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Pairing in excited nuclei: a review.
N Quang Hung1, N Dinh Dang2, L G Moretto3
1Institute of Fundamental and Applied Sciences, Duy Tan University, Ho Chi Minh city 700000, Vietnam.
Reports on Progress in Physics. Physical Society (Great Britain)
|February 9, 2019
Summary
This review explores pairing properties in many-body systems, including nuclei and solid-state materials. It highlights phenomena like pairing reentrance and its impact on nuclear properties.
Area of Science:
- Nuclear physics
- Condensed matter physics
- Thermodynamics
Background:
- Pairing correlations are fundamental in many-body systems, influencing properties from atomic nuclei to superconductors.
- Understanding these correlations at finite temperatures and angular momenta is crucial for describing excited states.
- The review focuses on systems where finite-size effects significantly alter pairing behavior.
Purpose of the Study:
- To review recent studies on the thermodynamic properties of pairing in diverse many-body systems.
- To discuss unique pairing phenomena arising from system finiteness, such as pairing reentrance.
- To analyze the influence of thermal pairing on nuclear structure and decay properties.
Main Methods:
- Review of theoretical studies on pairing in many-body systems.
- Analysis of nuclear reactions (heavy-ion fusion, [Formula: see text]-induced reactions, inelastic scattering) to form excited nuclei.
- Examination of experimental data for phenomena like pairing reentrance.
Main Results:
- Finiteness of systems leads to non-vanishing pairing gaps and smoothed phase transitions.
- Pairing reentrance is observed in excited nuclei and solid-state ferromagnets.
- Thermal pairing affects temperature-dependent giant dipole resonance width and radiative strength functions.
Conclusions:
- Pairing properties exhibit rich behavior in finite systems, deviating from bulk behavior.
- Pairing reentrance is a significant phenomenon with experimental evidence in both nuclear and solid-state physics.
- Thermodynamic pairing effects are crucial for accurately describing nuclear properties at finite excitation.
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