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Logo of nihpaAbout Author manuscriptsSubmit a manuscriptHHS Public Access; Author Manuscript; Accepted for publication in peer reviewed journal;
 
Angew Chem Int Ed Engl. Author manuscript; available in PMC 2010 November 13.
Published in final edited form as:
PMCID: PMC2980755
NIHMSID: NIHMS148800

Dynamic Nuclear Polarization using a Rigid Biradical**

Dynamic nuclear polarization (DNP) is an approach that can enhance NMR signal intensities of solids and liquids by two to three orders of magnitude. During a DNP experiment, the large Boltzmann polarization of an exogenous or endogenous paramagnetic species, such as a stable free radical, is transferred to the nuclei of interest by microwave (mw) irradiation of the sample at the electron paramagnetic resonance (EPR) frequency. The maximum theoretical enhancement achievable is given by the ratio γsI, where γs and γI are the gyromagnetic ratios of the electron and the nucleus, respectively. The enhanced nuclear polarization is of considerable interest in a variety of applications ranging from particle physics [1, 2] to structural biology [3, 4] and clinical imaging.[5] The mechanism that dominates the electron-nuclear polarization transfer depends on the relative sizes of the homogeneous linewidth, δ, and the inhomogeneous breadth, Δ of the EPR spectrum of the paramagnetic polarizing agent compared to the nuclear Larmor frequency, ω0I. When δ,Δ<ω0I DNP is dominated by the solid-effect (SE), whereas when Δ>ω0I>δ the cross-effect (CE) is operative.[3] In general, the largest signal enhancements observed at high magnetic fields (≥ 5 T) are in experiments where the CE controls the polarization transfer.[6, 7] The underlying mechanism of the CE is a two-step process that involving two electrons with Larmor frequencies ω0S1 and ω0S2 and a nucleus with a frequency ω0I. Initially, the EPR transition of one electron is irradiated and then nuclear polarization is generated in a subsequent three-spin flip-flop process through transitions such as |α1Sβ2SβI> ↔ |β1Sα2SαI> or |β1Sα2SβI> ↔ |α1Sβ2SαI>.[810] Therefore, the CE is optimized when there is a sufficiently strong dipolar coupling between the two electrons, and the difference between the electron Larmor frequencies approximates the nuclear Larmor frequency (ω0S1 – ω0S2 ≈ ± ω0I). These requirements can be more easily fulfilled within a biradical than among dispersed monoradicals,[11] and we have demonstrated that the optimal polarizing agent for experiments in glycerol/water is currently the TEMPO based biradical 1-(TEMPO-4-oxy)-3-(TEMPO-4-amino)propan-2-ol (TOTAPOL) [12] (Figure 1, bottom). However, at high magnetic fields the effective electron resonance frequency can depend strongly on the molecular orientation with respect to the external magnetic field, and in a biradical the matching condition is controlled by the relative orientations of the electron g-tensors. In particular, since the propan-2-ol tether in TOTAPOL is relatively flexible,[6] the relative orientation of the two TEMPO moieties is not well constrained and many orientations do not lead to the correct frequency separation. Therefore, a more rigid tether that locks the two TEMPO moieties at a desirable relative orientation should further increase the enhancement obtained from the polarizing agent.

Figure 1
Molecular Structure of the two biradicals used in DNP experiments described here. Top: bis-TEMPO-bis-ketal (bTbk). The axis system on each side of the molecule shows the direction of the principal g-tensor components of TEMPO for the assumed perfect perpendicular ...

In this report we demonstrate the utility of bis-TEMPO-bis-ketal (bTbk) (Figure 1, top), a biradical consisting of two TEMPO moieties connected with a rigid bis-ketal tether that was originally used to inhibit radical polymerization.[13] In particular we compare and characterized the performance of bTbk and TOTAPOL in DNP experiments under similar experimental conditions.

Earlier studies of a series of TEMPO-based biradicals as polarizing agents in high-field DNP experiments suggested that a conformation in which the two gzz (or gyy) tensor axes of the TEMPO moieties have a dihedral angle of 90° should exhibit improved performance due to efficient frequency matching [6]. This requirement is approximately fulfilled (vide infra) for bTbk (Figure 1, top) due to the odd number of spiranic junctions between the two TEMPO moieties. Specifically, the crystal structure of bTbk shows a dihedral angle between the TEMPO moieties of 82°. Furthermore a calculated average electron-electron distance of 1.18 nm (Figure S1, supporting information) has been confirmed by PELDOR measurements (Figure S2, supporting information). The dihedral angle restrains the gzz (or gyy) tensor components of the two TEMPO moieties in a perpendicular conformation, ensuring a large frequency separation for molecular orientations along these axes. At the same time the short distance provides the large electron-electron dipolar coupling required for an efficient DNP process.

