Abstract

Intense solvent signals in 1H solution-state NMR experiments typically cause severe distortion of spectra and mask nearby solute signals. It is often infeasible or undesirable to replace a solvent with its perdeuterated form, for example, when analyzing formulations in situ, when exchangeable protons are present, or for practical reasons. Solvent signal suppression techniques are therefore required. WATERGATE methods are well-known to provide good solvent suppression while enabling retention of signals undergoing chemical exchange with the solvent signal. Spectra of mixtures, such as pharmaceutical formulations, are often complicated by signal overlap, high dynamic range, the narrow spectral width of 1H NMR, and signal multiplicity. Here, we show that by combining WATERGATE solvent suppression with pure shift NMR, ultrahigh-resolution 1H NMR spectra can be acquired while suppressing intense solvent signals and retaining exchangeable 1H signals. The new method is demonstrated in the analysis of cyanocobalamin, a vitamin B12 supplement, and of an eye-drop formulation of atropine.
Stringent regulations apply to the production and marketing of pharmaceuticals to ensure that any adverse effects from their use are identified and minimized. Typically, full characterization of all active pharmaceutical ingredients (APIs), excipients, and impurities is required for components in excess of 0.1%.11H solution-state NMR spectroscopy is widely used for characterization and quantification purposes in such cases. Chemical shift information and scalar coupling constants are frequently used in NMR spectroscopy to aid in molecular structure elucidation. However, for complex systems such as pharmaceutical formulations, 1H NMR spectra are often complicated by low chemical shift dispersion, signal multiplicity patterns, and the concentration disparity between major compounds and impurities, which combine to cause significant spectral overlap and hinder spectral analysis. 1H NMR spectra are particularly complicated by the presence of intense signals from nondeuterated solvent (such as H2O), where the high dynamic range between the intense solvent signal and weak solute signals makes the latter difficult to observe. Pharmaceutical formulations, metabolomic samples, and biological samples are routinely analyzed in nondeuterated solvents either to mimic in vivo conditions, to retain signals from exchangeable protons, or to avoid perturbing the system of interest (for example, to avoid denaturing proteins).2
1H NMR spectra can be simplified by acquiring spectra containing only chemical shift information, using “pure shift” experiments.3−6 These increase spectral resolution by collapsing multiplet structures into a single line at the chemical shift of each proton environment. There are multiple types of 1D 1H pure shift experiment, which differ in the treatment of active (observed) and passive (coupled) spins. A J-refocusing element, composed of a hard 180° radiofrequency (RF) pulse and an active spin-refocusing (ASR) element, when placed in the middle of an evolution time, refocuses the scalar coupling evolution of active spins while allowing the chemical shift to evolve. High-sensitivity pure shift spectra can be obtained using a homonuclear band-selective decoupling (BS)7,8 ASR element. Broadband homonuclear decoupled spectra can be acquired using the Zangger–Sterk (ZS),9 bilinear rotation decoupling (BIRD),10 or pure shift yielded by chirp excitation (PSYCHE)11,12 ASR element, but all three have an intrinsic sensitivity penalty (of 1–2 orders of magnitude depending on the ASR element).6
For samples prepared in nondeuterated solvents, additional manipulation of the nuclear magnetization is necessary to suppress the large solvent signal. For samples with large solvent signal intensities, radiation damping13−16 becomes a significant problem and can cause intense artifacts throughout the spectrum acquired if adequate solvent suppression is not performed. A common solution to this problem is to use presaturation, to saturate and remove the large solvent signal(s).17 Although presaturation methods achieve good solvent suppression, signals from nuclei in chemical exchange with the solvent are also saturated and so are strongly attenuated. This unwanted signal suppression is also observed with the NOESY-presaturation method,18 which has recently been combined with pure shift techniques.19 Furthermore, presaturation requires a long, low-power continuous wave RF pulse applied during the recovery delay of the NMR experiment in order to saturate the solvent resonance, which can lead to an undesirably long experiment time.
