“…Low field experiments were carried out on a field-cycling NMR spectrometer with B 0 = 7 T that is described before [24]. High field experiments and ultralow field SABRE [25] experiments were carried out on a Bruker AVANCE III HD NMR spectrometer with B 0 = 9.4 T. Enhancement factors were obtained in respect to corresponding thermal signal at 9.4 T for 15 N and at 7 T for 1 H. All spectra shown in the main text were recorded with a single scan.…”
Section: Materials and Experimental Detailsmentioning
confidence: 99%
“…For this reason, first of all we would like to see whether the stabilized complex can be used for generating hyperpolarization in conventional low-field SABRE experiments (LF-SABRE). For this purpose we used a field-cycling NMR spectrometer with B 0 = 7 T that allows one to bubble pH 2 through the solution at variable magnetic field from 0.1 mT up to 7 T and to detect high-resolution 1 H-NMR spectra [24] at the detection field B 0 within < 0.4 s. The principal experimental scheme of a LF-SABRE experiment is shown in Figure 1A. The LF-SABRE experiment consists of three stages: (stage 1) SABRE polarization is created at a field B by bubbling pH 2 through the solution, then (stage 2) during the time period τ fs ≈ 0.4 s sample is transferred to the detection field B 0 = 7 T, and, finally, (stage 3) after a 90° RF pulse the free induction decay (FID) is measured.…”
Section: H-sabre Field Dependence (Low Field Sabre)mentioning
confidence: 99%
“…SABRE experiments at low magnetic fields are relatively simple, however, they require developing additional hardware for changing the external magnetic field and for shuttling the sample from the polarization to the detection field [24]. To get around these technical problems, recently several methods for generation of high-field SABRE polarization have been proposed [12,14,16,33].…”
Section: Sabre At High Field and 15 N-rfoff Pulse Sequencementioning
A strong limitation of nuclear magnetic resonance is its low inherent sensitivity that can be overcome by using an appropriate hyperpolarization technique. Presently, dynamic nuclear polarization and spin-exchange optical pumping are the only hyperpolarization techniques that are used in applied medicine. However, both are relatively complex in use and expensive. Here we present a modification of the signal amplification by reversible exchange (SABRE) hyperpolarization method -SABRE on stabilized Ir-complexes. A stabilized Ir-complex (here we used bipyridine for stabilization) can be hyperpolarized in a wide range of magnetic fields from a few μT upto 10 T with 15 N polarization of about 1-3%. Moreover, the investigated complex can be incorporated into biomolecules or other bulky molecules; in this situation exchange with para-hydrogen will allow one to continuously generate hyperpolarization.
“…Low field experiments were carried out on a field-cycling NMR spectrometer with B 0 = 7 T that is described before [24]. High field experiments and ultralow field SABRE [25] experiments were carried out on a Bruker AVANCE III HD NMR spectrometer with B 0 = 9.4 T. Enhancement factors were obtained in respect to corresponding thermal signal at 9.4 T for 15 N and at 7 T for 1 H. All spectra shown in the main text were recorded with a single scan.…”
Section: Materials and Experimental Detailsmentioning
confidence: 99%
“…For this reason, first of all we would like to see whether the stabilized complex can be used for generating hyperpolarization in conventional low-field SABRE experiments (LF-SABRE). For this purpose we used a field-cycling NMR spectrometer with B 0 = 7 T that allows one to bubble pH 2 through the solution at variable magnetic field from 0.1 mT up to 7 T and to detect high-resolution 1 H-NMR spectra [24] at the detection field B 0 within < 0.4 s. The principal experimental scheme of a LF-SABRE experiment is shown in Figure 1A. The LF-SABRE experiment consists of three stages: (stage 1) SABRE polarization is created at a field B by bubbling pH 2 through the solution, then (stage 2) during the time period τ fs ≈ 0.4 s sample is transferred to the detection field B 0 = 7 T, and, finally, (stage 3) after a 90° RF pulse the free induction decay (FID) is measured.…”
Section: H-sabre Field Dependence (Low Field Sabre)mentioning
confidence: 99%
“…SABRE experiments at low magnetic fields are relatively simple, however, they require developing additional hardware for changing the external magnetic field and for shuttling the sample from the polarization to the detection field [24]. To get around these technical problems, recently several methods for generation of high-field SABRE polarization have been proposed [12,14,16,33].…”
Section: Sabre At High Field and 15 N-rfoff Pulse Sequencementioning
A strong limitation of nuclear magnetic resonance is its low inherent sensitivity that can be overcome by using an appropriate hyperpolarization technique. Presently, dynamic nuclear polarization and spin-exchange optical pumping are the only hyperpolarization techniques that are used in applied medicine. However, both are relatively complex in use and expensive. Here we present a modification of the signal amplification by reversible exchange (SABRE) hyperpolarization method -SABRE on stabilized Ir-complexes. A stabilized Ir-complex (here we used bipyridine for stabilization) can be hyperpolarized in a wide range of magnetic fields from a few μT upto 10 T with 15 N polarization of about 1-3%. Moreover, the investigated complex can be incorporated into biomolecules or other bulky molecules; in this situation exchange with para-hydrogen will allow one to continuously generate hyperpolarization.
“…To couple light in and to direct it onto the sample one can use light‐guides or optical fibers. In the literature, schemes of sample irradiation from top as well as from the side have been described. In the latter case, irradiation is performed through a window of the NMR saddle‐shaped coil.…”
In this work, we review the hyperpolarization technique named chemically induced dynamic nuclear polarization (CIDNP), focusing on the time‐resolved variant of this method and its biological applications. We introduce the main principles of polarization formation in liquids at high magnetic fields, provided by the so‐called spin sorting mechanism. Applications of CIDNP to studying fast reactions of short‐lived free radicals of biologically important molecules are discussed, as well as the potential of the method to probe the structure and magnetic parameters of such radicals. We also explain the principles of protein CIDNP and discuss applications of time‐resolved CIDNP to studies of protein structure and dynamics.
“…SABRE hyperpolarization. [18] In this work, we have employed the flow system described in Refs. During the lifetime of the complex, the spin order of pH 2 is converted to nuclear hyperpolarization in analytes.…”
DOSY is an NMR spectroscopy technique that resolves resonances according to the analytes' diffusion coefficients. It has found use in correlating NMR signals and estimating the number of components in mixtures. Applications of DOSY in dilute mixtures are, however, held back by excessively long measurement times. We demonstrate herein, how the enhanced NMR sensitivity provided by SABRE hyperpolarization allows DOSY analysis of low-micromolar mixtures, thus reducing the concentration requirements by at least 100-fold.
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