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When this strategy is used, the maximum effective capacities in the region described in (5) can now be expressed as C 1 SN R 1 = - 1 θ 1 T B log e E z e - θ 1 T B τ log 2 1 + SN R 1 z 1 + 1 - τ log 2 1 + SN R 1 z 1 1 + SN R 1 z 2 / λ, (14) C 2 SN R 2 = - 1 θ 2 T B log e E z e - θ 2 T B τ log 2 1 + SN R 2 z 2 1 + λ SN R 2 z 1 + 1 - τ log 2 1 + SN R 2 z 2. (15).

Then, for a positive prediction (o ≥ t), its confidence value is set to (1 – sn).

Normally, the main Raman peaks from the different phases potentially present in CZTS system are CuS (~267 cm−1), SnS (~220 cm−1), SnS2 (~202 cm−1), Sn2S3 (~234 cm−1), ZnS (~219 Cu2SnS3Cu2SnS3 (~290 cm−1) and Cu2ZnSnS4 (~337 cm−1) [28].However, in present study, we have observed only a Raman peak in the range 334 338 cm−1 suggesting the existence of single phase CZTS films.

For example, a WSN composed of just 30 SNs would have 24 ∗ 30 = 2120 states.

Sentinel node biopsy showed 213 SNs.

For this comparison, we considered the top 50 SN markers (T50 SN), the top 50 SG markers (T50 SG) and the top X SG markers (Tx SG) that comprises a similar number genes as the T50 SNs.

16– 18 SNs were lamellated according to their size, fixed in neutral buffered formaldehyde, and completely embedded.

Fig. 7. Sn lateral velocity variations.

FTC-146, SN-56 and Vesamicol binding affinity to VAChT.

(6) Sn can finish the authentication phase processes.

WHILE i < imaxAND T > 0. sn ← generateNeighborSolution(s).