{"title":"Magnetic \u0026 Multiferroic Materials","description":null,"products":[{"product_id":"cuvp-s-copper-vanadium-phosphorus-trisulfide","title":"CuVP₂S₆ (Copper Vanadium Phosphorus Trisulfide)","description":"\u003cp\u003e\u003cmeta charset=\"UTF-8\"\u003e\u003cspan\u003eA layered van der Waals metal phosphochalcogenide of the CuInP₂S₆-related family, space group P2\/c, in which Cu⁺ and V cations jointly occupy the octahedral sites of the P₂S₆ framework. It combines \u003c\/span\u003e\u003cstrong\u003e(anti)ferroelectric polar order\u003c\/strong\u003e\u003cspan\u003e arising from off-centering of the Cu⁺ ions with \u003c\/span\u003e\u003cstrong\u003emagnetism\u003c\/strong\u003e\u003cspan\u003e from the V magnetic ions, making it one of the few candidate \u003c\/span\u003e\u003cstrong\u003emultiferroics\u003c\/strong\u003e\u003cspan\u003e that unite ferroelectricity and magnetism in a single two-dimensional material. This coexistence of polar and magnetic order makes CuVP₂S₆ an important platform for studying \u003c\/span\u003e\u003cstrong\u003etwo-dimensional multiferroicity, magnetoelectric coupling, and spin-polarization coupling\u003c\/strong\u003e\u003cspan\u003e.\u003c\/span\u003e\u003c\/p\u003e\n\u003cp\u003e\u003cspan\u003e\u003cmeta charset=\"UTF-8\"\u003e\n\u003cstrong\u003eSample specifications:\u003c\/strong\u003e Individual crystals measure approximately 3~5\u003cstrong\u003e mm\u003c\/strong\u003e, with a purity of up to \u003cstrong\u003e99.9999% (6N)\u003c\/strong\u003e, and multiple high-quality single-crystal pieces included in each package.\u003c\/span\u003e\u003c\/p\u003e","brand":"2D Material Supermarket","offers":[{"title":"Default Title","offer_id":53911825383608,"sku":"2MS-CuVP₂S₆","price":850.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0649\/0069\/4200\/files\/91f5a4b89f1b1ba558eefc49f65fe22e_caf419e0-268a-4815-853d-f5a0b49240ea.jpg?v=1786706207"},{"product_id":"crsb-chromium-antimonide","title":"CrSb (Chromium Antimonide)","description":"\u003cp\u003e\u003cmeta charset=\"UTF-8\"\u003e\u003cspan\u003eA binary transition-metal pnictide crystallizing in the hexagonal NiAs-type structure, space group P6₃\/mmc. It is a prominent candidate \u003c\/span\u003e\u003cstrong\u003ealtermagnet\u003c\/strong\u003e\u003cspan\u003e, a newly recognized magnetic class combining zero net magnetization (like an antiferromagnet) with spin-split electronic bands (like a ferromagnet); CrSb hosts a high magnetic ordering temperature (T_N well above room temperature, ~700 K) and a large momentum-dependent spin splitting confirmed by photoemission. This robust, room-temperature altermagnetic order makes CrSb a leading platform for studying \u003c\/span\u003e\u003cstrong\u003ealtermagnetism, spin-split transport, and antiferromagnetic spintronics\u003c\/strong\u003e\u003cspan\u003e without stray magnetic fields.\u003c\/span\u003e\u003c\/p\u003e\n\u003cp\u003e\u003cspan\u003e\u003cmeta charset=\"UTF-8\"\u003e\n\u003cstrong\u003eSample specifications:\u003c\/strong\u003e Individual crystals measure approximately \u003cstrong\u003e2–3 mm\u003c\/strong\u003e, with a purity of up to \u003cstrong\u003e99.9999% (6N)\u003c\/strong\u003e, and multiple high-quality single-crystal pieces included in each package.\u003c\/span\u003e\u003c\/p\u003e","brand":"2D Material Supermarket","offers":[{"title":"Default Title","offer_id":53930461987000,"sku":"2MS-CrSb","price":950.