve-Vrouw Clinic in Aalst, Belgium, Registration number: 2020/033). The full design and results of the parent study can be found published in EuroIntervention [15].
2.2. Coronary Angiography
Coronary angiography was performed via either the radial or femoral route using 6Fr guiding catheters. Isosorbide Dinitrate (0.2 mg) was administered intracoronary. A specialised coronary guidewire with a distal pressure and temperature sensor was advanced to the equalization position, and the aortic pressure (Pa) and distal coronary pressure (Pd) were equalized on the dedicated console (Coroflow, Coroventis, Uppsala, Sweden). The coronary guidewire was then advanced into the coronary to a distal position.
2.3. Continuous Thermodilution Measurements
Continuous thermodilution measurements were performed according to previously described methodology [22]. A dedicated monorail 2.52Fr infusion microcatheter with four distal side holes (Rayflow, Hexacath, Paris, France) [23] was connected to an automatic infusion pump and flushed outside the body with room temperature saline at a rate of between 10 and 20 mL/min. It was subsequently advanced over the specialised coronary guidewire and advanced to the first few millimetres of the coronary artery under investigation. A continuous recording of aortic pressure (Pa), distal coronary pressure (Pd) and Temperature was performed during infusion of room temperature saline at rates of 10 mL/min (resting) followed by 20 mL/min (hyperemic) until steady state was achieved [24]. Following this, the coronary guidewire was swiftly pulled back until the pressure/thermistor segment was within the Rayflow catheter to record the temperature of the infusate (Ti) at 20 mL/min followed by 10 mL/min. This process was then repeated once again in each patient to assess reproducibility.
2.4. Analysis of Traces
Continuous thermodilution traces were extracted from Coroflow into .csv format. A dedicated app was programmed using Python (Version 3.10.9, Python Software Foundation, Wilmington, DE, USA) with Plotly library (Plotly, Montreal, QC, Canada), that facilitated plotting of continuous thermodilution traces. The data was analysed in two stages.
In the first stage, the temperature trace was plotted using a 2 s moving average as is default in Coroflow. When a data point was clicked within the dedicated app, simultaneous 2,10,15, and 20 s averages of the Pd, Pa, and raw temperature up to that datapoint were automatically calculated and displayed within a table in the app. Accordingly, the analysis of each trace required four clicks: a click each within the usual “steady state” period of T and Ti, repeated at both saline infusion rates. For the purposes of this study, a 2 s average of data was considered the reference standard, as Coroflow defaults to a 2 s moving average. This analysis was used to determine the maximum acceptable average (see Section 2.7: Determination of Maximum Length of Average).
In the second stage, the data was re-plotted using a longer moving average filter as determined in the first stage. The data was then reanalysed in its entirety with the longer moving average filter in order to simulate the real-world consequences of lengthened smoothening of data (Figure 1).
2.5. Definition of a Moving Average Filter
A moving average filter is a data smoothing method that is used to minimise noise and emphasise patterns in a dataset. It works by taking the mean of a window size (a predetermined number of consecutive data points) and advancing this window over the dataset. A new set of data points is produced as a result, each of which represents the average value of the original data during a particular period of time. The resulting plots display less fluctuations and variability resulting in a smoother curve.
2.6. Calculation of Absolute Flow (Q)
The calculations of Q at different length averages were calculated as:
where “Q” is absolute flow, “Ti” is the infusate temperature, “T” is the distal mixed temperature, and “Qi” represents the infusion rate of saline.The remaining formulas used for the calculation of continuous thermodilution indices are supplied in the supplemental material (Supplementary Table S1). All indices were calculated using the corresponding averages of Ti, T, Pd, and Pa.