Alternative solvent suppression methods such as excitation sculpting20 and WATERGATE (water suppression by gradient-tailored excitation, WG)21,22 retain signals from exchangeable nuclei and do not require lengthy recovery delays. Instead, these methods use either selective pulses or binomial series of pulses, in combination with pulsed field gradients (PFGs), to refocus the off-resonance signal while dephasing the on-resonance solute signal. Excitation sculpting has previously been integrated into the PSYCHE experiment;11 however, that implementation provides poor solvent suppression. A WATERGATE pure shift method has also been reported in which WATERGATE was concatenated with the PSYCHE triple spin echo (TSE) experiment (W5n-TSE-PSYCHE where n represents the number of W5 elements).23 Although good solvent suppression has been reported with this method, the addition of separate WATERGATE elements causes unwanted scalar coupling evolution and leads to greatly increased chunking sidebands (Supporting Information, Section E).
Here, an integrated WATERGATE (iWG) pure shift experiment is introduced, and its performance is compared to that of previously published methods. The proposed pure shift iWG experiment enables retention of exchangeable proton signals, allows the use of short recovery delays for either fast data acquisition or acquisition of higher signal-to-noise ratio (SNR) spectra per unit time, and offers over a 1000-fold reduction in solvent signal intensity. As the WATERGATE element is integrated into the pure shift experiment, no extra scalar coupling evolution occurs. The usefulness of the proposed method is demonstrated in the analysis of cyanocobalamin (manufactured vitamin B12), where WATERGATE enables exchangeable amide signals to be observed in the pure shift spectra, and atropine eye-drop solution (a pharmaceutical formulation), where the ultrahigh resolution afforded by the new solvent-suppressed pure shift method aids the identification and characterization of degradation impurities in the atropine formulation.
Experimental Section
Sample Preparation
Cyanocobalamin (5 mM) was dissolved in 630 μL of phosphate buffer (H2O, pH 8.1, 0.1 M) with 70 μL of D2O added for locking purposes. 630 μL of a commercial sample of 1% atropine sulfate ophthalmic solution was added to 70 μL of D2O.
NMR Experiments
Spectra were recorded on a Bruker Avance 500 NEO spectrometer with a 5 mm room temperature triaxial gradient TBI probe with a maximum nominal GZ gradient strength of 67 G cm–1, and the results were processed using the Bruker Topspin software package (version 4.1.4).
All pure shift spectra shown in the main paper and Supporting Information were acquired with the following parameters unless otherwise stated. Sixteen increments of 1024 complex data points each were acquired with a spectral width of 10 kHz (20 ppm) and a recovery delay of 3 s, and the first 200 complex data points of each free induction decay were taken to construct the pure shift interferogram. The PSYCHE ASR element was used, with two saltire pulses of 30 ms duration, 20° flip angle β, 10 kHz bandwidth, and a simultaneous PFG of 1.5 G cm–1 nominal amplitude. Interferogram construction used the “pshift” macro (https://nmr.chemistry.manchester.ac.uk).
Experiment-specific WATERGATE, presaturation, and NOESY-presaturation parameters are given in figure captions. Further NMR acquisition and processing parameters are detailed in the Supporting Information. All raw data and the Bruker pulse program code used in this work are freely available at DOI: 10.48420/24600114.
Results and Discussion
NMR Method
The new PSYCHE-iWG pulse sequence is shown in Figure 1, with more specific details provided in the Supporting Information (Figure S1). The integration of WATERGATE (WG)21 into pure shift pulse sequences enables large solvent signals to be suppressed while solute signals are retained, even if in slow/medium chemical exchange with the solvent. Importantly, the appropriate incorporation of the WATERGATE element into a pure shift sequence enables chemical shift evolution to be retained without any net contribution to homonuclear scalar coupling evolution from these elements. The overall scalar coupling evolution is therefore refocused as usual at the midpoint of the data chunk to be acquired.3−6 WATERGATE works by applying a zero net rotation to the on-resonance signal, while off-resonance signals experience a 180° refocusing pulse. The PFGs flanking the WATERGATE element enforce the refocusing coherence transfer pathway (CTP), meaning that the on-resonance signal is dephased. The WATERGATE element achieves the desired effect using two low-power selective 90° pulses on either side of a hard 180° pulse. The selective 90° pulses are on resonance for the solvent signal and leave the solute signals unaffected. The overall sequence uses a triple spin echo (TSE)24 structure in which the WATERGATE elements refocus off-resonance signals, ensuring that timings remain balanced. The integration of two WATERGATE elements doubles the dephasing of the solvent signal, increasing the extent of the solvent suppression.
