2019
DOI: 10.1016/j.jmmm.2019.04.057
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Controlled charge and spin current rectifications in a spin polarized device

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Cited by 18 publications
(14 citation statements)
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“…As the net current through any dephasing lead is zero, the voltage (say) V i of the virtual electrodes can be derived by applying a small bias between the real electrodes with V S = V b and V D = 0 (V S and V D are the voltages associated with S and D). Under this condition, the net transmission probability becomes [29][30][31]40…”
Section: Theoretical Formulation Of Circular Spin Currentmentioning
confidence: 99%
See 1 more Smart Citation
“…As the net current through any dephasing lead is zero, the voltage (say) V i of the virtual electrodes can be derived by applying a small bias between the real electrodes with V S = V b and V D = 0 (V S and V D are the voltages associated with S and D). Under this condition, the net transmission probability becomes [29][30][31]40…”
Section: Theoretical Formulation Of Circular Spin Currentmentioning
confidence: 99%
“…The main attention is given in developing a suitable theory for describing circular spin current density, and thus circular current, in presence of dephasing. We introduce dephasing effect by connecting Büttiker probes [27][28][29][30][31] at each lattice sites of the bridging conductor, and it can be assumed as the most convincing and appropriate way to include phase randomization processes in transport phenomena. Instead of Büttiker probes, adding a constant damping factor one can also introduce dephasing into the system, as already reported in few works 5,32,33 , but in this mechanism all the essential features may not be captured.…”
Section: Introductionmentioning
confidence: 99%
“…Now, this spin-dependent transport [ 32 , 55 , 60 , 61 ] behavior can be tuned externally by modifying the characteristics of NM spacer and ferromagnetic layers. The site energies of the NM spacer is altered by cosine modulation following the AAH form [ 62 , 63 , 64 , 65 , 66 , 67 , 68 , 69 , 70 , 71 , 72 , 73 ], whereas the hopping parameter in ferromagnetic chains is rearranged by Floquet–Bloch anstaz [ 60 , 74 , 75 , 76 , 77 , 78 , 79 ] within a minimal coupling scheme due to light irradiation on them. The Hamiltonian of a layered nanojunction is constructed with the TB approximation [ 31 , 67 ] including only the contribution from the nearest-neighbor hopping (NNH) integral.…”
Section: Introductionmentioning
confidence: 99%
“…So far, various simple and complex molecular structures have been investigated theoretically for modulat-ing the rectification performance. For instance, molecular wires 4 , complex molecular structure with metallic electrodes 17 , quantum wires with correlated site potentials 22,23 , DNA molecular system with Fibonacci sequence 24 , etc. The rectification behavior has also been tested experimentally for several molecular systems, such as symmetric tetraphenyl and non-symmetric diblock dipyrimidinyldiphenyl molecules 9 , molecular rods 25 , single melamine molecule adsorbed on a Cu(100) surface 26 , etc.…”
Section: Introductionmentioning
confidence: 99%