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Due to the the short reads length of 100 bp we tested all the odd values for k ∈ [17, 47].
Since the short reads have a length of 100 bp, for the de Bruijn construction we tested all the odd values for k ∈ [17, 47].
Hence, for these runs, we used the set without errors for the short reads, SR-NE, and different odd values for k ∈ [17, 47].
Briefly, a PWM compiles information content (log odd values) for each nucleotide position using existing information on known binding sequences for the protein of interest.
We run LoRDEC with different odd values for k ∈ [15, 31] and aligned the corrected long reads on their reference DNA sequences with the method used by GAGE [ 16].
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Experimental studies on lithium clusters using photo ionization[1], evaporation[2], and Raman spectroscopy[3] have reported stability alternation in Li n depending on even or odd value for n, with even-sized clusters being more stable.
For both l =1 and l = 3, BER values for even values of ∆m are better than the BER values for odd values of ∆m.
For odd values of a similar design can be applied for a few special cases with some performance loss.
Recall the firing threshold manifolds for dynamic inhibition are the nonsingular canards, here shown for odd values of τ s between 1 15 (solid purple).
By Lemma 6, the inner sum over l vanishes for all odd values of m, and the remaining sums for all even values of m give ∑ k = 0 n ( n k ) Δ x n f ( k x ) = ∑ p = 0 n ( − 1 ) n − p ( n p ) f ( 2 p x ) = Δ 2 x n f ( 0 ).
Incorporating this change, we state the preceding result for odd values of l.
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