Dynamic Nuclear Polarization Polarizer Research Articles

Towards a unified picture of polarization transfer — pulsed DNP and chemically equivalent PHIP

Nuclear spin hyperpolarization techniques, such as dynamic nuclear polarization (DNP) and parahydrogen-induced polarization (PHIP), have revolutionized nuclear magnetic resonance and magnetic resonance imaging. In these methods, a readily available source of high spin order, either electron spins in DNP or singlet states in hydrogen for PHIP, is brought into close proximity with nuclear spin targets, enabling efficient transfer of spin order under external quantum control. Despite vast disparities in energy scales and interaction mechanisms between electron spins in DNP and nuclear singlet states in PHIP, a pseudo-spin formalism allows us to establish an intriguing equivalence. As a result, the important low-field polarization transfer regime of PHIP can be mapped onto an analogous system equivalent to pulsed-DNP. This establishes a correspondence between key polarization transfer sequences in PHIP and DNP, facilitating the transfer of sequence development concepts. This promises fresh insights and significant cross-pollination between DNP and PHIP polarization sequence developers.

Directly Bound Deuterons Increase X-Nuclei Hyperpolarization using Dynamic Nuclear Polarization.

Deuterated 13 C sites in sugars (D-glucose and 2-deoxy-D-glucose) showed 6.3-to-17.5-fold higher solid-state dynamic nuclear polarization (DNP) levels than their respective protonated sites at 3.35T. This effect was found to be unrelated to the protonation of the bath. Deuterated 15 N in sites bound to exchangeable protons ([15 N2 ]urea) showed a 1.3-fold higher polarization than their respective protonated sites at the same magnetic field. This relatively smaller effect was attributed to incomplete deuteration of the 15 N sites due to the solvent mixture. For a 15 N site that is not bound to protons or deuterons ([15 N]nitrate), deuteration of the bath did not affect the polarization level. These findings suggest a phenomenon related to DNP of X-nuclei directly bound to deuteron(s) as opposed to proton(s). It appears that direct binding to deuterons increases the solid-state DNP polarization level of X-nuclei which are otherwise bound to protons.

Deuterated TEKPol Biradicals and the Spin‐Diffusion Barrier in MAS DNP

AbstractThe sensitivity of NMR spectroscopy is considerably enhanced by dynamic nuclear polarization (DNP). In DNP polarization is transferred from unpaired electrons of a polarizing agent to nearby proton spins. In solids, this transfer is followed by the transport of hyperpolarization to the bulk via 1H‐1H spin diffusion. The efficiency of these steps is critical to obtain high sensitivity gains, but the pathways for polarization transfer in the region near the unpaired electron spins are unclear. Here we report a series of seven deuterated and one fluorinated TEKPol biradicals to probe the effect of deprotonation on MAS DNP at 9.4 T. The experimental results are interpreted with numerical simulations, and our findings support that strong hyperfine couplings to nearby protons determine high transfer rates across the spin diffusion barrier to achieve short build‐up times and high enhancements. Specifically, 1H DNP build‐up times increase substantially with TEKPol isotopologues that have fewer hydrogen atoms in the phenyl rings, suggesting that these protons play a crucial role transferring the polarization to the bulk. Based on this new understanding, we have designed a new biradical, NaphPol, which yields significantly increased NMR sensitivity, making it the best performing DNP polarizing agent in organic solvents to date.

Deuterated TEKPol Biradicals and the Spin-Diffusion Barrier in MAS DNP.

The sensitivity of NMR spectroscopy is considerably enhanced by dynamic nuclear polarization (DNP). In DNP polarization is transferred from unpaired electrons of a polarizing agent to nearby proton spins. In solids, this transfer is followed by the transport of hyperpolarization to the bulk via 1 H-1 H spin diffusion. The efficiency of these steps is critical to obtain high sensitivity gains, but the pathways for polarization transfer in the region near the unpaired electron spins are unclear. Here we report a series of seven deuterated and one fluorinated TEKPol biradicals to probe the effect of deprotonation on MAS DNP at 9.4 T. The experimental results are interpreted with numerical simulations, and our findings support that strong hyperfine couplings to nearby protons determine high transfer rates across the spin diffusion barrier to achieve short build-up times and high enhancements. Specifically, 1 H DNP build-up times increase substantially with TEKPol isotopologues that have fewer hydrogen atoms in the phenyl rings, suggesting that these protons play a crucial role transferring the polarization to the bulk. Based on this new understanding, we have designed a new biradical, NaphPol, which yields significantly increased NMR sensitivity, making it the best performing DNP polarizing agent in organic solvents to date.