Figure 1.
PSYCHE-iWG pulse sequence. Narrow, wide and short rectangles represent hard 90°, hard 180° and selective rectangular 90° radiofrequency pulses, respectively. Trapezoids with two diagonal arrows denote low-power saltire pulses of on-resonance flip angle β (typically 20°). The evolution time t1 is incremented in the interferogram acquisition mode. The chunk duration is equal to 1/SW1. τA controls the time at which J evolution is refocused during the chunk, and is equal to 1/4SW1. Shapes G1–4 represent field gradient pulses applied along z; G1, G2 and G4 are used for CTP selection and G3 is used for spatial encoding. Further details of the pulse sequence are given in the Supporting Information (Section A).
As an alternative to the original WATERGATE element, binominal multiple-pulse WATERGATE elements (e.g., W3/W5)22 could be integrated into the sequence. The binominal W5 element comprises a series of varying flip angle pulses with a fixed interpulse delay τ (Supporting Information, Figure S1). It accomplishes the same effect as the WATERGATE element, on-resonance signal experiencing a net 0° rotation. As in the original WATERGATE element, the suppression bandwidth is inversely proportional to the duration. However, the binominal sequence causes suppression not only on resonance but also at intervals of 1/τ Hz. This causes problems if a narrow suppression band is required, because the long interpulse delay τ leads to additional suppression notches within the spectrum of interest, potentially suppressing solute signals (Supporting Information, Figure S2c,d). Although more complicated to set up if the best suppression is required, the selective pulse WATERGATE element is therefore preferable to the binominal W5 element (unless multiple suppression notches are required). The selective pulse WATERGATE element was used in Figures 2 and 3.
Figure 2.
500.13 MHz 1H NMR spectra of 5 mM cyanocobalamin in 90:10 H2O/D2O at 12 °C and pH 8.1. (a) Conventional 1D 1H NMR spectrum. (b) NOESY-presaturation PSYCHE spectrum obtained with a presaturation period of 3 s and a NOESY mixing period of 100 ms. (c) PSYCHE-iWG spectrum obtained using 5.5 ms selective rectangular 90° pulses in the WATERGATE element. The PSYCHE element consisted of two saltire pulses of 10 kHz bandwidth, 30 ms duration, and 20° on-resonance flip angle. Sixteen chunks were acquired with a duration of 20 ms. Further experimental details are given in the Supporting Information. The exchangeable protons are highlighted in orange, and the aromatic signals starred.
Figure 3.
Expansions of 500.13 MHz 1H NMR spectra of 5 mM cyanocobalamin in 90:10 H2O/D2O at 12 °C and pH 8.1. (a) Conventional 1D 1H NMR spectrum. (b) NOESY-presaturation PSYCHE spectrum with 32 scans, a presaturation period of 3 s, and a 90° excitation flip angle. (c) PSYCHE-iWG spectrum with 32 scans, a recovery delay of 3 s, and a 90° excitation flip angle. (d) PSYCHE-iWG spectrum with 128 scans, a recovery delay of 0.5 s, and an Ernst angle (73°) excitation pulse. All three PSYCHE experiments had a duration of 30 min. The SNR improvement is detailed in Table S3 in the Supporting Information.
