Sharma, Devina and Kumar, Jagdish and Vajpayee, Arpita and Kumar, Ranjan and Ahluwalia, P. K. and Awana, V. P. S.
(2011)
*Comparative Experimental and Density Functional Theory (DFT)
Study of the Physical Properties of MgB2 and AlB2.*
Journal of Superconductivity and Novel Magnetism, 24 (6).
pp. 1925-1931.
ISSN 1557-1947

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## Abstract

In the present study, we report an intercomparison of various physical and electronic properties of MgB2 and AlB2. In particular, the results of phase formation, resistivity ρ(T), thermoelectric power S(T), magnetization M(T), heat capacity (C P ), and electronic band structure are reported. The original stretched hexagonal lattice with a=3.083 Å, and c=3.524 Å of MgB2 shrinks in c-direction for AlB2 with a=3.006 Å, and c=3.254 Å. The resistivity ρ(T), thermoelectric power S(T) and magnetization M(T) measurements exhibited superconductivity at 39 K for MgB2. Superconductivity is not observed for AlB2. Interestingly, the sign of S(T) is +ve for MgB2 the same is −ve for AlB2. This is consistent with our band structure plots. We fitted the experimental specific heat of MgB2 to Debye–Einstein model and estimated the value of Debye temperature (Θ D) and Sommerfeld constant (γ) for electronic specific heat. Further, from γ, the electronic density of states (DOS) at Fermi level N(E F) is calculated. From the ratio of experimental N(E F) and the one being calculated from DFT, we obtained value of λ to be 1.84, thus placing MgB2 in the strong coupling BCS category. The electronic specific heat of MgB2 is also fitted below T c using α-model and found that it is a two gap superconductor. The calculated values of two gaps are in good agreement with earlier reports. Our results clearly demonstrate that the superconductivity of MgB2 is due to very large phonon contribution from its stretched lattice. The same two effects are obviously missing in AlB2, and hence it is not superconducting. DFT calculations demonstrated that for MgB2, the majority of states come from σ and π 2p states of boron on the other hand σ band at Fermi level for AlB2 is absent. This leads to a weak electron phonon coupling and also to hole deficiency as π bands are known to be of electron type, and hence obviously the AlB2 is not superconducting. The DFT calculations are consistent with the measured physical properties of the studied borides, i.e., MgB2 and AlB2.

Item Type: | Article |
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Additional Information: | Copyright for this article belongs to M/s Springer Verlag. |

Uncontrolled Keywords: | MgB2; AlB2; Crystal structure; Electrical resistivity; Thermoelectric-power; Magnetization; Heat capacity and density functional theory |

Subjects: | Applied Physics/Condensed Matter Physics |

Divisions: | UNSPECIFIED |

Depositing User: | Mr. Abhishek Yadav |

Date Deposited: | 09 Nov 2012 11:35 |

Last Modified: | 09 Nov 2012 11:35 |

URI: | http://npl.csircentral.net/id/eprint/814 |

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