Next Article in Journal
Identification of Alternative Splicing in Proteomes of Human Melanoma Cell Lines without RNA Sequencing Data
Next Article in Special Issue
A Review of Applications of Solid-State Nuclear Magnetic Resonance (ssNMR) for the Analysis of Cyclodextrin-Including Systems
Previous Article in Journal
Microbiome Alterations in Alcohol Use Disorder and Alcoholic Liver Disease
Previous Article in Special Issue
Self-Diffusion in Confined Water: A Comparison between the Dynamics of Supercooled Water in Hydrophobic Carbon Nanotubes and Hydrophilic Porous Silica
 
 
Search for Articles:
Title / Keyword
Author / Affiliation / Email
Journal
Article Type
 
 
Advanced Search
 
Section
Special Issue
Volume
Issue
Number
Page
 
Journals
IJMS
Volume 24
Issue 3
10.3390/ijms24032465
ijms-logo
Submit to this Journal Review for this Journal Propose a Special Issue
► Article Menu

Article Menu

share Share announcement Help format_quote Cite question_answer Discuss in SciProfiles thumb_up
...
Endorse textsms
...
Comment
first_page
settings
Order Article Reprints
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Communication

SABRE Hyperpolarization with up to 200 bar Parahydrogen in Standard and Quickly Removable Solvents

by
Anton Duchowny
1,
Johannes Denninger
1,
Lars Lohmann
1,
Thomas Theis
2,
Sören Lehmkuhl
3 and
Alina Adams
1,*
1
Institut für Technische und Makromolekulare Chemie, RWTH Aachen University, 52074 Aachen, Germany
2
Department of Chemistry, North Carolina State University, Raleigh, NC 27695, USA
3
Institute of Microstructure Technology, Karlsruhe Institute of Technology, 76344 Eggenstein-Leopoldshafen, Germany
*
Author to whom correspondence should be addressed.
Int. J. Mol. Sci. 2023, 24(3), 2465; https://doi.org/10.3390/ijms24032465
Submission received: 26 December 2022 / Revised: 20 January 2023 / Accepted: 24 January 2023 / Published: 27 January 2023
(This article belongs to the Special Issue Modern NMR Characterization of Materials)
Browse Figures
Versions Notes

Abstract

:
Parahydrogen (p-H2)-based techniques are known to drastically enhance NMR signals but are usually limited by p-H2 supply. This work reports p-H2-based SABRE hyperpolarization at p-H2 pressures of hundreds of bar, far beyond the typical ten bar currently reported in the literature. A recently designed high-pressure setup was utilized to compress p-H2 gas up to 200 bar. The measurements were conducted using a sapphire high-pressure NMR tube and a 43 MHz benchtop NMR spectrometer. In standard methanol solutions, it could be shown that the signal intensities increased with pressure until they eventually reached a plateau. A polarization of about 2%, equal to a molar polarization of 1.2 mmol L−1, could be achieved for the sample with the highest substrate concentration. While the signal plateaued, the H2 solubility increased linearly with pressure from 1 to 200 bar, indicating that p-H2 availability is not the limiting factor in signal enhancement beyond a certain pressure, depending on sample composition. Furthermore, the possibility of using liquefied ethane and compressed CO2 as removable solvents for hyperpolarization was demonstrated. The use of high pressures together with quickly removable organic/non-organic solvents represents an important breakthrough in the field of hyperpolarization, advancing SABRE as a promising tool for materials science, biophysics, and molecular imaging.

