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We then solved the crystal structure of PXL2LRR determined at resolution of 3.6 Å (Fig. 2A).
We then solved the system of equations to calculate SFGD and RSGD.
First, h was estimated across a range of values ranging from 0 to 10 cm with an interval of 1 mm, and for each value of h we then solved for A and T0, providing different estimates in temperature for each h value.
We then solved the structural temperature-dependent-modulus problem.
We then solved our model of D1 dynamics 3060 times, comprising all combinations of 17 values of kD1dam, 15 values of kexc, and 12 values of xPSII 0) (see Table 1).
We then solved the resulting equation using Laplace transforms.
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We then solve this constrained minimization problem via the proximal gradient method.
We then solve a bi-objective disc brake design problem, which indeed converges quickly.
We then solve the resulting free boundary problem using matched asymptotic expansions.
We then solve the linear programming problem, where δ k ̂, n ̂ ∗ = 1.
Considering Rayleigh fading channel,, we then solve for the peak rate (A6).
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