Resistively-Detected NMR and Nuclear Resonance Imaging

By Yoshiro Hirayama

Department of Physics, Tohoku University, Sendai, Japan

Published on

Abstract

NMR provides us versatile tool to physical, chemical, biological, and medical characterizations. However, conventional NMR suffers low sensitivity and cannot be applied to semiconductor quantum systems, such as single quantum well or wire. To overcome these difficulties, resistively-detected NMR(RDNMR)has been developed, especially for GaAs based quantum structures [1].

The Knight-shift gives us information of electron spin polarization and nuclear relaxation (T1time) includes information of electron spin fluctuations. Many interesting physics are unveiled in two-dimensional electron systems, especially in the quantum Hall regime. The clear difference between ground and second Landau-level is clarified by Knight-shift measurements up to high temperature regime where fractional quantum Hall effect disappears [2]. The RDNMR measurements can be applied to not only GaAs but InSb two-dimensional systems. The interesting characteristics of quantum Hall ferromagnet is clarified by using RDNMR studies in InSb quantum systems [3]. Nuclear-related measurements are also powerful to study interaction between ensemble of nuclear spins and electron spins. The obtained results suggest novel possibilities including a super-radiance from nuclear spin ensembles [4].

It is interesting that the RDNMR measurements can be extended in nanoscale characterization. A combination of scanning gate technique and RDNMR results in successful two-dimensional mapping of Knight-shift, i.e. electron spin polarization, using quantum Hall breakdown phenomenaas an example [5]. Successful RDNMR of one-dimensional quantum-point contacts [6] can be connected to sensitive detection of microscopic strain distribution in semiconductor quantum devices [7].

Bio

Yoshiro Hirayama Professor Yoshiro Hirayama received his Ph.D. from the University of Tokyo in 1983 and joined NTT Basic Research Laboratories. In NTT, he served as Group Leader, Distinguished Technical Member and Executive Manager. He was a guest scientist in Max-Planck-Institute (Stuttgart) during 1990-1991 and in Paul-Drude-Institute (Belrin) in 2004. He was appointed Professor at Tohoku University in 2006. He is now director, Center for Science and Innovation in Spintronics (CSIS), Tohoku University, and coordinator, Graduate Program in Spintronics (GP-Spin), Tohoku University. His current research interests are transport properties of semiconductor heterostructurs and nanostructures, especially putting emphasis on carrier interactions and coherent control including manipulation of nuclear spins in semiconductors. He received JJAP Best Paper Award (2004, 2008), ISCS Quantum Device Award (2013), and other awards. He has been Fellow of Institute of Physics (IOP, London) and Fellow of the Japan Society of Applied Physics (JSAP). He is also serving MEXT Grant-in-Aid for Scientific Research on Innovative Areas “Science of Hybrid Quantum Systems” (2015-2020) as project leader.

Credits

These studies are supported by KAKENHI Grants Nos. 18H01811 and 15H05867

Sponsored by

References

  1. Y. Hirayama et al., Semicond. Sci. Technol. 24, 023001 (2009) [Topical Review]; Y. Hirayama, Chapter 38, Quantum Hall Effects (3rd Edition) (World Scientific, 2013).
  2. L. Tiemann et al., Science 335, 828 (2012); S. Hasegawa et al. (in preparation).
  3. H. W. Liu et al., Phys. Rev. B82, 241304(RC) (2010); K. F. Yang et al., Nature Comm. 8, 15084 (2017); K. F. Yang etal., New J.Physics 21, 083004 (2019).
  4. M. H. Fauzi et al., Phys. Rev. B90, 235308 (2014); Y. Hama et al., New J. Physics 18, 023027 (2016); Y. Hama et al., Phys. Rev. Lett. 120, 060403 (2018); M. H. Fauzi et al., (in preparation).
  5. K. Hashimoto et al., AIP Advances 6, 075024 (2016); K. Hashimoto et al., Nature Comm. 9, 2215 (2018).
  6. A. Noorhidayati et al., poster in this workshop.
  7. M. H. Fauzi et al., arXiv:1812.08935 [Phys. Rev. Lett. (under review)].

Cite this work

Researchers should cite this work as follows:

  • Yoshiro Hirayama (2020), "Resistively-Detected NMR and Nuclear Resonance Imaging," https://nanohub.org/resources/33427.

    BibTex | EndNote

Time

Location

Burton Morgan, Room 121, Purdue University, West Lafayette, IN

Tags

Resistively-Detected NMR and Nuclear Resonance Imaging
  • Resistively-detected NMR and nuclear resonance imaging 1. Resistively-detected NMR and n… 0
    00:00/00:00
  • Outline 2. Outline 17.617617617617618
    00:00/00:00
  • Outline 3. Outline 43.343343343343342
    00:00/00:00
  • Standard NMR: Advantage and Disadvantage 4. Standard NMR: Advantage and Di… 49.315982649315984
    00:00/00:00
  • Hyperfine Interaction in Quantum Systems 5. Hyperfine Interaction in Quant… 123.8571905238572
    00:00/00:00
  • Pump and Probe NMR Measurements 6. Pump and Probe NMR Measurement… 231.69836503169839
    00:00/00:00
  • Outline 7. Outline 306.07273940607274
    00:00/00:00
  • T1 time measurements 8. T1 time measurements 318.01801801801804
    00:00/00:00
  • Knight Shift in NMR Spectrum 9. Knight Shift in NMR Spectrum 387.42075408742079
    00:00/00:00
  • Knight Shift Measurements 10. Knight Shift Measurements 443.07640974307645
    00:00/00:00
  • RDNMR in InSb 2D electron system 11. RDNMR in InSb 2D electron syst… 568.968968968969
    00:00/00:00
  • Role of Chiral Edge for Nuclear Polarization 12. Role of Chiral Edge for Nuclea… 655.75575575575579
    00:00/00:00
  • Reciprocity of RDNMR Signal in QHF 13. Reciprocity of RDNMR Signal in… 696.2295628962296
    00:00/00:00
  • Outline 14. Outline 740.54054054054052
    00:00/00:00
  • Scanning Gate Probe and Microscopic Imaging 15. Scanning Gate Probe and Micros… 769.30263596930263
    00:00/00:00
  • Imaging of NR Signal in the QH Breakdown 16. Imaging of NR Signal in the QH… 781.247914581248
    00:00/00:00
  • Scanning Gate Probe : Tip Bias Effect 17. Scanning Gate Probe : Tip Bias… 815.58224891558223
    00:00/00:00
  • Microscopic NR by RF Electric Field 18. Microscopic NR by RF Electric … 845.17851184517849
    00:00/00:00
  • Two-Dimensional Mapping of NR Intensity 19. Two-Dimensional Mapping of NR … 899.9666332999667
    00:00/00:00
  • Two-Dimensional Mapping of NR Knight Shift 20. Two-Dimensional Mapping of NR … 947.34734734734741
    00:00/00:00
  • Knight Shift Variation vs. Breakdown Driving Current 21. Knight Shift Variation vs. Bre… 989.98998998999
    00:00/00:00
  • Successful RDNMR in QPC (Quantum Point Contact) 22. Successful RDNMR in QPC (Quant… 1050.1835168501837
    00:00/00:00
  • Strain Detection in Quantum Point Contact 23. Strain Detection in Quantum Po… 1096.6966966966968
    00:00/00:00
  • Concluding Remarks 24. Concluding Remarks 1191.5248581915248
    00:00/00:00
  • Acknowledgements 25. Acknowledgements 1265.6656656656658
    00:00/00:00