Imaging Acute Metabolic Changes in Patients with Mild Traumatic Brain Injury Using Hyperpolarized [1-13C]Pyruvate.

SummaryTraumatic brain injury (TBI) involves complex secondary injury processes following the primary injury. The secondary injury is often associated with rapid metabolic shifts and impaired brain function immediately after the initial tissue damage. Magnetic resonance spectroscopic imaging (MRSI) coupled with hyperpolarization of 13C-labeled substrates provides a unique opportunity to map the metabolic changes in the brain after traumatic injury in real-time without invasive procedures. In this report, we investigated two patients with acute mild TBI (Glasgow coma scale 15) but no anatomical brain injury or hemorrhage. Patients were imaged with hyperpolarized [1-13C]pyruvate MRSI 1 or 6 days after head trauma. Both patients showed significantly reduced bicarbonate (HCO3–) production, and one showed hyperintense lactate production at the injured sites. This study reports the feasibility of imaging altered metabolism using hyperpolarized pyruvate in patients with TBI, demonstrating the translatability and sensitivity of the technology to cerebral metabolic changes after mild TBI.

Increased flow rate of hyperpolarized aqueous solution for dynamic nuclear polarization-enhanced magnetic resonance imaging achieved by an open Fabry-Pérot type microwave resonator.

A continuous flow dynamic nuclear polarization (DNP) employing the Overhauser effect at ambient temperatures can be used among other methods to increase sensitivity of magnetic resonance imaging (MRI). The hyperpolarized state of water protons can be achieved by flowing aqueous liquid through a microwave resonator placed directly in the bore of a 1.5 T MRI magnet. Here we describe a new open Fabry-Pérot resonator as DNP polarizer, which exhibits a larger microwave exposure volume for the flowing liquid in comparison with a cylindrical TE microwave cavity. The Fabry-Pérot resonator geometry was designed using quasi-optical theory and simulated by CST software. Performance of the new polarizer was tested by MRI DNP experiments on a TEMPOL aqueous solution using a blood-vessel phantom. The Fabry-Pérot resonator revealed a 2-fold larger DNP enhancement with a 4-fold increased flow rate compared to the cylindrical microwave resonator. This increased yield of hyperpolarized liquid allows MRI applications on larger target objects.

Dynamic Nuclear Polarization with Vanadium(IV) Metal Centers

Summary Dynamic nuclear polarization (DNP) harnesses the large polarization of electron spins to dramatically increase nuclear magnetic resonance (NMR) sensitivity. This study expands the scope of DNP beyond its traditional focus on hyperpolarizing the solvent network using exogenous polarizing agents (PAs). We introduce 1H DNP with endogenous V4+ centers positioned in a set of vanadyl complexes with tunable V4+-1H distances. We traced the polarization transfer from V4+ to 1H spins, specifically differentiating between direct V4+-1Hs polarization transfer and the 1H spin-diffusion-mediated bulk solvent 1H polarization buildup and illuminated the effect of the V4+-1H distance on these processes. These results deepen our understanding of polarization pathways and expand the catalog of PAs to broad-line transition metals. This study establishes crucial first steps toward employing strategically positioned endogenous paramagnetic metal centers for DNP and the conceptual framework of hyperfine DNP spectroscopy that merges both spatial and chemical diagnosis of target nuclear spins.

A multisample 7 T dynamic nuclear polarization polarizer for preclinical hyperpolarized MR.

