An Application of Interacting Boson Fermion-Fermion Model (IBFFM) for <sup>134</sup>Cs Nucleus

Afrah Jawad Mohaisen; Saad Naji Abood

doi:doi:10.11648/j.ajme.20241001.12

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An Application of Interacting Boson Fermion-Fermion Model (IBFFM) for ¹³⁴Cs Nucleus

Afrah Jawad Mohaisen, Saad Naji Abood^*

Published in American Journal of Modern Energy (Volume 10, Issue 1)

Received: 31 January 2024 Accepted: 14 February 2024 Published: 17 April 2024

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Abstract

This work concerns the calculations of interacting boson fermion-fermion model (IBFFM) for the odd-odd nucleus ¹³⁴Cs. The energy levels (positive and negative parity states), electric transition probability B(E2), magnetic transition probability B(M1), quadrupole and magnetic dipole moments have been studied in this work. The IBFFM results are compared with the available experimental data. In the present work, the IBFFM pattern of total and parametric dependent level densities for the odd-odd nucleus ¹³⁴Cs is investigated and compared to the pattern found in previous investigations in the framework of combinatorial and spectral distribution approaches. When comparing the theoretical values with the available experimental values, it was found that there is a good match between them. This is due to the values of the Hamiltonian parameters that were found accurately, so this IBFFM model is considered one of the effective models in studying the nuclear structure of odd-odd nuclei. The level density of the odd-odd nucleus ¹⁹⁶Au is investigated in the interacting boson-fermion-fermion model (IBFFM) which accounts for collectivity and complex interaction between quasiparticle and collective modes. The IBFFM spin-dependent level densities show high-spin reduction with respect to Bethe formula. This can be well accounted for by a modified spin-dependent level density formula.

Published in	American Journal of Modern Energy (Volume 10, Issue 1)
DOI	10.11648/j.ajme.20241001.12
Page(s)	11-17
Creative Commons	This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited.
Copyright	Copyright © The Author(s), 2024. Published by Science Publishing Group

Keywords

IBFFM, Energy Levels, Electromagnetic Transitions

1. Introduction

A difficulty for theoretical investigations is the available data on the nucleus

, which has been the subject of intensive experimental investigation

[1-3]

The interacting boson model has been widely used to describe even-even and odd-even nuclei throughout the past ten years

[4, 5]

. This strategy was just recently expanded to odd-odd nuclei

[6-10]

. The IBFFM is a new model for odd-odd nuclei that was presented

[6-8]

. In a related advance, a few dynamical symmetries and supersymmetries, including odd-odd nuclei as well, have been created

[8-13]

2. The Interacting Boson Fermion-Fermion Model (IBFFM)

The Interacting Boson Fermion-Fermion Model (IBFFM) is an extension of the Interacting Boson-Fermion Model (IBFM) where the Interacting Boson Model (IBM) core is connected to two fermions. The Hamiltonian of IBFFM is given by

[6]

(1)

For odd-even nuclei containing an odd proton and odd neutron, the IBFM Hamiltonians are indicated by the symbols

and

[5]. The IBM Hamiltonian is represented by

[4]; the

stands for the residual proton-neutron interaction. The IBFFM code includes the residual interactions spin-spin, multipole-multipole, spin-spin-delta, and tensor interaction, which are represented by the study of Paar et al.,

[9]

(2)

where

(3)

is a surface delta-function interaction between the proton and neutron,

(4)

is a surface contact spin-spin interaction,

(5)

is a spin-spin interaction,

(6)

is a tensor interaction, and

(7)

the residual interaction Hamiltonian was calculated as follows:

(8)

where

, the parameters

and

are constants, and determined the strengths of the interactions.

IBFFM computation for ¹³⁴Cs was performed by coupling valence-shell proton and neutron quasiparticles to the IBM boson core.

