La siguiente tabla contiene una lista de constantes y series en matemáticas, con las siguientes columnas:
| Valor | Nombre | Símbolo | LaTeX | Fórmula | Tipo | OEIS | Fracción continua |
| 3.24697960371746706105000976800847962 | Plata, Tutte-Beraha constante | ς {\displaystyle \varsigma }  | 2 + 2 cos ( 2 π / 7 ) = 2 + 2 + 7 + 7 7 + ⋯ 3 3 3 1 + 7 + 7 7 + 7 7 + ⋯ 3 3 3 {\displaystyle 2+2\cos(2\pi /7)=\textstyle 2+{{frac}{2+{sqrt[{3}]{7+7{sqrt[{3}]{7+7{sqrt[{3}]{\,7+\cdots }}}}}}}{1+{\sqrt[{3}]{7+7{\sqrt[{3}]{7+7{\sqrt[{3}]{\,7+\cdots }}}}}}}}} ![{\displaystyle 2+2\cos(2\pi /7)=\textstyle 2+{\frac {2+{\sqrt[{3}]{7+7{\sqrt[{3}]{7+7{\sqrt[{3}]{\,7+\cdots }}}}}}}{1+{\sqrt[{3}]{7+7{\sqrt[{3}]{7+7{\sqrt[{3}]{\,7+\cdots }}}}}}}}}](https://www.alegsaonline.com/image/63c2ba5c39dd844946fe3ac7702fa5e6b6460472.svg) | 2+2 cos(2Pi/7) | T | A116425 | [3;4,20,2,3,1,6,10,5,2,2,1,2,2,1,18,1,1,3,2,...] |
| 1.09864196439415648573466891734359621 | Constante de París | C P a {\displaystyle C_{Pa}}  | ∏ n = 2 ∞ 2 φ φ + φ n , φ = F i {\displaystyle \prod _{n=2}^{infty }{frac {2\varphi }{varphi +\varphi _{n}};,\varphi ={Fi}}.  | | I | A105415 | [1;10,7,3,1,3,1,5,1,4,2,7,1,2,3,22,1,2,5,2,1,...] |
| 2.74723827493230433305746518613420282 | El radical anidado de Ramanujan R5 | R 5 {\displaystyle R_{5}}  | 5 + 5 + 5 - 5 + 5 + 5 - ⋯ = 2 + 5 + 15 - 6 5 2 {\displaystyle \scriptstyle {\sqrt {5+{sqrt}{5+{sqrt}{5-{sqrt}{5+{sqrt}{5+{sqrt}{5+{sqrt}{5-{sqrt}{5}{sqrt}{5}{sqrt}{sqrt}{5}};=textstyle {\frac {2+{sqrt {5}}+{sqrt {15-6{sqrt {5}}}}}{2}}  | (2+sqrt(5)+sqrt(15-6 sqrt(5)))/2 | I | | [2;1,2,1,21,1,7,2,1,1,2,1,2,1,17,4,4,1,1,4,2,...] |
| 2.23606797749978969640917366873127624 | Raíz cuadrada de 5, suma de Gauss | 5 {\displaystyle {\sqrt {5}}  | ∀ n = 5 , ∑ k = 0 n - 1 e 2 k 2 π i n = 1 + e 2 π i 5 + e 8 π i 5 + e 18 π i 5 + e 32 π i 5 {\displaystyle \scriptstyle \forall \,n=5,\displaystyle \\\\Nsuma _{k=0}^{n-1}e^{\\Nfrac {2k^{2}\pi i}{n}=1+e^{\frac {2\pi i}{5}+e^{\\Nfrac {8\pi i}{5}+e^{\Nfrac {18\pi i}{5}+e^{\Nfrac {32\pi i}{5}}  | Sum[k=0 a 4]{e^(2k^2 pi i/5)} | I | A002163 | [2;4,4,4,4,4,4,4,4,4,4,4,4,4,4,4,4,4,4,4,4,...] = [2;(4),...] |