Dynamic nuclear polarization (DNP) provides the opportunity to boost liquid state magnetic resonance (MR) signals from selected nuclear spins by several orders of magnitude. A cryostat running at a temperature of ~ 1 K and a superconducting magnet set to between 3 and 10 T are required to efficiently hyperpolarize nuclear spins. Several DNP polarizers have been implemented for the purpose of hyperpolarized MR and recent systems have been designed to avoid the need for user input of liquid cryogens. We herein present a zero boil-off DNP polarizer that operates at 1.35 ± 0.01 K and 7 T, and which can polarize two samples in parallel. The samples are cooled by a static helium bath thermally connected to a 1 K closed-cycle 4 He refrigerator. Using a modified version of the commercial fluid path developed for the SPINlab polarizer, we demonstrate that, within a 12-minute interval, the system can produce two separate hyperpolarized 13 C solutions. The 13 C liquid-state polarization of [1-13 C]pyruvate measured 26 seconds after dissolution was 36%, which can be extrapolated to a 55% solid state polarization. The system is well adapted for in vitro and in vivo preclinical hyperpolarized MR experiments and it can be modified to polarize up to four samples in parallel.

Abstract 1944: Detection of metabolic change in glioblastoma after radiotherapy using hyperpolarized 13C-MRI: Glycolytic metabolism in cancer stem cell-like cell-derived tumor model

Abstract OBJECTIVES: Since the cancer stem-like cells (CSCs) play an important role in the resistance against radiation therapy due to its different metabolic profile, investigation of the specific metabolic characteristics of CSCs is valuable. Dynamic nuclear polarization (DNP) technique using 13C-labeled substrates enables magnetic resonance imaging (MRI) to monitor specific enzymatic reactions in tumors. In this study, DNP-MRI along with hyperpolarized [1-13C] pyruvate was conducted to evaluate the metabolic change in glycolytic profiles after irradiation between a glioblastoma cell line and a CSC-derived glioma using orthotopic xenograft mouse model. A microarray analysis was also performed to compare to the imaging study. METHODS: DNP-MRI A 3T MRI scanner along with a custom-made head coil was used. To obtain hyperpolarized [1-13C] pyruvate, 30 μL of [1-13C] pyruvic acid containing 15 mM of OX063 (trityl radical compound) and 2.5 mM of the gadolinium chelate were polarized at 3.35 T and 1.4 K in the Hypersense DNP polarizer. The hyperpolarized sample dissolved in a buffered medium was injected via the tail vein followed by an acquisition of 13C-two-dimensional MR-spectroscopy to measure the pyruvate-to-lactate ratios (Lac/Pyr) in the tumor region and the contralateral normal brain separately. Cell lines A human glioblastoma cell line, U251 and a glioma CSC line, NSC11 were cultured for stereotactic intracranial injection. Animal model Orthotopic brain tumor model was developed in athymic nude mice by intracranial implantation. When the tumor volume reached 50 +/- 10 mm3 on T2-weighted MRI, a sequence of DNP-MRI scans was performed 24 hours before and 6, 16 and 24 after 6-Gy whole-brain irradiation (N = 4 each with a non-irradiated control group). Independently, a microarray analysis using the tumor tissue samples excised 6 and 24 hours after irradiation was performed on Affymetrix Human Genome U133 Plus 2.0 array. RESULTS: DNP-MRI showed a decrease in Lac/Pyr 6 and 16 hours after irradiation compared to the control group in U251 whereas no significant change was observed in the NSC11 tumor. The microarray analysis showed a significant down-regulation of lactate dehydrogenase A (LDH-A) expression in U251 6 and 24 hours after irradiation, consistent with the finding of DNP-MRI. In the microarray analysis, SIRT2 and KLF4 expression also changed in the U251 tumor, suggested to regulate the LDH-A activity/expression. CONCLUSION: DNP-MRI demonstrated the difference in radiation response in glycolytic metabolism between the glioblastoma cell line and the CSC-derived glioma. This technique might be a feasible diagnostic method evaluating metabolic profiles of the brain tumors in the clinical settings of pretreatment and post-treatment. Citation Format: Tatsuya Kawai, Murali C. Krishna, Tamalee Kramp, Jeffery R. Brender, Philip Tofilon, Kevin A. Camphausen. Detection of metabolic change in glioblastoma after radiotherapy using hyperpolarized 13C-MRI: Glycolytic metabolism in cancer stem cell-like cell-derived tumor model [abstract]. In: Proceedings of the American Association for Cancer Research Annual Meeting 2019; 2019 Mar 29-Apr 3; Atlanta, GA. Philadelphia (PA): AACR; Cancer Res 2019;79(13 Suppl):Abstract nr 1944.

