26–31 May 2024
Western University
America/Toronto timezone
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Quantum Sensing and Imaging of van der Waals Ferromagnet using Nitrogen- Vacancy Centers in Diamond

30 May 2024, 14:45
15m
PAB Rm 106 (cap. 96) (Physics & Astronomy Bldg., Western U.)

PAB Rm 106 (cap. 96)

Physics & Astronomy Bldg., Western U.

Oral (Non-Student) / Orale (non-étudiant(e)) Symposia Day (DQI/DPE - DIQ/DEP) - Q-STATE: Quantum Science, Technology, Applications, Training, and Education | Science, technologie, applications, formation et éducation quantiques (DQI) R2-1 Quantum Sensing | Détection quantique (DIQ)

Speaker

Dr Amandeep Singh (The Hebrew University of Jerusalem, Applied Physics Department, Jerusalem, Israel, IL)

Description

The nitrogen-vacancy (NV) centres in diamonds are solid-state quantum emitters exhibiting unique spin and optical properties at room temperature. They are sensitive to magnetic fields, temperature, pressure, and other physical quantities, making them valuable as probes for sensing all of these physical quantities. In our work, we use NVs to form a magnetic microscope, with a high spatial resolution (~250 nm) limited by the diffraction limit and sensitivity of <1 μT/sqrt(Hz). This
configuration is sometimes referred to as a Quantum Diamond Microscope (QDM) (1).
We use the QDM to reveal and understand the fundamental processes of magnetic domain pattern formation and their variation with temperature and external bias field, as well as characterizing the
Curie temperature (Tc) of recently discovered van der Waals (vdW) magnetic materials, namely Iron Germanium Telluride (Fe$_5$GeTe$_2$). We exfoliate these vdW materials down to a few nanometres. We observe that depending upon the thickness, their fundamental properties such as Tc, magnetization, domain pattern, etc. change.
We focus on measuring the Tc and imaging the domain structure of FGT flakes through out-of-plane magnetization. (Fig. 1). Our results (2) indicate structural features affecting magnetic orientation in these flakes, as well as a decrease in Tc as we are making the transition from bulk to 2D, which further decreases as the thickness of these 2D flakes decreases.
Figure 1. (a) Atomic Force Microscope (AFM) topography of the FGT flake. (b) Magnetic image of the same flake imaged by our QDM. Scale-bar units are nm (a) and μT/sqrt(Hz) (b).

References:

(1) Levine, Edlyn V., Turner, Matthew J., Kehayias, Pauli, Hart, Connor A., Langellier, Nicholas, Trubko, Raisa, Glenn, David R., Fu, Roger R. and Walsworth, Ronald L. "Principles and techniques of the quantum diamond microscope" Nanophotonics, vol. 8, no. 11, 2019, pp. 1945-
1973.

(2) Bindu, Bindu et. Al, in preparation.

Keyword-1 Quantum Sensing
Keyword-2 NV Centers in Diamond

Authors

Dr Amandeep Singh (The Hebrew University of Jerusalem, Applied Physics Department, Jerusalem, Israel, IL) Ms Bindu Bindu (The Hebrew University of Jerusalem, Applied Physics Department, Jerusalem, Israel, IL) Dr Nir Bar-Gill (The Hebrew University of Jerusalem, Applied Physics Department, Jerusalem, Israel, IL)

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