Evidence against the Efimov effect in $^{12}\mathrm{C}$ from spectroscopy and astrophysics

Phys. Rev. C 103, 051303 (2021) Background: The Efimov effect is a universal phenomenon in physics whereby three-body systems are stabilized via the interaction of an unbound two-body sub-systems. A hypothetical state in $^{12}\mathrm{C}$ at 7.458 MeV excitation energy, comprising of a loose structu...

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Hauptverfasser: Bishop, J, Rogachev, G. V, Ahn, S, Aboud, E, Barbui, M, Bosh, A, Hooker, J, Hunt, C, Jayatissa, H, Koshchiy, E, Malecek, R, Marley, S. T, Munch, M, Pollaco, E. C, Pruitt, C. D, Roeder, B. T, Saastamoinen, A, Sobotka, L. G, Upadhyayula, S
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creator Bishop, J
Rogachev, G. V
Ahn, S
Aboud, E
Barbui, M
Bosh, A
Hooker, J
Hunt, C
Jayatissa, H
Koshchiy, E
Malecek, R
Marley, S. T
Munch, M
Pollaco, E. C
Pruitt, C. D
Roeder, B. T
Saastamoinen, A
Sobotka, L. G
Upadhyayula, S
description Phys. Rev. C 103, 051303 (2021) Background: The Efimov effect is a universal phenomenon in physics whereby three-body systems are stabilized via the interaction of an unbound two-body sub-systems. A hypothetical state in $^{12}\mathrm{C}$ at 7.458 MeV excitation energy, comprising of a loose structure of three $\alpha$-particles in mutual two-body resonance, has been suggested in the literature to correspond to an Efimov state in nuclear physics. The existence of such a state has not been demonstrated experimentally. Method: Using the combined data sets from two recent experiments, one with the TexAT TPC to measure $\alpha$-decay and the other with Gammasphere to measure $\gamma$-decay of states in $^{12}\mathrm{C}$ populated by $^{12}\mathrm{N}$ and $^{12}\mathrm{B}$ $\beta$-decay respectively, we achieve high sensitivity to states in close-proximity to the $\alpha$-threshold in $^{12}\mathrm{C}$. Results: No evidence of a state at 7.458 MeV is seen in either data set. Using a likelihood method, the 95\% C.L. $\gamma$-decay branching ratio is determined as a function of the $\beta$-decay feeding strength relative to the Hoyle state. In parallel, calculations of the triple-alpha reaction rate show the inclusion of the Efimov corresponds to a large increase in the reaction rate around $5 \times 10^{7}$ K. Conclusion: From decay spectroscopy - at the 95\% C.L., the Efimov state cannot exist at 7.458 MeV with any $\gamma$-decay branching ratio unless the $\beta$-strength is less than 0.7\% of the Hoyle state. This limit is evaluated for a range of different excitation energies and the results are not favorable for existence of the hypothetical Efimov state in $^{12}\mathrm{C}$. Furthermore, the triple-alpha reaction rate with the inclusion of a state between 7.43 and 7.53 MeV exceeds the rate required for stars to undergo the red giant phase.
doi_str_mv 10.48550/arxiv.2012.08432
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C ; Pruitt, C. D ; Roeder, B. T ; Saastamoinen, A ; Sobotka, L. G ; Upadhyayula, S</creator><creatorcontrib>Bishop, J ; Rogachev, G. V ; Ahn, S ; Aboud, E ; Barbui, M ; Bosh, A ; Hooker, J ; Hunt, C ; Jayatissa, H ; Koshchiy, E ; Malecek, R ; Marley, S. T ; Munch, M ; Pollaco, E. C ; Pruitt, C. D ; Roeder, B. T ; Saastamoinen, A ; Sobotka, L. G ; Upadhyayula, S</creatorcontrib><description>Phys. Rev. C 103, 051303 (2021) Background: The Efimov effect is a universal phenomenon in physics whereby three-body systems are stabilized via the interaction of an unbound two-body sub-systems. A hypothetical state in $^{12}\mathrm{C}$ at 7.458 MeV excitation energy, comprising of a loose structure of three $\alpha$-particles in mutual two-body resonance, has been suggested in the literature to correspond to an Efimov state in nuclear physics. The existence of such a state has not been demonstrated experimentally. Method: Using the combined data sets from two recent experiments, one with the TexAT TPC to measure $\alpha$-decay and the other with Gammasphere to measure $\gamma$-decay of states in $^{12}\mathrm{C}$ populated by $^{12}\mathrm{N}$ and $^{12}\mathrm{B}$ $\beta$-decay respectively, we achieve high sensitivity to states in close-proximity to the $\alpha$-threshold in $^{12}\mathrm{C}$. Results: No evidence of a state at 7.458 MeV is seen in either data set. Using a likelihood method, the 95\% C.L. $\gamma$-decay branching ratio is determined as a function of the $\beta$-decay feeding strength relative to the Hoyle state. In parallel, calculations of the triple-alpha reaction rate show the inclusion of the Efimov corresponds to a large increase in the reaction rate around $5 \times 10^{7}$ K. Conclusion: From decay spectroscopy - at the 95\% C.L., the Efimov state cannot exist at 7.458 MeV with any $\gamma$-decay branching ratio unless the $\beta$-strength is less than 0.7\% of the Hoyle state. This limit is evaluated for a range of different excitation energies and the results are not favorable for existence of the hypothetical Efimov state in $^{12}\mathrm{C}$. 