Probing the strongly correlated magnetic state of Co2C nanoparticles at low temperatures using μ SR

Nirmal Roy; P C Mahato; Suprotim Saha; M Telling; J S Lord; D T Adroja; S S Banerjee

doi:10.1088/1361-648X/ad08ec

Probing the strongly correlated magnetic state of Co₂C nanoparticles at low temperatures using μ SR

J Phys Condens Matter. 2023 Nov 16;36(8). doi: 10.1088/1361-648X/ad08ec.

Authors

Nirmal Roy¹, P C Mahato¹, Suprotim Saha¹, M Telling², J S Lord², D T Adroja^{2

3}, S S Banerjee¹

Affiliations

¹ Indian Institute of Technology Kanpur, Kanpur, Uttar Pradesh 208016, India.
² ISIS Facility, Rutherford Appleton Laboratory, Chilton, Didcot Oxon OX11 0QX, United Kingdom.
³ Highly Correlated Matter Research Group, Physics Department, University of Johannesburg, PO Box 524, Auckland Park 2006, South Africa.

PMID: 37918015
DOI: 10.1088/1361-648X/ad08ec

Abstract

Co₂C nanoparticles (NPs) are amongst transition metal carbides whose magnetic properties have not been well explored. An earlier study (Royet al2021J. Phys.: Condens. Matter33375804) showed that a pellet made from Co₂C NPs exhibits exchange bias (EB) effect below a temperature,T_EB= 50 K and a spin glass (SG) feature emerges belowT_SG= 5 K. In the current study we use magnetic, electrical transport, specific heat, and muon spin rotation (μSR) measurements to explore further the magnetic properties of a pellet made with 40 nm diameter pure Co₂C NPs. We uncover the onset of Kondo localization at Kondo temperatureT_K(= 40.1 K), which is close to the onset temperature (T_EB) of the EB effect. A crossover from the Kondo-screened scenario to the Ruderman-Kittel-Kasuya-Yosida interaction-dominated regime is also observed forT<T_K. Temperature-dependent specific heat measurement further supports the Kondo localization scenario in the pellet and shows the heavy fermionic nature of the strongly correlated electronic state in Co₂C. The zero fieldμSR asymmetry spectra in the low-temperature regime are characterized by two distinct fast and slow relaxation rates. The spectra show the absence of long-range magnetic order in the sample. However, our analysis suggests the NPs-pellet shows the presence of a dominant magnetically disordered fraction and a smaller fraction with short-range order. Muons in the disordered fraction exhibit a slower relaxation rate, while muons in the smaller fraction with short-range order exhibit a faster relaxation rate. We observe an increase in this fast relaxation rate betweenT_EBandT_SG. This increase belowT_EB∼ 50 K suggests a slowing down of the fluctuating local magnetic environment around muons. Transverse field-μSR asymmetry spectra show the emergence of a stable, multi-peaked local magnetic field distribution in the pellet belowT_EB. Longitudinal fieldμSR spectra shows distinct changes in the dynamics of fluctuations suggesting the presence of a frozen glassy like state below 6 K. Based on our results, we suggest that belowT_EB,the pellet of Co₂C NPs develops a magnetic interface that separates the two magnetic fractions; one is a disordered fraction, and the other is a fraction with short-range order. The exchange interaction that sets in belowT_EBat the interface couples the two fractions, leading to a suppression of the fluctuations. With the suppression of magnetic fluctuations belowT_EB, strong correlation effects in the electronic state of Co₂C lead to Kondo localization.

Keywords: Kondo effect; exchange bias; magnetic nanoparticles; muon spin relaxation; spin glass.