3. Results and Discussion

3.1. Energy Spectra

The boson core fit the even-even nucleus in the transitional limit (O(6) limit) with the following parameters: A= 0.7, B = 0.8, C= 0.01, and N = 4 (total number of bosons). This parameters shows a

dependence on the potential energy surface, in qualitative accord with earlier computations for

even-even nuclei carried out in the classic collective model

[14-16].

The low-lying portion of the identical spectrum of ¹³²Xe was replicated in the second phase using the renormalized O(6) parameters and the boson space truncated to N = 2. This was done in order to minimize the scope of computations. The low-lying portion of the identical spectrum of ¹³²Xe was replicated in the second phase using the renormalized O(6) parameters and N = 2 is the truncated boson space. This was done in order to minimize the scope of calculations.

The appearance of dynamical symmetries linked to the O(6) limit is related to this property

[17]

. For the SU(3) limit, a comparable circumstance can be found

[18]

. The estimate for ¹³⁴Cs includes the low-lying valence-shell quasiparticle states corresponding to the adjacent odd-even nuclei, ¹³³Xe and ¹³³Cs. These are quasi-protons (g_7/2, d_5/2) and quasi-neutrons (d_3/2, d_5/2, s_1/2). The energies of quasiparticle for the protons g_7/2 and d_5/2 are 0 and 0.7 MeV, respectively with probability of occupation is 0.446 and 0.166.

The quasiparticle energies for d_3/2, d_5/2, and s_l/2 neutrons are 0, 0.7, and 0.9 MeV, with corresponding occupation probabilities of 0.785, 0.988, and 0.969 respectively. The occupancy probabilities are calculated using the BCS parameter proposed by Kisshnger-Sorensen

[19]

. Conversely, the energy levels of approximately ¹³⁴Cs are fitted with three quasiparticle energy spacings. This fits with earlier discussions of odd-odd nuclei in the context of the boson-fermion method

[20]

. Specifically, the quasiparticle energy normalization is caused by the boson-fermion interaction, which results in relative shifts of the quasi-proton quasi-neutron multiplets. As a result, the effective values used to describe odd-odd nuclei may differ from the experimental quasi-particle energies from the neighboring odd-even nuclei.

, the four lowest-lying positive-party levels are 4⁺, 5⁺, 3⁺, and the state at 0.174 MeV, which is designated as 2⁺ or 3⁺. In the

reaction, these states are significantly stimulated by

transfer, and in the (t,

) reaction, by

transfer. Assuming these four levels contain sizable components with (

and the 2⁺ member of the (

multiplets, this is consistent with the (

assumption

[21]

. We have examined in IBFFM how parameters affects the multiplet 2⁺, 3⁺, 4⁺, and 5⁺ splitting that is computed.

If the dynamical and exchange interaction strengths are relatively small (

), the estimated quadrupole moment of the 4⁺ ground state has a negative sign, which is in contradiction with experiment

[2]

It can be observed from examining the four-dimensional parameter space (

) that this pattern is comparatively stable within that range of values. However, it is important to notice that for

, this pattern is consistent with the parabolic rule

[21-23]

prediction.

However, by further increasing the parameter strengths for

, the states 4⁺, 5⁺, 3⁺, and 2⁺ (lie on a parabola) open up and become the domain of parametrization for which we can obtain the experimentally observed pattern, with the 4⁺ state acting as the ground state with positive quadrupole moment. Table 1 displays the calculated positive-parity levels of ¹³⁴Cs up to 0.300 MeV.

The computation employed the following boson-fermion interaction parameters:

MeV,

MeV. The 4⁺, 5⁺, 3⁺, and 2⁺ states wave functions are dominated by components that have

g_7/2 and

_5/2 configurations.

Including

, the quasiparticle with negative panty, additionally, we have determined the occupation probability for negative-parity states using Kisslinger-Sorensen (v²=0.850), attempting to replicate the intricate experimental pattern that would indicate a deformed parabola opening up.

With the exception of

MeV,

MeV, we utilize the same boson-fermion parametrization as for the positive-parity states to get the negative-parity levels depicted in Table 1 up to 0.600 MeV.