Initial DNP experiments using bTbk are presented in Figure 2. A typical 13C detected 1H bulk polarization build-up curve is shown together with spectra recorded with and without microwave irradiation at fields corresponding to the maximum positive (DNP(+)) and negative (DNP(−)) DNP enhancements (using the pulse sequence given in Figure S3, supporting information). Here, the 1H polarization is monitored by transferring the DNP-enhanced 1H polarization to the 13C nuclei of the urea molecule in a cross-polarization step.[14, 15] At a temperature of 93 K, the build-up time constant τB is 7 s, and a steady state enhancement of ε+ = 250 was observed (Figure 2) at a microwave power of ~2.5 W (estimated power at the sample position). This enhancement is larger than that of TOTAPOL (ε+ = 180), observed under identical experimental conditions (solvent, temperature, mw power).

Figure 2
1H bulk polarization build-up curve for bTbk recorded at a magnetic field position corresponding to DNP(+). The 1H polarization is indirectly detected on the 13C signal of urea via a CP step. The insets show the mw on- and off-signal recorded at field ...

A more reliable comparison between the two polarizing agents can be achieved by comparing the enhancement extrapolated to infinite microwave power ε± This value can be obtained from the microwave power dependence of the DNP enhancement given by

1ε±=1ε±(1+1aP),
(1)

with ε± the steady-state enhancement factor, P the microwave power, and a the saturation parameter, which depends on the microwave transmission efficiency and EPR relaxation properties [6]. Here different instrumental conditions such as the microwave transmission efficiency or EPR relaxation properties only affect ε± and a but not ε±.[6] Nevertheless, the experiments must be performed at similar temperatures for an accurate comparison.

Figure 3 shows the power dependence of the DNP enhancements for bTbk and TOTAPOL from which ε± can be calculated using equation (1). For bTbk and TOTAPOL, the ε+ values are 325 ± 15 and 227 ± 10, respectively. In Table 1 values of ε+ for a series of biradicals previously examined in DNP experiments are compared. Among the polarizing agents investigated to-date, bTbk yields the largest DNP enhancements, approximately 1.4 times larger than that of TOTAPOL.

Figure 3
Power dependence of the steady-state DNP enhancement (ε+) for bTbk and TOTAPOL, recorded under similar experimental conditions.
Table 1
DNP enhancements at infinite microwave powers for different TEMPO based biradicals

The DNP process is most efficient if the sample and the polarizing agent are dispersed in a matrix that forms a rigid glass at cryogenic temperatures. For example, mixtures of DMSO/water (60/40 weight/weight) or glycerol/water (60/40 weight/weight) form rigid glass matrices at 90 K regardless of the cooling rate.[3, 4, 16, 17] The ability of the solvent to form a glass is important in DNP experiments, because it ensures a homogeneous dispersion of the polarizing agent in the sample, and it can concurrently acts as a cryoprotectant. However, in the case of bTbk the main factor presently limiting its applicability in DNP experiments to biological samples is its sparse solubility in media such as glycerol/water (60/40), which is currently the solvent of choice for DNP experiments on proteins. While small amounts of bTbk are soluble in 60/40 DMSO/water, another mixture used frequently for DNP, the solubility is greater at higher DMSO concentrations. However, DMSO requires a minimum water content of 23 % for successful glass formation at 90 K. Therefore, all experiments reported here were performed using a 77/23 DMSO/water mixture.

The reduced water content has a dramatic impact on the observed enhancements. In measurements of ε+ for TOTAPOL in different solvent matrices with a DMSO content of 50, 64 and 77 % we observed that ε+ for 50/50 and 64/36 mixtures of DMSO/water are similar (ε+ ~260), while the observed enhancement is significantly lower at a water content of 23 % (ε+ ~230, see Table 1). This decrease is most likely due to the suboptimal glass forming properties of the 77/23 DMSO/water mixture. Nevertheless in this solvent matrix a maximum enhancement of ε+ = 325 was observed for bTbk: an increase by 40 % if the performance is compared under identical experimental conditions (ε+ = 230 for TOTAPOL). If ε+ is compared under optimal conditions for bTbk and TOTAPOL, then the increase is 25% (ε+ = 260 for TOTAPOL in DMSO/water 60/40). Taken together, these results suggest that still greater DNP enhancements can be expected for a water-soluble form of bTbk.

Since the gyrotron is a fixed frequency oscillator (operating at 139.662 GHz), the optimum field position for the DNP effect is determined by sweeping the magnetic field, B0, and recording the DNP enhancement for each field position. This yields the field-dependent DNP enhancement profile illustrated in Figure 4 (bottom). Besides identifying the fields for maximum enhancements (DNP(+) and DNP(–)), the DNP profile provides other important information that can lead to possible improvements of the performance of the polarizing agent.