1. Introduction

Although nuclear magnetic resonance (NMR) techniques are among the most important analytical methods for obtaining detailed information about materials on the molecular level, they suffer from inherently low sensitivity. Even when examining protons, which are ubiquitously present in organic molecules, only a tiny fraction effectively contributes to the detectable signals under thermal equilibrium conditions in standard NMR spectrometers. This low sensitivity can lead to lengthy measurement times. Stronger magnetic fields incrementally increase the spin polarization but are associated with exponentially increasing costs. Even at magnetic fields of ~24 T in modern GHz NMR spectrometers, proton spin polarization is only on the order of 10−4. Alternatively, polarizations approaching unity, associated with dramatic signal enhancements, can be obtained with hyperpolarization techniques. Important examples include dynamic nuclear polarization (DNP) [1,2] and para-hydrogen (p-H2) induced polarization (PHIP), including signal amplification by reversible exchange (SABRE) [3,4,5]. SABRE is based on the reversible association of p-H2 and a substrate with an iridium catalyst [6] (Figure 1(6)) and is currently a method of high interest as it provides a simple, low-cost route for signal enhancement. In addition, the enhanced NMR signals can be regenerated easily, for example, by simply re-shaking the samples or by resupplying new p-H2 via bubbling or with the help of continuous flow reactors [7,8,9,10].
Many factors influence the achievable SABRE hyperpolarization. They include exchange rates at the catalyst [11,12,13,14,15,16,17], the p-H2 supply (i.e., flow, bubbling, and shaking), the solubility [12,14,16,18,19,20], and the concentration [5,11,12,15,21,22] of the catalyst, hydrogen, and substrate in a chosen solvent. Further important parameters include the presence of co-substrates or additives [12,23,24,25] and the exact control of the polarization transfer field [11,12,13,14,15,17,26,27,28,29]. Another critical parameter that may often limit the hyperpolarization is the p-H2 pressure applied to the sample [11,12,13,14,26,28,30,31,32]. The often-encountered linear dependence between applied pressure and signal enhancement suggests that further signal enhancements are possible with increasing pressures. Yet, despite the development of dedicated high-pressure p-H2 generators [33,34,35,36,37], so far, SABRE hyperpolarization experiments have been performed below 10 bar of pressure. This limitation is probably due to the lack of a suitable setup for p-H2 supply at high pressures and a lack of low-cost, commercially available high-pressure NMR tubes. An easy-to-replicate and inexpensive high-pressure tube design was reported recently [38]. Moreover, a recent report has described a low-cost and versatile high-pressure setup employing a high-pressure sapphire tube, allowing spectroscopic analyses of samples pressurized up to 200 bar with a benchtop NMR spectrometer. It has been applied successfully to study compressed gases as well as gas–liquid and gas–solid interactions [39,40].
This work introduces the aforementioned high-pressure setup for p-H2 experiments as a simple way to overcome the current pressure limitations. The experimental setup is depicted in Figure 1, with more details provided in Section 4. Instead of exposing the sample to the p-H2 gas directly from the standard p-H2 generator, Figure 1(1), the p-H2 gas is redirected into a piston cylinder, Figure 1(2), which can also serve as a mixing reservoir. This detour allows for quick and easy pressure adjustments, independent of the maximum 7–10 bar output pressure of the p-H2 generator. The pressurized p-H2 alone, or in a mixture with another gas, is loaded into the high-pressure sapphire tube, Figure 1(3), containing the evacuated sample (substrate, catalyst, and possibly solvent). The loaded sapphire tube is physically connected to the high-pressure cylinder during the entire hyperpolarization experiment. First, the tube is shaken for 10 s, then it is inserted into a sinusoidal electromagnet, Figure 1(4), set to produce a magnetic field of 69 G for another 10 s, finally followed by insertion into the benchtop NMR equipment, Figure 1(5), for immediate measurement.
Three classes of experiments were performed using this setup. First, the ingress of hydrogen gas in deuterated methanol up to 200 bar is monitored to identify a possible solubility limit. In our study, a linear relationship without a solubility limitation of hydrogen gas was observed. Secondly, the first pyrazine SABRE hyperpolarization results with up to 200 bar p-H2 pressure measured in a 43 MHz benchtop NMR spectrometer are reported. Finally, since the high-pressure setup contains a mixing reservoir, alternative solvents for the substrate/catalyst were tested as a proof-of-concept. For instance, ethane liquefaction in an ethane/p-H2 mixture was exploited, similar to a different study [41]. However, in [41], propane was hyperpolarized by hydrogenating propene, whereas here, ethane merely serves as the carrier substance. Similarly, a CO2/p-H2 mixture was brought onto a solid catalyst–pyrazine mix free of solvent. In this case, the compressed CO2 liquefied the sample and dissolved p-H2, leading to signal enhancement.
The presented results open new avenues for low-cost and versatile high-pressure hyperpolarization and help to understand the effect of p-H2 pressure on signal enhancement, especially with respect to achieving high polarization at high substrate concentrations, i.e., high molar polarization. This work also provides a path to easily remove organic solvents, resulting in more biocompatible injectables better suited for biomolecular imaging and medical research. Removal of organic solvents is crucial before SABRE hyperpolarization can be efficiently deployed in vivo. The introduced methodology is also expected to play a significant role in analyzing trace substances and complex mixtures and in material characterization [12,22]. Moreover, the structure and dynamics of biopolymers may be studied, which are known to be affected by the application of pressure [42,43,44].

2. Results

2.1. Dissolution of Hydrogen in Deuterated Methanol

The dissolution of H2 gas in deuterated methanol (d-methanol, CD3OD) between 1 and 200 bar was examined to prove the absence of a solubility limit in the analyzed pressure range. A linear dependence can be seen for increasing and decreasing the H2 pressure, as demonstrated in Figure 2. In the investigated pressure range, no solubility limit was detected. Hence, increasing the H2 pressure results in an increased H2 concentration in the sample solution. Although deuterated methanol was utilized, the mole fraction of dissolved hydrogen could not be precisely quantified due to peak overlap. Nevertheless, the observed linear trend agrees with the published literature data [45,46,47,48]. The spectra were acquired a few seconds after pressure application, resembling the hyperpolarization experiments. Therefore, no temporal effects of H2 mixing or diffusion into the solvent need to be considered for data evaluation.

2.2. High-Pressure SABRE Hyperpolarization of Pyrazine in d-Methanol

Pyrazine, with its four chemically and magnetically equivalent protons, gives a single line in the proton NMR spectrum; thus, pyrazine was chosen as a model substrate to investigate the effect of pressure at different substrate concentrations on the SABRE signal enhancement. The effect of increasing the p-H2 pressure on the molar signal enhancement (= enhancement × concentration, directly proportional to total signal) of this substrate is depicted in Figure 3a. First, a sample with 60 mmol L−1 pyrazine in d-methanol was investigated. The catalyst/substrate ratio was 1/20 and this ratio was kept constant for all investigated samples. While a quasi-linear signal increase was observed at lower pressures, as already demonstrated by other studies [48,49], this is not the case beyond 10 bar. Instead, the signal gains level off. Nonetheless, a 3-fold enhancement was achieved by increasing the pressure from 10 to 200 bar. Moreover, for this 60 mmol L−1 sample, we achieved an enhancement of around 6 × 103 with a corresponding molar enhancement of 3.6 × 105 mmol L−1 (6 × 103 × 60 mmol L−1), which is equal to a polarization of about 2%. This corresponds to a molar polarization of 1.2 mmol L−1. However, we note that experimental reproducibility was associated with relatively large error bars, as depicted in Figure 3a. Utilizing an automated transfer shuttle from the polarization transfer magnet to the NMR magnet for detection would significantly improve the experimental reproducibility [7].
While a similar non-linear behavior with pressure was also detected for the 17.5 mmol L−1 sample, a constant signal enhancement was obtained with the lowest concentrated sample (4.8 mmol L−1) above 20 bar. A similar finding was reported in PHIP experiments with decreasing substrate concentration [22]. This finding is consistent with theoretical predictions [49], where at lower substrate concentrations, the achievable enhancements and hyperpolarization levels become limited by factors other than the p-H2 concentration. Hence, lower p-H2 pressures would be sufficient to conduct experiments with low substrate concentrations.
Furthermore, the effect of increasing p-H2 pressure on the hydride signals of the Ir catalyst was investigated. As exemplarily shown for the 4.8 mmol L−1 sample in d-methanol in Figure 3b, an increasing hydride signal was observed with increasing pressure, even though the pyrazine signal enhancement remained constant. This outcome illustrates that p-H2 was successfully brought into the sample and it is not the limiting factor for higher enhancements. Similar behavior was observed for the hydrides of the other two concentrations, as illustrated for the 17.5 mmol L−1 sample in Figure S1 of the Supplementary Information. Figure S2 shows that with increasing pressure, there is continued increase in the hydride signals in all samples. Moreover, the hydride spectra show no signs of a structural change in the catalytic complex with increasing p-H2 pressure. Thus, it can be assumed that the hyperpolarization mechanism is mostly independent of pressure in the sense that the active hyperpolarization transfer species does not change.
In summary, the results further substantiate that: (a) p-H2 can be brought into the solution efficiently at high pressures, (b) the polarization transfer mechanism seems to stay the same at elevated pressures, and (c) the observed enhancements at low pyrazine concentrations level off and are not limited by p-H2 availability at elevated pressures. However, higher p-H2 pressures generate a significant boost in signal enhancement for higher substrate concentrations (d). Such an enhancement boost is important, for example, when aiming for a maximum molar polarization for hyperpolarized MRI contrast agents.