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0649\/0069\/4200\/files\/91f5a4b89f1b1ba558eefc49f65fe22e_fe64723b-f29a-4c12-9b7b-5bf5572bb734.jpg?v=1786960081"},{"product_id":"ceti-bi-cerium-titanium-bismuthide","title":"CeTi₃Bi₄ (Cerium Titanium Bismuthide)","description":"\u003cp\u003e\u003cmeta charset=\"UTF-8\"\u003e\u003cspan\u003eA layered magnetic material of the RTi₃Bi₄ family (R = rare earth), in which Ti kagome nets combine with rare-earth chains within a Bi-based framework. It hosts \u003c\/span\u003e\u003cstrong\u003ekagome-lattice electronic features\u003c\/strong\u003e\u003cspan\u003e—flat bands, Dirac points, and van Hove singularities—coexisting with magnetism from the Ce sublattice, whose 4f moments introduce localized magnetism and possible Kondo physics with strong magnetic anisotropy. This intertwining of kagome band topology and rare-earth magnetism makes CeTi₃Bi₄ an important platform for studying \u003c\/span\u003e\u003cstrong\u003ecorrelated kagome magnets and magnetic topological states\u003c\/strong\u003e\u003cspan\u003e.\u003c\/span\u003e\u003c\/p\u003e\n\u003cp\u003e\u003cspan\u003e\u003cmeta charset=\"UTF-8\"\u003e\n\u003cstrong\u003eSample specifications:\u003c\/strong\u003e Individual crystals measure approximately \u003cstrong\u003e2–3 mm\u003c\/strong\u003e, with a purity of up to \u003cstrong\u003e99.9999% (6N)\u003c\/strong\u003e, and multiple high-quality single-crystal pieces included in each package.\u003c\/span\u003e\u003c\/p\u003e","brand":"2D Material Supermarket","offers":[{"title":"Default Title","offer_id":53930500161720,"sku":"2MS-CeTi₃Bi₄","price":950.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0649\/0069\/4200\/files\/93248b98d3b35db245f99126e1d7dfd1.jpg?v=1786961472"},{"product_id":"euti-bi-europium-titanium-bismuthide","title":"EuTi₃Bi₄ (Europium Titanium Bismuthide)","description":"\u003cp\u003e\u003cmeta charset=\"UTF-8\"\u003e\u003cspan\u003eA layered RTi₃Bi₄ kagome magnet in which Ti kagome nets coexist with a Eu sublattice. The divalent Eu²⁺ ions carry large, highly localized spin-7\/2 moments that order magnetically and produce pronounced \u003c\/span\u003e\u003cstrong\u003eanisotropic (Ising-like) magnetism\u003c\/strong\u003e\u003cspan\u003e, coupled to the \u003c\/span\u003e\u003cstrong\u003ekagome flat bands, Dirac crossings, and van Hove singularities\u003c\/strong\u003e\u003cspan\u003e of the Ti network. This strong interplay between large-moment rare-earth magnetism and kagome band topology makes EuTi₃Bi₄ a notable platform for studying \u003c\/span\u003e\u003cstrong\u003efield-tunable magnetic kagome physics and topological transport\u003c\/strong\u003e\u003cspan\u003e.\u003c\/span\u003e\u003c\/p\u003e\n\u003cp\u003e\u003cspan\u003e\u003cmeta charset=\"UTF-8\"\u003e\n\u003cstrong\u003eSample specifications:\u003c\/strong\u003e Individual crystals measure approximately \u003cstrong\u003e2–3 mm\u003c\/strong\u003e, with a purity of up to \u003cstrong\u003e99.9999% (6N)\u003c\/strong\u003e, and multiple high-quality single-crystal pieces included in each package.\u003c\/span\u003e\u003c\/p\u003e","brand":"2D Material Supermarket","offers":[{"title":"Default Title","offer_id":53930500817080,"sku":"2MS-EuTi₃Bi₄","price":950.