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- ...!\!\! (1) ~ ~ ~ \displaystyle (\hat ふ_{N} A)_n = \sum_{m=0}^{N-1} ふ_{n,m} A_m\) ...e ふ_{m,n}=\frac{1}{\sqrt{N}} \exp\! \left( \frac{- \mathrm i ~2 ~\pi}{N}~m~n\right)\)6 KB (1,032 words) - 18:48, 30 July 2019
- unsigned long n,mmax,m,j,istep,i; m=n >> 1;4 KB (571 words) - 15:00, 20 June 2013
- ...c_m=\frac{2}{\pi} \int_0^\pi f(x) \cos(mx) \mathrm d x~ ~ ~ \), \( ~ ~ ~ m>0\)3 KB (421 words) - 18:26, 30 July 2019
- \left ( \frac{1}{2} F(0) + \frac{ (-1)^m}{2} F(x_N) + \sum_{n=1}^{N} ~\cos(x_m x_n)~ F(x_n)~\right)\) \( \left ( \frac{1}{2} F_0 + \frac{ (-1)^m}{2} F_N + \sum_{n=1}^{N-1} ~\cos\left(\frac{\pi}{N} mn\right)~ F_n\right) \10 KB (1,447 words) - 18:27, 30 July 2019
- unsigned long n,mmax,m,j,istep,i; m=n >> 1;1 KB (184 words) - 15:00, 20 June 2013
- Then at points \(x_m=\pi m/N\), the field can be approximated with ...e Fourier coefficients for the symmetric field known at porints \(x_m\), \(m=0..N-1\), can be performed with6 KB (825 words) - 18:25, 30 July 2019
- : John. I'm sorry, dear, but for the First of May, I gave you a gallon of perfumes. (A :Guy. I'm standing far from you, let this be my excuse!34 KB (5,616 words) - 05:52, 18 November 2021
- ...ly, properties of the WrightOmega function had been published in 1959 by E.M.Wright E.M.Wright. Solution of the equation \(z\, e^z = a\).4 KB (610 words) - 10:22, 20 July 2020
- main(){ int m,n; double c,p,q; FILE *o; for(m=1;m<51;m++){ p/=m; c=pow(m+1.,m-1); fprintf(o,",%28.14f\n",c*p);}2 KB (87 words) - 15:01, 20 June 2013
- ..._N(z)=\frac{1}{z}\, \sum_{n=0}^{N} \, z^{-n}\, \sum_{m=0}^n\, a_{m,n} \ell^m\) Coefficients \(a_{n,m}\) in the expansion:14 KB (2,037 words) - 18:25, 30 July 2019
- z_type suzexo(z_type z){ int n,m; z_type L=log(-z); z_type c[21]; z_type s; for(m=n-1; m>=0; m--){ s*=L; s+=a[n][m]; }12 KB (682 words) - 07:06, 1 December 2018
- z_type LambertWo(z_type z){ int n,m=48; z_type d=-z; z_type s=LambertWoCoe[m]*d; for(n=m-1;n>0;n--){ s+=LambertWoCoe[n]; s*=d;}5 KB (287 words) - 15:01, 20 June 2013
- z_type AuZexAsy(z_type z){ int m=15,n; z_type s; s=AuZexAsyCo[m]*z; for(n=m-1;n>0;n--){s+=AuZexAsyCo[n]; s*=z;}3 KB (274 words) - 15:01, 20 June 2013
- F_M(z)=1+\sum_{n=1}^{M} a_n \exp(kz)^n\) where \(M>1\) is constant integer, and increment \(k=\ln( p)\).15 KB (2,495 words) - 18:43, 30 July 2019
- M.Ambrova, J.Jurisova, V.Danielik, J.Gabcova. On the solubility of lantanum o N. M. Bobkova. Thermal Expansion of Binary Borate Glasses and Their Structure.8 KB (1,239 words) - 11:32, 20 July 2020
- ...th [[fractional iterate]], iff \(~r\!=\!m/n~\) for some integer numbers \(~m, n~\) and (1) \(~ ~ ~ t_r^m(z)=T^n(z)~\)2 KB (272 words) - 18:25, 30 July 2019
- With coefficients \(c\) and expansion (12), for \(K>1\), for some integer \(M>1\), the zooming function can be defined as follows (21) \(~ ~ ~\displaystyle f_M(z)= K z + \sum_{m=1}^{M} c_m z^b\)10 KB (1,627 words) - 18:26, 30 July 2019
- ...or integen numbers \(m\) and \(n\!\ne\!0\), the [[regular iterate]] \(f=T^{m/n}\) is supposed to be [[fractional iterate]] of function \(T\), id est, fo (1) \( ~ ~ ~ f^n(z)=T^m(z)\)1 KB (178 words) - 06:42, 20 July 2020
- http://www.m-hikari.com/ams/ams-2013/ams-129-132-2013/kouznetsovAMS129-132-2013.pdf F_M(z)=-\ln(-z)+\sum_{m=1}^M \frac{\sum_{n=0}^m a_{m,n} \ln(-z)^n}{z^m}9 KB (1,285 words) - 18:25, 30 July 2019
- M.W. ROSENTHAL, P.R. KASTEN, and R.B. BRIGGS. M. Mitchell Waldrop. Nuclear energy: Radical reactors. 05 December 2012.125 KB (3,105 words) - 08:04, 26 December 2019
