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Background: Native myocardial T and T relaxation times are diagnostic tools used in clinical practice for adult and pediatric populations. Use of a mapping technique requires accurate knowledge of normal ranges in healthy patients, which is lacking in pediatric populations.
Purpose: To establish normal values for native T and T mapping in healthy pediatric subjects of different ages and sex.
Study Type: Prospective.
Population: Thirty-eight healthy children (9-18 years; mean age 14.0 ± 2.7).
Field Strength: Cardiac MR with a 3T scanner. T and T mapping using MyoMaps software.
Assessment: T and T relaxation times were calculated from a 0.7-1.0 cm region of interest placed at the mid-ventricular short-axis slice in the interventricular septum by two observers. Inter- and intraobserver variability was assessed.
Statistical Tests: The Student's t-test or the Mann-Whitney test for unpaired samples was applied to compare one continuous variable between two category groups. One-way analysis of variance (ANOVA) or a Kruskal-Wallis test was applied to compare one continuous variable between three category groups. Correlation between two continuous variables was assessed with a Pearson or Spearman test.
Results: The mean native T relaxation time was 1223 ± 29 msec and T relaxation time was 43 ± 4.5 msec. There was no correlation between T /T values and age or body surface area (for T P = 0.94 and 0.90 and for T P = 0.19 and 0.64, respectively). There was weak correlation between T values and body mass index (BMI) (r = 0.448, P = 0.005). T values were significantly higher in females compared with males (44.6 ± 4.2 vs. 40.4 ± 3.8 msec, P = 0.002). We found a significant rise of T relaxation time in the pubertal period (age 13-15 years) comparing to prepubertal (age 9-12 years). Inter- and intraobserver agreement of T (r = 0.93; r = 0.99) and T (r = 0.96; r = 0.95) were high.
Data Conclusion: We report normal values of native T and T relaxation times obtained with Myomaps software for 3T cardiac MR in a healthy pediatric population.
Level Of Evidence: 2 Technical Efficacy: Stage 2 J. Magn. Reson. Imaging 2020;51:912-918.
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http://dx.doi.org/10.1002/jmri.26886 | DOI Listing |
Langmuir
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Biophysical Chemistry Laboratory, Physical Chemistry Section, Department of Chemistry, Jadavpur University, Raja S. C. Mullick Road, Jadavpur, Kolkata 700032, India.
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School of Chemistry and Biochemistry, School of Materials Science and Engineering, Center for Organic Photonics and Electronics, Georgia Institute of Technology, Atlanta, GA, 30332, USA.
Molecular spin systems that can be chemically tuned, coherently controlled, and readily integrated within devices remain central to the realization of emerging quantum technologies. Organic high-spin materials are prime candidates owing to their similarity in electronic structure to leading solid-state defect-based systems, light element composition, and the potential for entanglement and qubit operations mediated through spin-spin exchange. However, the inherent instability of these species precludes their rational design, development, and application.
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Department of Bionanoscience and Kavli Institute of Nanoscience Delft, Delft University of Technology, Delft, 2629 HZ, The Netherlands. Electronic address:
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National Laboratory of Solid State Microstructures, School of Electronic Science and Engineering and Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China.
Two-dimensional (2D) materials offer strong light-matter interaction and design flexibility beyond bulk semiconductors, but an intrinsic limit is the low absorption imposed by the atomic thickness. A long-sought-after goal is to achieve complementary absorption enhancement through energy transfer (ET) to break this limit. However, it is found challenging due to the competing charge transfer (CT) process and lack of resonance in exciton states.
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