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A perfect quantum thermal plateau exists, and at T = 0, its value approaches a universal value,.
We propose a method to design shortcuts to adiabaticity for implementing perfect quantum state engineering by the combination of the counterdiabatic driving and the reverse engineering technique.
These Stark and Zeeman decelerators offer the revolutionary capability to produce packets of molecules with a tunable velocity, a narrow velocity and angular spread, and almost perfect quantum state purity [4 8].
We're discovering that our unconscious minds are the perfect quantum machine.
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With the calculated absorption spectrum, the maximum short circuit-current density under a perfect internal quantum process [11] is obtained by the equation: J SC = e hc ∫ 310 nm λ g I λ A λ λ d λ.
In the above optical simulation, we assumed a perfect internal quantum efficiency (i.e., IQE = 100%%), which neglects all kinds of recombination in carrier transportation progress inside the solar cells.
The designed bare DNH system exhibits an outstanding absorption capability with a photocurrent density (under perfect internal quantum process) predicted to be 27.93 mA/cm2, which is 17.39%, 26.17%, and over 100% higher than the best single-nanohole (SNH) system, SNH system with an identical Si volume, and equivalent planar configuration, respectively.
For these reasons, the photoactive absorption (Pabs) can be obtained by eliminating the top TCO absorption from the total absorption calculated from RCWA, and the total photocurrent Jtot is then predicted roughly from Pabs under the assumption of perfect internal quantum process.
Under a perfect internal quantum process, the upper limit of total photocurrent (Jtot) is obtained by integrating spectrally the absorption Pabs (which has excluded the absorptions from non-photoactive layers revised by FEM[14]) over the band of 300 ≤ λ ≤ 1,100 nm weighted by the standard AM 1.5spectra[19]].
For instance, GaAs is the perfect substrate for quantum luminescent devices, such as photoelectric detector [1], high-performance laser [2], quantum information processing [3], and so on.
Even for a perfect 200% quantum yield system, a higher solar cell response requires a reflective coating to reflect the isotropically emitted photons from the downconversion layer back towards the solar cell.
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