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The noise spectrum of a quantum dot Eitan Rothstein Netanel Gabdank Ora Entin-Wohlman* Amnon Aharony* Physics Department, Ben Gurion University of the Negev * Also at Tel Aviv University Mesoscopic Physics Meso = Intermidiate, in the middle. Mesoscopic physics = A mesoscopic system is really like a large molecule, but it is always, at least weakly, coupled to a much larger, essentially infinite, system – via phonos, many body excitation, and so on. (Y. Imry, Introduction to mesoscopic physics) A naïve definition: Something very small coupled to something very large. 2/10 Mesoscopic Physics 3/10 Quantum dot There are different types of quantum dots. A large atom connecting to two ledas A metallic grain on a surface Voltage gates on 2DEG 4/10 The model The model Quantum-Dot (QD) N∆ n Vn , k k … Left (L) electronic reservoir Vn , p ∆ Right (R) electronic reservoir p -N∆ Vg DC conductance Noise spectrum C ( ) dteit Iˆ(t )Iˆ(0) I GV I ( IL IR ) / 2 V L R G 2 / e 2 Iˆ Iˆ Iˆ Iˆ ( IˆL IˆR ) / 2 F / 5/10 2C ( ) / e2 No interaction Hartree Fock / The model The Hamiltonian N E Hˆ cˆ cˆ Vn,k (cˆ dˆn h.c) n dˆ dˆn C ( dˆn† dˆn N g ) 2 2 n n N N † † ˆ p cˆ p cˆ p Vn, p (cˆ p d n h.c) electronic Hˆ QD charging energy † k k k N † k † n states on QD momentum states in R/L reservoirs coupling R/L reservoir-QD Hartree Fock approximation Hˆ effQD dˆn†dˆn dˆm† dˆm dˆn†dˆn dˆm† dˆm dˆm† dˆm dˆn†dˆn dˆn†dˆm dˆm† dˆn dˆm† dˆn dˆn†dˆm N ˆ †dˆ E ( dˆ †dˆ N )dˆ † dˆ E ˆ † dˆ dˆ †dˆ [const .] d d n n n C nm n n m m C m n n m n N n m Hartree Fock Self-consistent calculation F d n†d m dE QD 1 Im[ E H eff i]nm N nm 6/10 / (L R ) / F / Level Occupancy and Effective Hamiltonian The effective Hamiltonian Hˆ effQD N ~ dˆ dˆ V n N † n n n n m ~ ˆ† ˆ mn d n d m ~n n EC ( N mm N nn N g ) m ~ Vnm EC N mn Level Occupancy N nn Effective single-e energies ~n F 3.5 F 3.5 (Hartree) (Hartree) EC N nn ; N nm * energy scaled with EC ~ ~n ;Vnm F 3.5 (Hartree Fock) F 3.5 (Hartree Fock) Hartree terms Hartree terms Fock terms Fock terms EC EC 7/10 The Scattering Formalism Treating the problem in the Landauer Büttiker formalism Tight-Binding model Current and correlations ( r L, t ) scattering states QD 1 i 2nm [ E H eff ]nm L S ( E ) 1 QD 1 1 i nm [ E H eff ]nm R L Iˆ (t ) Iˆ (t ' ) e2 (2 )2 Iˆ (t )Iˆ (t ' ) d 4E (2 )2 e2 (2 )2 L R R e Iˆ (t ) 2 S(E) ( r R , t ) scattering region scattering states dEdE ' A ( , E , E ' )aˆ † aˆ ei ( E E ') t 2 * A ( , E, E ' ) S ( E )S ( E ' ) e Ιˆ dE | S ( E ) |2 ( f ( E ) f ( E )) 2 A ( , E, E ' )A ( , E ' ' , E ' ' ' )aˆ ( E )aˆ ( E ' )aˆ ( E ' ' )aˆ ( E ' ' ' )e † † A ( , E , E ' )A ( , E ' , E ) f ( E )(1 f ( E ' )) e d E 2 8/10 i ( E E ')( t t ') (Landauer) i ( E E ' ) t i ( E '' E ' '' ) t ' e (Büttiker) The noise spectrum Noise spectrum C ( ) dteit Iˆ(t )Iˆ(0) Calculations performed for kBT 0 and L R F , so the noise given by F e2 C ( ) 4 dE[2 r * ( E )r ( E ) 2t * ( E )t ( E ) r '*( E )r ' ( E )] F 2C ( ) / e2 2C ( ) / e2 symmetric L R symmetric F 0.5 L R F 0 .2 EC [0,1] EC EC 0.6 Hartree No interaction Hartree Hartree Fock 2C ( ) / e * energy scaled with 2C ( ) / e2 2 symmetric L R F 0.5 asymmetric EC [0,1] EC R / L 9 F 0 .2 EC 0.6 Hartree Fock No interaction Hartree Hartree Fock 9/10 Summary “The noise is the signal” - R. Landauer The noise spectrum exhibits steps and dips o The steps quantum dot resonances o The dips energy difference between the resonances contain information on the coupling asymmetry The interaction effect t o Shifts levels to preserves neutrality o Shifts noise steps and dips Fock effect o Small quantitative effect – modifies the width of the levels Thanks 10/10