Jule Kuhn1, Kolja Them1, and Jan-Bernd Hövener1
1Section Biomedical Imaging, Department of Radiology and Neuroradiology, University Medical Center Schleswig - Holstein, Kiel University, Kiel, Germany
Synopsis
Keywords: Hyperpolarized MR (Non-Gas), Contrast Agent
The PHIP-X methodology is a novel approach to produce
contrast agents for metabolic MRI by hyperpolarization and combines the high polarization
resulting from pH
2 addition with the versatility of proton exchange.
However, the polarization yield and reproducibility have to be improved. The
proposed setup provides reproducible and well controlled experimental
conditions for PHIP-X, including a pH
2 pressure of up to 100 bar and a
magnetic field of up to 95 mT. Using this setup allowed to reach high
1H
polarizations of the transfer agent and to transfer the polarization to
13C
in the target molecule glucose successfully.
Introduction
MRI with hyperpolarized contrast agents has allowed imaging of metabolism
in real-time and with unprecedented sensitivity using different
hyperpolarization methods.
One hyperpolarization method uses parahydrogen (pH2) as a source
of spin order to polarize a target molecule. These methods are cost efficient and
usually fast. However, a limitation is the need of an unsaturated precursor for
hydrogenation (PHIP1 and PHIP-SAH2) or molecule that undergoes
reversible exchange with pH2 at a catalyst (SABRE3). Recently, it was proposed
to transfer the pH2-derived polarization to other molecules via
proton exchange (SABRE-RELAY4, PHIP-X5). PHIP-X combines high
polarization resulting from pH2 addition with the versatility of
proton exchange. Here, a transfer agent is polarized by addition of pH2 before the polarization is transferred via proton exchange to a target
molecule. However, for several applications, the polarization
yield and reproducibility must be improved.
Here, we propose a setup that provides reproducible and well controlled
experimental conditions for PHIP-X, including a pH2 pressure of up to
100 bar and a magnetic field of up to 95 mT.Methods
Chemistry:
100 µl of 830 mM 13C6-D-Glucose (Sigma Aldrich, CAS: 110187-42-3) in Dimethylsulfoxid-d6
(DMSO-d6, Sigma Aldrich, CAS: 2206-27-1), and 8 µl of Propargyl
alcohol (99%, Sigma Aldrich, CAS: 107-19-7) were mixed with 900 µl of 7 mM
catalyst ([Rh(dppb)(COD)]BF4, 98%, Sigma Aldrich, CAS: 79255-71-3) in acetone-d6
(Sigma Aldrich, CAS: 666-52-4).
Polarizer:
The polarizer consisted of a
copper tube with a resistive coil, programmable power supply, multifunctional
HPLC valve (Knauer Azura 4.1) and 1T benchtop NMR. The valve guided the pH2
into the copper tube (26 cm length, diameter 6 mm), holding the liquid sample,
and transferred it into the NMR (Spinsolve 43 Carbon, Magritek, Fig. 1). The
valve was controlled using a custom-made microprocessor circuit board. The coil
(1 mm copper wire, 5200 windings, NGL 202 power supply, Rohde & Schwarz) around
the tube generated a magnetic field during the hydrogenation of up to Bhydro = 95 mT.
Other components included a pressure control valve, flow regulator and two
exhausts. All parts were rated for pressures exceeding 100 bar. About 95%
enriched pH2 was produced using a
high-pressure pH2 generator at 25 K (unpublished).
Experiment:
After injecting the sample and
closing the reactor, the experiment was started in the NMR software, which set the
magnetic field and triggered the board controlling the valve (Fig. 2). The
valve connected the pH2 supply (35 bar) with the reactor, initiating the hydrogenation. After five
seconds, the valve connected the reactor to the tube inside the NMR, where the
data acquisition was started 1.5 seconds later (either pulse-acquisition 1H spectra
or spin order transfer from 1H to 13C using the DEPT sequence
(135° pulse, 140 Hz)). Note that the sample passed through earth magnetic field
during the transfer from Bhydro
to the detection field of 1 T.Results
First, we investigated the hyperpolarization
on the transfer agent. We conducted the experiment at four different magnetic
fields between 45 mT and 90 mT (five times each). A mean polarization of about
11% was observed (Fig. 3), with the highest polarization and the largest
variation at 45 mT. The polarization (P) and the standard deviation
(SD) decreased with increasing fields from P(1H) ≈ 11.5% to 11% and from SD = 1.4% (45 mT) to
0.4% (90 mT), respectively.
Next, we investigated the polarization transfer
from the transfer agent to the biological target molecule 13C6-D-glucose.
PHIP-X was conducted using a solution containing glucose, propargyl alcohol and
the catalyst at 35 bar pH2 and Bhydro
= 60 mT. Strong 13C signal enhancement was observed after 1H-to-13C
polarization transfer with DEPT (135°, 140 Hz). An enhancement of approx. 80-fold
was found with respect to thermal equilibrium using the same sequence,
corresponding to a polarization of 0.0071% (Fig. 4, across all 13C
resonances of glucose).Discussion
The presented setup allowed highly
automated and reproducible PHIP-X experiments with pH2 pressures of
35 bar and external magnetic fields of up to 90 mT. High 1H polarization
of the transfer agent of ≈11% was reached. SD was higher at lower fields, which may be connected to
changing relaxations and more chaotic spin dynamics at lower fields.
The polarization transfer to 13C
in the target glucose was successful, although on a lower level of P(13C)
≈ 0.0071%. This polarization
appears low with respect to other methods and for biomedical imaging, it should
be noted that the concentration was high (83 mM) and further optimizations are
ongoing. Specifically, the optimization of the chemical exchange rates between
transfer agent and target molecule appears to be very promising. The advantage
of polarization transfer via proton exchange remains that it is universally
applicable to all exchanging molecules
The removal of catalyst and
transfer agent after polarization is still a challenge for biomedical
applications and remains a future research scope.Conclusion
The presented setup allowed us
to conduct highly automated PHIP-X experiments and improving the
reproducibility significantly. A wide range of magnetic fields (up to 95 mT)
and a high pH2 pressures (up to 100 bar) assures fast hydrogenation
and facilitates parameter optimization. As a successful proof-of-concept, the setup
is the starting point for further optimizing this interesting variant of PHIP.Acknowledgements
We acknowledge support by the Emmy Noether Program “Metabolic and
Molecular MR” (HO 4604/2-2), the research training circle “Materials for
Brain” (GRK 2154/1-2019), DFG-RFBR grant (HO 4604/3-1, No 19-53-12013),
Cluster of Excellence “Precision Medicine in Inflammation” (PMI 2167),
German Federal Ministry of Education and Research (BMBF) within the
framework of the e:Med research and funding concept (01ZX1915C). Kiel
University and the Medical Faculty are acknowledged for supporting the
Molecular Imaging North Competence Center (MOIN CC, MOIN 4604/3). MOIN
CC was founded by a grant from the European Regional Development Fund
(ERDF) and the Zukunftsprogramm Wirtschaft of Schleswig-Holstein
(Project no. 122-09-053). The Russian team thanks the Russian Foundation
for Basic Research (Grant 19-53-12013) for financial support.References
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