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Hence we write (2).
Hence, we write z = ( 1 − t ) x + t y.
We often use g t as a function of x t (i.e. as a likelihood) and hence we write (g_{t}^{y}(x) ~triangleq ~ g_{t} y|x)).
Hence, we write (24) in the following form: min J ( u, w ) subject to e ( u, w ) = 0. Now, we give Theorem 3.1 on the existence of an optimal solution to the sixth-order convective Cahn-Hilliard equation.
Hence, we write absolute value function in Eq. (12) as (varphi (mathbf {I}^{2})=sqrt {(mathbf {I})^{2}+epsilon _{1}} equiv |mathbf {I}|), where ε1 is a small positive constant regularizer.
Then it is well known that ({operatorname{VI}}({varXi },mu F-gamma V)) is a singleton and hence we write ({operatorname{VI}}({varXi },mu F-gamma V) = {x^), that is, ({operatorname{VI}}({operatorname{VI}}({varOmega },mu F-gamma S),mu F-gamma V)={x^).
Similar(49)
Hence, we wrote in the original manuscript (and have left untouched in the revision), "It appears that the high and low points in this time series (2005 and 2008, respectively) may be outliers.
for which leads us to the fact that (3.16). is a Cauchy sequence of real numbers for every fixed Since is complete, it converges, so we write as Hence by using these infinitely many limits, we define the sequence.
Hence, firstly, we write the general form of the Schrödinger-like equation (Equation 3) in a rather more general form as [20, 21, 22, 23, 24, 25, 26, 27, 28, 29] d 2 ψ n s d s 2 + c 1 − c 2 s s 1 − c 3 s d ψ n s ds + − p 2 s 2 + p 1 s − p 0 s 2 1 − c 3 s 2 ψ n s = 0, Open image in new window (4).
Hence we may write.
Hence we can write (3.5).
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com