… trigger’s exit range If not specified, the exit range ’s end is set to "auto". 4.18. The AnimationTriggerBehavior enumeration enum AnimationTriggerBehavior "once" "repeat" "alternate" "state" }; once once repeat repeat alternate alternate state state 4.19. Model liveness This se…

…=== NOTE: Version 6.0.1 is the first public release by the author since version 4.18. All version 5 releases were test releases, so all V5 and V6 features are new in 2016 and you should look through them all. BUTTONS - New Implicit Button Type, social-reference: for social media …

…n atoms on NEMS surface.....................................................104 4.18 Representative fractional frequency noise spectra...................................................................106 4.19 Spectral density of fractional frequency noise contributed from gas...…

…e 4.12. Figure 4.13. Figure 4.14. Figure 4.15. Figure 4.16. Figure 4.17. Figure 4.18. Figure 4.19. Figure 4.20. xii Al K-edge EXELFS from Al metal. 78 Partial energy-differential cross sections of Al K edge. 80 Al K-edge EXELFS from Al metal weighted by k? (solid line). 82 Magnit…

…,k− 12 ∆t ©­ x i+ 12 , j,k+ 21 ® + Hy | n−11 Hy |i+ 1 , j,k = i+ 2 , j,k ∆z ∆x (4.18) As a further example, we write down E x component used in Hx above: ∆t © = ­ Ex | 1 i+ 2 , j,k+ 12 n− 12 Hz | n−11 i+ 2 , j+ 12 ,k+ 12 i+ 2 , j− 12 ,k+ 12 ∆y n−1 − Jx |i+ + Ex | , j,k+ 1 Hy | n−…

…Changes from Version 1.1, Revision 2 4.17. Changes from Version 1.1, Revision 3 4.18. Changes from Version 1.1, Revision 4 4.19. Changes from Version 1.1, Revision 5 4.20. Changes from Version 1.1, Revision 6 4.21. Changes from Version 1.1, Revision 7 4.22. Changes from Version 1…

…ulti-scale , 5.55 Temporal vagueness , 5.45 Spatial vagueness , 5.60 Validation 4.18 Dissemination of 3D geological data Rachel Heaven ▶ Full use case description (click to expand): The British Geological Survey (BGS), like all Geological Survey Organizations (GSOs), has as one o…

…) –0.14 (–1.51) Lagged Public Debt (–2) 0.20** (1.82) –0.05 (–0.53) σ 0.02*** (14.18) 0.02*** (15.40) Switching Parameters Regime 1 (S=1) Regime 1 (S=1) Peaks of the wealth cycle Troughs of the wealth cycle Constant 0.004** (1.83) 0.04*** (10.90) Lagged Dependent Var. 0.58*** (8.…

…4.94 74.5 5.02 94.5 5.07 15.0 4.14 35.0 4.77 55.0 4.94 75.0 5.02 95.0 5.07 15.5 4.18 35.5 4.78 55.5 4.94 75.5 5.02 95.5 5.07 16.0 4.21 36.0 4.78 56.0 4.95 76.0 5.02 96.0 5.07 16.5 4.24 36.5 4.79 56.5 4.95 76.5 5.02 96.5 5.07 17.0 4.27 37.0 4.79 57.0 4.95 77.0 5.03 97.0 5.07 17.5 …

…ulation inversion factor using useful macroscopic quantities: nsp = 1− 2ntr −1 (4.18) Though this is a very approximated expression that should be used with caution, it gives a simple way to calculate the population inversion factor that gives the correct behavior. It is unity in…

…(%) fraction (%) 10.00 14.13 ± 2.48 10.07 20.00 12.68 ± 2.32 9.39 30.00 15.47 ± 4.18 9.54 The model further predicts a higher fraction of engulfment with higher freezing front velocities (Fig. 3.12(a)) and longer whiskers (Fig. 3.12(b)). The higher engulfment fraction is caused b…

…aracter spacing, including also even tsumegumi , is defined in JIS X 4051, sec. 4.18.1 b.) 書籍における アキ組 は，次のような場合に利用されている．（アキ組については， 均等詰め を含めてJIS X 4051の4.18.1のb）に規定されている．） To achieve a balance between running heads with few and with many characters. Fixed inter-character spacing i…

…entum: E(k) = E(k0 ) + vF (k − k0 ) + u2 (k − k0 )2 + u3 (k − k0 )3 + O(k 4 ). (4.18) To justify the validity of the det-formula, which is based on the linear dispersion of a chiral mode, we must have k − k0 ∆kc = Min(vF /u2 , vF /u3 ). Therefore, the impurity strength should be …

…re 4.17 Supermodes of a Strongly Coupled Tailored Gain Chirped Array 150 Figure 4.18 “Offset Stripe”? Geometry Tailored Gain Chirped Array ..... 154 Chapter 5. Tailored Gain Broad Area Lasers Figure 5.1 Graded Halftone Pattern 2.1... .. cee cee eee 160 Figure 5.2 “Halftone” Tailo…

…xtension of Eqs. (4.1) and (4.4) to NLQM: pN L (α, β| Aa, Bb ) = hα, β|α, βi , (4.18) where if Alice and Bob’s measurement events are spacelike separated Ψc|α,β = P̂β Âφ A(T A) (t2, t1 ) B̂φB (T B ) (t2, t1 ) P̂α Ûφ1 (T1 ) (t1, t0 ) |Ψini i , (4.19) and N = α,β hΨc | α, β | Ψc …