2.7. Determination of Maximum Length of Average
To ascertain the maximum acceptable length of averaged data, it was determined that each tested average must meet the following criteria when compared to the reference standard of a 2-s average: the Q (rest and hyperemic) values should have a mean bias no greater than ±5 mL/min. Hyperemic Microvascular Resistance (Rµ,hyper) should have a mean bias no greater than ±5 Woods Units (WU). CFR should have a mean bias no greater than ±0.1 CFR points. MRR should have mean bias no greater than ±0.1 MRR points. Additionally, it was mandated that the longer averages display a diagnostic accuracy (see Section 2.8: Statistical Analysis) of ≥90% for CFR (cut off < 2.5) and Rµ,hyper (cut off > 400) when compared to 2 s average as a reference standard.
2.8. Statistical Analysis
The distribution of continuous variables was assessed visually using Q-Q plots and histograms. Continuous data are expressed as mean (±standard deviation), or median (25th–75th percentile) as appropriate. Mean bias is expressed as Mean (95% Confidence Intervals). Correlations were assessed using Pearson’s r. The Intraclass Correlation Coefficient (ICC) was calculated using a single measure, two-way mixed effect model with measures of absolute agreement. Bland–Altman analysis was used to quantify the agreement between repeated measurements. Diagnostic accuracy was calculated using the formula:
where “TP” = true positive, “TN” = true negative, “FP” = false positive, “FN” = false negative. Variability was calculated as a relative difference of two measurements (A and B) and expressed as a percentage according to the formula:All analyses were performed using SPSS (IBM, New York, NY, USA). A p value of <0.05 was considered statistically significant.
3. Results
3.1. Baseline and Procedural Data
All 102 patients included in the parent study were included in this sub-analysis. No traces were excluded on the basis of insufficient steady state periods. The full baseline and procedural data can be viewed as published in EuroIntervention [15].
3.2. Determination of Maximum Acceptable Average
With pooled test and re-test data of the three averages tested (10, 15 and 20 s), only the average of 10 s fulfilled all the criteria to be acceptable as a longer average (Table 1). Compared to the reference standard, the mean bias of Qrest was −1.02 (95% CI −1.66–−0.39) mL/min, the mean bias of Qhyper was 2.71 (95% CI 0.91–4.51) mL/min, the mean bias of CFR was 0.07 (95% CI 0.05–0.10), the mean bias of MRR was 0.1 (95% CI 0.06–0.13), and the mean bias of Rµ,hyper was −4.86 (95% CI −7.86–−1.87) WU (Table 1). All indices at 10 s averages were highly correlated with their reference standard counterpart (r = 0.97–0.99, p < 0.001 for all) (Supplementary Figure S1).
Similarly, of the three averages tested, only the average of 10 s fulfilled the diagnostic accuracy criteria, with a CFR accuracy of 90%, and a Rµ,hyper accuracy of 95%. The complete list of accuracies of each average CFR and Rµ,hyper is located within Table 1.
3.3. Re-Analysis with a 10 s Moving Average Filter
Following re-analysis of the traces with a 10 s moving average filter applied, the mean bias from the combined data (test and re-test) of indices calculated with a 10 s moving average were compared to indices calculated with a 2 s average as a reference standard. The mean bias of Qrest was 1.81 (95% CI 1.02–2.59) mL/min, the mean bias of Qhyper was −2.47 (95% CI −4.53–−0.41) mL/min, the mean bias of CFR was −0.09 (95% CI −0.12–−0.06), the mean bias of MRR was −0.11 (95% CI −0.15–−0.07), and the mean bias of Rµ,hyper was 4.08 (95% CI 0.22–7.95) WU (Supplementary Table S2). All indices derived using a 10 s moving average filter were highly correlated with their reference standard counterparts (r = 0.96–0.98, p < 0.001) (Supplementary Table S2). With a 10 s moving average filter applied, the diagnostic accuracy of CFR was 89% (CFR < 2.5), and Rµ,hyper was 94% (Rµ,hyper > 400), when compared to the reference standard.