| 3.62560990822190831193068515586767200 | Gamma(1/4) | Γ ( 1 4 ) {\displaystyle \Gamma ({\tfrac {1}{4}})}  | ¡4 ( 1 4 ) ! ¡= ( - 3 4 ) ! {\displaystyle 4\\a izquierda({\frac {1}{4}{directo)!=\a izquierda(-{\frac {3}{4}{directo)!}  | ¡4(1/4)! | T | A068466 | [3;1,1,1,2,25,4,9,1,1,8,4,1,6,1,1,19,1,1,4,1,...] |
| 0.18785964246206712024851793405427323 | MRB constante, Marvin Ray Burns | C M R B {\displaystyle C_{MRB}}  | ∑ n = 1 ∞ ( - 1 ) n ( n 1 / n - 1 ) = - 1 1 + 2 2 - 3 3 + 4 4 ... {{displaystyle \\\}suma _{n=1}^{infty }({-}1)^{n}(n^{1/n}{-}1)=-{{sqrt[{1}]{1}+{{sqrt[{2}]{2}}+{{sqrt[{3}]{3}}+{{sqrt[{4}]{4}{,\dots } ![{\displaystyle \sum _{n=1}^{\infty }({-}1)^{n}(n^{1/n}{-}1)=-{\sqrt[{1}]{1}}+{\sqrt[{2}]{2}}-{\sqrt[{3}]{3}}+{\sqrt[{4}]{4}}\,\dots }](https://www.alegsaonline.com/image/870bc7fa0415cfa4f3c3fb9253254c65e8e9d967.svg) | Sum[n=1 a ∞]{(-1)^n (n^(1/n)-1)} | T | A037077 | [0;5,3,10,1,1,4,1,1,1,1,9,1,1,12,2,17,2,2,1,...] |
| 0.11494204485329620070104015746959874 | Constante de Kepler-Bouwkamp | ρ {\displaystyle {\rho }}  | ∏ n = 3 ∞ cos ( π n ) = cos ( π 3 ) cos ( π 4 ) cos ( π 5 ) ... {\displaystyle \\\n=3}^{{infty }\cos \left({\frac {\pi }{n}}right)=\cos \left({\frac {\pi }{3}{right)\ncos \left({\frac {\pi }{4}{right)\ncos \left({\frac {\pi }{5}{right)\n}  | prod[n=3 a ∞]{cos(pi/n)} | T | A085365 | [0;8,1,2,2,1,272,2,1,41,6,1,3,1,1,26,4,1,1,...] |
| 1.78107241799019798523650410310717954 | Función Exp(gamma) G-Barnes | e γ {\displaystyle e^{\gamma }}  | ∏ n = 1 ∞ e 1 n 1 + 1 n = ∏ n = 0 ∞ ( ∏ k = 0 n ( k + 1 ) ( - 1 ) k + 1 ( n k ) ) 1 n + 1 = {\displaystyle \{prod _{n=1}^{infty }{{frac {e^{frac {1}{n}}}{1+{\tfrac {1}{n}}}}=prod _{n=0}^{infty }{left(\{prod _{k=0}^{n}(k+1)^{(-1)^{k+1}{n \\\_}right)^{{frac {1}{n+1}=}  ( 2 1 ) 1 / 2 ( 2 2 1 ⋅ 3 ) 1 / 3 ( 2 3 ⋅ 4 1 ⋅ 3 3 ) 1 / 4 ( 2 4 ⋅ 4 4 1 ⋅ 3 6 ⋅ 5 ) 1 / 5 ... {\displaystyle \textstyle \left({\frac {2}{1}\right)^{1/2}left({\frac {2^{2}{1\cdot 3}\right)^{1/3}left({\frac {2^{3}{cdot 4}{1\cdot 3^{3}} {directo)^{1/4} {puntos a la izquierda({frac {2^{4}{cdot 4^{4}{1\cdot 3^{6}{cdot 5}} {directo)^{1/5}  | Prod[n=1 a ∞]{e^(1/n)}/{1 + 1/n} | T | A073004 | [1;1,3,1,1,3,5,4,1,1,2,2,1,7,9,1,16,1,1,1,2,...] |
