<p>This study investigates the synthesis of superheavy elements through various fusion reactions, focusing on optimizing the conditions for successful production. By analyzing the excitation functions for reactions such as <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(^{48}\text {Ca} + ^{244}\text {Pu}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>48</mn> </mmultiscripts> <mtext>Ca</mtext> <msup> <mo>+</mo> <mn>244</mn> </msup> <mtext>Pu</mtext> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(^{48}\text {Ca} + ^{248}\text {Cm}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>48</mn> </mmultiscripts> <mtext>Ca</mtext> <msup> <mo>+</mo> <mn>248</mn> </msup> <mtext>Cm</mtext> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(^{36}\text {S} + ^{238}\text {U}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>36</mn> </mmultiscripts> <mtext>S</mtext> <msup> <mo>+</mo> <mn>238</mn> </msup> <mtext>U</mtext> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(^{48}\text {Ca} + ^{238}\text {U}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>48</mn> </mmultiscripts> <mtext>Ca</mtext> <msup> <mo>+</mo> <mn>238</mn> </msup> <mtext>U</mtext> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(^{50}\text {Ti} + ^{249}\text {Cf}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>50</mn> </mmultiscripts> <mtext>Ti</mtext> <msup> <mo>+</mo> <mn>249</mn> </msup> <mtext>Cf</mtext> </mrow> </math></EquationSource> </InlineEquation>, we examine the compound nucleus formation probability (<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(P_\textrm{CN}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>P</mi> <mtext>CN</mtext> </msub> </math></EquationSource> </InlineEquation>), survival probability (<InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(W_\textrm{sur}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>W</mi> <mtext>sur</mtext> </msub> </math></EquationSource> </InlineEquation>), fusion cross-section (<InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\sigma _\textrm{fus}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>σ</mi> <mtext>fus</mtext> </msub> </math></EquationSource> </InlineEquation>), and evaporation residue cross-section (<InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\sigma _\textrm{ER}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>σ</mi> <mtext>ER</mtext> </msub> </math></EquationSource> </InlineEquation>). The peak in <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\sigma _\textrm{ER}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>σ</mi> <mtext>ER</mtext> </msub> </math></EquationSource> </InlineEquation> aligns with the optimal energy range, supported by the quasi-elastic barrier distribution. The present hypothesis is applied to the Ti&#xa0;+ Cf fusion reaction for the synthesis of the superheavy element 120. It predicts a maximum cross section of 86.8 fb at an optimal energy of <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(225 \pm 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>225</mn> <mo>±</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> MeV. These findings are crucial for maximizing the synthesis of superheavy elements and demonstrate that energy optimization enhances the formation of evaporation residues.</p>

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Exploration of the mechanism of fusion excitation function in heavy ion fusion

  • H. C. Manjunatha,
  • P. S. Damodara Gupta,
  • N. Manjunath

摘要

This study investigates the synthesis of superheavy elements through various fusion reactions, focusing on optimizing the conditions for successful production. By analyzing the excitation functions for reactions such as \(^{48}\text {Ca} + ^{244}\text {Pu}\) 48 Ca + 244 Pu , \(^{48}\text {Ca} + ^{248}\text {Cm}\) 48 Ca + 248 Cm , \(^{36}\text {S} + ^{238}\text {U}\) 36 S + 238 U , \(^{48}\text {Ca} + ^{238}\text {U}\) 48 Ca + 238 U , and \(^{50}\text {Ti} + ^{249}\text {Cf}\) 50 Ti + 249 Cf , we examine the compound nucleus formation probability ( \(P_\textrm{CN}\) P CN ), survival probability ( \(W_\textrm{sur}\) W sur ), fusion cross-section ( \(\sigma _\textrm{fus}\) σ fus ), and evaporation residue cross-section ( \(\sigma _\textrm{ER}\) σ ER ). The peak in \(\sigma _\textrm{ER}\) σ ER aligns with the optimal energy range, supported by the quasi-elastic barrier distribution. The present hypothesis is applied to the Ti + Cf fusion reaction for the synthesis of the superheavy element 120. It predicts a maximum cross section of 86.8 fb at an optimal energy of \(225 \pm 2\) 225 ± 2 MeV. These findings are crucial for maximizing the synthesis of superheavy elements and demonstrate that energy optimization enhances the formation of evaporation residues.