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Single crystal growth and physical properties of tetragonal BaMn

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Contribution ID:151 Type:Oral Presentation

Single crystal growth and physical properties of tetragonal BaMn 2 P 2

Wednesday, 5 July 2023 14:40 (20 minutes)

The discovery of unconventional superconductivity (SC) in doped iron-based arsenide BaFe2As2[1] crystal- lizing in ThCr2Si2-type structure ignited interest in 122 tetragonal systems. Substituting iron with other 3d or 4dtransition metal ions that constitute the metal-pnictide sublattice in similar systems have yielded inter- esting results including, but not limited to, low-temperature SC [2], half-metallic behaviour [3], new layered magnetic phases [4] and highly frustrated itinerant magnetism [5]. The Mn based BaMn2P n2 compounds [P n= P, As, Sb, Bi] are small band gap semiconductors with stacked-square-lattice of Mn ions that order antiferromagnetically at temperatures higher than room temperature. Although As, Sb and Bi based com- pounds have been thoroughly investigated [6-9], the experimental work on BaMn2P2 is dated and limited [10,11]. In this contribution, we report the synthesis and growth of single crystals of BaMn2P2as well as its structural, electronic, magnetic and thermal properties. Electrical resistivity and heat capacity measurements indicate that BaMn2P2has an insulating ground state with a small band gap. Anisotropic magnetic suscepti- bility measurements show that similar to its As-, Sb- and Bi- counterparts, BaMn2P2has collinear Néel type antiferromagnetism belowTN= 795(15) K, which is the highest value for 122- pnictide compounds reported so far. The magnetic susceptibility increases aboveTNsuggesting that antiferromagnetic correlations persist above the magnetic ordering temperature—a feature which was also observed in the As-, Sb- and Bi- based compounds. This can be explored further through hole-doping studies as in the case of BaMn2As2withTN= 618 K, which resulted in half-metallic behaviour withTc= 100 K which is of significance as highTchalf-metals are ideal for spin-polarized transport-based applications. These results were recently published in Phys. Rev.

Mater.7, 044410 (2023).

[1] D. C. Johnston, Adv. Phys.59, 803 (2010).

[2] V. K. Anand, H. Kim, M. A. Tanatar, R. Prozorov, and D. C. Johnston, Phys. Rev. B87, 224510 (2013).

[3] A. Pandey and D. C. Johnston, Phys. Rev. B92, 174401 (2015).

[4] A. Pandey, S. L. Samal, and D. C. Johnston, Inorg. Chem.57, 3206 (2018).

[5] A. Sapkota, B. G. Ueland, V. K. Anand, N. S. Sangeetha, D. L. Abernathy, M. B. Stone, J. L Niedziela, D. C.

Johnston, A. Kreyssig, A. I. Goldman, and R. J. McQueeney, Phys. Rev. Lett.119, 147201 (2017).

[6] Y. Singh, A. Ellern, and D. C. Johnston, Phys. Rev. B79, 094519 (2009).

[7] N. S. Sangeetha, V. Smetana, A.-V. Mudring, and D. C. Johnston, Phys. Rev. B97, 014402 (2018).

[8] B. Saparov and A. S. Sefat, J. Solid State Chem.204, 32 (2013).

[9] S. Calder, B. Saparov, H. B. Cao, J. L. Niedziela, M. D. Lumsden, A. S. Sefat, and A. D. Christianson, Phys.

Rev. B89, 064417 (2014).

[10] S. L. Brock, J. E. Greedan, and S. M. Kauzlarich, J. Solid State Chem.109, 416 (1994).

[11] S. L. Brock, J. E. Greedan, and S. M. Kauzlarich, J. Solid State Chem.113, 303 (1994).

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Primary authors: Dr JACOBS, Bincy Susan (University of Johannesburg); Dr PANDEY, Abhishek (University of the Witwatersrand)

Presenter: Dr JACOBS, Bincy Susan (University of Johannesburg)

Session Classification: Physics of Condensed Matter and Materials Track 1 Track Classification: Track A - Physics of Condensed Matter and Materials

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