3.4. Assessment of Reproducibility
The reproducibility data from duplicate measurements of continuous thermodilution derived indices using a 10 s moving average filter, as well as continuous thermodilution derived indices using a 2 s average are displayed in Table 2. Overall, there was no significant improvement in reproducibility when a 10 s moving average filter was applied, however, no significant deterioration was observed. Figure 2 and Figure 3, illustrate the individual correlations, scatter plots, and Bland–Altman analyses for repeated measurements of CFR and Rµ,hyper, respectively, analysed using both a 2 s and 10 s moving average filter.
4. Discussion
4.1. Summary of Results
This study is the first of its kind to examine the accuracy and reproducibility of alternative methods of interpreting raw invasive pressure/thermistor data acquired during continuous thermodilution measurements. We tested the hypothesis that a longer moving average filter would smoothen any irregularities within the continuous thermodilution traces resulting in less variation in measurements on a test–retest basis. Conclusively, we have not demonstrated superiority of a longer moving average filter for three main reasons: Firstly, there was no demonstrated improvement in reproducibility, variability (%), or correlation of test–retest when compared to the reference standard. Secondly, when a longer 10 s moving average filter was applied, there was a loss of fidelity in the temperature traces. Lastly, a clinically unacceptable level of diagnostic mismatch occurs when a longer filter is applied.
4.2. Reproducibility
There was no demonstrated improvement in reproducibility noted after re-analysis with a 10 s moving average filter. Of note, during the determination of the longest acceptable average, there was a slight numerical improvement in some of the reproducibility metrics (Supplementary Table S3); however, at this stage of the analysis, the temperature data was plotted using the standard 2 s moving average filter (see first stage of the analysis of traces) allowing the “steady state” portions of the traces to be identified easily. When a 10 s moving average filter is applied, a short “steady state” period can be lost within the slope of the temperature curve and any appreciable benefit is lost.
4.3. Loss of Fidelity with 10 s Moving Average
A 10 s moving average filter results in the smoothening of any peaks or troughs caused by variations in flow due to irregular heart rhythms, ventricular extrasystoles, or deep inspiration. However, as we have noted during analysis, this also results in a loss of fidelity and inadvertent loss of crucial sections of the trace.
In several of the analysed traces, the “steady state” period during Ti measurement can be brief, as there is often a phenomenon of irregular temperature traces noted immediately after the wire is pulled back into the Rayflow catheter. This phenomenon is likely to be caused by sudden pressure changes related to the proximity of the coronary guidewire pressure transducer to the Rayflow catheter spray, as noted in the Pd trace which climbs to supraphysiological levels during this portion of the measurement. Normally, this irregular temperature trace takes around 10–15 s to re-settle following the pullback manoeuvre, before slowly reaching a steady state from which the Ti measurement can be selected. If the steady state period is short, it can be lost when a 10 s moving average is applied. Moreover, another portion of the Ti phase can subsequently appear to be longer and more stable therefore shifting the position of Ti measurement entirely. As a result, the traces become harder to interpret, rather than easier. Of note, this is not a perceivable issue during the T portion of the measurement.
4.4. Diagnostic Mismatch
When a 10 s moving average is applied, a numerically respectable diagnostic accuracy (CFR accuracy 89%, Rµ,hyper accuracy 94%) is achieved; however, when considered from a clinical standpoint, it reflects an unacceptable level of diagnostic mismatch. To illustrate further, when microvascular phenotypes (structural or functional, versus no CMD) are determined, there is a 12% diagnostic mismatch when a 10 s moving average filter is applied (Figure 4).
5. Limitations
There are several limitations. First, this is a retrospective sub-analysis; however, the original intention for the data, as well as its quality, rendered it ideal for this analysis. Second, as these were high quality data, we cannot rule out the possibility of this method working for lower quality data. Third, the trace analysis was performed by a single unblinded assessor which may introduce bias. This was mitigated by analysing all the first test traces consecutively and uninterrupted, before moving to the second test traces using a separate datasheet. Finally, a dedicated app was encoded for the purposes of the analysis, and although unlikely, there may be small differences in how the native Coroflow software handles the data.