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C 103, 051303 (2021) Background: The Efimov effect is a universal phenomenon in physics whereby three-body systems are stabilized via the interaction of an unbound two-body sub-systems. A hypothetical state in $^{12}\mathrm{C}$ at 7.458 MeV excitation energy, comprising of a loose structure of three $\alpha$-particles in mutual two-body resonance, has been suggested in the literature to correspond to an Efimov state in nuclear physics. The existence of such a state has not been demonstrated experimentally. Method: Using the combined data sets from two recent experiments, one with the TexAT TPC to measure $\alpha$-decay and the other with Gammasphere to measure $\gamma$-decay of states in $^{12}\mathrm{C}$ populated by $^{12}\mathrm{N}$ and $^{12}\mathrm{B}$ $\beta$-decay respectively, we achieve high sensitivity to states in close-proximity to the $\alpha$-threshold in $^{12}\mathrm{C}$. Results: No evidence of a state at 7.458 MeV is seen in either data set. Using a likelihood method, the 95\% C.L. $\gamma$-decay branching ratio is determined as a function of the $\beta$-decay feeding strength relative to the Hoyle state. In parallel, calculations of the triple-alpha reaction rate show the inclusion of the Efimov corresponds to a large increase in the reaction rate around $5 \times 10^{7}$ K. Conclusion: From decay spectroscopy - at the 95\% C.L., the Efimov state cannot exist at 7.458 MeV with any $\gamma$-decay branching ratio unless the $\beta$-strength is less than 0.7\% of the Hoyle state. This limit is evaluated for a range of different excitation energies and the results are not favorable for existence of the hypothetical Efimov state in $^{12}\mathrm{C}$. 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T</creatorcontrib><creatorcontrib>Saastamoinen, A</creatorcontrib><creatorcontrib>Sobotka, L. G</creatorcontrib><creatorcontrib>Upadhyayula, S</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Bishop, J</au><au>Rogachev, G. V</au><au>Ahn, S</au><au>Aboud, E</au><au>Barbui, M</au><au>Bosh, A</au><au>Hooker, J</au><au>Hunt, C</au><au>Jayatissa, H</au><au>Koshchiy, E</au><au>Malecek, R</au><au>Marley, S. T</au><au>Munch, M</au><au>Pollaco, E. C</au><au>Pruitt, C. D</au><au>Roeder, B. T</au><au>Saastamoinen, A</au><au>Sobotka, L. G</au><au>Upadhyayula, S</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Evidence against the Efimov effect in $^{12}\mathrm{C}$ from spectroscopy and astrophysics</atitle><date>2020-12-15</date><risdate>2020</risdate><abstract>Phys. Rev. C 103, 051303 (2021) Background: The Efimov effect is a universal phenomenon in physics whereby three-body systems are stabilized via the interaction of an unbound two-body sub-systems. A hypothetical state in $^{12}\mathrm{C}$ at 7.458 MeV excitation energy, comprising of a loose structure of three $\alpha$-particles in mutual two-body resonance, has been suggested in the literature to correspond to an Efimov state in nuclear physics. The existence of such a state has not been demonstrated experimentally. Method: Using the combined data sets from two recent experiments, one with the TexAT TPC to measure $\alpha$-decay and the other with Gammasphere to measure $\gamma$-decay of states in $^{12}\mathrm{C}$ populated by $^{12}\mathrm{N}$ and $^{12}\mathrm{B}$ $\beta$-decay respectively, we achieve high sensitivity to states in close-proximity to the $\alpha$-threshold in $^{12}\mathrm{C}$. Results: No evidence of a state at 7.458 MeV is seen in either data set. Using a likelihood method, the 95\% C.L. $\gamma$-decay branching ratio is determined as a function of the $\beta$-decay feeding strength relative to the Hoyle state. In parallel, calculations of the triple-alpha reaction rate show the inclusion of the Efimov corresponds to a large increase in the reaction rate around $5 \times 10^{7}$ K. Conclusion: From decay spectroscopy - at the 95\% C.L., the Efimov state cannot exist at 7.458 MeV with any $\gamma$-decay branching ratio unless the $\beta$-strength is less than 0.7\% of the Hoyle state. This limit is evaluated for a range of different excitation energies and the results are not favorable for existence of the hypothetical Efimov state in $^{12}\mathrm{C}$. Furthermore, the triple-alpha reaction rate with the inclusion of a state between 7.43 and 7.53 MeV exceeds the rate required for stars to undergo the red giant phase.</abstract><doi>10.48550/arxiv.2012.08432</doi><oa>free_for_read</oa></addata></record>
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title Evidence against the Efimov effect in $^{12}\mathrm{C}$ from spectroscopy and astrophysics
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