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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 the11 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 th7 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_29 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 photoc8 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 \(J^n f\) may9 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 cul9 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 cul20 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 revolt11 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 othe3 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 complex5 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 with6 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 it116 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^24 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
- : \(\mathrm{Factorial}(\mathrm{Bart}+t)=\mathrm{Homer} +\frac{1}{2}\mathrm{Factorial''}(\mathrm{Bart}) t^23 KB (376 words) - 18:26, 30 July 2019
- f_{\vec p}(z+T) = \exp\left(\frac{-\mathrm i p ^2}{2k} T \right) f_{\vec p}(z)\) In the usual case, \(T\) is considered as real parameter, that has sense of the length of propagat3 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 the8 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 t3 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 demissio97 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=11193 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
- : \(\displaystyle 1-J_0(z)=\int_0^z J_1(t)~\mathrm d t \)3 KB (439 words) - 18:26, 30 July 2019
- z_type BesselJ0o(z_type z){ int n; z_type c,s,t; s=1.; c=1.; t=-z*z/4.; for(n=1;n<32;n++) {c/=0.+n*n; c*=t; s+=c;}2 KB (190 words) - 18:47, 30 July 2019
- z_type BesselJ1o(z_type z){ int n; z_type c,s,t; s=1.; c=1.; t=-z*z/4.;2 KB (159 words) - 14:59, 20 June 2013
- \cos(z \cos(t)) \sin(t)^{2 \nu} ~t~ \mathrm d t ...{2}{\pi} \int_0 ^\infty \sin(x \cos(t) - \pi \nu/2) \cos(\nu t) \mathrm d t\)13 KB (1,592 words) - 18:25, 30 July 2019
- z_type BesselY0B(z_type z){ z_type q, f,c,s, u,v, t; int n; f=z-M_PI/4.; c=cos(f); s=sin(f); q=sqrt((2./M_PI)/z); t=-0.25/(z*z);4 KB (370 words) - 18:46, 30 July 2019
- : \( \vec x_n=\vec x_n(t)\)25 KB (335 words) - 18:33, 30 July 2019
- : \( \displaystyle \vec P= \sum_{n=1}^N ~ m_n ~ \dot {\vec x}_n(t)\)6 KB (113 words) - 18:33, 30 July 2019
- Still think that Earth isn't round <br> Isn't it a perfect system?!<br>45 KB (958 words) - 07:17, 1 December 2018
- ...tion is interpreted as trajectory. The time is often denoted with letter \(t\). : \(\vec x_n=\vec x_n(t)\), \(n=1.. N\).4 KB (560 words) - 18:26, 30 July 2019
- ...e frightened by [[Pussy Riot]]. They are essentially a concept and you can't stop a concept.39 KB (1,236 words) - 06:49, 1 December 2018
- {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;}6 KB (1,032 words) - 18:48, 30 July 2019
- At time \(t\!=\!0\) the 0-th elementary body passes the lowest part of its trajectory; ==Notations and case \(t\le 0\)==8 KB (1,036 words) - 18:25, 30 July 2019
- ...\(L=L(q(t),\dot q(t),t)\); dot means the derivative with respect to time \(t\); \(q\) are (generalized) coordinates. :\( S=\int_{a}^{b} L(q,\dot q, t) \mathrm d t \)10 KB (1,317 words) - 18:25, 30 July 2019
- \frac {\mathrm d \vec v}{\mathrm d t}= - \frac{1}{\rho} \nabla p + f\) : \(\displaystyle \frac {\mathrm d \vec v}{\mathrm d t} = \dot{\vec v} + \vec v_{,a} v_a\)4 KB (466 words) - 18:26, 30 July 2019
