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We then consider extremal CFTs at large central charge, and consider the quantum corrections to the classical spectrum.
Several hundred classical hits will be available as ringtones, including Stravinsky's Petrushka and, at the more popular endof the classical spectrum, Tchaikovsky's Nutcracker Suite or Danny Boy.
But in the spirit of Einstein's probabilistic treatment of radiation, one could still compare the spectrum of a statistical ensemble of such atoms with the classical spectrum" (Darrigol 1992, p. 126; emphasis original).
Moreover there is only a statistical agreement since classically all the frequencies will be given off together, while quantum mechanically only a single photon is emitted with a single frequency in any given transition between stationary states; hence, one must consider a statistical ensemble of atoms to compare with the classical spectrum.
In his 1984 Physics Today article "The Correspondence Principle Revisited," Richard Liboff argues that Bohr's correspondence principle is not a general claim about recovering classical mechanics from quantum mechanics, but the following more restricted claim: "the quantum frequency spectrum of a periodic system approaches the classical spectrum in the limit of large n" (Liboff 1984, p. 52).
In this way, the SCSL not only achieves the primary goal of friendly jamming but also grants more resources (time or frequency) to the jammers and MUE, allowing a performance improvement for both jammers and MUE compared with the classical spectrum leasing.
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Over supported HPW and microporous Cs salt, the classical spectra of the pyridinium species were observed.
Theorem 3.6 demonstrates that certain choices of the pair ((p, J_{m})) yield spectra with desirable properties analogous to the classical spectra of linear maps.
Since the jammers already obtain the resource in the beginning of the superframe (i.e., has already utilized the period β indicated in Fig. 2 a), the MUE has no need to pause the transmission to give way for the jammers and thus saves the cost of performance loss in the second stage compared with classical spectrum leasing.
The Doppler spectrum is shown in Figure 2. Comparing Figure 2 with the classical Jakes spectrum [3], we observe that the maximum Doppler shift exceeds that suggested by Jakes due to the movement of the scatterers.
Correlating with the thickness drop, strong PL was observed at 1.55 eV, indicating the formation of singly charged oxygen vacancies V+O, following the classical PL spectrum interpretation from the literature.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com