Photogenerated Radical in Phenylglyoxylic Acid for in Vivo Hyperpolarized 13C MR with Photosensitive Metabolic Substrates

Whether for 13C magnetic resonance studies in chemistry, biochemistry, or biomedicine, hyperpolarization methods based on dynamic nuclear polarization (DNP) have become ubiquitous. DNP requires a source of unpaired electrons, which are commonly added to the sample to be hyperpolarized in the form of stable free radicals. Once polarized, the presence of these radicals is unwanted. These radicals can be replaced by nonpersistent radicals created by the photoirradiation of pyruvic acid (PA), which are annihilated upon dissolution or thermalization in the solid state. However, since PA is readily metabolized by most cells, its presence may be undesirable for some metabolic studies. In addition, some 13C substrates are photosensitive and therefore may degrade during the photogeneration of a PA radical, which requires ultraviolet (UV) light. We show here that the photoirradiation of phenylglyoxylic acid (PhGA) using visible light produces a nonpersistent radical that, in principle, can be used to hyperpolarize any molecule. We compare radical yields in samples containing PA and PhGA upon photoirradiation with broadband and narrowband UV–visible light sources. To demonstrate the suitability of PhGA as a radical precursor for DNP, we polarized the gluconeogenic probe 13C-dihydroxyacetone, which is UV-sensitive, using a commercial 3.35 T DNP polarizer and then injected this into a mouse and followed its metabolism in vivo.

Abstract 4110: Metabolic imaging of glioblastoma using hyperpolarized 13C-MRI: Glycolytic metabolism in cancer stem cell-like cell-derived tumor model

Abstract OBJECTIVES: Since the cancer stem-like cells (CSCs) play an important role in the resistance against radiation and/or chemotherapy due to its different metabolic profile, to investigate the specific metabolic characteristics of CSCs is valuable. Dynamic nuclear polarization (DNP) technique using 13C-labeled substrates enables magnetic resonance imaging (MRI) to monitor specific enzymatic reactions in tumors. In this study, DNP-MRI along with hyperpolarized [1-13C] pyruvate was conducted to evaluate the difference in glycolytic profile between a glioblastoma cell line and a CSC-derived glioma using orthotopic xenograft mouse model. The imaging findings were compared to those in immunohistology and cell cultures. METHODS: A 3T MRI scanner along with a custom-made head coil was used for imaging. To obtain hyperpolarized [1-13C] pyruvate, 30 μL of [1-13C] pyruvic acid containing 15 mM of OX063 (trityl radical compound) and 2.5 mM of the gadolinium chelate were polarized at 3.35 T and 1.4 K in the Hypersense DNP polarizer. The hyperpolarized sample dissolved in a buffered medium was injected via the tail vein followed by a 13C-two-dimensional spectroscopic imaging. During the acquisition, the body temperature was kept in the range of 35.0 to 36.9 Celsius degrees. Orthotopic brain tumor model was developed in nude mice by intracranial implantation of glioblastoma cell lines, U251 and glioma stem-like cells, NSC11. DNP-MRI was performed when the tumor size ranged 50 + 10 mm3 on T2-weighted MRI. Independently, immunofluorescent analyses of monocarboxylate transporter 1(MCT1) and MCT4 was performed using paraffin-embedded tumor tissue. Expressed protein level of lactate dehydrogenase A (LDHA), LDHB, MCT1 and MCT4 under the normal cell culture conditions were evaluated by Western blotting. RESULTS: 13C-MRI showed an increase in lactate-to-pyruvate ratio (Lac/Pyr) both in U251 and NSC11 compared to the contralateral normal brain tissue, suggested elevated anaerobic glycolysis (P<0.05). The extent of the increase in Lac/Pyr compared to the normal brain tissue was higher in U251 than NSC11 except for one U251 case. Western blotting showed both LDHA and LHDB expression in U251 was lower than NSC11. The expression of MCT4 was higher in U251 than NSC11, whereas they were almost the same for MCT1. Immunohistochemistry showed relative weak staining for MCT4 in NSC11, consistent with the result of Western blotting. CONCLUSION: The quality of 13C-DNP-MRI using [1-13C] pyruvate was validated and considered to be feasible to apply to the brain tumors. The result was reasonable in that malignant tumors enhance anaerobic glycolytic pathway even in the aerobic environment. 13C-DNP-MRI also demonstrated a difference in the extent of Lac/Pyr in relation to the normal brain between the two tumor models probably related to expression levels of glycolysis-related proteins. Citation Format: Tatsuya Kawai, Murali C. Krishna, Jeffery R. Brender, Jennifer Lee, Tamalee Kramp, Kazu Yamamoto, Shun Kishimoto, Tomohiro Seki, Kevin A. Camphausen. Metabolic imaging of glioblastoma using hyperpolarized 13C-MRI: Glycolytic metabolism in cancer stem cell-like cell-derived tumor model [abstract]. In: Proceedings of the American Association for Cancer Research Annual Meeting 2018; 2018 Apr 14-18; Chicago, IL. Philadelphia (PA): AACR; Cancer Res 2018;78(13 Suppl):Abstract nr 4110.