- ...nternet consensus Thomas Jefferson did not actually say it. But that doesn't make them any less true. Dissent is the Highest Form of Patriotism. By stan ...nternet consensus Thomas Jefferson did not actually say it. But that doesn't make them any less true. Dissent is the Highest Form of Patriotism. By stan73 KB (1,209 words) - 18:38, 30 July 2019
- \(x=0\), \(t=0\) corresponds to the top of the wave. ...ion]], the term with \(\nu \nabla^2 \vec V\) where \(\vec V=\vec V(\vec X, t)\) describes viscosity of the fluid;12 KB (1,879 words) - 18:26, 30 July 2019
- : \( X=X(x,y,t)= \Re( \mathrm{Serega}( k x - \omega t + \mathrm i y))\) : \( Y=Y(x,y,t)= \Im( \mathrm{Serega}( k x - \omega t + \mathrm i y))\)5 KB (674 words) - 18:25, 30 July 2019
- If \(T\) is temperature of the pump light, and \(t\) is temperature of the heat drain, then, the maximal efficiency \(\eta\) s :\( \eta= (T-t)/T\)5 KB (739 words) - 18:25, 30 July 2019
- : \(\!\!\!\!\!\!\!\!\!\!\!(2) ~ ~ ~ ~ F(z\!+\!1) = T(F(z))\) for the [[transfer function]] \(T=\mathrm{LogisticOperator}_s\) by equation (1)7 KB (886 words) - 18:26, 30 July 2019
- :\(\!\!\!\!\!\!\!\!\!\! (1) ~ ~ ~ T(z)=\mathrm{LogisticOperator}_s(z)= s\, z\, (1\!-\!z)\) :\(\!\!\!\!\!\!\!\!\!\! (2) ~ ~ ~ \mathrm{ArcLogisticSequence}_s(T(z))= \mathrm{ArcLogisticSequence}_s(z)+1\)3 KB (380 words) - 18:25, 30 July 2019
- [[File:Logi1a345T300.png|600px|thumb|<small> Various iterates of \(T^c=\mathrm{LogisticOperator}_s\) for : \(\!\!\!\!\!\!\!\!\!\!\!(2) ~ ~ ~ ~ F(z\!+\!1)=T(F(z))\)6 KB (817 words) - 19:54, 5 August 2020
- ...T.png|400px|thumb|Iterates of the Keller function: \(y\!=\!\mathrm{Keller}^t(x)\)]] Using [[Shoka function|Shoka]] and [[ArcShoka]], the \(t\)th iterate of the [[Keller function]] can be expressed as follows:10 KB (1,479 words) - 05:27, 16 December 2019
- ...!2 n)\mathrm i + t\) for integer values of \(n\) and positive values of \(t\). :\( \!\!\!\!\!\!\!\!\!\! (5) ~ ~ ~ T(z)=\mathrm {Keller}(z)=\ln\Big(1+\mathrm e \,(\mathrm e^z-1)\Big)\)10 KB (1,507 words) - 18:25, 30 July 2019
- ...comparison of various [[superfunction]]s \(F\) of the transfer functions \(T\) of realistic physical systems, the extension to the complex plane seems t :\( T(F(z))=F(z\!+\!1)\)3 KB (441 words) - 18:26, 30 July 2019
- in general, the \(t\)th iteration of the Keller function can be written as follows: ...e ~ ~ ~ \mathrm{Keller}^t(z)= z+t+\ln\!\Big(1-\mathrm e^{-z}(1-\mathrm e^{-t}) \Big)\)4 KB (545 words) - 18:26, 30 July 2019
- z_type lofp1(z_type z){DB x=Re(z),y=Im(z), t=x*x+y*y; if(t<2.) return lofp0(z);3 KB (353 words) - 15:01, 20 June 2013
- z_type t=(log(z)-F0)/c2; z_type v=sqrt(t); z_type u=v*(1.+v*(p+A*t))995 bytes (148 words) - 18:46, 3 September 2023
- ...e above gives the expansion of superfunction \(f\) for the base function \(T\!=\!\mathrm{zex}\) in the following form:7 KB (1,076 words) - 18:25, 30 July 2019
- ...correspondant à ce nombre dans le Système international d'unités est T (téra).9 KB (919 words) - 19:47, 6 January 2020
- ...yle (\hbar \omega)/(kT)\), а не как \(\displaystyle (\hbar \omega/k)*T\).8 KB (210 words) - 18:33, 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.)1 KB (209 words) - 15:01, 20 June 2013
- ...ystyle +\frac{226287557 t^9}{37623398400}\) \(\displaystyle -\frac{5776369 t^{10}}{1515591000} +..\)3 KB (223 words) - 18:48, 30 July 2019
- [[SuZex]] is [[superfuncton]] for the [[transfer function]] \(T=\,\,\)[[zex]]; (1) \(~ ~ ~ T(z)=\mathrm{zex}(z) = z\,\exp(z)~\)14 KB (2,037 words) - 18:25, 30 July 2019
- // which is [[superfunction]] for the [[transfer function]] T(z)=[[zex]](z)= z exp(z) <br>12 KB (682 words) - 07:06, 1 December 2018
- z_type LambertWe(z_type z){ int n,m=100; z_type t=1./M_E+z; t*=2*M_E; t=sqrt(t); z_type s=LambertWeCoe[m]*t; for(n=m-1; n>0; n--) { s+=LambertWeCoe[n]; s*=t;} return -1.+s;}5 KB (287 words) - 15:01, 20 June 2013
- [[AuZex]] is [[Abel function]] for the [[transfer function]] \(T\!=\,\)[[zex]], which has the only one real [[fixed point]] \(L\!=\!0\). Aim ...an be implemented for any reasonable holomorphic transfer function. Case \(T=\mathrm{zex}\) is important example of the transfer [[function]], for which6 KB (899 words) - 18:44, 30 July 2019
- Steven T. Corneliussen.5 KB (833 words) - 07:03, 1 December 2018
- ...often it is assumed that \(a\) is real. The real-real plot of function \(T(z)\!=\!z^a\) is shown in Fig.1 for several values of \(a\). \(T(z)= \mathrm{Pow}_{c,r}(z)= c \, z^{1+r}\)15 KB (2,495 words) - 18:43, 30 July 2019
- </ref>, because it begins with letter \(T\), often used to denote the [[Transfer function]]. The question, wether to ...modification is described in this section. Let the [[Transfer function]] \(T\) be defined with9 KB (1,320 words) - 11:38, 20 July 2020
- \( \!\!\!(1) ~ ~ ~ T(f(z))=f(kz)\)<br> \(\!\!\! (9) ~ ~ ~ \displaystyle x=\frac{h\cdot (T-T_0)}{k T T_0}\)3 KB (47 words) - 18:36, 30 July 2019
- (1) \(~ ~ ~ g\Big(T(z)\Big)= s \, g(z)\) where function \(~T~\) is supposed to be given, while constant \(s\) and function\(~g~\) should8 KB (1,239 words) - 11:32, 20 July 2020
- For a given function \(~T~\), [[holomorphic function|holomorphic]] in vicinity of its [[fixed point]] \(t_r=T^r\) is called as \(~r\)th [[fractional iterate]], iff \(~r\!=\!m/n~\) for s2 KB (272 words) - 18:25, 30 July 2019
- ...onian]] of the system is given and the state of the system, say, at time \(t\!=\!0\) is specified, this determines the state of the system at any moment7 KB (1,021 words) - 18:27, 30 July 2019
- (1) \(~ ~ ~ T\big(f(z)\big)= f( K\, z)~\) ...nction such that \(T(0)\!=\!0\) and \(~K~\) is constant, that depends on \(T\).10 KB (1,627 words) - 18:26, 30 July 2019
- ...[[transfer function]], at its [[fixed point]] \(L\) is such [[iterate]] \(T^n\) that is regular at \(L\) even at non–integer values of \(n\). ...ate]] \(f=T^{m/n}\) is supposed to be [[fractional iterate]] of function \(T\), id est, for \(z\) in vicinity of point \(L\),1 KB (178 words) - 06:42, 20 July 2020
- ...e frightened by [[Pussy Riot]]. They are essentially a concept and you can't stop a concept.20 KB (1,323 words) - 07:03, 1 December 2018
- Clear [n, m, M, T] t[1] = Extract[Solve [Coefficient[s[1], x^2] == 0, {a[1, 1]}], 1]9 KB (1,285 words) - 18:25, 30 July 2019
- ...nfair by begrudging us something we need which is useless to you. Dogs don't eat hay, but you will not let us near it.'3 KB (138 words) - 15:02, 20 June 2013
- ...or my children if, after they grew up, they ever asked me, 'Mama, why didn't you leave?'"</i></ref>, несмотря на заявления власт ...the disaster at the nearby Fukushima Daiichi nuclear reactor. He still can't go back. //125 KB (3,105 words) - 08:04, 26 December 2019
- Steven T. Corneliussen. NOAA’s climate overview for 2012 draws media skepticism.38 KB (1,245 words) - 19:16, 6 August 2022
