<p>Employing the mean-field approximation founded on the Gibbs-Bogoliubov inequality, the magnetic and critical behaviors of an Ising system with mixed spins (<InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8252_Article_IEq3.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(\sigma = 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>σ</mi> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>; <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8252_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="59" /> </InlineMediaObject> <EquationSource Format="TEX">\(S = 3/2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>S</mi> <mo>=</mo> <mn>3</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>) on a two-dimensional CrI<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8252_Article_IEq5.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\(_3-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>like structure were examined. The effects of exchange couplings (<InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8252_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(J_{\sigma }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>J</mi> <mi>σ</mi> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8252_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(J_S\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>J</mi> <mi>S</mi> </msub> </math></EquationSource> </InlineEquation>), crystal fields (<InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8252_Article_IEq8.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta _{\sigma }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Δ</mi> <mi>σ</mi> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8252_Article_IEq9.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta _S\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Δ</mi> <mi>S</mi> </msub> </math></EquationSource> </InlineEquation>), temperature (<i>T</i>), and external magnetic field (<i>h</i>) on the lattice’s magnetization, susceptibility, phase diagrams, and hysteresis loops were investigated. This CrI<InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8252_Article_IEq10.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\(_3-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>like monolayer features second- and first-order phase transitions, isolated critical points, and compensation behavior. For selected system parameter values, the values <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8252_Article_IEq11.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="86" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta _{\sigma } = -3.75\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Δ</mi> <mi>σ</mi> </msub> <mo>=</mo> <mo>-</mo> <mn>3.75</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8252_Article_IEq12.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="79" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta _S = -7.5\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Δ</mi> <mi>S</mi> </msub> <mo>=</mo> <mo>-</mo> <mn>7.5</mn> </mrow> </math></EquationSource> </InlineEquation> correspond to the points at <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8252_Article_IEq13.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="44" /> </InlineMediaObject> <EquationSource Format="TEX">\(T=0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>T</mi> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, where a first-order phase transition occurs between two ferrimagnetic phases. Furthermore, the compensation phenomenon appears in the following ranges: <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8252_Article_IEq14.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="87" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta _{\sigma } &gt; -3.75\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Δ</mi> <mi>σ</mi> </msub> <mo>&gt;</mo> <mo>-</mo> <mn>3.75</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8252_Article_IEq15.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="88" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta _S &gt; -5.48\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Δ</mi> <mi>S</mi> </msub> <mo>&gt;</mo> <mo>-</mo> <mn>5.48</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8252_Article_IEq16.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="70" /> </InlineMediaObject> <EquationSource Format="TEX">\(J_{\sigma } &lt; 4.62\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>J</mi> <mi>σ</mi> </msub> <mo>&lt;</mo> <mn>4.62</mn> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8252_Article_IEq17.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="70" /> </InlineMediaObject> <EquationSource Format="TEX">\(J_S &gt; 0.83\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>J</mi> <mi>S</mi> </msub> <mo>&gt;</mo> <mn>0.83</mn> </mrow> </math></EquationSource> </InlineEquation>. We also demonstrated the existence of multiple hysteresis loops under certain physical conditions. The results achieved in this work could contribute to the advancement of potential CrI<InlineEquation ID="IEq18"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8252_Article_IEq18.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>-based applications, such as spintronics, sensing, magnetic information storage, and magneto-optical recording.</p>

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Magnetic behavior of a CrI3-like monolayer by mean-field approach

  • Y. Chegrane,
  • A. Boukhal,
  • N. Hachem,
  • M. El Bouziani

摘要

Employing the mean-field approximation founded on the Gibbs-Bogoliubov inequality, the magnetic and critical behaviors of an Ising system with mixed spins ( \(\sigma = 1\) σ = 1 ; \(S = 3/2\) S = 3 / 2 ) on a two-dimensional CrI \(_3-\) 3 - like structure were examined. The effects of exchange couplings ( \(J_{\sigma }\) J σ and \(J_S\) J S ), crystal fields ( \(\Delta _{\sigma }\) Δ σ and \(\Delta _S\) Δ S ), temperature (T), and external magnetic field (h) on the lattice’s magnetization, susceptibility, phase diagrams, and hysteresis loops were investigated. This CrI \(_3-\) 3 - like monolayer features second- and first-order phase transitions, isolated critical points, and compensation behavior. For selected system parameter values, the values \(\Delta _{\sigma } = -3.75\) Δ σ = - 3.75 and \(\Delta _S = -7.5\) Δ S = - 7.5 correspond to the points at \(T=0\) T = 0 , where a first-order phase transition occurs between two ferrimagnetic phases. Furthermore, the compensation phenomenon appears in the following ranges: \(\Delta _{\sigma } > -3.75\) Δ σ > - 3.75 , \(\Delta _S > -5.48\) Δ S > - 5.48 , \(J_{\sigma } < 4.62\) J σ < 4.62 , and \(J_S > 0.83\) J S > 0.83 . We also demonstrated the existence of multiple hysteresis loops under certain physical conditions. The results achieved in this work could contribute to the advancement of potential CrI \(_3\) 3 -based applications, such as spintronics, sensing, magnetic information storage, and magneto-optical recording.