2015
DOI: 10.1038/ncomms7549
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Coherent creation and destruction of orbital wavepackets in Si:P with electrical and optical read-out

Abstract: The ability to control dynamics of quantum states by optical interference, and subsequent electrical read-out, is crucial for solid state quantum technologies. Ramsey interference has been successfully observed for spins in silicon and nitrogen vacancy centres in diamond, and for orbital motion in InAs quantum dots. Here we demonstrate terahertz optical excitation, manipulation and destruction via Ramsey interference of orbital wavepackets in Si:P with electrical read-out. We show milliradian control over the … Show more

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Cited by 38 publications
(43 citation statements)
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“…Terahertz (THz) optical excitations (tuned to an energy-level spacing of approximately meV) can be used to manipulate and detect Rydberg states of donors by using a free-electron laser [16][17][18][19]. In the density range where donor pairs are dominant, the optical field has been used to detect and control the electron tunneling between donor pairs of phosphorus and antimony [20], while in three-donor clusters, the optical excitation (de-excitation) of a shallower "control" donor has the potential to switch on (off) the exchange interaction between the other two deeper donors, thus forming an optically controlled quantum gate [21,22].…”
Section: Introductionmentioning
confidence: 99%
“…Terahertz (THz) optical excitations (tuned to an energy-level spacing of approximately meV) can be used to manipulate and detect Rydberg states of donors by using a free-electron laser [16][17][18][19]. In the density range where donor pairs are dominant, the optical field has been used to detect and control the electron tunneling between donor pairs of phosphorus and antimony [20], while in three-donor clusters, the optical excitation (de-excitation) of a shallower "control" donor has the potential to switch on (off) the exchange interaction between the other two deeper donors, thus forming an optically controlled quantum gate [21,22].…”
Section: Introductionmentioning
confidence: 99%
“…Electrical detection is sensitive. Typically, in these experiments we detect the ionization of about one donor in 10 4 , within a volume of ∼3 × 10 −9 m −3 implying a total of ∼10 7 excited electrons, and, as Fig. 6 shows, the limit is certainly an order of magnitude better than this.…”
Section: Discussionmentioning
confidence: 86%
“…However, phonon emission channels in Si lead to the rapid decay of excited states without a useful photon signal and this limits the number of excited donors which can be detected optically [3]. Very recently we have demonstrated the coherent creation and destruction, via Ramsey interference of picosecond pulse pairs, of orbital wave packets in Si:P with both optical and electrical read-out [4]. The electrical detection mechanism, termed photothermal ionization spectroscopy, is based on the much higher thermal ionization probability for an excited 2p ± state than the ground 1s state, implying that at finite temperature the sample conductivity directly reflects the strength of the 1s to 2p ± orbital transitions [4][5][6][7].…”
Section: Introductionmentioning
confidence: 99%
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“…In a Ramsey interference experiment the coherence produced by the pump pulse can be either enhanced or destroyed by a second pulse depending on their phase difference, and the envelope of the fringes reveals T * 2 [8]. In each of these cases frequency-domain experiments can be used to obtain the same information, but time-domain versions can be preferable when there are multiple processes responsible for the decays as well as static, inhomogeneous broadening effects that must be separated from dynamics.…”
Section: Introductionmentioning
confidence: 99%