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The vertical axis is logarithmic in (a) and linear in (b).
In the simplest case, F is linear in b such that begin{aligned} F(b)=F_0left( 1-f_1 bright), end{aligned} (4.11 where (F_0) and (f_1) are positive constants.
When the model is linear in b the derivatives in 2 reduces to the vector x.
If L is considered to be a constant, the running time becomes linear in b.
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The objective function (31) is concave since its Hessian is positive semi-definite [42], and the problem (P4) has a combination of linear and non-linear (polynomial in B) constraints.
At low V b, current is linear in V b with a conductivity WC g V 0 μ 0/L, determined by the low field mobility, as expected.
At high V b, current is again linear in V b, but now with a conductivity of WC g v sat /2 and an offset determined by the gate voltage.
We can see that the Landau levels show a linear dependence in B as expected.
Note the use of a linear scale in (B ).
D, diffusion coefficients of bidirectional RNPs on the microtubule (calculated from the slopes of the linear fits in B using MSD = 2Dt).
In both cases, experimental results (circles) and their linear (or piece-wise linear, in case (b)) interpolations (solid line) are shown.
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