2.3. High-Pressure SABRE Hyperpolarization with Quickly Removable Solvents

Methanol is a solvent not suited for medical applications because of its toxicity. However, it is typically the solvent of choice for SABRE because of its reduced hydrogen solubility and non-optimal exchange kinetics in water. Here, we provide proof-of-concept experiments that replace methanol with removable gaseous solvents that are only liquefied at sufficiently high pressures.
In the first experiment, the liquefaction of ethane as a SABRE solvent was investigated. For this purpose, a 50/50 mixture comprising ethane and p-H2 at 12 bar was produced in the piston cylinder of the high-pressure setup. Subsequently, the mixture was compressed to 200 bar total pressure. Up to ~40 bar partial pressure at ambient temperature, ethane is gaseous and mixes with the p-H2 gas. Once the partial pressure exceeds this value, ethane liquefies, thus obtaining a liquid p-H2/ethane system that can be brought into the sample. Upon decreasing the pressure, both p-H2 and ethane can evaporate. Although this approach is promising in theory, it was found that liquefied ethane did not dissolve the catalyst nor pyrazine, and hence, pyridine as a substrate was chosen instead and the same catalyst was supplied in a d-methanol solution (catalyst/pyridine 1/20 molar ratio).
The feasibility of this approach was confirmed by the experimental data showing hyperpolarized pyridine peaks, illustrated in Figure 4a. Comparing the peak’s signal-to-noise levels before and after hyperpolarization yields an enhancement factor of at least 78. This enhancement factor is a lower bound of the actual value because the hyperpolarized sample is partially carried out of the spectrometer’s sensitive volume upon releasing the gas. Accordingly, exact quantification was not possible in this first feasibility study, yet with certainty, we can maintain that large enhancements in excess of seventy-eight were achieved.
In a second proof-of-concept experiment, CO2 was used to avoid methanol completely. CO2 is considered a green solvent with great potential to replace organic solvents because it is inexpensive, non-toxic, environmentally more acceptable, and non-flammable [50,51]. It is a suitable solvent for pyrazine at moderate temperatures and pressures, even when not supercritical [52]. The required conditions to dissolve pyrazine in CO2 at room temperature can easily be achieved when operating the presented experimental setup at higher pressures. As in the previous experiment, gaseous CO2 was mixed with p-H2 in the piston cylinder, compressed to 200 bar total pressure, and filled into the NMR tube. This time, the sample comprised only the solid catalyst and pyrazine (1:20 molar ratio) without any d-methanol (Figure S3). The compressed CO2 liquefied the solids (Figure S4) and transferred the p-H2 to the catalyst and analyte, as demonstrated by the hyperpolarized signal shown in Figure 4b. However, only a small droplet was formed in the sapphire tube that partially filled the sensitive volume. The unevenly filled sensitive volume led to a broad linewidth and lower signal-to-noise ratio. The observed signal enhancement, in this case, was around twelve compared to the spectrum acquired at thermal equilibrium (pressurized and liquefied sample in CO2).
Additionally, the hydrides between −20 and −30 ppm were strongly enhanced in the hyperpolarized spectrum and have a similar signal strength to the hydrides from samples dissolved in d-methanol (Figure S5). However, the spectral signatures differ in appearance due to the formation of different complexes [53,54]. After releasing the gas, the liquefied chemicals recrystallized again (Figure S3), and no signal could be detected. This is due to the solid-state dipolar broadening in the crystalline solid, which could not be removed with the used liquid probe head. The observation of a comparable hydride signal strength in CO2 and d-methanol, yet much lower pyrazine enhancement, indicates that the polarization transfer to the substrate is inefficient in CO2. Possible reasons include the different polarity of CO2 compared to methanol, possible conformation changes of the catalyst and/or substrate in the presence of CO2, and a diminished lifetime of the catalytic SABRE complex, not allowing enough time for the polarization transfer. Yet, given the strong hydride peaks, strong binding and insufficient exchange of pyrazine at the catalytic complex is the most likely explanation. By resolving some of these possible limitations, it can be expected that significant further signal enhancement will become possible by fine-tuning the experimental conditions.

