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DC Field | Value | Language |
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dc.contributor.author | DHIA, KHALID | - |
dc.contributor.author | KHUDIER | - |
dc.date.accessioned | 2023-01-17T19:50:30Z | - |
dc.date.available | 2023-01-17T19:50:30Z | - |
dc.date.issued | 2011-01-01 | - |
dc.identifier.issn | 1681-6900 | - |
dc.identifier.uri | http://localhost:8080/xmlui/handle/123456789/9345 | - |
dc.description.abstract | In this project, the location of the phase transition in the two dimensional Ising model will be determined using Monte Carlo simulation with importance sampling. the magnetization per site [m ], energy per site [J ], magnetic susceptibility, specific heat of a Ferromagnetic materials are Calculated as a function of temperature T for 10´10, 20´ 20, 40´ 40 , 50´50 spin lattice interaction by using Monte Carlo Simulation of the 2D Ising Model for some experimental values of ferromagnetic materials such as Gadolinium Chloride ( ) 3 GdCl at Curie temperature c T B = 2.2 J k , and ferromagnetic thin film from Nickel ( ) i N growth on cooper (Cu)at Curie temperature c B T = 2.772 J k , in zero and nonzero magnetic field. It was noticed that above a certain temperature ( ) c T the material will be in a paramagnetic state, this will lead to that the average magnetization will be decrease and the average energy increase, while below that temperature ,it will be in a ferromagnetic state, and the average magnetization will increase and the average energy decrease. Moreover, above a certain temperature spontaneous magnetization will be zero. | en_US |
dc.language.iso | en | en_US |
dc.publisher | Eng. & Tech. Journal, Vol.29, No.2, 2011 | en_US |
dc.subject | Ferromagnetic Material | en_US |
dc.subject | Ising Model | en_US |
dc.subject | Monte Carlo Steps | en_US |
dc.subject | Metropolis Algorithm Method | en_US |
dc.title | The Phase Transition of the 2D-Ising Model By Using Monte Carlo Method | en_US |
dc.type | Article | en_US |
Appears in Collections: | كلية الصيدلة |
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