Table 1. IBFFM calculations and experimental data

[24]

for low-lying positive parity energy states for ¹³⁴Cs nucleus (in MeV units).

Positive parity states

Negative parity states

Levels

Exp.

[24]

IBFFM

Levels

Exp.

[24]

IBFFM

0.0

0.138

0.142

0.0112

0.010

0.1764

0.170

0.0600

0.077

0.193

0.211

0.173

0.167

0.257

0.289

0.176

0.180

0.267

0.271

0.190

0.195

0.344

0.376

0.197

0210

0.382

0.391

0.209

0.218

0.434

0.442

0.234

0.239

0.450

0.481

0.274

0.281

0.483

0.510

0.290

0.301

0.570

0.589

0.377

0.367

0.613

0.633

0.451

0.433

0.624

0.645

0.454

0.476

0.643

0.681

0.502

0.511

0.684

0.697

0.519

0.522

0.701

0.721

0.539

0.559

0.715

0.20

0.579

0.588

0.752

0.755

0.584

0.611

0.783

0.792

It should be emphasized that there are certain uncertainties in the experimental data about the occupation of g_9/2, such as whether v²(g_7/2) is marginally over or under 0.52 [20]. As a result, we looked into potential parameterizations withv²(g_7/2) > 0.52 in IBFFM. Nevertheless, in this instance, we were unable to replicate the characteristics of the experimentally observed low-lying positive and negative-parity multiplets. The

state wave function, which was produced by diagonalizing H_IBFFM in basis

, has the following biggest components (see Table 2):

Table 2. The wave function components of some of the lowest lying levels in ¹³⁴Cs nucleus as calculated in the IBFFM model.

levels	Wavefunction components

	0.593

The wavefunctions of IBFFM do not show a single component, as would be expected for such a complex nucleus, indicating that assuming simply a one-quasi-proton-one quasi-neutron configuration as a zeroth-order approximation would be overly simplistic. Interestingly, though, we get the low-lying states that one would anticipate based on the zeroth-order approximation (

. even if the wave functions are more complicated, 2⁺, 3⁺, 4⁺, 5⁺, and

,...,

. Furthermore, many characteristics of these states can be roughly explained within the context of the zeroth-order classification and the simple parabolic rule

[21-23]

3.2. Electromagnetic Properties

The eigenstates of the IBFFM-2 Hamiltonian enable us to determine the electric quadrupole (E2) and magnetic dipole (M1) properties of odd-odd nuclei

[6]

(9)

the boson operator is written as

[6]

(10)

where

is the boson effective charge in (e. b) units and

stands for the quadrupole operator is takes by

[6]

(11)

the fermion E2 operator adopts the form

[6]

(12)

with

standing for the effective fermion charge,

is fitted to reproduced the experimental

value of the corresponding even-even boson-core nuclei, as in earlier research [12, 13], whereas

is assumed to be equal to

for all the investigated odd-mass nuclei. The quadrupole moments equation is given by

[6, 17]

(13)

where the reduced electric transition probability

value is given as

[17]

(14)

The magnetic M1 transition operator is given by the formula

[12]

(15)

The M1 boson operator is proportional to the angular momentum operator of boson

with the gyro-magnetic factor

given in terms of the magnetic moment

of the

state of the even-even nucleus. The M1 operator for fermion part is given by

[12, 17]

(16)

Table 3 displays the computed moments of the electric quadrupole and magnetic dipole of the energy states corresponding to the lowest-lying positive and negative-parity multiplets.

The usual values for the effective proton and neutron charges are

and

, respectively, whereas the boson charge,

, is aligned with the 4⁺ state electric quadrupole moment. For medium-heavy nuclei, the boson charges range (

) that was formerly employed is qualitatively consistent with this result. According to conventional values, the ratios of gyromagnets are

. The concordance between the measured and estimated magnetic moment of the ground state is improved by a little decrease in

. The table illustrates how successfully the g-values that were used to simulate the magnetic dipole moments of states 5⁺ and

Now let us discuss the sign of

. Upon nearer examination, the off-diagonal boson contributions of

are responsible for the major partial contributions to

Table 3. Electric quadrupole moments and Magnetic dipole moments for states in ¹³⁴Cs.

levels

Q(e.b).