3. Materials and Methods

The high-pressure setup used in this work has been described in the literature previously [40]. In brief, gas was filled into a piston cylinder with two physically separated compartments. Turning a 3-way valve redirected the sample gas to the high-pressure NMR tube containing the sample solution. By applying pressure to the other compartment of the piston cylinder, a movable piston compressed the sample gas until the pressure was equilibrated. Additionally, the setup was equipped with several safety features. A safety valve releases gas when a pressure above 206 bar is reached and is attached to the high-pressure line connecting to the piston-cylinder, since this line will always be pressurized. Pressure ratings for all other parts are beyond 400 bar. Furthermore, check valves were installed after the gas inlet ports, preventing highly pressurized gas from flowing back into the gas bottle.
The employed NMR tube was made of sapphire, capable of withstanding high pressures. However, it is brittle and susceptible to lateral forces from bending or impacts. Hence, special care must be taken when performing the experiments, especially while shaking and inserting the tube into the polarization transfer or NMR magnet. A spacer made of foam was attached below the high-pressure tube attachment to soften the impact of inserting the pressurized tube into the NMR magnet. This spacer also ensured that the sample was always in the same region of the sensitive volume. Likewise, the electromagnet had a foam insert, which guaranteed that samples were always exposed to the same magnetic field and reduced the chance of hitting the tube. Employing an automated sample transferring shuttle, such as in Ref. [7], could greatly improve the safety aspect of the high-pressure experimental setup.
A p-H2 generator (Bruker BioSpin GmbH, Karlsruhe, Germany) was attached at the sample gas inlet port, filling the piston-cylinder with up to 7 bar of p-H2 (Figure 1). The proton NMR experiments were recorded using a 1 T 1H-frequency benchtop spectrometer (Magritek GmbH, Aachen, Germany) working at a proton frequency of 43 MHz. For the hyperpolarization experiments conducted below 8 bar, the generator was connected directly to the high-pressure tube.
For the experiments including gaseous solvents, p-H2 and ethane or CO2 must be filled successively into the piston cylinder. After filling p-H2, the piston cylinder’s valve was closed and the p-H2 generator was exchanged with the ethane or CO2 gas bottle. After flushing and evacuating the high-pressure lines multiple times with ethane or CO2, the second gas component was filled into the piston cylinder until the desired mixing ratio was reached. From this point on, the experimental procedure is the same as above.
Pyrazine and pyridine were purchased from Sigma-Aldrich (Merck KGaA, Darmstadt, Germany) and methanol-d4 from Eurisotop (Cambridge Isotope Laboratories Inc., Tewksbury, MA, USA). These chemicals were dried and degassed thoroughly before usage. The iridium-based catalyst was synthesized in-house according to Ref. [26], stored under an argon atmosphere, and shielded from sunlight. Samples with 60, 17.5, and 4.8 mmol L−1 pyrazine were prepared with a 1/20 catalyst/pyrazine molar ratio. The same molar ratio of 1/20 was also used for the catalyst/pyridine sample. H2 5.0 (99.999% purity), CO2 4.5 (99.995% purity), and ethane 3.5 (99.95% purity) were purchased from Westfalen AG (Münster, Germany) and used without further purification.

4. Conclusions

SABRE hyperpolarization experiments at pressures up to 200 bar are reported. A simple, low-cost, and versatile high-pressure setup was attached to a standard commercially available p-H2 generator to exceed its maximum achievable pressure. The proposed experimental setup can be a viable alternative to the current state-of-the-art setups for generating pressurized p-H2.
The applicability of this novel approach was demonstrated by hyperpolarizing pyrazine with an iridium-based catalyst dissolved in d-methanol in a high-pressure NMR tube. The presented results demonstrated that pressures beyond the current maximum of ~10 bar allow further signal enhancement, albeit not following the quasi-linear trend observed at low pressures. It was shown that the higher the substrate concentration, the higher the molar polarization. In contrast to the substrate signals, the hydride signal intensity increased steadily with pressure, which shows that this polarization can potentially be better harnessed by changing other experimental parameters, such as temperature and sample composition.
Furthermore, the versatile design of the high-pressure setup allowed applying ethane and CO2 as alternative and easily removable solvents in the hyperpolarization experiments. Highly pressurized CO2 liquefied the solid catalyst and substrate, in which p-H2 subsequently dissolved, and thus a signal enhancement could be detected. In contrast, ethane could neither dissolve the catalyst nor pyrazine. However, the feasibility of exploiting the ethane liquefaction at high pressure was demonstrated with pyridine and might be useful in different hyperpolarization substrates and settings. Eliminating standard SABRE organic solvents such as methanol in hyperpolarization techniques is a prerequisite for molecular medical research. Even if the practical approach to high-pressure SABRE hyperpolarization needs to be fine-tuned, this work highlights that it is possible to overcome current experimental limitations.

Supplementary Materials

The corresponding supporting information can be downloaded at: https://www.mdpi.com/article/10.3390/ijms24032465/s1.

Author Contributions

A.D.—Conceptualization, investigation, data curation, writing—original draft. J.D.—investigation, software, data curation, writing—review and editing. L.L.—investigation, methodology, writing—review and editing. T.T.—formal analysis, writing—review and editing. S.L.—conceptualization, investigation, data curation, formal analysis, validation, writing—review and editing. A.A.—conceptualization, methodology, supervision, writing—original draft, writing—review and editing, project administration, resources. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not appliable.

Informed Consent Statement

Not appliable.

Data Availability Statement

Not appliable.

Acknowledgments

We thank our colleague Stefan Appelt for lending the sinusoidal electromagnet to us and the many fruitful discussions. Special thanks also go to Jürgen Kolz from Magritek for his support with all issues related to the benchtop NMR equipment.

Conflicts of Interest

Thomas Theis holds shares in Vizma Life Sciences LLC (VLS) and currently acts as president of VLS. VLS is developing products related to the research being reported. The terms of this arrangement have been reviewed and approved by NC State University in accordance with its policy on objectivity in research.

