2023
DOI: 10.3390/axioms12090880
|View full text |Cite
|
Sign up to set email alerts
|

Calculation of Thermodynamic Quantities of 1D Ising Model with Mixed Spin-(s,(2t − 1)/2) by Means of Transfer Matrix

Hasan Akın

Abstract: In this paper, we consider the one-dimensional Ising model (shortly, 1D-MSIM) having mixed spin-(s,(2t−1)/2) with the nearest neighbors and the external magnetic field. We establish the partition function of the model using the transfer matrix. We compute certain thermodynamic quantities for the 1D-MSIM. We find some precise formulas to determine the model’s free energy, entropy, magnetization, and susceptibility. By examining the iterative equations associated with the model, we use the cavity approach to inv… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1

Citation Types

0
3
0

Year Published

2024
2024
2024
2024

Publication Types

Select...
2

Relationship

1
1

Authors

Journals

citations
Cited by 2 publications
(3 citation statements)
references
References 29 publications
(65 reference statements)
0
3
0
Order By: Relevance
“…It may be written as the total of all conceivable states, each of which is weighted by the Boltzmann factor e − β H [36]. The subsequent procedure involves employing the bond representation and breaking down the Boltzmann weights into pairwise factors, essentially decomposing the bonds [16,36]. So, we get We define σ N+1 to be equal to σ 1 in order to establish periodic boundary conditions (see [30] for details).…”
Section: Discussionmentioning
confidence: 99%
See 2 more Smart Citations
“…It may be written as the total of all conceivable states, each of which is weighted by the Boltzmann factor e − β H [36]. The subsequent procedure involves employing the bond representation and breaking down the Boltzmann weights into pairwise factors, essentially decomposing the bonds [16,36]. So, we get We define σ N+1 to be equal to σ 1 in order to establish periodic boundary conditions (see [30] for details).…”
Section: Discussionmentioning
confidence: 99%
“…So, we get We define σ N+1 to be equal to σ 1 in order to establish periodic boundary conditions (see [30] for details). Therefore, from (A2) we obtain the partition function as Now, it is feasible to define the entire thermodynamic properties of the model by utilizing either the partition function and the finite-size free energy or one of its derived forms [16,29,30,35]. From (A4), we obtain the free energy associated with the model as Many researchers have examined other thermodynamic properties as a result of derivatives of the free energy function provided in (A5) with regard to certain parameters [16,29,30,35].…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation