(a) Schematic of a SHPM setup. (b) An optical image of the Hall sensor (scale bar 20 μm) and an electron micrograph of the Hall cross (scale bar 1 μm). (c) Schematic of the local heating in an Au/Ge/Pb/SiO2/Si multilayer by the STM tip. Superconductivity is suppressed in near a vortex. (d) SHPM image of a vortex lattice (individual vortex size ~1 μm). (e) SHPM image after applying a tunneling current and then lifting up the STM tip for Hall probe imaging. A vortex cluster forms at the tip position due to the local quenching of the hot spot.[1]

Scanning Hall probe microscope (SHPM) is a variety of a scanning probe microscope which incorporates accurate sample approach and positioning of the scanning tunnelling microscope with a semiconductor Hall sensor. Developed in 1996 by Oral, Bending and Henini,[2] SHPM allows mapping the magnetic induction associated with a sample. Current state of the art SHPM systems utilize 2D electron gas materials (e.g. GaAs/AlGaAs) to provide high spatial resolution (~300 nm) imaging with high magnetic field sensitivity. Unlike the magnetic force microscope the SHPM provides direct quantitative information on the magnetic state of a material. The SHPM can also image magnetic induction under applied fields up to ~1 tesla and over a wide range of temperatures (millikelvins to 300 K).[3]

The SHPM can be used to image many types of magnetic structures such as thin films, permanent magnets, MEMS structures, current carrying traces on PCBs, permalloy disks, and recording media

Advantages to other magnetic raster scanning methods

SHPM is a superior magnetic imaging technique due to many reasons. Although MFM provides higher spatial resolution (~30 nm) imaging, unlike the MFM technique, the Hall probe exerts negligible force on the underlying magnetic structure and is noninvasive. Unlike the magnetic decoration technique, the same area can be scanned over and over again. The magnetic field caused by hall probe is so minimal it has a negligible effect on sample it is measuring. The sample does not need to be an electrical conductor, unless using STM for height control. The measurement can be performed from 5 – 500 K in ultra high vacuum (UHV) and is nondestructive to the crystal lattice or structure. Tests requires no special surface preparation or coating. The detectable magnetic field sensitivity, is approximately 0.1 uT – 10 T. SHPM can be combined with other scanning methods such as STM.

Limitations

There are some shortcomings or difficulties when working with an SHPM. High resolution scans become difficult due to the thermal noise of extremely small hall probes. There is a minimum scanning height distance due to the construction of the hall probe. (This is especially significant with 2DEG semi-conductor probes due to their multi-layer design). The scanning (lift) height affects obtained image. Scanning large areas takes a significant amount of time. There is a relatively short practical scanning range (order of 1000s micrometer) along any direction. The housing is important to shield electromagnetic noise (Faraday cage), acoustic noise (anti-vibrating tables), air flow (air isolation cupboard), and static charge on the sample (ionizing units).

References

  1. ↑ Ge, Jun-Yi; Gladilin, Vladimir N.; Tempere, Jacques; Xue, Cun; Devreese, Jozef T.; Van De Vondel, Joris; Zhou, Youhe; Moshchalkov, Victor V. (2016). "Nanoscale assembly of superconducting vortices with scanning tunnelling microscope tip". Nature Communications. 7: 13880. arXiv:1701.06316. Bibcode:2016NatCo...713880G. doi:10.1038/ncomms13880. PMC 5155158. PMID 27934960.
  2. ↑ Oral, A.; Bending, S.J.; Henini, M. (1996). "Real‐time scanning Hall probe microscopy". Applied Physics Letters. 69 (9): 1324–1326. doi:10.1063/1.117582.
  3. ↑ Chang, A. M.; Hallen, H. D.; Harriott, L.; Hess, H. F.; Kao, H. L.; Kwo, J.; Miller, R. E.; Wolfe, R.; Van Der Ziel, J.; Chang, T. Y. (1992). "Scanning Hall probe microscopy". Appl. Phys. Lett. 61 (16): 1974. Bibcode:1992ApPhL..61.1974C. doi:10.1063/1.108334. S2CID 121741603.
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