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dc.contributor.authorCan, Thach V
dc.contributor.authorWalish, Joseph John
dc.contributor.authorSwager, Timothy M
dc.contributor.authorGriffin, Robert Guy
dc.date.accessioned2022-02-07T20:01:01Z
dc.date.available2017-06-26T20:14:24Z
dc.date.available2022-02-07T20:01:01Z
dc.date.issued2015-08
dc.date.submitted2015-04
dc.identifier.issn0021-9606
dc.identifier.issn1089-7690
dc.identifier.urihttps://hdl.handle.net/1721.1/110278.2
dc.description.abstractWe present results of a pulsed dynamic nuclear polarization (DNP) study at 0.35 T (9.7 GHz/14.7 MHz for electron/1H Larmor frequency) using a lab frame-rotating frame cross polarization experiment that employs electron spin locking fields that match the 1H nuclear Larmor frequency, the so called NOVEL (nuclear orientation via electron spin locking) condition. We apply the method to a series of DNP samples including a single crystal of diphenyl nitroxide (DPNO) doped benzophenone (BzP), 1,3-bisdiphenylene-2-phenylallyl (BDPA) doped polystyrene (PS), and sulfonated-BDPA (SA-BDPA) doped glycerol/water glassy matrices. The optimal Hartman-Hahn matching condition is achieved when the nutation frequency of the electron matches the Larmor frequency of the proton, ω[subscript 1S] = ω[subscript 0I], together with possible higher order matching conditions at lower efficiencies. The magnetization transfer from electron to protons occurs on the time scale of ∼100 ns, consistent with the electron-proton couplings on the order of 1-10 MHz in these samples. In a fully protonated single crystal DPNO/BzP, at 270 K, we obtained a maximum signal enhancement of ε = 165 and the corresponding gain in sensitivity of ε(T[subscript 1]/T[subscript B])[superscript 1/2] = 230 due to the reduction in the buildup time under DNP. In a sample of partially deuterated PS doped with BDPA, we obtained an enhancement of 323 which is a factor of ∼3.2 higher compared to the protonated version of the same sample and accounts for 49% of the theoretical limit. For the SA-BDPA doped glycerol/water glassy matrix at 80 K, the sample condition used in most applications of DNP in nuclear magnetic resonance, we also observed a significant enhancement. Our findings demonstrate that pulsed DNP via the NOVEL sequence is highly efficient and can potentially surpass continuous wave DNP mechanisms such as the solid effect and cross effect which scale unfavorably with increasing magnetic field. Furthermore, pulsed DNP is also a promising avenue for DNP at high temperature.en_US
dc.description.sponsorshipNational Institute for Biomedical Imaging and Bioengineering (U.S.) (Grant No. EB-002804)en_US
dc.description.sponsorshipNational Institute for Biomedical Imaging and Bioengineering (U.S.) (Grant No. EB-002026)en_US
dc.description.sponsorshipNational Institute of General Medical Sciences (U.S.) (Grant No. GM095843)en_US
dc.language.isoen_US
dc.publisherAIP Publishingen_US
dc.relation.isversionofhttp://dx.doi.org/10.1063/1.4927087en_US
dc.rightsArticle is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use.en_US
dc.sourcePMCen_US
dc.titleTime domain DNP with the NOVEL sequenceen_US
dc.typeArticleen_US
dc.identifier.citationCan, T. V., J. J. Walish, T. M. Swager, and R. G. Griffin. “Time Domain DNP with the NOVEL Sequence.” J. Chem. Phys. 143, no. 5 (August 7, 2015): 054201. © 2015 AIP Publishing LLC.en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Chemistryen_US
dc.contributor.departmentFrancis Bitter Magnet Laboratory (Massachusetts Institute of Technology)en_US
dc.contributor.mitauthorCan, Thach V
dc.contributor.mitauthorWalish, Joseph John
dc.contributor.mitauthorSwager, Timothy M
dc.contributor.mitauthorGriffin, Robert Guy
dc.relation.journalJournal of Chemical Physicsen_US
dc.eprint.versionFinal published versionen_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/PeerRevieweden_US
dspace.orderedauthorsCan, T. V.; Walish, J. J.; Swager, T. M.; Griffin, R. G.en_US
dspace.embargo.termsNen_US
dc.identifier.orcidhttps://orcid.org/0000-0001-9092-612X
dc.identifier.orcidhttps://orcid.org/0000-0003-1589-832X
mit.licensePUBLISHER_POLICYen_US
mit.metadata.statusReady for Final Reviewen_US


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