References

  1. Kemsley, J. Sensitizing NMR. Chem. Eng. News Arch. 2008, 86, 12–15. [Google Scholar] [CrossRef]
  2. Abraham, M.; McCausland, M.A.H.; Robinson, F.N.H. Dynamic Nuclear Polarization. Phys. Rev. Lett. 1959, 2, 449–451. [Google Scholar] [CrossRef]
  3. Barskiy, D.A.; Kovtunov, K.V.; Koptyug, I.V.; He, P.; Groome, K.A.; Best, Q.A.; Shi, F.; Goodson, B.M.; Shchepin, R.V.; Truong, M.L.; et al. In situ and ex situ low-field NMR spectroscopy and MRI endowed by SABRE hyperpolarization. ChemPhysChem 2014, 15, 4100–4107. [Google Scholar] [CrossRef] [Green Version]
  4. Richardson, P.M.; Parrott, A.J.; Semenova, O.; Nordon, A.; Duckett, S.B.; Halse, M.E. SABRE hyperpolarization enables high-sensitivity 1H and 13C benchtop NMR spectroscopy. Analyst 2018, 143, 3442–3450. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  5. Eshuis, N.; Hermkens, N.; van Weerdenburg, B.J.A.; Feiters, M.C.; Rutjes, F.P.J.T.; Wijmenga, S.S.; Tessari, M. Toward nanomolar detection by NMR through SABRE hyperpolarization. J. Am. Chem. Soc. 2014, 136, 2695–2698. [Google Scholar] [CrossRef]
  6. Adams, R.W.; Aguilar, J.A.; Atkinson, K.D.; Cowley, M.J.; Elliott, P.I.P.; Duckett, S.B.; Green, G.G.R.; Khazal, I.G.; López-Serrano, J.; Williamson, D.C. Reversible interactions with para-hydrogen enhance NMR sensitivity by polarization transfer. Science 2009, 323, 1708–1711. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  7. TomHon, P.; Akeroyd, E.; Lehmkuhl, S.; Chekmenev, E.Y.; Theis, T. Automated pneumatic shuttle for magnetic field cycling and parahydrogen hyperpolarized multidimensional NMR. J. Magn. Reson. 2020, 312, 106700. [Google Scholar] [CrossRef]
  8. Lehmkuhl, S.; Wiese, M.; Schubert, L.; Held, M.; Küppers, M.; Wessling, M.; Blümich, B. Continuous hyperpolarization with parahydrogen in a membrane reactor. J. Magn. Reson. 2018, 291, 8–13. [Google Scholar] [CrossRef] [PubMed]
  9. Bordonali, L.; Nordin, N.; Fuhrer, E.; MacKinnon, N.; Korvink, J.G. Parahydrogen based NMR hyperpolarisation goes micro: An alveolus for small molecule chemosensing. Lab Chip 2019, 19, 503–512. [Google Scholar] [CrossRef] [Green Version]
  10. TomHon, P.M.; Han, S.; Lehmkuhl, S.; Appelt, S.; Chekmenev, E.Y.; Abolhasani, M.; Theis, T. A Versatile Compact Parahydrogen Membrane Reactor. Chemphyschem 2021, 22, 2526–2534. [Google Scholar] [CrossRef]
  11. Truong, M.L.; Theis, T.; Coffey, A.M.; Shchepin, R.V.; Waddell, K.W.; Shi, F.; Goodson, B.M.; Warren, W.S.; Chekmenev, E.Y. 15N Hyperpolarization by Reversible Exchange Using SABRE-SHEATH. J. Phys. Chem. C 2015, 119, 8786–8797. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  12. Lehmkuhl, S.; Emondts, M.; Schubert, L.; Spannring, P.; Klankermayer, J.; Blümich, B.; Schleker, P.P.M. Hyperpolarizing Water with Parahydrogen. ChemPhysChem 2017, 18, 2426–2429. [Google Scholar] [CrossRef] [PubMed]
  13. Green, R.A.; Adams, R.W.; Duckett, S.B.; Mewis, R.E.; Williamson, D.C.; Green, G.G.R. The theory and practice of hyperpolarization in magnetic resonance using parahydrogen. Prog. Nucl. Magn. Reson. Spectrosc. 2012, 67, 1–48. [Google Scholar] [CrossRef] [PubMed]
  14. Zeng, H.; Xu, J.; Gillen, J.; McMahon, M.T.; Artemov, D.; Tyburn, J.-M.; Lohman, J.A.B.; Mewis, R.E.; Atkinson, K.D.; Green, G.G.R.; et al. Optimization of SABRE for polarization of the tuberculosis drugs pyrazinamide and isoniazid. J. Magn. Reson. 2013, 237, 73–78. [Google Scholar] [CrossRef] [Green Version]
  15. Lloyd, L.S.; Asghar, A.; Burns, M.J.; Charlton, A.; Coombes, S.; Cowley, M.J.; Dear, G.J.; Duckett, S.B.; Genov, G.R.; Green, G.G.R.; et al. Hyperpolarisation through reversible interactions with parahydrogen. Catal. Sci. Technol. 2014, 4, 3544–3554. [Google Scholar] [CrossRef]
  16. Spannring, P.; Reile, I.; Emondts, M.; Schleker, P.P.M.; Hermkens, N.K.J.; van der Zwaluw, N.G.J.; van Weerdenburg, B.J.A.; Tinnemans, P.; Tessari, M.; Blümich, B.; et al. A New Ir-NHC Catalyst for Signal Amplification by Reversible Exchange in D2O. Chem. Eur. J. 2016, 22, 9277–9282. [Google Scholar] [CrossRef] [Green Version]
  17. Zhivonitko, V.V.; Skovpin, I.V.; Koptyug, I.V. Strong 31P nuclear spin hyperpolarization produced via reversible chemical interaction with parahydrogen. Chem. Commun. 2015, 51, 2506–2509. [Google Scholar] [CrossRef]
  18. Moreno, K.X.; Nasr, K.; Milne, M.; Sherry, A.D.; Goux, W.J. Nuclear spin hyperpolarization of the solvent using signal amplification by reversible exchange (SABRE). J. Magn. Reson. 2015, 257, 15–23. [Google Scholar] [CrossRef] [Green Version]
  19. Colell, J.F.P.; Emondts, M.; Logan, A.W.J.; Shen, K.; Bae, J.; Shchepin, R.V.; Ortiz, G.X.; Spannring, P.; Wang, Q.; Malcolmson, S.J.; et al. Direct Hyperpolarization of Nitrogen-15 in Aqueous Media with Parahydrogen in Reversible Exchange. J. Am. Chem. Soc. 2017, 139, 7761–7767. [Google Scholar] [CrossRef] [Green Version]
  20. Shi, F.; He, P.; Best, Q.A.; Groome, K.; Truong, M.L.; Coffey, A.M.; Zimay, G.; Shchepin, R.V.; Waddell, K.W.; Chekmenev, E.Y.; et al. Aqueous NMR Signal Enhancement by Reversible Exchange in a Single Step Using Water-Soluble Catalysts. J. Phys. Chem. C 2016, 120, 12149–12156. [Google Scholar] [CrossRef]
  21. Olaru, A.M.; Burns, M.J.; Green, G.G.R.; Duckett, S.B. SABRE hyperpolarisation of vitamin B3 as a function of pH. Chem. Sci. 2017, 8, 2257–2266. [Google Scholar] [CrossRef] [Green Version]
  22. Gong, Q.; Gordji-Nejad, A.; Blümich, B.; Appelt, S. Trace analysis by low-field NMR: Breaking the sensitivity limit. Anal. Chem. 2010, 82, 7078–7082. [Google Scholar] [CrossRef] [PubMed]
  23. Shen, K.; Logan, A.W.J.; Colell, J.F.P.; Bae, J.; Ortiz, G.X.; Theis, T.; Warren, W.S.; Malcolmson, S.J.; Wang, Q. Diazirines as Potential Molecular Imaging Tags: Probing the Requirements for Efficient and Long-Lived SABRE-Induced Hyperpolarization. Angew. Chem. 2017, 129, 12280–12284. [Google Scholar] [CrossRef]
  24. Reile, I.; Eshuis, N.; Hermkens, N.K.J.; van Weerdenburg, B.J.A.; Feiters, M.C.; Rutjes, F.P.J.T.; Tessari, M. NMR detection in biofluid extracts at sub-μM concentrations via para-H2 induced hyperpolarization. Analyst 2016, 141, 4001–4005. [Google Scholar] [CrossRef] [Green Version]
