2012
DOI: 10.1103/physrevb.86.041107
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Tunable charge and spin Seebeck effects in magnetic molecular junctions

Abstract: We study the charge and spin Seebeck effects in a spin-1 molecular junction as a function of temperature, applied magnetic field, and magnetic anisotropy (D) using Wilson's numerical renormalization group. A hard-axis magnetic anisotropy produces a large enhancement of the charge Seebeck coefficient Sc (∼ kB/|e|) whose value only depends on the residual interaction between quasiparticles in the low temperature Fermi-liquid regime. In the underscreened spin-1 Kondo regime, the high sensitivity of the system to … Show more

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Cited by 25 publications
(26 citation statements)
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“…The similar conclusions have been confirmed in double quantum dot molecular junction [18,19]. Since the thermoelectric effect in molecular junction can reveal transport mechanisms through the molecular junction [20] and the experiments have demonstrated the capability of measuring the Seebeck coefficient in atomic and molecular junctions [21,Resonance Tunnelling 22], the thermoelectric effect of the single molecule devices attracts much interest [5,17,[23][24][25][26][27].…”
Section: Introductionsupporting
confidence: 51%
“…The similar conclusions have been confirmed in double quantum dot molecular junction [18,19]. Since the thermoelectric effect in molecular junction can reveal transport mechanisms through the molecular junction [20] and the experiments have demonstrated the capability of measuring the Seebeck coefficient in atomic and molecular junctions [21,Resonance Tunnelling 22], the thermoelectric effect of the single molecule devices attracts much interest [5,17,[23][24][25][26][27].…”
Section: Introductionsupporting
confidence: 51%
“…An accurate description of the spectral and transport properties in the most challenging (nonperturbative) regime of intermediate temperatures and bias voltages T, φ T K has however not been feasible until recently. While the electronic transport has been studied extensively, the thermoelectric transport theory mostly focused on the linear response regime 13,25,[71][72][73][74][75][76][77][78][79][80][81][82][83][84][85][86][87][88][89] . The nonlinear regime has been addressed mainly in the weak coupling limit 32,78,[90][91][92][93][94][95][96][97] , a systematic analysis including renormalization effects 66,67,98,99 beyond the perturbative regime is still missing.…”
Section: Introductionmentioning
confidence: 99%
“…However, usually the anisotropy D ∼ µeV is much smaller than other energy scales (∼meV) of interest. Thus, the effect of magnetic anisotropy will be insignificant except in the extremely low temperature regime, where the Kondo effect may play a role 32,[37][38][39][40][41][42][43][44][45] and is beyond the scope of the present work. For large spin cases without anisotropy, they share quantitatively the same behaviors as the spin-half case that we will discuss in detail in the following.…”
Section: Resultsmentioning
confidence: 98%