2012
DOI: 10.1016/j.jpcs.2011.11.020
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Analysis of temperature-dependent electrical resistivity of ZnO nano-structures

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Cited by 19 publications
(12 citation statements)
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“…Given the above discussion on appearance of magnetic order in LNO/STO hybrid structure, it is quite reasonable to assume that the observed temperature behaviour of resistivity can be attributed to the manifestation of strong long-range spin fluctuations with a characteristic energy hω sf ≃ k B T sf corresponding to low-energy spin dynamics spectrum measured by inelastic neutron scattering experiments. It should be pointed out that a rather significant scattering of conduction electrons by spin fluctuations is well documented for many different materials, see, e.g., [19][20][21][22][23][24][25][26] and further references therein. Recently, we suggested a simple phenomenological model based on the resonant like features of SDW type spectrum which result in the observed universal temperature dependence of the resistivity, see [27] for more discussion.…”
Section: Resultsmentioning
confidence: 99%
“…Given the above discussion on appearance of magnetic order in LNO/STO hybrid structure, it is quite reasonable to assume that the observed temperature behaviour of resistivity can be attributed to the manifestation of strong long-range spin fluctuations with a characteristic energy hω sf ≃ k B T sf corresponding to low-energy spin dynamics spectrum measured by inelastic neutron scattering experiments. It should be pointed out that a rather significant scattering of conduction electrons by spin fluctuations is well documented for many different materials, see, e.g., [19][20][21][22][23][24][25][26] and further references therein. Recently, we suggested a simple phenomenological model based on the resonant like features of SDW type spectrum which result in the observed universal temperature dependence of the resistivity, see [27] for more discussion.…”
Section: Resultsmentioning
confidence: 99%
“…The electron effective mass, m n * for n-type ZnO is taken as equal to 0.23 m e [ 53 ]. The electron attempts to escape frequency, ν = 8.54 × 10 12 s −1 , is estimated from the relation hν = kT D [ 54 ], where the Debye temperature, T D , for wurtzite ZnO is 410 K [ 55 ], and all other symbols have their common meaning. From Equation (1) it follows that the values of w and qφ t can be determined from the slope of the plot lnJ versus V and the intersection of the extension of this plot toward the lnJ axis at V = 0.…”
Section: Resultsmentioning
confidence: 99%
“…In case of Xe +17 ions with the increasing radiation dose, the conductivity decreases and at fluence greater than (5 × 10 10 ) m −2 ., polyvacancy complexes and amorphous phase nuclei begin to form. As a result, energy barriers between the disordered regions and the conductive surface emerge in the structure [18]. The magnitude of the barrier depends on the radiation dose and is determined by the size and properties of disordered regions, which impede the movement of electrons.…”
Section: Resultsmentioning
confidence: 99%