Dynamic nuclear polarization and ESR hole burning in As doped silicon

dc.contributor.authorJ. Järvinen D. Zvezdov
dc.contributor.authorJ. Ahokas
dc.contributor.authorS. Sheludiakov
dc.contributor.authorL. Lehtonen
dc.contributor.authorS. Vasiliev
dc.contributor.authorL. Vlasenko
dc.contributor.authorY. Ishikawad
dc.contributor.authorY. Fujiid
dc.contributor.organizationfi=Wihurin fysiikantutkimuslaboratorio|en=Wihuri Physical Laboratory|
dc.contributor.organizationfi=kvanttioptiikan laboratorio|en=Laboratory of Quantum Optics|
dc.contributor.organizationfi=teoreettisen fysiikan laboratorio|en=Laboratory of Theoretical Physics|
dc.contributor.organization-code1.2.246.10.2458963.20.14547848953
dc.contributor.organization-code1.2.246.10.2458963.20.26581883332
dc.contributor.organization-code1.2.246.10.2458963.20.63398691327
dc.contributor.organization-code2606701
dc.converis.publication-id48443441
dc.converis.urlhttps://research.utu.fi/converis/portal/Publication/48443441
dc.date.accessioned2022-10-28T12:41:15Z
dc.date.available2022-10-28T12:41:15Z
dc.description.abstractWe present an experimental study of the Dynamic Nuclear Polarization (DNP) of Si-29 nuclei in silicon crystals of natural abundance doped with As in the temperature range 0.1-1 K and in a strong magnetic field of 4.6 T. This ensures a very high degree of electron spin polarization, extremely slow nuclear relaxation and optimal conditions for realization of Overhauser and resolved solid effects. We found that the solid effect DNP leads to the appearance of a pattern of holes and peaks in the ESR line, separated by the super-hyperfine interaction between the donor electron and Si-29 nuclei closest to the donor. On the contrary, the Overhauser effect DNP mainly affects the remote Si-29 nuclei having the weakest interaction with the donor electron. This leads to the appearance of a very narrow (approximate to 3 mG wide) hole in the ESR line. We studied relaxation of the holes after burning, which is caused by the nuclear spin diffusion. Analyzing the dynamics of the hole in the spectrum with a simple one-dimensional diffusion model leads to a value of the diffusion coefficient D = 8(3) x 10(-9) G(2) s(-1). Our data indicate that the spin diffusion is not completely prevented even in the frozen core near the donors. The emergence of the narrow hole after the Overhauser DNP may be explained by a partial "softening" of the frozen core caused by decoupling of the donor electron and remote Si-29 nuclei.
dc.format.pagerange10227
dc.format.pagerange10237
dc.identifier.eissn1463-9084
dc.identifier.jour-issn1463-9076
dc.identifier.olddbid178229
dc.identifier.oldhandle10024/161323
dc.identifier.urihttps://www.utupub.fi/handle/11111/37410
dc.identifier.urnURN:NBN:fi-fe2021042826061
dc.language.isoen
dc.okm.affiliatedauthorJärvinen, Jarno
dc.okm.affiliatedauthorAhokas, Janne
dc.okm.affiliatedauthorSheludiakov, Sergei
dc.okm.affiliatedauthorLehtonen, Lauri
dc.okm.affiliatedauthorVasiliev, Sergey
dc.okm.discipline114 Physical sciencesen_GB
dc.okm.discipline114 Fysiikkafi_FI
dc.okm.internationalcopublicationinternational co-publication
dc.okm.internationalityInternational publication
dc.okm.typeA1 ScientificArticle
dc.publisherROYAL SOC CHEMISTRY
dc.relation.doi10.1039/c9cp06859g
dc.relation.ispartofjournalPhysical Chemistry Chemical Physics
dc.relation.issue18
dc.relation.volume22
dc.source.identifierhttps://www.utupub.fi/handle/10024/161323
dc.titleDynamic nuclear polarization and ESR hole burning in As doped silicon
dc.year.issued2020

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