2014
DOI: 10.1103/physreva.89.013847
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Scaling laws, pressure anisotropy, and thermodynamic effects for blackbody radiation in a finite cavity

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Cited by 8 publications
(6 citation statements)
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“…The band emissivity of the selective emitter from ambient temperature to 250 °C is plotted in Figure S6 in the Supporting Information. In particular, the proposed emitter has a microcavity structure, and its band emissivity can be calculated according to Stefan–Boltzmann Law concerning the size and temperature effects of the cavity …”
Section: Resultsmentioning
confidence: 99%
“…The band emissivity of the selective emitter from ambient temperature to 250 °C is plotted in Figure S6 in the Supporting Information. In particular, the proposed emitter has a microcavity structure, and its band emissivity can be calculated according to Stefan–Boltzmann Law concerning the size and temperature effects of the cavity …”
Section: Resultsmentioning
confidence: 99%
“…The work in Ref. [18] investigated the near-field radiative entropy density and entropy flux that is valid for both thermal non-equilibrium as well thermal equilibrium cases, and it shows an agreement with the theory of blackbody radiation in the far-field limit, due to multiple reflections, interference and diffraction of light [18,162,168,169].…”
Section: Entropy Transfer: Entropy Due To Near-field Radiative Energy...mentioning
confidence: 67%
“…3(b), these reductions of up to 30% are evident around 7 GHz and 13 GHz. This finding indicates an alternative explanation for the deviations: a modification of the spectral intensity of the BBR inside our apparatus [37][38][39][40][41][42][43]. Such a modification could be caused by a density of modes influenced by the presence of the cell walls and other structures such as supports and field coils close to the cell.…”
Section: Discussionmentioning
confidence: 87%
“…We find that our experimental results deviate significantly from theoretical calculations [17][18][19][20][21][22] in welldefined ranges of n. We attribute these deviations to the spectral intensity distribution of the BBR within the apparatus [37][38][39][40][41][42][43]. Placing additional electrodes around the MOT leads to further changes in the observed transition rates, which indicates that under suitable conditions BBR-induced transitions could also be suppressed in our setup, thus increasing the lifetimes of the Rydberg states without the need for cooling down the apparatus [44].…”
Section: Introductionmentioning
confidence: 89%