  25. Eshuis, N.; Aspers, R.L.E.G.; van Weerdenburg, B.J.A.; Feiters, M.C.; Rutjes, F.P.J.T.; Wijmenga, S.S.; Tessari, M. 2D NMR Trace Analysis by Continuous Hyperpolarization at High Magnetic Field. Angew. Chem. Int. Ed. 2015, 54, 14527–14530. [Google Scholar] [CrossRef]
  26. Cowley, M.J.; Adams, R.W.; Atkinson, K.D.; Cockett, M.C.R.; Duckett, S.B.; Green, G.G.R.; Lohman, J.A.B.; Kerssebaum, R.; Kilgour, D.; Mewis, R.E. Iridium N-heterocyclic carbene complexes as efficient catalysts for magnetization transfer from para-hydrogen. J. Am. Chem. Soc. 2011, 133, 6134–6137. [Google Scholar] [CrossRef] [Green Version]
  27. Colell, J.F.P.; Logan, A.W.J.; Zhou, Z.; Shchepin, R.V.; Barskiy, D.A.; Ortiz, G.X.; Wang, Q.; Malcolmson, S.J.; Chekmenev, E.Y.; Warren, W.S.; et al. Generalizing, Extending, and Maximizing Nitrogen-15 Hyperpolarization Induced by Parahydrogen in Reversible Exchange. J. Phys. Chem. C 2017, 121, 6626–6634. [Google Scholar] [CrossRef]
  28. Mewis, R.E.; Atkinson, K.D.; Cowley, M.J.; Duckett, S.B.; Green, G.G.R.; Green, R.A.; Highton, L.A.R.; Kilgour, D.; Lloyd, L.S.; Lohman, J.A.B.; et al. Probing signal amplification by reversible exchange using an NMR flow system. Magn. Reson. Chem. 2014, 52, 358–369. [Google Scholar] [CrossRef] [Green Version]
  29. Dücker, E.B.; Kuhn, L.T.; Münnemann, K.; Griesinger, C. Similarity of SABRE field dependence in chemically different substrates. J. Magn. Reson. 2012, 214, 159–165. [Google Scholar] [CrossRef] [Green Version]
  30. Hövener, J.-B.; Schwaderlapp, N.; Lickert, T.; Duckett, S.B.; Mewis, R.E.; Highton, L.A.R.; Kenny, S.M.; Green, G.G.R.; Leibfritz, D.; Korvink, J.G.; et al. A hyperpolarized equilibrium for magnetic resonance. Nat. Commun. 2013, 4, 2946. [Google Scholar] [CrossRef]
  31. Suefke, M.; Lehmkuhl, S.; Liebisch, A.; Blümich, B.; Appelt, S. Para-hydrogen raser delivers sub-millihertz resolution in nuclear magnetic resonance. Nat. Phys. 2017, 13, 568–572. [Google Scholar] [CrossRef]
  32. Truong, M.L.; Shi, F.; He, P.; Yuan, B.; Plunkett, K.N.; Coffey, A.M.; Shchepin, R.V.; Barskiy, D.A.; Kovtunov, K.V.; Koptyug, I.V.; et al. Irreversible catalyst activation enables hyperpolarization and water solubility for NMR signal amplification by reversible exchange. J. Phys. Chem. B 2014, 118, 13882–13889. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  33. Chapman, B.; Joalland, B.; Meersman, C.; Ettedgui, J.; Swenson, R.E.; Krishna, M.C.; Nikolaou, P.; Kovtunov, K.V.; Salnikov, O.G.; Koptyug, I.V.; et al. Low-Cost High-Pressure Clinical-Scale 50% Parahydrogen Generator Using Liquid Nitrogen at 77 K. Anal. Chem. 2021, 93, 8476–8483. [Google Scholar] [CrossRef] [PubMed]
  34. Birchall, J.R.; Coffey, A.M.; Goodson, B.M.; Chekmenev, E.Y. High-Pressure Clinical-Scale 87% Parahydrogen Generator. Anal. Chem. 2020, 92, 15280–15284. [Google Scholar] [CrossRef] [PubMed]
  35. Ellermann, F.; Pravdivtsev, A.; Hövener, J.-B. Open-source, partially 3D-printed, high-pressure (50-bar) liquid-nitrogen-cooled parahydrogen generator. Magn. Reson. 2021, 2, 49–62. [Google Scholar] [CrossRef]
  36. Hövener, J.-B.; Bär, S.; Leupold, J.; Jenne, K.; Leibfritz, D.; Hennig, J.; Duckett, S.B.; von Elverfeldt, D. A continuous-flow, high-throughput, high-pressure parahydrogen converter for hyperpolarization in a clinical setting. NMR Biomed. 2013, 26, 124–131. [Google Scholar] [CrossRef] [PubMed]
  37. Feng, B.; Coffey, A.M.; Colon, R.D.; Chekmenev, E.Y.; Waddell, K.W. A pulsed injection parahydrogen generator and techniques for quantifying enrichment. J. Magn. Reson. 2012, 214, 258–262. [Google Scholar] [CrossRef] [Green Version]
  38. Duchowny, A.; Ortiz Restrepo, S.A.; Adams, M.; Thelen, R.; Adams, A. Refined high-pressure tube design for improved resolution in high-pressure NMR spectroscopy. Analyst 2022, 147, 3827–3832. [Google Scholar] [CrossRef]
  39. Duchowny, A.; Mohnke, O.; Thern, H.; Dupuy, P.M.; Widerøe, H.C.; Faanes, A.; Paulsen, A.; Küppers, M.; Blümich, B.; Adams, A. Composition analysis of natural gas by combined benchtop NMR spectroscopy and mechanistical multivariate regression. Energy Rep. 2022, 8, 3661–3670. [Google Scholar] [CrossRef]
  40. Duchowny, A.; Dupuy, P.M.; Widerøe, H.C.; Berg, O.J.; Faanes, A.; Paulsen, A.; Thern, H.; Mohnke, O.; Küppers, M.; Blümich, B.; et al. Versatile high-pressure gas apparatus for benchtop NMR: Design and selected applications. J. Magn. Reson. 2021, 329, 107025. [Google Scholar] [CrossRef]
  41. Burueva, D.B.; Romanov, A.S.; Salnikov, O.G.; Zhivonitko, V.V.; Chen, Y.-W.; Barskiy, D.A.; Chekmenev, E.Y.; Hwang, D.W.; Kovtunov, K.V.; Koptyug, I.V. Extending the Lifetime of Hyperpolarized Propane Gas through Reversible Dissolution. J. Phys. Chem. C 2017, 121, 4481–4487. [Google Scholar] [CrossRef]
  42. Alderson, T.R.; Charlier, C.; Torchia, D.A.; Anfinrud, P.; Bax, A. Monitoring Hydrogen Exchange During Protein Folding by Fast Pressure Jump NMR Spectroscopy. J. Am. Chem. Soc. 2017, 139, 11036–11039. [Google Scholar] [CrossRef] [Green Version]
  43. Kuwata, K.; Li, H.; Yamada, H.; Batt, C.A.; Goto, Y.; Akasaka, K. High pressure NMR reveals a variety of fluctuating conformers in beta-lactoglobulin. J. Mol. Biol. 2001, 305, 1073–1083. [Google Scholar] [CrossRef] [PubMed]
  44. Roche, J.; Royer, C.A.; Roumestand, C. Monitoring protein folding through high pressure NMR spectroscopy. Prog. Nucl. Magn. Reson. Spectrosc. 2017, 102–103, 15–31. [Google Scholar] [CrossRef] [PubMed]
  45. Brunner, E.; Hültenschmidt, W.; Schlichthärle, G. Fluid mixtures at high pressures IV. Isothermal phase equilibria in binary mixtures consisting of (methanol + hydrogen or nitrogen or methane or carbon monoxide or carbon dioxide). J. Chem. Thermodyn. 1987, 19, 273–291. [Google Scholar] [CrossRef]
  46. Descamps, C.; Coquelet, C.; Bouallou, C.; Richon, D. Solubility of hydrogen in methanol at temperatures from 248.41 to 308.20 K. Thermochim. Acta 2005, 430, 1–7. [Google Scholar] [CrossRef]
  47. d’Angelo, J.V.H.; Francesconi, A.Z. Gas−Liquid Solubility of Hydrogen in n -Alcohols (1 ≤ n ≤ 4) at Pressures from 3.6 MPa to 10 MPa and Temperatures from 298.15 K to 525.15 K. J. Chem. Eng. Data 2001, 46, 671–674. [Google Scholar] [CrossRef]