Although shown with the PSYCHE ASR in Figure 1, the proposed WATERGATE pure shift experiment is compatible with a range of different ASR elements. The BS element is often used for acquisition of high-sensitivity spectra but is of limited general applicability as it is not broadband. The ZS ASR element enables acquisition of broadband spectra, but typically with lower sensitivity than its PSYCHE counterpart. The BIRD ASR is not appropriate here; it restricts observation to protons directly bonded to 13C, so it excludes signals likely to show exchange with solvent and in any case has intrinsic water suppression. The pulse program code (Supporting Information, Section F) enables the user to choose the most appropriate ASR element (BS, ZS, or PSYCHE) for a given sample; see the Supporting Information, Figure S7 for example spectra.
As mentioned earlier, the W5 WATERGATE and PSYCHE pulse sequence elements have been combined previously, by concatenation, for benchtop NMR.23 Although such methods can provide excellent solvent suppression, placing the WATERGATE block before the PSYCHE element (Supporting Information, Figure S3d) causes extra, unwanted scalar coupling evolution. This leads to signal discontinuities in the constructed interferogram that Fourier transform to give large undesirable chunking sidebands (Supporting Information, Figure S11b–d). A possible remedy would be to use the perfect-echo version of WATERGATE25 in a concatenated WGn/W5n-TSE-PSYCHE experiment (Supporting Information, Figures S10 and S11e). This would give a lower SNR than PSYCHE-iWG, but could be preferable in the presence of strong coupling.
Cyanocobalamin
The corrinoid cyanocobalamin (Figure 2), a synthetic vitamin B12, is used in cases of vitamin B12 deficiency anemia,26,27 typically as an oral supplement. Pure shift NMR simplifies the spectrum, collapsing multiplets into singlets and improving resolution, but solvent suppression is required to avoid intense artifacts obscuring the pure shift spectrum. Figure 2 compares spectra acquired using a 1H pulse-acquire experiment (Figure 2a), NOESY-presaturation PSYCHE19 (Figure 2b), and the new PSYCHE-iWG (Figure 2c).
Both PSYCHE-iWG and NOESY-presaturation PSYCHE offer good solvent signal suppression (2000- and 500-fold, respectively). Eliminating signal overlap facilitates discrimination between chemical environments and, coupled with 2D correlation methods, increases the ease of structure assignment (Supporting Information, Table S4).
Cyanocobalamin contains multiple exchangeable amide signals, seen between 6 and 8 ppm (expansion shown in Figure 3). The triplet at 8.3 ppm (Figure 3a) is attributed to the secondary amide. Due to its low exchange rate, this signal survives in both the NOESY-presaturation PSYCHE and PSYCHE-iWG spectra, showing as a clear singlet at 8.3 ppm in the latter. As a result of restricted rotation, 12 distinct primary amide signals are observed (highlighted in orange in Figure 2). These signals have a much faster chemical exchange with the solvent and are therefore saturated by the NOESY-presaturation element (Figures 2b and 3b). WATERGATE solvent suppression is preferable here, as it enables retention of signals undergoing chemical exchange, as demonstrated in the PSYCHE-iWG spectra (Figures 2c and 3c). The primary amide proton signals are largely retained, though some signal loss is inevitable due to transverse relaxation; the sequence duration should be minimized if T2 relaxation is a limiting factor. Because PSYCHE-iWG does not require a long recovery delay for presaturation, it allows more scans to be acquired per unit time than NOESY-presaturation PSYCHE. Setting the initial excitation pulse to the Ernst angle,28 it is possible to boost the SNR of the resultant PSYCHE-iWG spectrum (see Figure 3d, and Table S3 in the Supporting Information).
