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While various novel contacts exist at the nanoscale with unique density of states, the simplest ones are the ohmic contacts used to inject and extract the charge carriers.
The advantages of quantum dots over quantum wells are due to their unique density of states resulting from three-dimensional confinement of carriers [3].
Low dimensional materials open new routes to high performance thermoelectric properties due to their unique density of states with confined electrons and holes.
Gleason's theorem can now be invoked to identify the states on A with the density operators on H: to each state ω in ω(AH) there corresponds a unique density
If (mathcal{R}^{s}>0) and (beta(i >alpha(i), iinmathbb{S}), then there exists a unique density (u_ x,y,i)) such that lim_{ttoinfty}sum_{i=1}^{N} iint_{mathbb{R}^{2}} biglvert u t,x,y,i -u_ x,i -u_ xgrvert,yx,iy=0.
If (mathcal{R}^{s}>0) and (beta (i >alpha (i varepsilon (i +gamma (i))), (iin mathbb{S}), then there exists a unique density (u_ x,y,i)) such that lim_{tto infty }sum_{i=1}^{N} iint_{mathbb{R}^{2}} biglvert u t,x,y,i -u _(x,i -u bigrvert,dx,dy=0.
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The arrangement of these unique densities is such that they are likely involved in binding with the membrane-bound a subunit at the V1VO-interface [19], [26].
By their definition, they imply a unique probability density function.
For (tgeq0), suppose that (tilde{h} t, cdot)) has a unique asymptotic density μ associated with (h_{0}).
In fact, each data point would correspond to a unique probability density value that represents its likelihood or unique occurrence rate.
Suppose that ({widetilde{h} t, cdot)}) has a unique asymptotic density, that is, a (muinmathcal{M}[c, d]) such that (tilde{h} t,cdot)rightharpoonupmu) as (trightarrow infty).
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