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0649\/0069\/4200\/files\/93248b98d3b35db245f99126e1d7dfd1_7b243fee-8db2-4d47-a608-55ee01853723.jpg?v=1786961507"},{"product_id":"ndti-bi-neodymium-titanium-bismuthide","title":"NdTi₃Bi₄ (Neodymium Titanium Bismuthide)","description":"\u003cp\u003e\u003cmeta charset=\"UTF-8\"\u003e\u003cspan\u003eA layered RTi₃Bi₄ kagome magnet combining Ti kagome nets with quasi-one-dimensional Nd chains. The Nd³⁺ 4f moments order with strong \u003c\/span\u003e\u003cstrong\u003emagnetic anisotropy\u003c\/strong\u003e\u003cspan\u003e, and their coupling to the \u003c\/span\u003e\u003cstrong\u003ekagome-derived flat bands, Dirac points, and van Hove singularities\u003c\/strong\u003e\u003cspan\u003e yields anisotropic magnetotransport and anomalous Hall responses. This combination of low-dimensional rare-earth magnetism and kagome band structure makes NdTi₃Bi₄ an important platform for studying \u003c\/span\u003e\u003cstrong\u003emagnetic kagome metals and correlated topological states\u003c\/strong\u003e\u003cspan\u003e.\u003c\/span\u003e\u003cspan\u003e\u003c\/span\u003e\u003c\/p\u003e\n\u003cp\u003e\u003cspan\u003e\u003cmeta charset=\"UTF-8\"\u003e\n\u003cstrong\u003eSample specifications:\u003c\/strong\u003e Individual crystals measure approximately \u003cstrong\u003e2–3 mm\u003c\/strong\u003e, with a purity of up to \u003cstrong\u003e99.9999% (6N)\u003c\/strong\u003e, and multiple high-quality single-crystal pieces included in each package.\u003c\/span\u003e\u003c\/p\u003e","brand":"2D Material Supermarket","offers":[{"title":"Default Title","offer_id":53930501931192,"sku":"2MS-NdTi₃Bi₄","price":950.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0649\/0069\/4200\/files\/93248b98d3b35db245f99126e1d7dfd1_42d643f3-ff8d-4bf8-b1cc-c707674987b7.jpg?v=1786961538"},{"product_id":"tbti-bi-terbium-titanium-bismuthide","title":"TbTi₃Bi₄ (Terbium Titanium Bismuthide)","description":"\u003cp\u003e\u003cmeta charset=\"UTF-8\"\u003e\u003cspan\u003eA layered RTi₃Bi₄ kagome magnet in which Ti kagome nets coexist with a Tb sublattice arranged in chains. The Tb³⁺ ions carry large 4f moments with strong \u003c\/span\u003e\u003cstrong\u003eIsing-like magnetic anisotropy\u003c\/strong\u003e\u003cspan\u003e, producing highly anisotropic magnetic order coupled to the \u003c\/span\u003e\u003cstrong\u003ekagome flat bands, Dirac crossings, and van Hove singularities\u003c\/strong\u003e\u003cspan\u003e of the Ti network. The strong single-ion anisotropy and field-tunable metamagnetic transitions make TbTi₃Bi₄ a prominent platform for studying \u003c\/span\u003e\u003cstrong\u003eanisotropic magnetic kagome metals and topological magnetotransport\u003c\/strong\u003e\u003cspan\u003e.\u003c\/span\u003e\u003cspan\u003e\u003c\/span\u003e\u003c\/p\u003e\n\u003cp\u003e\u003cspan\u003e\u003cmeta charset=\"UTF-8\"\u003e\n\u003cstrong\u003eSample specifications:\u003c\/strong\u003e Individual crystals measure approximately \u003cstrong\u003e2–3 mm\u003c\/strong\u003e, with a purity of up to \u003cstrong\u003e99.9999% (6N)\u003c\/strong\u003e, and multiple high-quality single-crystal pieces included in each package.\u003c\/span\u003e\u003c\/p\u003e","brand":"2D Material Supermarket","offers":[{"title":"Default Title","offer_id":53930503078072,"sku":"2MS-TbTi₃Bi₄","price":950.