  48. Bezanehtak, K.; Combes, G.B.; Dehghani, F.; Foster, N.R.; Tomasko, D.L. Vapor−Liquid Equilibrium for Binary Systems of Carbon Dioxide + Methanol, Hydrogen + Methanol, and Hydrogen + Carbon Dioxide at High Pressures. J. Chem. Eng. Data 2002, 47, 161–168. [Google Scholar] [CrossRef]
  49. Barskiy, D.A.; Pravdivtsev, A.N.; Ivanov, K.L.; Kovtunov, K.V.; Koptyug, I.V. A simple analytical model for signal amplification by reversible exchange (SABRE) process. Phys. Chem. Chem. Phys. 2016, 18, 89–93. [Google Scholar] [CrossRef]
  50. Campalani, C.; Amadio, E.; Zanini, S.; Dall’Acqua, S.; Panozzo, M.; Ferrari, S.; de Nadai, G.; Francescato, S.; Selva, M.; Perosa, A. Supercritical CO2 as a green solvent for the circular economy: Extraction of fatty acids from fruit pomace. J. CO2 Util. 2020, 41, 101259. [Google Scholar] [CrossRef]
  51. Nalawade, S.P.; Picchioni, F.; Janssen, L. Supercritical carbon dioxide as a green solvent for processing polymer melts: Processing aspects and applications. Prog. Polym. Sci. 2006, 31, 19–43. [Google Scholar] [CrossRef] [Green Version]
  52. Shen, Z.; Li, D.; McHugh, M.A. Solubility of Pyrazine and Its Derivatives in Supercritical Carbon Dioxide. J. Chem. Eng. Data 2006, 51, 2056–2064. [Google Scholar] [CrossRef]
  53. Knecht, S.; Hadjiali, S.; Barskiy, D.A.; Pines, A.; Sauer, G.; Kiryutin, S.A.; Ivanov, K.L.; Yurkovskaya, A.V.; Buntkowsky, G. Indirect Detection of Short-Lived Hydride Intermediates of Iridium N-Heterocyclic Carbene Complexes via Chemical Exchange Saturation Transfer Spectroscopy. J. Phys. Chem. C 2019, 123, 16288–16293. [Google Scholar] [CrossRef] [Green Version]
  54. Lin, K.; Patrick TomHon, P.; Lehmkuhl, S.; Laasner, R.; Theis, T.; Blum, V. Density Functional Theory Study of Reaction Equilibria in Signal Amplification by Reversible Exchange. ChemPhysChem 2021, 22, 1947–1957. [Google Scholar] [CrossRef] [PubMed]
Ijms 24 02465 g001 550
Figure 1. Overview of the high-pressure p-H2 SABRE setup: para-hydrogen generator (1), high-pressure cylinder (2), high-pressure sapphire tube (not shown to scale for a better view) (3), electromagnet (4), benchtop NMR device (5), along with the SABRE polarization transfer mechanism in the iridium-based catalyst employed in this study (6).
Figure 1. Overview of the high-pressure p-H2 SABRE setup: para-hydrogen generator (1), high-pressure cylinder (2), high-pressure sapphire tube (not shown to scale for a better view) (3), electromagnet (4), benchtop NMR device (5), along with the SABRE polarization transfer mechanism in the iridium-based catalyst employed in this study (6).
Ijms 24 02465 g001
Ijms 24 02465 g002 550
Figure 2. Peak integral of H2 dissolved in d-methanol between 1 and 200 bar. Only the right half of the H2 peak was integrated to reduce the influence of the overlapping OH peak from residual non-deuterated methanol. The dotted lines are linear fits of H2 peak integrals obtained when raising the pressure from 0 to 200 bar (purple) or lowering it from 200 to 1 bar (orange).
Figure 2. Peak integral of H2 dissolved in d-methanol between 1 and 200 bar. Only the right half of the H2 peak was integrated to reduce the influence of the overlapping OH peak from residual non-deuterated methanol. The dotted lines are linear fits of H2 peak integrals obtained when raising the pressure from 0 to 200 bar (purple) or lowering it from 200 to 1 bar (orange).
Ijms 24 02465 g002
Ijms 24 02465 g003 550
Figure 3. (a) Molar enhancements achieved with high-pressure SABRE hyperpolarization at different pyrazine concentrations in d-methanol. The pyrazine/catalyst ratio was 1/20. The thermal signal of a reference sample was used for determining the signal enhancement. The dotted lines serve as a visual guide. The measurement for each pressure point was conducted three times to determine the error bars. (b) Hydride signals of hyperpolarized solutions with 4.8 mmol L−1 pyrazine and 0.24 mmol L−1 catalyst at different pressures.
Figure 3. (a) Molar enhancements achieved with high-pressure SABRE hyperpolarization at different pyrazine concentrations in d-methanol. The pyrazine/catalyst ratio was 1/20. The thermal signal of a reference sample was used for determining the signal enhancement. The dotted lines serve as a visual guide. The measurement for each pressure point was conducted three times to determine the error bars. (b) Hydride signals of hyperpolarized solutions with 4.8 mmol L−1 pyrazine and 0.24 mmol L−1 catalyst at different pressures.
Ijms 24 02465 g003
Ijms 24 02465 g004 550
Figure 4. Parahydrogen hyperpolarization in quickly removable solvents. (a) 1H NMR spectrum of pyridine in d-methanol hyperpolarized by liquefying a p-H2/ethane mixture with a signal enhancement of about 78 (red). The insert shows a 200-fold magnification of the thermal pyridine signal. The polarization transfer field for this experiment is the earth’s magnetic field. (b) Hyperpolarization of solid pyrazine and catalyst with a pressurized p-H2/CO2 50:50 mixture at 200 bar. The achieved signal enhancement is about 12. Reference thermal polarization spectra are depicted in blue.
Figure 4. Parahydrogen hyperpolarization in quickly removable solvents. (a) 1H NMR spectrum of pyridine in d-methanol hyperpolarized by liquefying a p-H2/ethane mixture with a signal enhancement of about 78 (red). The insert shows a 200-fold magnification of the thermal pyridine signal. The polarization transfer field for this experiment is the earth’s magnetic field. (b) Hyperpolarization of solid pyrazine and catalyst with a pressurized p-H2/CO2 50:50 mixture at 200 bar. The achieved signal enhancement is about 12. Reference thermal polarization spectra are depicted in blue.
Ijms 24 02465 g004
Disclaimer/Publisher’s Note: The statements, opinions and data contained in all publications are solely those of the individual author(s) and contributor(s) and not of MDPI and/or the editor(s). MDPI and/or the editor(s) disclaim responsibility for any injury to people or property resulting from any ideas, methods, instructions or products referred to in the content.