6. Conclusions
Applying a longer moving average of 10 s to the continuous thermodilution traces has a negligible effect on reproducibility. Furthermore, it has a deleterious effect on the interpretability of the traces due to loss of fidelity. Lastly, it results in unacceptable levels of diagnostic mismatch relative to the reference standard. As a result, it is advisable to maintain the current practice. Notwithstanding, offering comprehensive guidance on cursor placement during trace analysis could prove beneficial for inexperienced users. Accordingly, a standardisation of continuous thermodilution methodology would be a welcome addition to the literature base.
Conceptualization, S.F., J.R.D., G.V.K. and T.R.K.; Data curation, D.M., T.M. (Thabo Mahendiran), E.G., T.M. (Takuya Mizukami) and B.D.B.; Formal analysis, S.F.; Investigation, D.M., E.G., T.M. (Takuya Mizukami) and B.D.B.; Methodology, S.F., T.M. (Thabo Mahendiran), S.A.K., R.F.G.S., J.S., C.M.C., J.R.D. and T.R.K.; Software, S.F.; Supervision, B.D.B. and T.R.K.; Visualization, S.F.; Writing—original draft, S.F.; Writing—review and editing, D.M., T.M. (Thabo Mahendiran), E.G., T.M. (Takuya Mizukami), S.A.K., R.F.G.S., J.S., C.M.C., J.R.D., G.V.K., B.D.B. and T.R.K. All authors have read and agreed to the published version of the manuscript.
The study was conducted in accordance with the Declaration of Helsinki and the study protocol was approved by the institutional review board (IRB of the Onze-Lieve-Vrouw Clinic in Aalst, Belgium, Registration number: 2020/033).
Informed consent was obtained from all subjects involved in the study.
The data presented in this study are available in the main article and
T. Mizukami reports research grants from Boston Scientific, and speaker fees from Abbott Vascular, Cathworks, Boston Scientific. T. Mahendiran is supported by a research grant from the Swiss National Science Foundation. D. Munhoz reports a research grant provided by the Cardiopath PhD program and speaker fees from Abbott Vascular. B. De Bruyne reports institutional consulting relationships with Boston Scientific, Abbott Vascular, CathWorks, Siemens, GE Healthcare, and Coroventis Research; has received institutional research grants from Abbott Vascular, Coroventis Research, CathWorks, and Boston Scientific; and holds minor equities in Philips, Siemens, GE Healthcare, Edwards Lifesciences, HeartFlow, Opsens, and Celiad. Christopher M Cook is a consultant for Philips Healthcare and Viz.ai, receives speaker fees from Boston Scientific and has equity in Cerebria.ai. J. R Davies reports research grants from Abbott Vascular and Medtronic, and speaker fees from Boston Scientific. T. R Keeble reports honoraria and institutional research funding from Abbott Vascular, Medtronic, Hexacath, Terumo, Zoll and Shockwave; consulting fees from BD; and speaker fees from Cardionovum, Abbott Vascular and Astra Zeneca. J. Svanerud is the CEO and Founder of Coroventis Research AB. The remaining authors have no relevant disclosures.
ANOCA | Angina with Non-Obstructive Coronary Artery Disease |
CFR | Coronary Flow Reserve |
CMD | Coronary Microvascular Dysfunction |
FFR | Fractional Flow Reserve |
MRR | Microvascular Resistance Reserve |
Pa | Aortic pressure |
Pa,rest | Aortic pressure at rest (mmHg) |
Pa,hyper | Aortic pressure at maximum coronary hyperemia (mmHg) |
Pd | Distal coronary pressure |
Pd,rest | Distal coronary pressure at rest (mmHg) |
Pd,hyper | Distal coronary pressure at maximum coronary hyperemia (mmHg) |
PET | Positron Emission Tomography |
Q | Absolute Coronary Flow (mL/min) |
Qrest | Absolute Coronary Flow at rest (mL/min) |
Qhyper | Absolute Coronary Flow during hyperemia (mL/min) |
Qi | Saline Infusion Rate |
Rµ,hyper | Hyperemic Microvascular Resistance |
WU | Woods Units |
T | Distal Coronary Mixed Temperature |
Ti | Difference between blood temperature and the temperature of saline at the exit of the infusion catheter (°C) |
Footnotes
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Scheme 1. Experimental Assessment of Longer Continuous Thermodilution Moving Average Filter. Temperature trace (blue), Pd trace (green), Pa trace (red).