μ(μ_N)

Exp.

[24]

IBFFM

Exp.

[24]

IBFFM

0.39

0.389

2.99

2.83

0.044

2.33

3.33

-0.55

2.40

-0.39

1.99

1.33

1.10

1.18

0.97

-1.99

0.71

-0.98

0.55

0.47

0.45

-0.24

1.32

0.89

The big components relation (1) and the tiny components relation (2) are the off-diagonal matrix elements, respectively. The latter two tiny coefficients contribute 2.9% and 0.62%, respectively, to the

state wave function.

The computed and experiment ratios are compared in T a ble 4 between the multiplets with the lowest positive and negative parity. The reduced transition probabilities for the

transitions that have been calculated are:

There is consistency between the huge

and the high value of B(E2). The partial contributions incoherence is the cause of

decrease.

The

state half-life,

, is obtained by tabulating internal conversion coefficients and using the computed B (M 1) and B(E2) values for the

transition. This is in reasonable with experimental data of 45 ns.

With the help of the half-life of the

state

using the experimental branching ratio

and the calculated internal conversion constants, this corresponds reasonably well with the experimental measurement of 12 ns. These values are calculated for the

and

transitions. As a result, the distribution of boson charges found from matches the available lifetimes

[23, 24]

Table 4. Electromagnetic transition multiplet for ¹³⁴Cs nucleus.

transitions	Excitation Energy (MeV)
transitions	Excitation Energy (MeV)	Exp.	IBFFM
	0.112	1	1
	0.060	1	0.06
	0.048		0.03
	1.139	1	0.18
	1.738	0.01	1
	0.173	1	1
	0.741	1	0.9
	0.106	-	0.10
	0.931	-	0.008
	1.184	1	1
	0.653	0.03	0.061
	2.056	1	0.92
	0.873	0.23	0.29
	0.767	-	0.009

4. Conclusion

In this work the nuclear structure and electromagnetic transition for ¹³⁴Cs nucleus within IBFFM model have been studied. Theoretically, the transitions between the levels for

have the strongest branches at

and

respectively. The majority of the

transitions are M1 type, which is consistent with experimental results.

The single-particle values are similar to the calculated B(M1) values between the negative-parity states

Conflicts of Interest

The authors declare no conflicts of interest.

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APA Style

Mohaisen, A. J., Abood, S. N. (2024). An Application of Interacting Boson Fermion-Fermion Model (IBFFM) for 134Cs Nucleus. American Journal of Modern Energy, 10(1), 11-17. https://doi.org/10.11648/j.ajme.20241001.12

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ACS Style

Mohaisen, A. J.; Abood, S. N. An Application of Interacting Boson Fermion-Fermion Model (IBFFM) for 134Cs Nucleus. Am. J. Mod. Energy 2024, 10(1), 11-17. doi: 10.11648/j.ajme.20241001.12

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AMA Style

Mohaisen AJ, Abood SN. An Application of Interacting Boson Fermion-Fermion Model (IBFFM) for 134Cs Nucleus. Am J Mod Energy. 2024;10(1):11-17. doi: 10.11648/j.ajme.20241001.12