Share and Cite

MDPI and ACS Style

Duchowny, A.; Denninger, J.; Lohmann, L.; Theis, T.; Lehmkuhl, S.; Adams, A. SABRE Hyperpolarization with up to 200 bar Parahydrogen in Standard and Quickly Removable Solvents. Int. J. Mol. Sci. 2023, 24, 2465. https://doi.org/10.3390/ijms24032465

AMA Style

Duchowny A, Denninger J, Lohmann L, Theis T, Lehmkuhl S, Adams A. SABRE Hyperpolarization with up to 200 bar Parahydrogen in Standard and Quickly Removable Solvents. International Journal of Molecular Sciences. 2023; 24(3):2465. https://doi.org/10.3390/ijms24032465

Chicago/Turabian Style

Duchowny, Anton, Johannes Denninger, Lars Lohmann, Thomas Theis, Sören Lehmkuhl, and Alina Adams. 2023. "SABRE Hyperpolarization with up to 200 bar Parahydrogen in Standard and Quickly Removable Solvents" International Journal of Molecular Sciences 24, no. 3: 2465. https://doi.org/10.3390/ijms24032465

APA Style

Duchowny, A., Denninger, J., Lohmann, L., Theis, T., Lehmkuhl, S., & Adams, A. (2023). SABRE Hyperpolarization with up to 200 bar Parahydrogen in Standard and Quickly Removable Solvents. International Journal of Molecular Sciences, 24(3), 2465. https://doi.org/10.3390/ijms24032465

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop