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  • ...ns \(f(x)\!=\!\sin(2x)\) , \(f(x)\!=\!\sin(kx)\) , \(f(x)\!=\!\sin(2 \pi x/T)\) and so on separately, it is sufficient to have function \(\sin\). In the
    11 KB (1,501 words) - 18:44, 30 July 2019
  • {z_type u,w,t; int i,j,k,l,e=1,L,p,q,m; for(i=0;i<p;i++){ if(i<j) { t=a[j]; a[j]=a[i]; a[i]=t;}
    1 KB (238 words) - 14:33, 20 June 2013
  • For a given function \(T\), called [[transfer function]], the holomorphic solution \(F\) of [[Transf : \( \!\!\!\!\!\!\!\!\!\!\!\! (1) ~ ~ ~ F(z+1)=T(F(z)) \)
    11 KB (1,565 words) - 18:26, 30 July 2019
  • ...he general expression of the \(c\)th iteration of some transfer function \(T\) through its [[superfunction]] \(F\) and the corresponding [[Abel function : \(\!\!\!\!\!\!\!\!\!\!\!\!\!(3) ~ ~ ~ \displaystyle T^c(z)=F(c+G(z))\)
    5 KB (750 words) - 18:25, 30 July 2019
  • ...h>\!\!\!\!\!\!\!\!\!\! (1) ~ ~ ~ \mathrm i ~\hbar~ \partial \psi /\partial t = \hat H ~\psi</math> where time \\[t\\]is real-valued parameter, and \\[\hbar\\]is universal constant, called th
    7 KB (1,006 words) - 18:26, 30 July 2019
  • [[File:PowIteT.jpg|400px|thumb|Fig.1. Iterates of \(T(z)=z^2~\): \(~y\!=\!T^n(x)\!=\!x^{2^n}~\) for various \(n\)]] ...le:ExpIte4T.jpg|360px|thumb|Fig.3. Iterates of \(T(z)=\exp(z)~\): \(~y\!=\!T^n(x)\!=\!\exp^n(x)~\) ]]
    14 KB (2,203 words) - 06:36, 20 July 2020
  • main(){ int j,k,K, m,M, n,N, u,U,v,V; DB s,t; s=0; DO(u,U) DO(v,V){ t=0.+b[U*v+u]; if(t>s) s=t; }
    9 KB (1,551 words) - 18:26, 30 July 2019
  • {{\rm d}t} \frac{{\rm d}n_1}{{\rm d}t}=-W_{\rm u} n_1 + W_{\rm d} n_2
    9 KB (1,441 words) - 14:33, 20 June 2013
  • Jun Chen, Jack Ng, Zhifang Lin, and C. T. Chan.
    1 KB (209 words) - 14:33, 20 June 2013
  • [[transfer function]] \(T\), the distribution of intensity inside is determined by the [[superfunctio J.-F.Bisson, D.Kouznetsov, K.Ueda, S.T.Fredrich-Thornton, K.Petermann, G.Huber. Switching of emissivity and photoc
    8 KB (1,147 words) - 18:44, 30 July 2019
  • : \(x=a+t A\) и ...x_1,x_2,x_3\}\) является вектором координат, а \(t\) и \(u\) - вещественные параметры. В случае,
    17 KB (263 words) - 18:33, 30 July 2019
  • // #include "1_third_cup_marijuana" /*comment out if won't compile on your system*/ #include "1_cup_nuts" /*comment out if won't compile*/
    9 KB (1,350 words) - 14:34, 20 June 2013
  • ...= \frac{1}{(n\!-\!1)!} \int_a^x\left(x\!-\!t\right)^{n-1} f(t)\,\mathrm{d} t \) ...the expression \((x\!-\!t)^{n-1}\) is interpreted as \(\exp\big(\ln(x\!-\!t) (n\!-\!1) \big)\). Due to the cut line of the logarithm, the \(J^n f\) may
    9 KB (1,321 words) - 18:26, 30 July 2019
  • ...tatistical analysis. In the past, the agency has said similar studies didn't indicate fraud but simply reflected peculiarities of Russia's electoral cul
    9 KB (1,079 words) - 15:16, 12 January 2019
  • ...tatistical analysis. In the past, the agency has said similar studies didn't indicate fraud but simply reflected peculiarities of Russia's electoral cul
    20 KB (1,345 words) - 14:34, 20 June 2013
  • Mr. Black: Can't they propose anything by themselves?
    9 KB (1,574 words) - 19:25, 20 June 2013
  • ...hat, if they stop [[vodka|vodking]] and [[smoking]]?" – "Then even I can't save you!" ...hat, if they stop [[vodka|vodking]] and [[smoking]]?" – "Then even I can't save you!" (2013)
    4 KB (495 words) - 20:04, 28 November 2019
  • Mr. Black: Among thousands of Russian officials, couldn't we find a hundred smart persons to make them ministers, judges and "deputat Mrs. Gold (finish): For their balls. Don't worry, Mr. White, are all in team.
    10 KB (1,732 words) - 07:04, 1 December 2018
  • Nikolay Mizulin, Partner// nmizulin(a)mayerbrown.com // Brussels// T +32 2 551 5967 // F +32 2 502 5421 //
    94 KB (1,481 words) - 17:20, 20 December 2020
  • Martin Sixsmith. Why Russia won't revolt
    11 KB (1,243 words) - 18:25, 30 July 2019
  • Alfred Heinz. Henry Kissinger: "If You Can't Hear the Drums of War You Must Be Deaf". 27/11/2011 09:40. ...superpower left, and that one will be the global government that wins. Don't forget, the United States, has the best weapons, we have stuff that no othe
    3 KB (525 words) - 14:36, 20 June 2013
  • ...нной голоморфной передаточной функции \(T\) записывается в виде : \( \!\!\!(1) ~ ~ ~ T(f(z))=f(kz)\)
    5 KB (116 words) - 18:37, 30 July 2019
  • ...e TaniaS(z_type z){int n; z_type s,t=z+z_type(2.,-M_PI);t*=2./9.; t=I*sqrt(t); s=-1.+t*(3.+t*(-3.+t*(.75+t*(.3+t*(.9/16.+t*(-.3/7.+t*(-12.51/224. //+t*(-.9/28.)
    2 KB (258 words) - 10:19, 20 July 2020
  • <i>.. I don't have a working generic algorithm for any generic complex
    5 KB (707 words) - 21:33, 13 July 2020
  • T(F(z))=F(z+1) where \(~T~\) is given [[transfer function]] and \(~F~\) is holomorphic solution with
    6 KB (987 words) - 10:20, 20 July 2020
  • THEY DID AND LIVED IN PORT, BUT COULDN'T LOOK @dmytrokarpenko 6:15 I still can't understand what started it
    116 KB (1,670 words) - 07:33, 10 March 2024
  • z_type s=0.,t=1.; for(k=0;k<K;k++) { s+=DER3[k]*t; t*=z; }
    9 KB (654 words) - 07:00, 1 December 2018
  • : \(\displaystyle \cos(t)=1-\frac{1}{2}t^2+\frac{1}{4!} t^4-\frac{1}{6!} t^6+ ..\) ...le 1-\cos(t)=\frac{1}{2}t^2-\frac{1}{4!} t^4+\frac{1}{6!} t^6-\frac{1}{8!} t^8+ ..\)
    5 KB (754 words) - 18:47, 30 July 2019
  • : \(\mathrm{Cip}(f_0+t)=x_0+b_2 t^2+ b_3 t^3 +b_4 t^4 + ...\) : \(\mathrm{ArcCip}(x_0+t)=f_0 + c_1 \sqrt{z-x_0} +c_2 (z-x_0) + c_3 (z-x_0)^{3/2} + ...\)
    8 KB (1,211 words) - 18:25, 30 July 2019
  • z_type infac(z_type z){DB x=Re(z),y=Im(z),t=x*x+y*y; if(t<1.)return infac0(z); if( fabs(y)> 5. || (x>0 && t>25) ) return exp(-fracti(z));
    4 KB (487 words) - 07:00, 1 December 2018
  • \arcsin(z)=\int_0^z \frac{\mathrm d t}{\sqrt{1-t^2}}\) ...{\pi}{2}+t\right) = -1+ \frac{t^2}{2}-\frac{t^4}{24}+\frac{t^6}{720}-\frac{t^8}{40320}+..\)
    9 KB (982 words) - 18:48, 30 July 2019
  • ...+t)=J+\frac{\mathrm{coshc}''(H)}{2!} t^2 + \frac{\mathrm{coshc}'''(H)}{3!} t^3+..\) ...}{3H}{t^3}+ \frac{(8\!+\!H^2)J}{24 H^3}{t^4} -\frac{(10\!+\!H^2)J}{30 H^3}{t^5}+..\)
    4 KB (509 words) - 18:26, 30 July 2019
  • : \(\!\!\!\!\!\!\!\!\!\! \displaystyle \mathrm{acosc}(\mathrm{Tarao}\!+\!t)=\mathrm{Sazae} -\Bigg(\frac{- 2 ~ t}{\mathrm{Tarao}}\Bigg)^{\! 1/2}
    8 KB (1,137 words) - 18:27, 30 July 2019
  • : \(\mathrm{cosc}(\mathrm{Sazae}+t)= \mathrm{Tarao}}{2}t^2
    4 KB (649 words) - 18:26, 30 July 2019
  • main(){ int j,k,m,n; DB x,y, p,q, t; z_type z,c,d;
    4 KB (656 words) - 18:25, 30 July 2019
  • z_type acoscB(z_type z){ z_type t=0.33650841691839534+z, u=sqrt(t), s; int n;
    1 KB (219 words) - 18:46, 30 July 2019
  • z_type acoscB(z_type z){ z_type t=0.33650841691839534+z, u=sqrt(t), s; int n; z_type acosc1R(z_type z){int n; z_type s,t,u; t=Tarao1-z; u=sqrt(t);
    3 KB (436 words) - 18:47, 30 July 2019
  • : \(\mathrm{Factorial}(\mathrm{Bart}+t)=\mathrm{Homer} +\frac{1}{2}\mathrm{Factorial''}(\mathrm{Bart}) t^2
    3 KB (376 words) - 18:26, 30 July 2019
  • f_{\vec p}(z+T) = \exp\left(\frac{-\mathrm i p ^2}{2k} T \right) f_{\vec p}(z)\) In the usual case, \(T\) is considered as real parameter, that has sense of the length of propagat
    3 KB (496 words) - 18:25, 30 July 2019
  • with matrix \(T\) defined with P. Amodio, T. Levitina, G. Settanni, and E. B. Weinmu ̈ller. On the Calculation of the
    8 KB (1,183 words) - 10:21, 20 July 2020
  • where \(\Psi=\Psi(\vec x, t)\) is [[wave function]] of a particle in the coordinate representation, \(m ...aystyle \!\!\!\!\!\!\!\!\!\! (4) ~ ~ ~ \Psi=\mathrm e ^{- \mathrm i \omega t} \psi\)
    15 KB (2,070 words) - 18:47, 30 July 2019
  • \frac{1}{\pi}\int_0^\pi \cos\!\big( z \cos (t) \big)~ \mathrm d t DB jnz(int v, int k){ DB x,t; t=M_PI*(k+.5*v-.25); x= t - (v*v-.25)*.5/t;
    6 KB (913 words) - 18:25, 30 July 2019
  • : \(\!\!\!\!\!\!\!\! \mathrm{ArcSinc}(1\!-\!t)= \sqrt{6 t} \left( : \(\!\!\!\!\!\!\!\!\!\displaystyle \mathrm{sinc}(\mathrm{Namihei}\!-\!t)=
    4 KB (563 words) - 18:27, 30 July 2019
  • ...sel function \(J_\nu(x)\). Then the finite \(\nu\)-Hankel transform of \(f(t)\) is defined to be the set of numbers \(g_m\) given by, g_m = \int_0^1 t~\mathrm d t ~ J_\nu(j_{\nu,m}t)~ f(t),
    7 KB (1,063 words) - 18:25, 30 July 2019
  • ...tic approximation]], the exponential dependence of wave function on time \(t\) is assumed: ...aystyle \!\!\!\!\!\!\!\!\!\! (4) ~ ~ ~ \Psi = \psi ~ \exp(\mathrm i \omega t)\)
    5 KB (743 words) - 18:47, 30 July 2019
  • -z \cosh(t) \Big) ~ \mathrm d t
    3 KB (394 words) - 18:26, 30 July 2019
  • \displaystyle Y_0(x)=\frac{-2}{\pi} \int_0^\infty \cos(x \cosh(t)) \mathrm d t\)
    3 KB (445 words) - 18:26, 30 July 2019
  • http://www.falter.at/web/print/detail.php?id=1139 Florian Klenk. 'Den T?tungsauftrag erteilt'. 2009 wurde Umar Israilov in Wien ermordet. Nun geht ...a. Le policier en chef du district - qui dement l'existence d'un gang - a ?t? limoge. 'Si les bandits parviennent a acheter leur lib?ration, je demissio
    97 KB (4,215 words) - 02:27, 17 April 2022
  • . *Знание AutoCAD‚ Компас‚ Solid Works‚ T-Flex‚ Unigraphics или других аналогичных програ https://www.youtube.com/watch?v=U1Wc6rhBpF8#t=11
    193 KB (2,752 words) - 23:58, 31 October 2019
  • : \((1) ~ ~ ~\hat S=\exp\Big(\frac{\rm i}{\hbar} \hat H t\Big)\) where \(\hat H\) is [[Hamiltonian]] of the system, and \(t\) is [[time]].
    9 KB (117 words) - 18:48, 30 July 2019

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