Atropine Eye-Drop Solution
Many pharmaceuticals are formulated in aqueous solution; the example used here, atropine eye-drops (Figure 4) for topical ocular administration, is used for conditions including myopia, cycloplegia, and amblyopia.29,30 The formulation contains a large concentration range of molecules, including the API, degradation products, impurities, and excipients. NMR analysis, already challenging due to the presence of multiple species with high dynamic range, is further complicated by the intense H2O signal (Figure 5a). The solvent suppression and ultrahigh resolution offered by the PSYCHE-iWG experiment (Figure 5b) simplify the identification of API signals and reduce signal overlap, allowing key signals from degradation products to be identified. Combining PSYCHE-iWG with 2D correlation structure elucidation methods (data not shown) enabled the characterization of the API and several impurities (Figures 4 and 5).
Figure 4.
Atropine API (assignments in black) and impurities. Atropine hydrolyzes to form tropine and tropic acid (assignments in gray). A NMe rearrangement product (partial assignments in brown) is in slow exchange.
Figure 5.
500.13 MHz 1H NMR spectra of an atropine eye-drop solution (90%) in D2O (10%), recorded at 25 °C. (a) Conventional 1D 1H NMR and (b) PSYCHE-iWG spectrum. Selective rectangular 90° pulses of 6 ms duration were used in the WATERGATE element. The PSYCHE element consisted of two saltire pulses of 10 kHz bandwidth, 70 ms duration, and 20° on-resonance flip angle. Sixteen chunks were acquired with a duration of 20 ms. Further experimental details are given in the Supporting Information. Atropine signal assignments are shown in black, hydrolysis products in gray, and NMe rearrangement product signals in brown.
The significant spectral overlap in the conventional 1H NMR spectrum (Figure 5a) is largely avoided in the PSYCHE-iWG spectrum (Figure 5b). The WATERGATE elements completely suppress the solvent signal while retaining solute signals that are close in frequency (e.g., H9 in atropine). The API signals (in black) are immediately evident due to their higher intensity, and full assignment is provided in Figure 5b. With the improved spectral resolution observed in Figure 5b, the impurity signals, no longer eclipsed by the more intense API signals, are easier to identify. The identification of degradation products is of importance as it provides insight into the stability of the API. Hydrolysis of the ester bond cleaves atropine into tropine and tropic acid (Figure 4; peaks assigned in gray in Figure 5b). It is possible to use these signals as markers to assess the shelf life of the eye-drop solution. A further impurity, partially assigned in brown, is attributed to reversible rearrangement of the NMe group.31 The preferred configuration of the NMe group is equatorial (NOEs between H17 and H12, H13 prove this), and the minor configuration is axial (NOEs between H17 and H10, H15 are seen). The reversible rearrangement was confirmed by NOESY experiments, which showed exchange peaks between atropine signals and this rearrangement product (data not shown).
Conclusions
The proposed PSYCHE-iWG pure shift method has great potential utility in the analysis of complex samples with strong solvent signals. A key benefit is the ability to retain signals undergoing chemical exchange with the solvent such as NH signals in proteins and peptides. The integration of WATERGATE directly into the pure shift pulse sequence enables the use of short recovery delays, boosting the SNR of the resultant spectrum compared with methods using presaturation.
Such sequences have further potential application in multidimensional pure shift experiments, such as TOCSY-PSYCHE,32 which would enable acquisition of ultrahigh-resolution correlation experiments in nondeuterated solvents. Furthermore, as PSYCHE-iWG provides chemical shift information for each multiplet, ultraselective 1D correlation NMR experiments (such as the GEMSTONE family of experiments)33−36 can be used as fast alternatives to 2D experiments for characterization.
Acknowledgments
This work was funded by an iCASE award from Johnson Matthey and by the Engineering and Physical Sciences Research Council (grant numbers EP/V519613/1 2509660, EP/V007580/1, and EP/R018790/1), by the University of Manchester (Dame Kathleen Ollerenshaw Fellowship to LC), and the Consejería de Educación, Juventud y Deporte, Comunidad de Madrid (grant number 2022-T1/BMD-24030 to LC). For the purpose of open access, the authors have applied a Creative Commons Attribution (CC-BY) licence to any Author-Accepted Manuscript version arising. The authors thank Drs. G. Dal Poggetto, A. DiCaprio, R. D. Cohen, and M. Reibarkh for sharing a preprint (DOI: 10.26434/chemrxiv-2023-cfpdp) describing related work, carried out independently. The authors thank Iris Pereira for preliminary work conducted during her master’s degree and Dr. Jonathan Farjon for providing the W5n-TSE-PSYCHE pulse program code.
