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Published equation contexts

σdose∝1Nphotons\sigma_{\text{dose}} \propto \frac{1}{\sqrt{N_{\text{photons}}}}

Why this formula appears here

Frederick Chen’s analysis of a real 3-nanometer via layer measured this directly: at typical exposure conditions (roughly 60–89 mJ/cm² depending on resist chemistry), the observed missing-via rate came in at the parts-per-million level — “many orders of magnitude higher than expected from basic estimates” that treat each pixel’s exposure as statistically independent [ 3 ] . The gap between the naive estimate and the measured rate is explained by correlation between neighboring exposed pixels: a defect does not need every pixel in a feature to fail independently, it needs a contiguous cluster of neighboring pixels to under- or over-expose together, which happens far more often than…

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σdose\sigma_{\text{dose}}

Symbol sigma_dose

sigmada_dose is a part of this expression. Its role is fixed by the surrounding article and by the operations shown in the formula.

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NphotonsN_{\text{photons}}

Symbol N_photons

NpN_photons occurs below the fraction bar. The quantity above the bar is divided by this expression; zero is excluded as a denominator.

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Nphotons\sqrt{N_{\text{photons}}}

Denominator: sqrtN_photons

The complete quantity below the fraction bar; it must be nonzero for this division.

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How to interpret it

With a fixed numerator, increasing a nonzero denominator reduces the fraction.

Research cited beside this formula

Published contexts (1)

A symbol can carry a different meaning in another article. Each occurrence keeps its own guide and term definitions.

σdose∝1Nphotons\sigma_{\text{dose}} \propto \frac{1}{\sqrt{N_{\text{photons}}}}

Equation 1 · Semiconductors

Advanced Semiconductor Fabrication in Practice: An Advanced Technical Guide

This mathematical expression combines the displayed quantities; its precise role follows from the surrounding article text.

Frederick Chen’s analysis of a real 3-nanometer via layer measured this directly: at typical exposure conditions (roughly 60–89 mJ/cm² depending on resist chemistry), the observed missing-via rate came in at the parts-per-million level — “many orders of magnitude higher than expected from basic estimates” that treat each pixel’s exposure as statistically independent [ 3 ] . The gap between the naive estimate and the measured rate is explained by correlation between neighboring exposed pixels: a defect does not need every pixel in a feature to fail independently, it needs a contiguous cluster of neighboring pixels to under- or over-expose together, which happens far more often than…

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