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NSR database version of May 10, 2024.

Search: Author = M.A.Jafarizadeh

Found 19 matches.

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2024JA02      Nucl.Phys. A1042, 122814 (2024)

M.A.Jafarizadeh, N.Amiri, M.Seidi, M.Ghapanvari

Quantum entanglement of SO(6)-U(5) transitional nuclei in the interacting boson model-2 (IBM-2)

NUCLEAR STRUCTURE 122,124,126,128,130,132,134,136Ce; calculated entanglement entropy values of the low-lying states using IBM-1 and IBM-2; deduced the minimal entanglement entropy for the s-d bosons in the U(5) limit, while maximal entanglement entropy in the O(6) limit.

doi: 10.1016/j.nuclphysa.2023.122814
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2022JA02      Phys.Rev. C 105, 014307 (2022)

M.A.Jafarizadeh, M.Ghapanvari, N.Amiri

Entanglement entropy as a signature of a quantum phase transition in nuclei in the framework of the interacting boson model and interacting boson-fermion model

NUCLEAR STRUCTURE 102,104,106,108,110Pd, 122,123,124,125,126,127,128,129,130,131,132,133,134Xe; calculated entanglement entropy of quantum phase transition, and Q2 for even-A nuclei in the interacting boson model (IBM) and interacting boson-fermion model (IBFM) using affine SU(1, 1) Lie algebra and Schmidt decomposition. Comparison with experimental Q2 values for even-A Pd nuclei.

doi: 10.1103/PhysRevC.105.014307
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2021GH12      Phys.Part. and Nucl.Lett. 18, 511 (2021)

M.Ghapanvari, M.A.Jafarizadeh, N.Amiri, M.Seidi

Supersymmetric Algebraic Model for Descriptions of Transitional Even-Even and Odd-A Nuclei near the Critical Point of the Vibrational to γ-Unstable Shapes

NUCLEAR STRUCTURE 134,135Ba, 130,131Xe; calculated energy levels, J, π, B(E2), expectation values of the d-boson number operator for the lowest states and the fermion number operator. Comparison with available data.

doi: 10.1134/S154747712105006X
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2020AM03      Nucl.Phys. A1002, 121961 (2020)

N.Amiri, M.Ghapanvari, M.A.Jafarizadeh, S.Vosoughi

Nuclear structure and phase transition of odd-odd Cu isotopes: A neutron-proton interacting boson-fermion-fermion model calculation

NUCLEAR STRUCTURE 60,62,64,66Cu; calculated energy levels, J, π, neutron separation energies, Q-values. Comparison with experimental values.

doi: 10.1016/j.nuclphysa.2020.121961
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2018GH03      Nucl.Phys. A971, 51 (2018)

M.Ghapanvari, A.H.Ghorashi, Z.Ranjbar, M.A.Jafarizadeh

High-spin level structure and Ground-state phase transition in the odd-mass 103-109Rh isotopes in the framework of exactly solvable sdg interacting boson-fermion model

NUCLEAR STRUCTURE 103,105,107,109Rh; calculated negative-parity levels, J, π, 2n separation energies, γ-vibration band signature splitting, α-decay energy, 2β-decay energy, Q(α), Q(2β-) using sd- and sdg-IBFM. Compared with available data.

doi: 10.1016/j.nuclphysa.2018.01.009
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2018JA01      Nucl.Phys. A969, 114 (2018)

M.A.Jafarizadeh, Z.Ranjbar, N.Fouladi, M.Ghapanvari

Exactly solvable model of transitional nuclei based on dual algebraic structure for the three level pairing model in the framework of sdg interacting boson model

NUCLEAR STRUCTURE 104,106,108,110Pd; calculated positive parity levels, J, π, B(E2), B(E4), signature splitting of γ-bands using two versions of IBM model. Compared to data.

doi: 10.1016/j.nuclphysa.2017.09.007
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2018JA04      Nucl.Phys. A972, 86 (2018)

M.A.Jafarizadeh, N.Amiri, N.Fouladi, M.Ghapanvari, Z.Ranjbar

Study of phase transition of even and odd nuclei based on q-deforme SU(1, 1) algebraic model

NUCLEAR STRUCTURE 120,122,124,126,128Xe; calculated levels, J, π, quadrupole coefficients, B(E2) using IBM-1, IBM-2, qIBFM-1, qIBFM-2. 123,125,127,129,131Xe; calculated levels, J, π using IBFM. Compared to data.

doi: 10.1016/j.nuclphysa.2018.02.002
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2018JA06      Eur.Phys.J. A 54, 36 (2018)

A.Jalili Majarshin, H.Sabri, M.A.Jafarizadeh

Energy spectra of vibron and cluster models in molecular and nuclear systems

NUCLEAR STRUCTURE 8Be, 12C, 16O; calculated energy, J, π, 2α, 3α, 4α using algebraic cluster model (vibron model with extensions for the collective structure), gs band levels, J, π. Cluster model; compared with available data.