Supporting Information Available
The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acs.analchem.3c05379.
Pulse program code; experimental details and further sample analysis (PDF)
Author Contributions
The manuscript was written through contributions from all authors. All authors have given approval to the final version of the manuscript. L.C. and J.P.B. contributed to funding acquisition. L.C., R.W.A., and E.L.G. contributed to conception. E.L.G. contributed to data curation. All authors contributed to data analysis and to the development of the methodology during project meetings.
The authors declare no competing financial interest.
Supplementary Material
References
- Pilaniya K.; Chandrawanshi H. K.; Pilaniya U.; Manchandani P.; Jain P.; Singh N. Recent Trends in the Impurity Profile of Pharmaceuticals. J. Adv. Pharm. Technol. Res. 2010, 1 (3), 302–310. 10.4103/0110-5558.72422. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Bellissent-Funel M. C.; Hassanali A.; Havenith M.; Henchman R.; Pohl P.; Sterpone F.; Van Der Spoel D.; Xu Y.; Garcia A. E. Water Determines the Structure and Dynamics of Proteins. Chem. Rev. 2016, 116 (13), 7673–7697. 10.1021/acs.chemrev.5b00664. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Adams R. W. Pure Shift NMR Spectroscopy. EMagRes 2007, 3 (4), 295–309. 10.1002/9780470034590.emrstm1362. [DOI] [Google Scholar]
- Zangger K. Pure Shift NMR. Prog. Nucl. Magn. Reson. Spectrosc. 2015, 86–87, 1–20. 10.1016/j.pnmrs.2015.02.002. [DOI] [PubMed] [Google Scholar]
- Castañar L.; Parella T. Broadband 1H Homodecoupled NMR Experiments: Recent Developments, Methods and Applications. Magn. Reson. Chem. 2015, 53 (6), 399–426. 10.1002/mrc.4238. [DOI] [PubMed] [Google Scholar]
- Castañar L. Pure Shift 1H NMR: What Is Next?. Magn. Reson. Chem. 2017, 55 (1), 47–53. 10.1002/mrc.4545. [DOI] [PubMed] [Google Scholar]
- Castañar L.; Nolis P.; Virgili A.; Parella T. Full Sensitivity and Enhanced Resolution in Homodecoupled Band-Selective NMR Experiments. Eur. J. Chem. 2013, 19 (51), 17283–17286. 10.1002/chem.201303235. [DOI] [PubMed] [Google Scholar]
- Ying J.; Roche J.; Bax A. Homonuclear Decoupling for Enhancing Resolution and Sensitivity in NOE and RDC Measurements of Peptides and Proteins. J. Magn. Reson. 2014, 241 (1), 97–102. 10.1016/j.jmr.2013.11.006. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Zangger K.; Sterk H. Homonuclear Broadband-Decoupled NMR Spectra. J. Magn. Reson. 1997, 124 (2), 486–489. 10.1006/jmre.1996.1063. [DOI] [Google Scholar]
- Garbow J. R.; Weitekamp D. P.; Pines A. Bilinear Rotation Decoupling of Homonuclear Scalar Interactions. Chem. Phys. Lett. 1982, 93 (5), 504–509. 10.1016/0009-2614(82)83229-6. [DOI] [Google Scholar]