| 1.28242712910062263687534256886979172 | Constante de Glaisher-Kinkelin | A {\displaystyle {A}}  | e 1 12 - ζ ′ ( - 1 ) = e 1 8 - 1 2 ∑ n = 0 ∞ 1 n + 1 ∑ k = 0 n ( - 1 ) k ( n k ) ( k + 1 ) 2 ln ( k + 1 ) {\displaystyle e^{{frac {1}{12}}-\zeta ^{{prime }(- 1)1)}=e^{{frac {1}{8}}-{{frac {1}{2}}suma \Nde los límites _{n=0}^{infty}}{{frac {1}{n+1}}suma \Nde los límites _{k=0}^{n}{izquierda(-1\a la derecha)^{k}{binom {n}{k}{izquierda(k+1\a la derecha)^{2}{ln(k+1)}}  | e^(1/2-zeta'{-1}) | T | A074962 | [1;3,1,1,5,1,1,1,3,12,4,1,271,1,1,2,7,1,35,...] |
| 7.38905609893065022723042746057500781 | Constante cónica de Schwarzschild | e 2 {\displaystyle e^{2}}  | ¡∑ n = 0 ∞ 2 n n ! ¡= 1 + 2 + 2 2 2 ! ¡+ 2 3 3 ! ¡+ 2 4 4 ! ¡+ 2 5 5 ! + ... {\displaystyle \ {{n=0}^{infty }{{2^{n}{n!}}=1+2+{frac {2^{2}{2!}}+{frac {2^{3}{3!}}+{frac {2^{4}{4!}+{frac {2^{5}{5!}}+{puntos}  | Suma[n=0 a ∞]{2^n/n!} | T | A072334 | [7;2,1,1,3,18,5,1,1,6,30,8,1,1,9,42,11,1,...] = [7,2,(1,1,n,4*n+6,n+2)], n = 3, 6, 9, etc. |
| 1.01494160640965362502120255427452028 | Constante de Gieseking | G G i {\displaystyle {G_{Gi}}  | 3 3 4 ( 1 - ∑ n = 0 ∞ 1 ( 3 n + 2 ) 2 + ∑ n = 1 ∞ 1 ( 3 n + 1 ) 2 ) = {\displaystyle {\frac {3{cuadro {3}}{4}\left(1-)\\N - suma _{n=0}^{infty }{frac {1}(3n+2)^{2}}+{suma _{n=1}^{infty }{frac {1}(3n+1)^{2}} {directo)=}  3 3 4 ( 1 - 1 2 2 + 1 4 2 - 1 5 2 + 1 7 2 - 1 8 2 + 1 10 2 ± ... ) {\displaystyle \textstyle {\frac {3{sqrt {3}}{4}left(1-{frac {1}{2^{2}}+{frac {1}{4^{2}}-{frac {1}{5^{2}}+{frac {1}{8^{2}}+{frac {1}{10^{2}}pm \dots \right)} . | | T | A143298 | [1;66,1,12,1,2,1,4,2,1,3,3,1,4,1,56,2,2,11,...] |
| 2.62205755429211981046483958989111941 | Lemniscata constante | ϖ {\displaystyle {\varpi }}  | π G = 4 2 π ( 1 4 ! ) 2 {\displaystyle \pi \\\},{G}=4{{sqrt {\tfrac {2}{\pi }},({\tfrac {1}{4}})^{2}}  | 4 sqrt(2/pi) (1/4!)^2 | T | A062539 | [2;1,1,1,1,1,4,1,2,5,1,1,1,14,9,2,6,2,9,4,1,...] |