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@article{10.11648/j.ajme.20241001.12,
  author = {Afrah Jawad Mohaisen and Saad Naji Abood},
  title = {An Application of Interacting Boson Fermion-Fermion Model (IBFFM) for 134Cs Nucleus
},
  journal = {American Journal of Modern Energy},
  volume = {10},
  number = {1},
  pages = {11-17},
  doi = {10.11648/j.ajme.20241001.12},
  url = {https://doi.org/10.11648/j.ajme.20241001.12},
  eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajme.20241001.12},
  abstract = {This work concerns the calculations of interacting boson fermion-fermion model (IBFFM) for the odd-odd nucleus 134Cs. The energy levels (positive and negative parity states), electric transition probability B(E2), magnetic transition probability B(M1), quadrupole and magnetic dipole moments have been studied in this work. The IBFFM results are compared with the available experimental data. In the present work, the IBFFM pattern of total and parametric dependent level densities for the odd-odd nucleus 134Cs is investigated and compared to the pattern found in previous investigations in the framework of combinatorial and spectral distribution approaches. When comparing the theoretical values with the available experimental values, it was found that there is a good match between them. This is due to the values of the Hamiltonian parameters that were found accurately, so this IBFFM model is considered one of the effective models in studying the nuclear structure of odd-odd nuclei. The level density of the odd-odd nucleus 196Au is investigated in the interacting boson-fermion-fermion model (IBFFM) which accounts for collectivity and complex interaction between quasiparticle and collective modes. The IBFFM spin-dependent level densities show high-spin reduction with respect to Bethe formula. This can be well accounted for by a modified spin-dependent level density formula.
},
 year = {2024}
}

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TY  - JOUR
T1  - An Application of Interacting Boson Fermion-Fermion Model (IBFFM) for 134Cs Nucleus

AU  - Afrah Jawad Mohaisen
AU  - Saad Naji Abood
Y1  - 2024/04/17
PY  - 2024
N1  - https://doi.org/10.11648/j.ajme.20241001.12
DO  - 10.11648/j.ajme.20241001.12
T2  - American Journal of Modern Energy
JF  - American Journal of Modern Energy
JO  - American Journal of Modern Energy
SP  - 11
EP  - 17
PB  - Science Publishing Group
SN  - 2575-3797
UR  - https://doi.org/10.11648/j.ajme.20241001.12
AB  - This work concerns the calculations of interacting boson fermion-fermion model (IBFFM) for the odd-odd nucleus 134Cs. The energy levels (positive and negative parity states), electric transition probability B(E2), magnetic transition probability B(M1), quadrupole and magnetic dipole moments have been studied in this work. The IBFFM results are compared with the available experimental data. In the present work, the IBFFM pattern of total and parametric dependent level densities for the odd-odd nucleus 134Cs is investigated and compared to the pattern found in previous investigations in the framework of combinatorial and spectral distribution approaches. When comparing the theoretical values with the available experimental values, it was found that there is a good match between them. This is due to the values of the Hamiltonian parameters that were found accurately, so this IBFFM model is considered one of the effective models in studying the nuclear structure of odd-odd nuclei. The level density of the odd-odd nucleus 196Au is investigated in the interacting boson-fermion-fermion model (IBFFM) which accounts for collectivity and complex interaction between quasiparticle and collective modes. The IBFFM spin-dependent level densities show high-spin reduction with respect to Bethe formula. This can be well accounted for by a modified spin-dependent level density formula.

VL  - 10
IS  - 1
ER  -

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Author Information

Afrah Jawad Mohaisen

Physics Department, College of Science, AL-Nahrain University, Baghdad, Iraq

Contact Email
Saad Naji Abood

Physics Department, College of Science, AL-Nahrain University, Baghdad, Iraq

Contact Email

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Table 1

Table 1. IBFFM calculations and experimental data [24] for low-lying positive parity energy states for ¹³⁴Cs nucleus (in MeV units).
Table 2

Table 2. The wave function components of some of the lowest lying levels in ¹³⁴Cs nucleus as calculated in the IBFFM model.
Table 3

Table 3. Electric quadrupole moments and Magnetic dipole moments for states in ¹³⁴Cs.
Table 4

Table 4. Electromagnetic transition multiplet for ¹³⁴Cs nucleus.