- Foroozandeh M.; Adams R. W.; Meharry N. J.; Jeannerat D.; Nilsson M.; Morris G. A. Ultrahigh-Resolution NMR Spectroscopy. Angew. Chem., Int. Ed. 2014, 53 (27), 6990–6992. 10.1002/anie.201404111. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Foroozandeh M.; Morris G. A.; Nilsson M. PSYCHE Pure Shift NMR Spectroscopy. Eur. J. Chem. 2018, 24 (53), 13988–14000. 10.1002/chem.201800524. [DOI] [PubMed] [Google Scholar]
- Abragam A.The Principles of Nuclear Magnetism; Oxford Univ. Press, 1961; p 73. [Google Scholar]
- Bax A.; Sklenar V.; Clore G. M.; Gronenborn A. M. Water Suppression in Two-Dimensional Spin-Locked Nuclear Magnetic Resonance Experiments Using a Novel Phase-Cycling Procedure. J. Am. Chem. Soc. 1987, 109 (21), 6511–6513. 10.1021/ja00255a047. [DOI] [Google Scholar]
- Guéron M.; Plateau P.; Decorps M. Solvent Signal Suppression in NMR. Prog. Nucl. Magn. Reson. Spectrosc. 1991, 23 (2), 135–209. 10.1016/0079-6565(91)80007-O. [DOI] [Google Scholar]
- Mao X. A.; Ye C. H. Understanding Radiation Damping in a Simple Way. Concepts Magn. Reson.: Educ. J. 1997, 9 (3), 173–187. . [DOI] [Google Scholar]
- Hoult D. I. Solvent Peak Saturation with Single Phase and Quadrature Fourier Transformation. J. Magn. Reson. (1969) 1976, 21 (2), 337–347. 10.1016/0022-2364(76)90081-0. [DOI] [Google Scholar]
- Nicholson J. K.; Foxall P. J. D.; Spraul M.; Farrant R. D.; Lindon J. C. 750 MHz 1H and 1H-13C NMR Spectroscopy of Human Blood Plasma. Anal. Chem. 1995, 67 (5), 793–811. 10.1021/ac00101a004. [DOI] [PubMed] [Google Scholar]
- Bertho G.; Lordello L.; Chen X.; Lucas-Torres C.; Oumezziane I. E.; Caradeuc C.; Baudin M.; Nuan-Aliman S.; Thieblemont C.; Baud V.; Giraud N. Ultrahigh-Resolution NMR with Water Signal Suppression for a Deeper Understanding of the Action of Antimetabolic Drugs on Diffuse Large B-Cell Lymphoma. J. Proteome Res. 2022, 21 (4), 1041–1051. 10.1021/acs.jproteome.1c00914. [DOI] [PubMed] [Google Scholar]
- Hwang T. L.; Shaka A. J. Water Suppression That Works. Excitation Sculpting Using Arbitrary Wave-Forms and Pulsed-Field Gradients. J. Magn. Reson., Ser. A 1995, 112 (2), 275–279. 10.1006/jmra.1995.1047. [DOI] [Google Scholar]
- Piotto M.; Saudek V.; Sklenář V. Gradient-Tailored Excitation for Single-Quantum NMR Spectroscopy of Aqueous Solutions. J. Biomol. NMR 1992, 2 (6), 661–665. 10.1007/BF02192855. [DOI] [PubMed] [Google Scholar]
- Liu M.; Mao X. A.; Ye C.; Huang H.; Nicholson J. K.; Lindon J. C. Improved Watergate Pulse Sequences for Solvent Suppression in NMR Spectroscopy. J. Magn. Reson. 1998, 132 (1), 125–129. 10.1006/jmre.1998.1405. [DOI] [Google Scholar]
- Kunjir S.; Rodriguez-Zubiri M.; Coeffard V.; Felpin F.-X.; Giraudeau P.; Farjon J. Merging Gradient-Based Methods to Improve Benchtop NMR Spectroscopy: A New Tool for Flow Reaction Optimization. ChemPhysChem 2020, 21 (20), 2311–2319. 10.1002/cphc.202000573. [DOI] [PubMed] [Google Scholar]