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0649\/0069\/4200\/files\/93248b98d3b35db245f99126e1d7dfd1_3bfd93ef-cd98-4a6b-9344-b9e6e628022d.jpg?v=1786961587"},{"product_id":"agvp-se-silver-vanadium-phosphorus-triselenide","title":"AgVP₂Se₆ (Silver Vanadium Phosphorus Triselenide)","description":"\u003cp\u003e\u003cmeta charset=\"UTF-8\"\u003e\u003cspan\u003eA layered van der Waals metal phosphochalcogenide of the CuInP₂S₆-related family, in which Ag⁺ and magnetic V cations occupy the octahedral sites of the P₂Se₆ framework. It combines \u003c\/span\u003e\u003cstrong\u003epolar (ferroelectric\/antiferroelectric) order\u003c\/strong\u003e\u003cspan\u003earising from off-centering of the Ag⁺ ions with \u003c\/span\u003e\u003cstrong\u003emagnetism\u003c\/strong\u003e\u003cspan\u003e from the V sublattice, making it a candidate two-dimensional \u003c\/span\u003e\u003cstrong\u003emultiferroic\u003c\/strong\u003e\u003cspan\u003e; selenization gives it a narrower bandgap and stronger spin-orbit effects than its sulfide analogue. This coexistence of switchable polarization and magnetic order makes AgVP₂Se₆ an important platform for studying \u003c\/span\u003e\u003cstrong\u003etwo-dimensional multiferroicity and magnetoelectric coupling\u003c\/strong\u003e\u003cspan\u003e.\u003c\/span\u003e\u003c\/p\u003e\n\u003cp\u003e\u003cmeta charset=\"UTF-8\"\u003e\u003cstrong\u003eSample specifications:\u003c\/strong\u003e\u003cspan\u003e Individual crystals measure approximately 3~4\u003c\/span\u003e\u003cstrong\u003e mm\u003c\/strong\u003e\u003cspan\u003e, with a purity of up to \u003c\/span\u003e\u003cstrong\u003e99.9999% (6N)\u003c\/strong\u003e\u003cspan\u003e, and multiple high-quality single-crystal pieces included in each package.\u003c\/span\u003e\u003c\/p\u003e","brand":"2D Material Supermarket","offers":[{"title":"Default Title","offer_id":53937147314360,"sku":"2MS-AgVP₂Se₆","price":690.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0649\/0069\/4200\/files\/93248b98d3b35db245f99126e1d7dfd1_dc54ddde-870d-4ae4-a1e0-ec30d21b906e.jpg?v=1787045330"},{"product_id":"cr-s-chromium-sulfide","title":"Cr₂S₃ (Chromium Sulfide)","description":"\u003cp\u003eCr₂S₃ is a layered van der Waals magnetic semiconductor from the chromium sulfide system, adopting a trigonal (rhombohedral) phase. Its lattice is composed of Cr–S octahedra, and the magnetic exchange between Cr³⁺ ions gives rise to antiferromagnetic\/ferrimagnetic ordering with an appreciable magnetic transition temperature. Combining magnetism with semiconducting behavior, Cr₂S₃ holds strong potential for spintronics, magneto-optical coupling, and van der Waals magnetic heterostructures.\u003cbr\u003e　　Sample specifications: Individual crystals are approximately 1 mm in size, \u003cmeta charset=\"UTF-8\"\u003e\u003cspan\u003ewith a purity of up to \u003c\/span\u003e\u003cstrong\u003e99.9999% (6N),\u003c\/strong\u003ewith each package containing roughly 15–20 pieces.\u003c\/p\u003e","brand":"2D Material Supermarket","offers":[{"title":"Default Title","offer_id":54104311365816,"sku":"2MS-Cr₂S₃","price":550.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0649\/0069\/4200\/files\/8301f43d9055f372af0de60cc59a10d6.jpg?v=1789475558"}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0649\/0069\/4200\/collections\/8301f43d9055f372af0de60cc59a10d6_dfaa2849-b8cd-4ba9-ba22-49dcc4f74b5b.jpg?v=1789478003","url":"https:\/\/2dmaterialsupermarket.com\/collections\/magnetic-multiferroic-materials.oembed","provider":"2D Material Supermarket","version":"1.0","type":"link"}