ATOMIC PHYSICS H, Cl; calculated levels, J using cluster model.

doi: 10.1140/epja/i2018-12463-0
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2018JA13      Nucl.Phys. A977, 129 (2018)

M.A.Jafarizadeh, N.Amiri, M.Ghapanvari, N.Fouladi

Algebraic solutions for q - sdl- and q - sdll'-boson systems in the transitional region

NUCLEAR STRUCTURE 126,128,130,132,134,136Ba; calculated levels, J, π, energy rates E(4+1)/E(2+1) and E(0+1)/E(2+1) using spdf-IBM, spd-IBM, q-spdf-IBM and q-spd-IBM. Compared with data.

doi: 10.1016/j.nuclphysa.2018.07.002
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2017GH04      Int.J.Mod.Phys. E26, 1750036 (2017)

M.Ghapanvari, M.A.Jafarizadeh, N.Fouladi, Z.Ranjbar, N.Amiri

Isospin excitation and shape phase transition in odd-mass Cu isotopes

NUCLEAR STRUCTURE 61,63,65,67,69Cu; calculated energies, J, π, B(E2). Comparison with experimental values.

doi: 10.1142/S0218301317500367
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2017JA13      Int.J.Mod.Phys. E26, 1750070 (2017)

M.A.Jafarizadeh, Z.Ranjbar, N.Fouladi, M.Ghapanvari

Investigation of triaxiality in 122-12854Xe isotopes in the framework of sdg-IBM

NUCLEAR STRUCTURE 122,124,126,128Xe; calculated J, π, B(E2). Transitional interacting boson model (IBM).

doi: 10.1142/S0218301317500707
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2017JA15      Nucl.Phys. A968, 287 (2017)

A.Jalili Majarshin, M.A.Jafarizadeh

Photo scattering and absorption cross section in framework of the sdfp-interacting boson model

NUCLEAR STRUCTURE 124,126,128,130,132,134Xe; calculated sdfp levels, J, π, quadrupole-octupole coupled states using IBM, B(E2), B(E1), B(M1), quadrupole moment, σ(γ, x), σ(γ, γ'). Compared with available data.

doi: 10.1016/j.nuclphysa.2017.08.003
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2016JA05      Int.J.Mod.Phys. E25, 1650048 (2016)

M.A.Jafarizadeh, N.Fouladi, M.Ghapanvari, H.Fathi

Phase transition studies of the odd-mass 123-135Xe isotopes based on SU(1, 1) algebra in IBFM

NUCLEAR STRUCTURE 123,125,127,129,131,133,135Xe; calculated energy surfaces, B(E2), energy levels, J, π. Comparison with experimental data.

doi: 10.1142/S0218301316500488
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2016JA06      J.Phys.(London) G43, 095108 (2016)

M.A.Jafarizadeh, A.Jalili Majarshin, N.Fouladi, M.Ghapanvari

Investigation of quantum phase transitions in the spdf interacting boson model based on dual algebraic structures for the four-level pairing model

NUCLEAR STRUCTURE 98,100,102,104,106,108,110Ru; calculated energy levels, J, π, B(E2). Comparison with available data.

doi: 10.1088/0954-3899/43/9/095108
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2016JA10      Int.J.Mod.Phys. E25, 1650089 (2016)

M.A.Jafarizadeh, A.Jalili Majarshin, N.Fouladi

Simultaneous description of low-lying positive and negative parity states in spd, sdf and spdf interacting boson model

NUCLEAR STRUCTURE 108Pd, 98,100,102,104,106,108,110Ru; calculated energy levels, J, π, B(E2), B(E1). Comparison with available data.

doi: 10.1142/S0218301316500890
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2015JA06      Phys.Rev. C 92, 054306 (2015)

M.A.Jafarizadeh, M.Ghapanvari, N.Fouladi

Algebraic solutions for UBF (5) - OBF (6) quantum phase transition in odd-mass-number nuclei

NUCLEAR STRUCTURE 101,103,105,107,109Rh, 127,129,131,133,135,137Ba; calculated levels, J, π, expectation values of the d-boson number, B(E2), S(2n). Dual algebraic structures and the affine SU(1, 1) Lie algebra within the framework of interacting boson-fermion model. Comparison with experimental data. Evidence for U(5) to O(6) quantum phase transition for negative-parity states in odd-A Rh and positive-parity states in odd-A Ba isotopic chains.

doi: 10.1103/PhysRevC.92.054306
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2014FA14      Int.J.Mod.Phys. E23, 1450045 (2014)

H.Fathi, M.Ghadami, H.Sabri, N.Fouladi, M.A.Jafarizadeh

Investigation of shape phase transition in the U(5) <-> SO(6) transitional region by catastrophe theory and critical exponents of some quantities

NUCLEAR STRUCTURE 100,102,104,106,108,110Ru, 102,104,106,108,110Pd; calculated energy levels, potential energy surfaces. Comparison with experimental data.

doi: 10.1142/S0218301314500451
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2013SA49      Eur.Phys.J.Plus 127, 64 (2013)

H.Sabri, B.Rashidian Maleki, J.Fouladi, N.Fouladi, M.A.Jafarizadeh

Pairing effect on spectral statistics of even and odd mass nuclei

NUCLEAR STRUCTURE Z=16-82; calculated spacing distributions by employing the kernel density and maximum-likelihood estimation technique; deduced deviation to more regular dynamics for even-mass nuclei in comparison to the odd-mass ones, effects due to unclosed proton shells.

doi: 10.1140/epjp/i2013-13064-6
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2012JA12      Nucl.Phys. A890-891, 29 (2012)

M.A.Jafarizadeh, N.Fouladi, H.Sabri, B.Rashidian Maleki

Investigation of spectral statistics of nuclear systems by maximum likelihood estimation method

doi: 10.1016/j.nuclphysa.2012.07.007
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