added conclusion
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@ -168,7 +168,7 @@ Returning to the specifications, this allows 1.55μm to be expressed as 1.28x10
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\end_inset
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J or approximately 0.8 eV.
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J or approximately 0.800 eV.
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\end_layout
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\begin_layout Standard
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@ -180,7 +180,7 @@ This energy value will be the same as the total interband transition for
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\begin_layout Standard
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\begin_inset Formula
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\begin{equation}
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E_{g,transition}=E_{1h}+E_{g}+E_{1e}\thickapprox0.8\unit{eV}\label{eq:Energy-Gap-Sum}
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E_{g,transition}=E_{1h}+E_{g}+E_{1e}\thickapprox0.800\unit{eV}\label{eq:Energy-Gap-Sum}
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\end{equation}
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\end_inset
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@ -1617,6 +1617,16 @@ status open
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\end_layout
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\begin_layout Plain Layout
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\align center
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Green: 2nm - 4nm
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\end_layout
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\begin_layout Plain Layout
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\align center
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Purple: 6nm - 8nm
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\end_layout
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\begin_layout Plain Layout
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\begin_inset Caption Standard
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@ -1729,6 +1739,36 @@ P\left(6\unit{nm}\leq x\leq8\unit{nm}\right)\thickapprox0.263
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\end_layout
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\begin_layout Subsection
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Conclusions
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\end_layout
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\begin_layout Standard
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Considering these two probabilities it is clear that it is more likely for
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the electron to be found between 6nm and 8nm than between 2nm and 4nm across
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the well.
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This is as expected as 6nm to 8nm places the interval towards the center
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of the well.
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As the probability density function is a
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\begin_inset Formula $\sin^{2}$
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\end_inset
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function, the maxium area will be towards the center.
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Referring to figure
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\begin_inset CommandInset ref
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LatexCommand ref
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reference "fig:Probability-plot-with-bounds"
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plural "false"
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caps "false"
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noprefix "false"
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\end_inset
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this can be seen graphically as the region created by the purple lines
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has a far greater area under the probability density function than the
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region between the green lines.
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\end_layout
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\begin_layout Standard
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\begin_inset Newpage pagebreak
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\end_inset
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@ -1740,6 +1780,10 @@ P\left(6\unit{nm}\leq x\leq8\unit{nm}\right)\thickapprox0.263
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Application of Nanomaterials
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\end_layout
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\begin_layout Standard
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Word count:
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\end_layout
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\begin_layout Standard
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\begin_inset Newpage pagebreak
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\end_inset
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