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dc.contributor.authorNi, Qing Zhe
dc.contributor.authorDaviso, Eugenio
dc.contributor.authorMarkhasin, Evgeny
dc.contributor.authorHerzfeld, Judith
dc.contributor.authorGriffin, Robert Guy
dc.contributor.authorTemkin, Richard J
dc.contributor.authorCan, Thach V
dc.contributor.authorSwager, Timothy M
dc.contributor.authorJawla, Sudheer K.
dc.date.accessioned2015-02-18T21:21:16Z
dc.date.available2015-02-18T21:21:16Z
dc.date.issued2013-04
dc.date.submitted2012-12
dc.identifier.issn0001-4842
dc.identifier.issn1520-4898
dc.identifier.urihttp://hdl.handle.net/1721.1/94622
dc.description.abstractDuring the three decades 1980–2010, magic angle spinning (MAS) NMR developed into the method of choice to examine many chemical, physical, and biological problems. In particular, a variety of dipolar recoupling methods to measure distances and torsion angles can now constrain molecular structures to high resolution. However, applications are often limited by the low sensitivity of the experiments, due in large part to the necessity of observing spectra of low-γ nuclei such as the I = [1 over 2] species [superscript 13]C or [superscript 15]N. The difficulty is still greater when quadrupolar nuclei, such as [superscript 17]O or [superscript 27]Al, are involved. This problem has stimulated efforts to increase the sensitivity of MAS experiments. A particularly powerful approach is dynamic nuclear polarization (DNP) which takes advantage of the higher equilibrium polarization of electrons (which conventionally manifests in the great sensitivity advantage of EPR over NMR). In DNP, the sample is doped with a stable paramagnetic polarizing agent and irradiated with microwaves to transfer the high polarization in the electron spin reservoir to the nuclei of interest. The idea was first explored by Overhauser and Slichter in 1953. However, these experiments were carried out on static samples, at magnetic fields that are low by current standards. To be implemented in contemporary MAS NMR experiments, DNP requires microwave sources operating in the subterahertz regime, roughly 150–660 GHz, and cryogenic MAS probes. In addition, improvements were required in the polarizing agents, because the high concentrations of conventional radicals that are required to produce significant enhancements compromise spectral resolution. In the last two decades, scientific and technical advances have addressed these problems and brought DNP to the point where it is achieving wide applicability. These advances include the development of high frequency gyrotron microwave sources operating in the subterahertz frequency range. In addition, low temperature MAS probes were developed that permit in situ microwave irradiation of the samples. And, finally, biradical polarizing agents were developed that increased the efficiency of DNP experiments by factors of ~4 at considerably lower paramagnet concentrations. Collectively, these developments have made it possible to apply DNP on a routine basis to a number of different scientific endeavors, most prominently in the biological and material sciences. This Account reviews these developments, including the primary mechanisms used to transfer polarization in high frequency DNP, and the current choice of microwave sources and biradical polarizing agents. In addition, we illustrate the utility of the technique with a description of applications to membrane and amyloid proteins that emphasizes the unique structural information that is available in these two cases.en_US
dc.description.sponsorshipNational Institutes of Health (U.S.) (Grant EB-001960)en_US
dc.description.sponsorshipNational Institutes of Health (U.S.) (Grant EB-002804)en_US
dc.description.sponsorshipNational Institutes of Health (U.S.) (Grant EB-003151)en_US
dc.description.sponsorshipNational Institutes of Health (U.S.) (Grant EB-001035)en_US
dc.description.sponsorshipNational Institutes of Health (U.S.) (Grant GM-095843)en_US
dc.description.sponsorshipNational Institutes of Health (U.S.) (Grant EB-002026)en_US
dc.language.isoen_US
dc.publisherAmerican Chemical Society (ACS)en_US
dc.relation.isversionofhttp://dx.doi.org/10.1021/ar300348nen_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.titleHigh Frequency Dynamic Nuclear Polarizationen_US
dc.typeArticleen_US
dc.identifier.citationNi, Qing Zhe, Eugenio Daviso, Thach V. Can, Evgeny Markhasin, Sudheer K. Jawla, Timothy M. Swager, Richard J. Temkin, Judith Herzfeld, and Robert G. Griffin. “High Frequency Dynamic Nuclear Polarization.” Accounts of Chemical Research 46, no. 9 (September 17, 2013): 1933–1941.en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Chemistryen_US
dc.contributor.departmentMassachusetts Institute of Technology. Plasma Science and Fusion Centeren_US
dc.contributor.departmentFrancis Bitter Magnet Laboratory (Massachusetts Institute of Technology)en_US
dc.contributor.mitauthorNi, Qing Zheen_US
dc.contributor.mitauthorDaviso, Eugenioen_US
dc.contributor.mitauthorCan, Thach Vanen_US
dc.contributor.mitauthorMarkhasin, Evgenyen_US
dc.contributor.mitauthorSwager, Timothy Manningen_US
dc.contributor.mitauthorTemkin, Richard J.en_US
dc.contributor.mitauthorJawla, Sudheer Kumaren_US
dc.contributor.mitauthorGriffin, Robert Guyen_US
dc.relation.journalAccounts of Chemical Researchen_US
dc.eprint.versionAuthor's final manuscripten_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/PeerRevieweden_US
dspace.orderedauthorsNi, Qing Zhe; Daviso, Eugenio; Can, Thach V.; Markhasin, Evgeny; Jawla, Sudheer K.; Swager, Timothy M.; Temkin, Richard J.; Herzfeld, Judith; Griffin, Robert G.en_US
dc.identifier.orcidhttps://orcid.org/0000-0003-1589-832X
dc.identifier.orcidhttps://orcid.org/0000-0001-9813-0177
dc.identifier.orcidhttps://orcid.org/0000-0001-9092-612X
mit.licensePUBLISHER_POLICYen_US
mit.metadata.statusComplete


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