Electron Decoupling with Dynamic Nuclear Polarization in Rotating Solids.

Dynamic nuclear polarization (DNP) can enhance NMR sensitivity by orders of magnitude by transferring spin polarization from electron paramagnetic resonance (EPR) to NMR. However, paramagnetic DNP polarizing agents can have deleterious effects on NMR signals. Electron spin decoupling can mitigate these paramagnetic relaxation effects. We demonstrate electron decoupling experiments in conjunction with DNP and magic-angle-spinning NMR spectroscopy. Following a DNP and spin diffusion period, the microwave irradiation frequency is quickly tuned on-resonance with electrons on the DNP polarizing agent. The electron decoupling performance shows a strong dependence on the microwave frequency and DNP polarization time. Microwave frequency sweeps through the EPR line shape are shown as a time domain strategy to significantly improve electron decoupling. For 13C spins on biomolecules frozen in a glassy matrix, electron decoupling reduces the line widths by 11% (47 Hz) and increases the intensity by 14%.

Molecular Rationale for Improved Dynamic Nuclear Polarization of Biomembranes.

Dynamic nuclear polarization (DNP) enhanced solid-state NMR can provide orders of magnitude in signal enhancement. One of the most important aspects of obtaining efficient DNP enhancements is the optimization of the paramagnetic polarization agents used. To date, the most utilized polarization agents are nitroxide biradicals. However, the efficiency of these polarization agents is diminished when used with samples other than small molecule model compounds. We recently demonstrated the effectiveness of nitroxide labeled lipids as polarization agents for lipids and a membrane embedded peptide. Here, we systematically characterize, via electron paramagnetic (EPR), the dynamics of and the dipolar couplings between nitroxide labeled lipids under conditions relevant to DNP applications. Complemented by DNP enhanced solid-state NMR measurements at 600 MHz/395 GHz, a molecular rationale for the efficiency of nitroxide labeled lipids as DNP polarization agents is developed. Specifically, optimal DNP enhancements are obtained when the nitroxide moiety is attached to the lipid choline headgroup and local nitroxide concentrations yield an average e(-)-e(-) dipolar coupling of 47 MHz. On the basis of these measurements, we propose a framework for development of DNP polarization agents optimal for membrane protein structure determination.

Solid effect DNP polarization dynamics in a system of many spins

We discuss the polarization dynamics during solid effect dynamic nuclear polarization (DNP) in a central spin model that consists of an electron surrounded by many nuclei. To this end we use a recently developed formalism and validate first its performance by comparing its predictions to results obtained by solving the Liouville von Neumann master equation. The use of a Monte Carlo method in our formalism makes it possible to significantly increase the number of spins considered in the model system. We then analyse the dependence of the nuclear bulk polarization on the presence of nuclei in the vicinity of the electron and demonstrate that increasing the minimal distance between nuclei and electrons leads to a rise of the nuclear bulk polarization. These observations have implications for the design of radicals that can lead to improved values of nuclear spin polarization. Furthermore, we discuss the potential to extend our formalism to more complex spin systems such as cross effect DNP.

