Abstract:The magnetic state of a single magnetic ion (Mn2+) embedded in an individual quantum dot is optically probed using microspectroscopy. The fine structure of a confined exciton in the exchange field of a single Mn2+ ion (S=5/2) is analyzed in detail. The exciton-Mn2+ exchange interaction shifts the energy of the exciton depending on the Mn2+ spin component and six emission lines are observed at zero magnetic field. Magneto-optic measurements reveal that the emission intensities in both circular polarizations are… Show more
“…6b. The fitted Landé factors of the electron (g e = −1.1), the hole (g h = 0.3) and the Mn atom (g Mn = 2.0), the splitting between J z = ±1 and J z = ±2 excitons (= 1 meV) and the diamagnetic factor (γ = 2.45 µeV T −2 ) agree well with previous works [8,14]. Parameters δ 2 and δ Mn were adjusted to fit the zero field data, as explained earlier.…”
Section: Spin Properties Of Manganese-doped Quantum Dots Under Magnetsupporting
confidence: 79%
“…Since the dipolar interaction operator does not affect the Mn d electrons, the final states involve only the Mn 2+ states |S z Mn with the same spin component [14]. In this framework, at zero magnetic field, the QD emission presents a fine structure composed of six doubly degenerate transitions roughly equally spaced in energy …”
Section: Exciton-manganese Exchange Interaction In Symmetric Quantum mentioning
confidence: 99%
“…These lines correspond to the radiative ("bright") exciton states J z = ±1 coupled to the six spin components of the Mn atom (S = 5/2). Analysis of the line intensities gives the occupation probability of the six Mn spin states [14]. The three low intensity lines on the low energy side of the structure (Fig.…”
Section: Interplay Between Electron-hole and Exciton-manganese Exchanmentioning
The magnetic state of a single magnetic ion (Mn 2+ ) embedded in an individual quantum dot is optically probed using microspectroscopy. The fine structure of a confined exciton in the exchange field of a single Mn 2+ ion (S = 5/2) is analyzed in detail. The exciton-Mn 2+ exchange interaction shifts the energy of the exciton depending on the Mn 2+ spin component and six emission lines are observed at zero magnetic field. The emission spectra of individual quantum dots containing a single magnetic Mn atom differ strongly from dot to dot. The differences are explained by the influence of the system geometry, specifically the in-plane asymmetry of the quantum dot and the position of the Mn atom. Depending on both these parameters, one has different characteristic emission features which either reveal or hide the spin state of the magnetic atom. The observed behavior in both zero field and under magnetic field can be explained quantitatively by the interplay between the exciton-manganese exchange interaction (dependent on the Mn position) and the anisotropic part of the electron-hole exchange interaction (related to the asymmetry of the quantum dot).
“…6b. The fitted Landé factors of the electron (g e = −1.1), the hole (g h = 0.3) and the Mn atom (g Mn = 2.0), the splitting between J z = ±1 and J z = ±2 excitons (= 1 meV) and the diamagnetic factor (γ = 2.45 µeV T −2 ) agree well with previous works [8,14]. Parameters δ 2 and δ Mn were adjusted to fit the zero field data, as explained earlier.…”
Section: Spin Properties Of Manganese-doped Quantum Dots Under Magnetsupporting
confidence: 79%
“…Since the dipolar interaction operator does not affect the Mn d electrons, the final states involve only the Mn 2+ states |S z Mn with the same spin component [14]. In this framework, at zero magnetic field, the QD emission presents a fine structure composed of six doubly degenerate transitions roughly equally spaced in energy …”
Section: Exciton-manganese Exchange Interaction In Symmetric Quantum mentioning
confidence: 99%
“…These lines correspond to the radiative ("bright") exciton states J z = ±1 coupled to the six spin components of the Mn atom (S = 5/2). Analysis of the line intensities gives the occupation probability of the six Mn spin states [14]. The three low intensity lines on the low energy side of the structure (Fig.…”
Section: Interplay Between Electron-hole and Exciton-manganese Exchanmentioning
The magnetic state of a single magnetic ion (Mn 2+ ) embedded in an individual quantum dot is optically probed using microspectroscopy. The fine structure of a confined exciton in the exchange field of a single Mn 2+ ion (S = 5/2) is analyzed in detail. The exciton-Mn 2+ exchange interaction shifts the energy of the exciton depending on the Mn 2+ spin component and six emission lines are observed at zero magnetic field. The emission spectra of individual quantum dots containing a single magnetic Mn atom differ strongly from dot to dot. The differences are explained by the influence of the system geometry, specifically the in-plane asymmetry of the quantum dot and the position of the Mn atom. Depending on both these parameters, one has different characteristic emission features which either reveal or hide the spin state of the magnetic atom. The observed behavior in both zero field and under magnetic field can be explained quantitatively by the interplay between the exciton-manganese exchange interaction (dependent on the Mn position) and the anisotropic part of the electron-hole exchange interaction (related to the asymmetry of the quantum dot).
“…These magnetic atoms have six quantized spin states |m , with corresponding eigenvalues m = −5/2,−3/2,−1/2,1/2,3/2,5/2. 4 In Fig.2(a), initial state |ψ M (0) of the magnetic atom is set to be any of the six quantized states. In all cases the magnetic atom is driven to the final state |5/2 .…”
Section: Manipulation Of a Magnetic Atom With Spin M=5/2mentioning
confidence: 99%
“…In dilute II-VI semiconductor quantum dots (QD), interaction between a manganese (Mn) atom and a carrier can be effectively described with the sp − d exchange interaction. [4][5][6] Based on the impurity-carrier coupling, electrical control of the single magnetic atom is feasible by injecting different charges in the magnetic atom doped QD. 6 As shown both in experiment 2 and theory, 7 electrons can directly tunnel through a Mn atom by taking its spin states.…”
We consider theoretically a magnetic impurity spin driven by polarized electrons tunneling through a double quantum dot system. Spin blockade effect and spin conservation in the system make the magnetic impurity sufficiently interact with each transferring electron. As a results, a single collected electron carries information about spin change of the magnetic impurity. The scheme may develop all electrical manipulation of magnetic atoms by means of single electrons, which is significant for the implementation of scalable logical gates in information processing systems.
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