Figure 4
Field dependence of the DNP enhancement profiles and EPR spectrum of bTbk. Top: 140 GHz echo detected EPR spectrum of bTbk in DMSO/H2O (77/23), T = 20 K, tp(π/2) = 60 ns, τ = 300 ns. Bottom: 1H detected DNP field profile of bTbk (solid ...

The DNP enhancement profile is closely related to the high-field EPR spectrum, which is shown for bTbk in Figure 4 (top). Since the electron-electron dipolar coupling is relatively small (~ 30 MHz) compared to the breadth of the EPR spectrum, the lineshape resembles that of a monomeric nitroxide-based radical at high fields, dominated by the large anisotropy of the g and the 14N hyperfine tensors. Since the overall inhomogeneous spectral width at 140 GHz is Δ ~ 640 MHz, the CE is the dominant DNP mechanism. In our current DNP instrument, the microwave excitation bandwidth is in the range of a few MHz, and is small compared to the inhomogeneous breadth of the EPR spectrum, Δ. Hence, only a small portion of the EPR spectrum is excited by the microwave radiation, corresponding to a particular set of molecular orientations. This phenomenon is referred to as ‘orientation selection’ and is well known in EPR/ENDOR spectroscopy.[18, 19] For nitroxide-based radicals, the orientation selection is facilitated by the large anisotropy of the g- and the 14N hyperfine tensor (gxx = 2.00980, gyy = 2.00622, gzz = 2.00220, Axx = 17.0, Ayy = 20.5, Azz = 95.9 MHz for TEMPO [20]). Furthermore, among the excited spins, only those satisfying the matching condition ω0S1 – ω0S2 ≈ ± ω0I contribute significantly to the DNP effect.[9, 10] Thus, for an inhomogeneously broadened EPR line with δ> ω0I > Δ, this two step process (orientation selection and frequency matching) governs the field dependence of the DNP effect.

The field-dependent DNP enhancement profile of bTbk (Figure 4, bottom) shows a maximum positive enhancement at a field position corresponding to 212.058 MHz 1H Larmor frequency (DNP(+)) and a maximum negative enhancement at 211.516 MHz (DNP(−)), separated by 542 kHz (357 MHz for e). The zero crossing occurs at ~211.8 MHz coinciding with the maximum absorption in the EPR spectrum (gyy tensor component of TEMPO).

The DNP enhancement profile recorded for bTbk shows a pronounced asymmetry across the EPR line, conveniently described by the ratio of the maximum negative and positive enhancement ε+, which is 0.62 for bTbk (Figure 4, bottom, solid line). The same asymmetry is observed if the 1H polarization is measured through indirect 13C detection, giving enhancement factors of ε+ = 250 and ε = 155 (see Figure 2, insets). This asymmetry of the enhancement profile observed for bTbk is more pronounced than for previously studied biradicals, including TOTAPOL and BTUrea, for which a smaller asymmetry of ε+ = 0.84 is observed [12] (Figure 4). In addition, other TEMPO based biradicals, such as BT2E showed a similar asymmetry factor of ~0.8,[12] while the DNP enhancement profile for monomeric TEMPO is almost symmetric (ε+ ~ 1).[21, 22] These observations suggest that the origin of the asymmetry is an intrinsic feature of TEMPO based biradicals, and that the extent of the observed asymmetry is a result the flexibility/rigidity of the connecting tether and the relative orientation of the two TEMPO rings. Numerical simulations are currently in progress to investigate this behavior in more detail.

In conclusion, our experiments demonstrate the superior performance of the biradical bTbk when compared to other TEMPO biradicals thus far used in DNP experiments. The enhancement factors obtained with bTbk are about 1.4 times larger than for TOTAPOL under identical experimental conditions. However, due to its limited solubility, bTbk requires the use of a modified solvent matrix with reduced water content. This compromises the DNP efficiency, and limits the applicability of bTbk to biological systems that require glycerol/water matrices. Concurrently, the larger enhancements observed under these suboptimal conditions provides the motivation for the development of H2O soluble bTbk derivatives and other polarizing agents with strong e-e dipole couplings, rigid tethers, and the correct relative orientations of their associated g-tensors.

Experimental Section

Synthesis

The biradical bTbk was synthesized in a two-step sequence with 35% overall yield. The bispiroketal skeleton was obtained by reacting pentaerythritol (0.87 g, 6.4 mmol) with 2,2,6,6-tetramethyl-4-piperidone (2.00 g, 12.8 mmol) in the presence of p-toluenesulfonic acid (2.21 g, 12.8 mmol) in toluene at reflux. The biradical bTbk was obtained as orange crystals by oxidation of the corresponding diamine at 0°C by 1.5 equivalents of MCPBA in CH2Cl2. Detailed instructions and characterization are provided as supporting information.