Figure 1. Demonstration of continuous thermodilution traces visualised with a 2 s moving average (above), and 10 s moving average (below). Temperature trace (blue), Pd trace (green), Pa trace (red).
Figure 2. Reproducibility of CFR. Scatter plot of first and second CFR measurement using 2 s average (A), and associated Bland–Altman plot (B). Scatter plot of first and second CFR measurement using 10 s average (C), and associated Bland–Altman plot (D). “CFR” = Coronary Flow Reserve, “R” = Pearson’s r, “ICC” = Intraclass Correlation Coefficient.
Figure 3. Reproducibility of Rµ,hyper. Scatter plot of first and second Rµ,hyper measurement using 2 s average (A), and associated Bland–Altman plot (B). Scatter plot of first and second Rµ,hyper measurement using 10 s average (C), and associated Bland–Altman plot (D). “Rµ,hyper” = Hyperemic Microvascular Resistance, “R” = Pearson’s r, “ICC” = Intraclass Correlation Coefficient.
Figure 4. Sankey chart of microvascular phenotypes classification. Classified on left using reference standard 2 s average, followed by direction of classification using 10 s moving average filter applied.
Determination of maximum acceptable averages of continuous thermodilution indices. Acceptable (green), not acceptable (red).
2 s Average (Reference) | 10 s Average | 15 s Average | 20 s Average | |
---|---|---|---|---|
Mean Bias | Mean Bias | Mean Bias | ||
Qrest | 82 ± 30 mL/min | | | |
Qhyper | 211 ± 77 mL/min | | | |
Rµ,hyper | 403 ± 135 WU | | | |
CFR | 2.67 ± 0.81 | | | |
MRR | 3.24 ± 0.96 | | | |
Accuracy (%) | ||||
CFR (<2.5) | | | | |
Rµ,hyper (>400) | | | |
“Qrest” = Resting coronary flow, “Qhyper” = Hyperemic absolute coronary flow, “Rµ,hyper” = Hyperemic microvascular resistance, “CFR” = Coronary Flow Reserve, “MRR” = Microvascular Resistance Reserve.
Means ± SD of Test 1 and Test 2 continuous thermodilution indices analysed with 2 and 10 s averages. Comparison of test–retest reproducibility of a 2 s average (reference), versus a 10 s moving average filter. “CFR” = Coronary Flow Reserve, “MRR” = Microvascular resistance reserve, “Rµ,hyper” = Hyperemic Microvascular Resistance, “Qrest” = resting absolute flow, “Qhyper” = hyperemic absolute flow. “R” = Pearson’s r, “ICC” = Intraclass Correlation Coefficient. “Var (%)” = Variability Percentage, “CI” = Confidence interval.