Rapid-melt Dynamic Nuclear Polarization

In recent years, Dynamic Nuclear Polarization (DNP) has re-emerged as a means to ameliorate the inherent problem of low sensitivity in nuclear magnetic resonance (NMR). Here, we present a novel approach to DNP enhanced liquid-state NMR based on rapid melting of a solid hyperpolarized sample followed by ‘in situ’ NMR detection. This method is applicable to small (10nl to 1μl) sized samples in a microfluidic setup. The method combines generic DNP enhancement in the solid state with the high sensitivity of stripline 1H NMR detection in the liquid state. Fast cycling facilitates options for signal averaging or 2D structural analysis. Preliminary tests show solid-state 1H enhancement factors of up to 500 for H2O/D2O/d6-glycerol samples doped with TEMPOL radicals. Fast paramagnetic relaxation with nitroxide radicals, In nonpolar solvents such as toluene, we find proton enhancement factors up to 400 with negligible relaxation losses in the liquid state, using commercially available BDPA radicals. A total recycling delay (including sample freezing, DNP polarization and melting) of about 5s can be used. The present setup allows for a fast determination of the hyper-polarization as function of the microwave frequency and power.Even at the relatively low field of 3.4T, the method of rapid melting DNP can facilitate the detection of small quantities of molecules in the picomole regime.

An Alderman–Grant resonator for S-Band Dynamic Nuclear Polarization

An Alderman–Grant resonator with resonance at 2GHz (S-Band) was simulated, developed and constructed for Dynamic Nuclear Polarization (DNP) experiments at 73mT. The resonator fits into magnet bores with a minimum diameter of 20mm and is compatible with standard 3mm NMR tubes. The compact resonator design achieves good separation of electric and magnetic fields and therefore can be used with comparatively large sample volumes with only small sample heating effects comparable to those obtained with optimized X- and W-Band DNP setups. The saturation efficiency and sample heating effects were investigated for Overhauser DNP experiments of aqueous solutions of TEMPOL radical, showing relative saturation better than 0.9 and sample heating not exceeding a few Kelvin even at high microwave power and long irradiation time. An application is demonstrated, combining the DNP setup with a commercial fast field cycling NMR relaxometer. Using this resonator design at low microwave frequencies can provide DNP polarization for a class of low-field and time-domain NMR experiments and therefore may enable new applications that benefit from increased sensitivity.

Dynamic nuclear polarization of spherical nanoparticles

Spherical silica nanoparticles of various particle sizes (~10 to 100 nm), produced by a modified Stoeber method employing amino acids as catalysts, are investigated using Dynamic Nuclear Polarization (DNP) enhanced Nuclear Magnetic Resonance (NMR) spectroscopy. This study includes ultra-sensitive detection of surface-bound amino acids and their supramolecular organization in trace amounts, exploiting the increase in NMR sensitivity of up to three orders of magnitude via DNP. Moreover, the nature of the silicon nuclei on the surface and the bulk silicon nuclei in the core (sub-surface) is characterized at atomic resolution. Thereby, we obtain unique insights into the surface chemistry of these nanoparticles, which might result in improving their rational design as required for promising applications, e.g. as catalysts or imaging contrast agents. The non-covalent binding of amino acids to surfaces was determined which shows that the amino acids not just function as catalysts but become incorporated into the nanoparticles during the formation process. As a result only three distinct Q-types of silica signals were observed from surface and core regions. We observed dramatic changes of DNP enhancements as a function of particle size, and very small particles (which suit in vivo applications better) were hyperpolarized with the best efficiency. Nearly one order of magnitude larger DNP enhancement was observed for nanoparticles with 13 nm size compared to particles with 100 nm size. We determined an approximate DNP penetration-depth (~4.2 or ~5.7 nm) for the polarization transfer from electrons to the nuclei of the spherical nanoparticles. Faster DNP polarization buildup was observed for larger nanoparticles. Efficient hyperpolarization of such nanoparticles, as achieved in this work, can be utilized in applications such as magnetic resonance imaging (MRI).

