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where A is the absorption and Nphoton is the photon number of AM 1.5G per unit area per unit wavelength.
In terms of number of photons emitted per unit path length and per unit wavelength, (3) becomes frac{dN}{dl cdot dlambda} = 2pialpha left(1 - frac{1}{beta^{2} n^{2}(lambda)}right) frac{1}{lambda^{2}} (4).
Right: Number of Cerenkov photons emitted per unit path length and per unit wavelength by a particle with charge e and β=0.9 in a medium with n=1.4.
To investigate the effective reflection of the Si nanostructures on the solar cell performance under the solar radiation spectrum (i.e., the terrestrial air mass 1.5 global (AM 1.5G) [20]), we calculated the SWR, as given in the following equation [21]: SWR = ∫ R λ N photon dλ ∫ N photon dλ, where R is the reflectance and Nphoton is the photon number of AM 1.5G per unit area per unit wavelength.
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The factors affecting chip loading of unit wave, namely the length of the wavelength, the cutters numbers of unit wavelength, saw blade thickness, the equivalent cutting depth per tooth, the cutting overlap-area ratio per cutter edge, the pitch per each cutter, the cutting overlap-area factor, and the proportional factor of sinusoidal amplitude are investigated.
Production cost (per unit input).
It is shown that the normalized response of the concentrated mass depends on the ratio of the plate mass per unit area times wavelength squared to the value of the concentrated mass.
The sensing sensitivity of refractive index sensor, defined as the shift in the peak/dip1/dip2 wavelength per unit variations of the refractive index dλ/dn is 333.3, 368.3, and 293.3 nm/RIU respectively.
The photocurrent, incident power per unit area P, and excitation wavelength are denoted by I, P and λ respectively.
The definition is shown in Eq. (6) where A is the absorption inside nanowires as a function of the incident wavelength, and N is the number of photons per unit area per second for the incident wavelength from the standard solar spectrum.
If the coupler length is shorter than the characteristic wavelength of the device one of the modes can be neglected and effective two-conductor per-unit-length capacitance and inductance matrices can be introduced.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com