2 s Average | 10 s Moving Average Filter | |||||||||
---|---|---|---|---|---|---|---|---|---|---|
Test 1 | Test 2 | R (95% CI) | ICC (95% CI) | Var (%) | Test 1 | Test 2 | R (95% CI) | ICC (95% CI) | Var (%) | |
CFR | 2.73 ± 0.80 | 2.61 ± 0.82 | 0.74 (0.63–0.81) | 0.73 (0.62–0.81) | 17.8 ± 12.4 | 2.62 ± 0.73 | 2.54 ± 0.76 | 0.74 (0.63–0.81) | 0.73 (0.63–0.81) | 16.2 ± 12.1 |
MRR | 3.27 ± 0.95 | 3.22 ± 0.97 | 0.72 (0.61–0.80) | 0.72 (0.61–0.80) | 16.5 ± 12.4 | 3.16 ± 0.89 | 3.11 ± 0.91 | 0.73 (0.63–0.81) | 0.73 (0.63–0.81) | 16.2 ± 11.8 |
Rµ,hyper | 408 ± 142 | 398 ± 129 | 0.88 (0.83–0.92) | 0.88 (0.82–0.91) | 11.9 ± 9.9 | 412 ± 139 | 403 ± 137 | 0.89 (0.83–0.92) | 0.89 (0.83–0.92) | 11.4 ± 10 |
Qrest | 79 ± 28 | 86 ± 32 | 0.73 (0.62–0.81) | 0.70 (0.57–0.79) | 20.3 ± 16.0 | 80 ± 28 | 88 ± 34 | 0.77 (0.76–0.84) | 0.73 (0.59–0.82) | 20 ± 14.8 |
Qhyper | 207 ± 73 | 216 ± 81 | 0.87 (0.81–0.91) | 0.86 (0.80–0.90) | 12.5 ± 11.1 | 202 ± 67 | 215 ± 81 | 0.89 (0.84–0.92) | 0.86 (0.79–0.91) | 13 ± 11.1 |
Supplementary Materials
The following supporting information can be downloaded at:
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Abstract
Continuous Thermodilution is a novel method of quantifying coronary flow (Q) in mL/min. To account for variability of Q within the cardiac cycle, the trace is smoothened with a 2 s moving average filter. This can sometimes be ineffective due to significant heart rate variability, ventricular extrasystoles, and deep inspiration, resulting in a fluctuating temperature trace and ambiguity in the location of the “steady state”. This study aims to assess whether a longer moving average filter would smoothen any fluctuations within the continuous thermodilution traces resulting in improved interpretability and reproducibility on a test–retest basis. Patients with ANOCA underwent repeat continuous thermodilution measurements. Analysis of traces were performed at averages of 10, 15, and 20 s to determine the maximum acceptable average. The maximum acceptable average was subsequently applied as a moving average filter and the traces were re-analysed to assess the practical consequences of a longer moving average. Reproducibility was then assessed and compared to a 2 s moving average. Of the averages tested, only 10 s met the criteria for acceptance. When the data was reanalysed with a 10 s moving average filter, there was no significant improvement in reproducibility, however, it resulted in a 12% diagnostic mismatch. Applying a longer moving average filter to continuous thermodilution data does not improve reproducibility. Furthermore, it results in a loss of fidelity on the traces, and a 12% diagnostic mismatch. Overall, current practice should be maintained.
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1 Essex Cardiothoracic Centre, Basildon Hospital, Nether Mayne, Basildon SS16 5NL, UK; Medical Technology Research Centre (MTRC), Anglia-Ruskin University, Chelmsford CM1 1SQ, UK
2 Cardiovascular Center Aalst, OLV Clinic, 9300 Aalst, Belgium; Department of Advanced Biomedical Sciences, University Federico II, 80138 Naples, Italy
3 Cardiovascular Center Aalst, OLV Clinic, 9300 Aalst, Belgium; Lausanne University Hospital, 1005 Lausanne, Switzerland
4 Cardiovascular Center Aalst, OLV Clinic, 9300 Aalst, Belgium; Division of University Cardiology, IRCCS Ospedale Galeazzi Sant’Ambrogio, 20157 Milan, Italy
5 Cardiovascular Center Aalst, OLV Clinic, 9300 Aalst, Belgium; Division of Clinical Pharmacology, Department of Pharmacology, Showa University, Tokyo 142-0064, Japan
6 Coroventis Research AB, 756 51 Uppsala, Sweden
7 School of Medicine, Attikon University Hospital, National and Kapodistrian University of Athens, 157 72 Athens, Greece