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  • 1
    Online Resource
    Online Resource
    IOP Publishing ; 2024
    In:  Journal of Physics G: Nuclear and Particle Physics Vol. 51, No. 6 ( 2024-06-01), p. 065105-
    In: Journal of Physics G: Nuclear and Particle Physics, IOP Publishing, Vol. 51, No. 6 ( 2024-06-01), p. 065105-
    Abstract: Semi-empirical thermodynamic quantities (TQs) of 78 nuclei ranging from 43 Sc to 243 Pu have been systematically investigated in the temperature region below 1 MeV using the thermodynamic canonical ensemble. The latter is carried out by taking into account the experimental nuclear level density (NLD) data measured using the Oslo method for the low-excitation region below the neutron binding energy B n combining with the back-shifted Fermi gas NLD model for the excitation energy from B n to about 250 MeV. In particular, the uncertainty of the TQs propagating from the fluctuation of the experimental NLD data has been, for the first time, calculated. The results obtained indicate that the uncertainty of TQs due to the experimental NLD is incomparable with the changes caused by the nuclear structure effects. The free energy of even–even nuclei behaves differently from that of odd- A ones. The total energy in the low-temperature region below T E ≃ 0.4 − 0.6 MeV for medium-mass nuclei and T E ≃ 0.2 − 0.4 MeV for heavy-mass ones slowly varies. When temperature is from T E to 1 MeV, the total energy increases extremely faster than the increase of temperature, exhibiting the constant-temperature behavior. The entropy exhibits an abrupt change in their slope at T S ≃ 0.2 − 0.4 MeV in medium-mass nuclei and T S ≃ 0.5 − 0.6 MeV in heavy-mass ones. The existence of T E and T S has been interpreted due to the breaking of the first Cooper pair. Finally, the heat capacity shows a strongly pronounced S-shape in nuclei belonging to the rare-earth region. The temperatures defined at the center of the S − shaped heat capacities, which are known to closely relate to the critical temperature of the pairing phase transition T C , are quite close to those theoretically predicted, namely T C ≈ 0.5Δ − 0.6Δ with Δ = 12 A −1/2 being the empirical pairing gap at zero temperature. The semi-empirical TQs obtained in the present work can be, therefore, a reliable data source to test and/or validate many nuclear thermodynamical models and to examine some nuclear structure properties such as pairing and deformation.
    Type of Medium: Online Resource
    ISSN: 0954-3899 , 1361-6471
    RVK:
    Language: Unknown
    Publisher: IOP Publishing
    Publication Date: 2024
    detail.hit.zdb_id: 1472964-7
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  • 2
    Online Resource
    Online Resource
    IOP Publishing ; 2022
    In:  Journal of Physics G: Nuclear and Particle Physics Vol. 49, No. 10 ( 2022-10-01), p. 105102-
    In: Journal of Physics G: Nuclear and Particle Physics, IOP Publishing, Vol. 49, No. 10 ( 2022-10-01), p. 105102-
    Abstract: The empirical heat capacities of some hot-rotating A ∼ 200 nuclei ( 184 Re, 200 Tl, 211 Po, and 212 At) have been investigated by combining the angular-momentum dependent back-shifted Fermi gas (BSFG) model of nuclear level density (NLD) with the experimental NLD data extracted from the neutron-evaporation spectra at the average total angular momentum ⟨ J ⟩ = 12 ℏ . The parameters of the BSFG are obtained by fitting its NLD to the corresponding measured data using an advanced package of program modeling (CPM) provided by Python feature of IBM decision optimization CPLEX. The results obtained show that the shell correction plays an important role in the formation of empirical S -shaped heat capacity, which serves as a fingerprint for the pairing phase transition in finite nuclear systems. The 184 Re nucleus, which is deformed and has small shell correction, exhibits a weaker S -shaped heat capacity than the remaining three spherical 200 Tl, 211 Po, and 212 At nuclei that have large shell effects. This result contrasts with that recently predicted by the microscopic exact pairing plus independent-particle model at finite temperature (EP + IPM), in which the S -shaped heat capacity was predicted in 184 Re only. This discrepancy between the heat capacities obtained within the BSFG and EP + IPM models suggests that an NLD model capable of well describing the experimental data while also having intrinsic and as complete as possible physical interpretations is still required in order to provide the exact description of nuclear thermodynamic quantities. In addition, more experimental NLD data in other mass and higher energy regions are also demanded.
    Type of Medium: Online Resource
    ISSN: 0954-3899 , 1361-6471
    RVK:
    Language: Unknown
    Publisher: IOP Publishing
    Publication Date: 2022
    detail.hit.zdb_id: 1472964-7
    Location Call Number Limitation Availability
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  • 3
    In: Semiconductor Science and Technology, IOP Publishing, Vol. 32, No. 2 ( 2017-02-01), p. 025005-
    Type of Medium: Online Resource
    ISSN: 0268-1242 , 1361-6641
    RVK:
    Language: Unknown
    Publisher: IOP Publishing
    Publication Date: 2017
    detail.hit.zdb_id: 54647-1
    detail.hit.zdb_id: 1361285-2
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