Plain Text BibTeX RIS

APA Style

Mohaisen, A. J., Abood, S. N. (2024). An Application of Interacting Boson Fermion-Fermion Model (IBFFM) for 134Cs Nucleus. American Journal of Modern Energy, 10(1), 11-17. https://doi.org/10.11648/j.ajme.20241001.12

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Mohaisen, A. J.; Abood, S. N. An Application of Interacting Boson Fermion-Fermion Model (IBFFM) for 134Cs Nucleus. Am. J. Mod. Energy 2024, 10(1), 11-17. doi: 10.11648/j.ajme.20241001.12

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AMA Style

Mohaisen AJ, Abood SN. An Application of Interacting Boson Fermion-Fermion Model (IBFFM) for 134Cs Nucleus. Am J Mod Energy. 2024;10(1):11-17. doi: 10.11648/j.ajme.20241001.12

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@article{10.11648/j.ajme.20241001.12,
  author = {Afrah Jawad Mohaisen and Saad Naji Abood},
  title = {An Application of Interacting Boson Fermion-Fermion Model (IBFFM) for 134Cs Nucleus
},
  journal = {American Journal of Modern Energy},
  volume = {10},
  number = {1},
  pages = {11-17},
  doi = {10.11648/j.ajme.20241001.12},
  url = {https://doi.org/10.11648/j.ajme.20241001.12},
  eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajme.20241001.12},
  abstract = {This work concerns the calculations of interacting boson fermion-fermion model (IBFFM) for the odd-odd nucleus 134Cs. The energy levels (positive and negative parity states), electric transition probability B(E2), magnetic transition probability B(M1), quadrupole and magnetic dipole moments have been studied in this work. The IBFFM results are compared with the available experimental data. In the present work, the IBFFM pattern of total and parametric dependent level densities for the odd-odd nucleus 134Cs is investigated and compared to the pattern found in previous investigations in the framework of combinatorial and spectral distribution approaches. When comparing the theoretical values with the available experimental values, it was found that there is a good match between them. This is due to the values of the Hamiltonian parameters that were found accurately, so this IBFFM model is considered one of the effective models in studying the nuclear structure of odd-odd nuclei. The level density of the odd-odd nucleus 196Au is investigated in the interacting boson-fermion-fermion model (IBFFM) which accounts for collectivity and complex interaction between quasiparticle and collective modes. The IBFFM spin-dependent level densities show high-spin reduction with respect to Bethe formula. This can be well accounted for by a modified spin-dependent level density formula.
},
 year = {2024}
}

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TY  - JOUR
T1  - An Application of Interacting Boson Fermion-Fermion Model (IBFFM) for 134Cs Nucleus

AU  - Afrah Jawad Mohaisen
AU  - Saad Naji Abood
Y1  - 2024/04/17
PY  - 2024
N1  - https://doi.org/10.11648/j.ajme.20241001.12
DO  - 10.11648/j.ajme.20241001.12
T2  - American Journal of Modern Energy
JF  - American Journal of Modern Energy
JO  - American Journal of Modern Energy
SP  - 11
EP  - 17
PB  - Science Publishing Group
SN  - 2575-3797
UR  - https://doi.org/10.11648/j.ajme.20241001.12
AB  - This work concerns the calculations of interacting boson fermion-fermion model (IBFFM) for the odd-odd nucleus 134Cs. The energy levels (positive and negative parity states), electric transition probability B(E2), magnetic transition probability B(M1), quadrupole and magnetic dipole moments have been studied in this work. The IBFFM results are compared with the available experimental data. In the present work, the IBFFM pattern of total and parametric dependent level densities for the odd-odd nucleus 134Cs is investigated and compared to the pattern found in previous investigations in the framework of combinatorial and spectral distribution approaches. When comparing the theoretical values with the available experimental values, it was found that there is a good match between them. This is due to the values of the Hamiltonian parameters that were found accurately, so this IBFFM model is considered one of the effective models in studying the nuclear structure of odd-odd nuclei. The level density of the odd-odd nucleus 196Au is investigated in the interacting boson-fermion-fermion model (IBFFM) which accounts for collectivity and complex interaction between quasiparticle and collective modes. The IBFFM spin-dependent level densities show high-spin reduction with respect to Bethe formula. This can be well accounted for by a modified spin-dependent level density formula.

VL  - 10
IS  - 1
ER  -

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