Rapid sequential injections of hyperpolarized [1-13C]pyruvate in vivo using a sub-kelvin, multi-sample DNP polarizer

The development of hyperpolarized technology utilizing dynamic nuclear polarization (DNP) has enabled the rapid measurement of 13C metabolism in vivo with very high SNR. However, with traditional DNP equipment, consecutive injections of a hyperpolarized compound in an animal have been subject to a practical minimum time between injections governed by the polarization build-up time, which is on the order of an hour for [1-13C]pyruvate. This has precluded the monitoring of metabolic changes occurring on a faster time scale. In this study, we demonstrated the ability to acquire in vivo dynamic magnetic resonance spectroscopy (MRS) and 3D magnetic resonance spectroscopic imaging (MRSI) data in normal rats with a 5min interval between injections of hyperpolarized [1-13C]pyruvate using a prototype, sub-Kelvin dynamic nuclear polarizer with the capability to simultaneously polarize up to 4 samples and dissolve them in rapid succession. There were minimal perturbations in the hyperpolarized spectra as a result of the multiple injections, suggesting that such an approach would not confound the investigation of metabolism occurring on this time scale. As an initial demonstration of the application of this technology and approach for monitoring rapid changes in metabolism as a result of a physiological intervention, we investigated the pharmacodynamics of the anti-cancer agent dichloroacetate (DCA), collecting hyperpolarized data before administration of DCA, 1min after administration, and 6min after administration. Dramatic increases in 13C-bicarbonate were detected just 1min (as well as 6min) after DCA administration.

A Super-Wide Bore DNP System for Multiple Sample Polarization: Cryogenic Performance and Polarization at Low Temperature

The volume of polarized sample and the delay required between successive polarizations of samples represent serious constraints for dynamic nuclear polarization (DNP) applications. With these limitations in mind, a DNP polarizer, based on a super-wide bore (150-mm diameter) vertical magnet operating at 3.35 T, was designed. The working diameter for loading/unloading samples is equal to 46 mm and the microwave cavity can accommodate up to three samples. The cryostat can be cooled to 4.2 K in typically 2 h and filled with liquid helium in 1 h. Once filled with liquid helium, the cryostat hold time is on the order of 4 h and a minimum temperature of 1.19 K can be reached. In situ polarization levels at low temperature were measured between 5 and 10 % in single and multiple samples of 13C-labeled urea and glycine.

A Mobile DNP Polarizer for Continuous Flow Applications

Despite its wide applicability in natural sciences, nuclear magnetic resonance (NMR) still suffers from its inherently low sensitivity. This could be overcome by hyperpolarization of molecules via dynamic nuclear polarization (DNP). Here, we introduce a substantial improvement of a mobile Overhauser DNP polarizer, based on an inexpensive Halbach magnet operating at 0.35 T. It shows an almost vanishing magnetic flux at its outer side and does not disturb other instruments. It can be placed directly next to a superconducting magnet, thus reducing the transport time of the hyperpolarized liquid. However, two problems for DNP applications remain. Firstly, radicals are needed which are often toxic. This problem becomes crucial with regard to medical applications. Secondly, the sample must be transported from the polarization magnet to the place of detection like a magnetic resonance imaging (MRI) scanner, and polarization losses due to T1 relaxation may occur. We have implemented a flow system into the mobile DNP polarizer, which overcomes both obstacles. The radicals are immobilized in a gel matrix and the hyperpolarized radical-free fluid is subsequently directly pumped into the MRI scanner. It is shown that even at flow conditions, the NMR signal is enhanced due to Overhauser DNP in the Halbach magnet as well as in the MRI scanner (4.7 T) at a distance of 1.4 m. Acquired images demonstrate the use of enhanced and, due to dipolar coupling, inverted NMR signals, which provide an excellent MRI contrast even for small enhancements.