Sample preparation

For DNP experiments 9 mM solutions of bTbk or TOTAPOL in d6-DMSO/D2O/H2O (77/17/6) were prepared. The small amount of H2O is required to optimize the diffusion of the local DNP enhanced nuclear polarization to neighboring nuclei, and is held fixed at 6 % for all samples. For matrix studies two more TOTAPOL samples were prepared in d6-DMSO/D2O/H2O (64/30/6) and d6-DMSO/D2O/H2O (50/44/6). The TOTAPOL concentration was held constant at 9 mM in order to facilitate a direct comparison with bTbk. All DNP samples contained 2M 13C-urea to optimize detection of the NMR signal. The high concentration facilitates observation of the microwave off-signal (no DNP enhancement) in a reasonable time period. For EPR measurements a 2 mM solution of bTbk in DMSO/H2O (77/23) was prepared. All solvent mixtures are given in weight percentage.

DNP experiments

DNP experiments were performed on a custom designed DNP/NMR spectrometer using a triple-resonance cryogenic MAS probe (e, 1H, and 13C) with a commercial 2.5 mm rotor stator (Revolution NMR Inc.). The spectrometer operates at a magnetic field of 5 T, corresponding to a Larmor frequency of 140 GHz for e and 211 MHz for 1H. The enhanced 1H polarization was indirectly detected, via observation of the cross-polarized 13C spectrum. The high power microwave radiation is generated by a gyrotron, a vacuum electron device capable of producing high-power (>10 W) millimeter waves, running at a frequency of 139.662 GHz [21, 23, 24]. The DNP sample is placed in a 2.5 mm sapphire rotor. Finally, the 5 T superconducting magnet is equipped with a superconducting sweep coil that allows the field to be swept over ±750 G to record the DNP field profile and to adjust the magnetic field for maximum enhancements.

EPR experiments

EPR experiments were performed on a custom designed high field EPR spectrometer described earlier [18, 21] running at a microwave frequency of 139.504 GHz. The sample of ~ 250 nL is placed in Suprasil quartz tube of 0.55 mm outer diameter. EPR spectra were recorded using a two-pulse echo sequence (π/2 – τ – π̃ – τ – echo) by integrating the echo intensity while sweeping the magnetic field. Detailed experimental conditions are given in the figure caption. For accurate field measurements the spectrometer is equipped with a field/frequency lock system.[25]

Supplementary Material

Supp fig 01

Footnotes

**The authors thank Sandrine Lambert for technical assistance, Galia Debelouchina, Albert Smith, Alexander Barnes and Jean-Pierre Finet for many stimulating discussions. This research was supported by the National Institutes of Health through grants EB002804, EB002026, EB009866, EB001965 and EB001035 and by the EU-Design Study Bio-DNP in Framework 6. T.M. acknowledges receipt of a postdoctoral fellowship of the Deutsche Forschungs Gemeinschaft. Y.M. acknowledges partial financial support from the Naito foundation.

Supporting information for this article is available on the WWW under http://www.angewandte.org or from the author.

Contributor Information

Dr. Yoh Matsuki, Francis Bitter Magnet Laboratory and Department of Chemistry, Massachusetts Institute of Technology, Cambridge MA 02139 (USA) Department of Chemistry, Brandeis University, Waltham MA 02454 (USA)

Dr. Thorsten Maly, Francis Bitter Magnet Laboratory and Department of Chemistry, Massachusetts Institute of Technology, Cambridge MA 02139 (USA)

Dr. Olivier Ouari, CNRS-UMR 6517, Chemistry, Biology and Free Radicals, University of Aix-Marsailles I et III, Marseille (France)

Dr. Hakim Karoui, LCP CNRS-UMR 6264, University de Provence, 13397 Marseilles Cedex 20 (France)

Dr. François Le Moigne, LCP CNRS-UMR 6264, University de Provence, 13397 Marseilles Cedex 20 (France)

Dr. Egon Rizzato, LCP CNRS-UMR 6264, University de Provence, 13397 Marseilles Cedex 20 (France)

Dr. Sevdalina Lyubenova, Institute of Physical and Theoretical Cchemistry and Center for Biomolecular Magnetic Resonance, 60438 Frankfurt (Germany)

Judith Herzfeld, Department of Chemistry, Brandeis University, Waltham MA 02454 (USA)

Thomas Prisner, Institute of Physical and Theoretical Cchemistry and Center for Biomolecular Magnetic Resonance, 60438 Frankfurt (Germany)

Paul Tordo, CNRS-UMR 6517, Chemistry, Biology and Free Radicals, University of Aix-Marsailles I et III, Marseille (France)

Robert G. Griffin, Francis Bitter Magnet Laboratory and Department of Chemistry, Massachusetts Institute of Technology, Cambridge MA 02139 (USA)

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