- Foroozandeh M.; Adams R. W.; Kiraly P.; Nilsson M.; Morris G. A. Measuring Couplings in Crowded NMR Spectra: Pure Shift NMR with Multiplet Analysis. Chem. Commun. 2015, 51 (84), 15410–15413. 10.1039/C5CC06293D. [DOI] [PubMed] [Google Scholar]
- Adams R. W.; Holroyd C. M.; Aguilar J. A.; Nilsson M.; Morris G. A. Perfecting” WATERGATE: Clean Proton NMR Spectra from Aqueous Solution. Chem. Commun. 2013, 49 (4), 358–360. 10.1039/C2CC37579F. [DOI] [PubMed] [Google Scholar]
- Stabler S. P. Clinical Practice. Vitamin B12 Deficiency. N. Engl. J. Med. 2013, 368 (2), 149–160. 10.1056/NEJMcp1113996. [DOI] [PubMed] [Google Scholar]
- Smith A. D.; Warren M. J.; Refsum H. Vitamin B12. Adv. Food Nutr. Res. 2018, 83, 215–279. 10.1016/bs.afnr.2017.11.005. [DOI] [PubMed] [Google Scholar]
- Ernst R. R.; Anderson W. A. Application of Fourier Transform Spectroscopy to Magnetic Resonance. Rev. Sci. Instrum. 1966, 37, 93–102. 10.1063/1.1719961. [DOI] [Google Scholar]
- North R. V.; Kelly M. E. A Review of the Uses and Adverse Effects of Topical Administration of Atropine. Ophthalmic Physiol. Opt. 1987, 7 (2), 109–114. 10.1111/j.1475-1313.1987.tb01004.x. [DOI] [PubMed] [Google Scholar]
- Wu P. C.; Chuang M. N.; Choi J.; Chen H.; Wu G.; Ohno-Matsui K.; Jonas J. B.; Cheung C. M. G. Update in Myopia and Treatment Strategy of Atropine Use in Myopia Control. Eye 2019, 33 (1), 3–13. 10.1038/s41433-018-0139-7. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Shen S.; Yao J.; Shi Y. Quantitative Proton Nuclear Magnetic Resonance for the Structural and Quantitative Analysis of Atropine Sulfate. J. Pharm. Biomed. Anal. 2014, 89, 118–121. 10.1016/j.jpba.2013.10.036. [DOI] [PubMed] [Google Scholar]
- Foroozandeh M.; Adams R. W.; Nilsson M.; Morris G. A. Ultrahigh-Resolution Total Correlation NMR Spectroscopy. J. Am. Chem. Soc. 2014, 136 (34), 11867–11869. 10.1021/ja507201t. [DOI] [PubMed] [Google Scholar]
- Kiraly P.; Nilsson M.; Morris G. A.; Adams R. W. Single-Scan Ultra-Selective 1D Total Correlation Spectroscopy. Chem. Commun. 2021, 57 (19), 2368–2371. 10.1039/D0CC08033K. [DOI] [PubMed] [Google Scholar]
- Kiraly P.; Kern N.; Plesniak M. P.; Nilsson M.; Procter D. J.; Morris G. A.; Adams R. W. Single-Scan Selective Excitation of Individual NMR Signals in Overlapping Multiplets. Angew. Chem., Int. Ed. 2021, 60 (2), 666–669. 10.1002/anie.202011642. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Taylor D. A.; Kiraly P.; Bowyer P.; Nilsson M.; Castañar L.; Morris G. A.; Adams R. W. Ultra-Selective 1D Clean in-Phase Correlation Spectroscopy. Chem. Commun. 2023, 59 (44), 6734–6737. 10.1039/D3CC01333B. [DOI] [PubMed] [Google Scholar]
- Gates E. L.; Smith M. J.; Bradley J. P.; Johnson M.; Widmalm G.; Nilsson M.; Morris G. A.; Adams R. W.; Castañar L. Ultra-Selective, Ultra-Clean 1D Rotating-Frame Overhauser Effect Spectroscopy. Chem. Commun. 2023, 59 (39), 5854–5857. 10.1039/D3CC00550J. [DOI] [PubMed] [Google Scholar]
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.





