2022
DOI: 10.1103/physreva.105.022420
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Feasibility study of quantum computing using trapped electrons

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Cited by 17 publications
(12 citation statements)
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“…An Oscillatory motion of an electron can couple to the readout mode and it allows for the coupling of phonon mode to the propagating mode with the rate ∼ 33 kHz, as discussed in the previous Section. One can immediately see that this cooling rate well surpasses the thermal population of the phonon n th < 20 at the cryogenic temperature multiplied by a conservatively assessed phonon-bath coupling of ∼ 10 Hz [13]. Thanks to this, the phonon mode equilibrates well with the thermal bath, which yields the mean phonon number of 6 at 300 mK environment.…”
Section: Cooling Using a Microwave Cavitymentioning
confidence: 79%
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“…An Oscillatory motion of an electron can couple to the readout mode and it allows for the coupling of phonon mode to the propagating mode with the rate ∼ 33 kHz, as discussed in the previous Section. One can immediately see that this cooling rate well surpasses the thermal population of the phonon n th < 20 at the cryogenic temperature multiplied by a conservatively assessed phonon-bath coupling of ∼ 10 Hz [13]. Thanks to this, the phonon mode equilibrates well with the thermal bath, which yields the mean phonon number of 6 at 300 mK environment.…”
Section: Cooling Using a Microwave Cavitymentioning
confidence: 79%
“…At 300 mK environment with motional frequency of 1 GHz, mean phonon occupation number n can be roughly estimated by assuming the Bose-Einstein distribution to be n ≃ 6. Moreover, it is revealed that the heating rate for trapped electrons amounts 140 quanta per second [13], which may compete the resistive-cooling rate. Other ways than just using dilution refrigerator to cool the trapped electrons are highly demanded, and in this Section, we discuss two cooling methods: one using a cavity mode and another one using a transmon qubit and its measurement.…”
Section: Cooling With Superconducting Circuitsmentioning
confidence: 99%
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