| Literature DB >> 34760217 |
Junu Bae1, Guannan Zhang1, Hyejin Park1, Warren S Warren1,2,3, Qiu Wang1.
Abstract
Azide moieties, unique linear species containing three nitrogen atoms, represent an attractive class of molecular tag for hyperpolarized magnetic resonance imaging (HP-MRI). Here we demonstrate (15N)3-azide-containing molecules exhibit long-lasting hyperpolarization lifetimes up to 9.8 min at 1 T with remarkably high polarization levels up to 11.6% in water, thus establishing (15N)3-azide as a powerful spin storage for hyperpolarization. A single (15N)-labeled azide has also been examined as an effective alternative tag with long-lived hyperpolarization. A variety of biologically important molecules are studied in this work, including choline, glucose, amino acid, and drug derivatives, demonstrating great potential of 15N-labeled azides as universal hyperpolarized tags for nuclear magnetic resonance imaging applications. This journal is © The Royal Society of Chemistry.Entities:
Year: 2021 PMID: 34760217 PMCID: PMC8565375 DOI: 10.1039/d1sc04647k
Source DB: PubMed Journal: Chem Sci ISSN: 2041-6520 Impact factor: 9.969
Fig. 1(15N)3-Azide as a practical and effective tag for HP-MRI.
Enhancements (ε), polarization levels (P) and relaxation times (T1) for (15N)3-azides 1–6 by d-DNPa
| Cmpd | Molecular structure |
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|---|---|---|---|---|---|---|
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| Nα | Nβ | Nγ | |||
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| 336 700 | 11.6 | (2.4 ± 0.2) | (2.9 ± 0.2) | (3.3 ± 0.2) |
| (0.36 ± 0.03) | (0.10 ± 0.01) | (0.25 ± 0.02) | ||||
|
|
| 254 900 | 8.8 | (3.0 ± 0.2) | (4.0 ± 0.2) | (7.6 ± 0.3) |
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| 322 300 | 11.1 | (3.0 ± 0.3) | (5.6 ± 0.3) | (8.1 ± 0.2) |
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| 142 500 | 4.9 | (3.5 ± 0.3) | (6.2 ± 0.9) | (9.8 ± 1.7) |
|
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| 80 200 | 2.8 | (1.9 ± 0.2) | (4.0 ± 0.3) | (6.8 ± 0.9) |
|
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| 196 800 | 6.8 | (2.5 ± 0.1) | (3.6 ± 0.1) | (5.3 ± 0.1) |
Each experiment repeated twice. Measurements performed at B = 1 T unless noted otherwise. Enhancements and polarization levels averaged over all 15N sites. T1 lifetimes derived by fitting the experimental data to a single exponential decay function and then compensating the effect of using the small flip angle pulses (see ESI for details).
T 1 lifetime measured at B = 16.4 T using thermally polarized 1 in D2O.
Fig. 215N-NMR spectra of thermally polarized (15N)3-azide 1 (253 mM in D2O) acquired with (top) and without (bottom) 1H decoupling. The 15N spectra were measured at a magnetic field of 16.4 T.
Fig. 3(a) Comparison of T1 relaxation times of (15N)3-azides (see Table 1 for T1 values). (b) T1 lifetime curves for (15N)3-azides. The experimental data points were fitted to an exponential decay function. The first 8 data points are shown.
Enhancements (ε), polarization levels (P) and relaxation times (T1) for (15N) (14N)2-azide 7–9 by d-DNPa
| Cmpd | Molecular structure |
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| ||
|---|---|---|---|---|---|---|
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| Nα | Nβ | Nγ | |||
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| 76 000 | 2.6 | — | — | (3.2 ± 0.3) |
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| 121 500 | 4.2 | — | — | (7.6 ± 0.3) |
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| 28 600 | 1.0 | — | — | (5.6 ± 0.6) |
Each experiment repeated twice. Measurements performed at B = 1 T. Enhancements and polarization levels measured for 15Nγ sites. T1 lifetimes derived by fitting the experimental data to a single exponential decay function and then compensating the effect of using the small flip angle pulses (see ESI for details).
Signal to noise ratio too low for Nα.
Enhancements (ε), polarization levels (P) and relaxation times (T1) for (15N)3-azide 3 by SABRE-SHEATHa
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|---|---|---|---|---|
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| Nα | 3060 | 0.11 | (2.9 ± 0.9) |
| Nβ | 27 600 | 0.95 | (5.8 ± 0.1) | |
| Nγ | 16 100 | 0.56 | (9.2 ± 1.1) |
Each experiment repeated twice by SABRE-SHEATH measured at 1 T. Detailed hyperpolarization conditions in ESI.