| 0.83462684167407318628142973279904680 | Constante de Gauss | G {\displaystyle {G}}  | ¡1 a g m ( 1 , 2 ) = 4 2 ( 1 4 ! ) 2 π 3 / 2 A g m : A r i t h m e t i c - g e o m e t r i c m e n t e {{displaystyle}} {{Agm:\};Aritmética-geométrica{{};media}{{frac {1}{mathrm {agm} (1,{\sqrt {2})}}={{frac {4{sqrt {2}},({\tfrac {1}{4}}!)^{2}}{pi ^{3/2}}}}}}  | (4 sqrt(2)(1/4!)^2)/pi^(3/2) | T | A014549 | [0;1,5,21,3,4,14,1,1,1,1,1,3,1,15,1,3,7,1,...] |
| 1.01734306198444913971451792979092052 | Zeta(6) | ζ ( 6 ) {\a6)  | π 6 945 = ∏ n = 1 ∞ 1 1 - p n - 6 p n : p r i m o = 1 1 - 2 - 6 ⋅ 1 1 - 3 - 6 ⋅ 1 1 - 5 - 6 . . . {\displaystyle {\frac {\pi ^{6}}{945}=\prod _{n=1}^{{infty}}{{p_{n}}:\{{primo}} {{frac}{1}{p_{n}^-6}}={{frac}{1{-}2^{-6}} {{cdot}} {{frac}{1}{-}3^{-6}} {{cdot}} {{1}{-}5^{-6}}...}  | Prod[n=1 a ∞] {1/(1-ésimo(n)^-6)} | T | A013664 | [1;57,1,1,1,15,1,6,3,61,1,5,3,1,6,1,3,3,6,1,...] |
| 0,60792710185402662866327677925836583 | Constante de Hafner-Sarnak-McCurley | 1 ζ ( 2 ) {\displaystyle {\frac {1}{zeta (2)}}  | 6 π 2 = ∏ n = 0 ∞ ( 1 - 1 p n 2 ) p n : p r i m o = ( 1 - 1 2 2 ) ( 1 - 1 3 2 ) ( 1 - 1 5 2 ) ... {\displaystyle {\frac {6}{pi ^{2}}=}prod _{n=0}^{\infty }{{p_{n}}:\{{primo}} {Izquierda(1-{frac {1}{p_{n}^2}}Derecha)}}=}textstyle {Izquierda(1{-}{frac {1}{2^2}}Derecha)}{Izquierda(1{-}{frac {1}{3^{2}}Derecha)}{{{puntos}}}  | Prod{n=1 a ∞} (1-1/ithprime(n)^2) | T | A059956 | [0;1,1,1,1,4,2,4,7,1,4,2,3,4,10,1,2,1,1,1,...] |
| 1.11072073453959156175397024751517342 | La relación entre un cuadrado y los círculos circunscritos o inscritos | π 2 2 {\displaystyle {\frac {\pi }{2{sqrt {2}}}}}  | ∑ n = 1 ∞ ( - 1 ) ⌊ n - 1 2 ⌋ 2 n + 1 = 1 1 + 1 3 - 1 5 - 1 7 + 1 9 + 1 11 - ... {\displaystyle \\\Nsum _{n=1}^{infty }{{{1)^{lfloor {\frac {n-1}{2}{rfloor}}{2n+1}={frac {1}{1}+{frac {1}{3}}-{frac {1}{5}}-{frac {1}{7}+{frac {1}{9}}+{frac {1}{11}{puntos}}  | suma[n=1 a ∞]{(-1)^(piso((n-1)/2))/(2n-1)} | T | A093954 | [1;9,31,1,1,17,2,3,3,2,3,1,1,2,2,1,4,9,1,3,...] |
| 2.80777024202851936522150118655777293 | Constante Fransén-Robinson | F {\displaystyle {F}}  | ∫ 0 ∞ 1 Γ ( x ) d x . = e + ∫ 0 ∞ e - x π 2 + ln 2 x d x {\displaystyle \int _{0^{infty }{frac {1}{Gamma (x)}},dx.=e+int _{0}^{infty }{frac {e^{x}}{pi ^{2}+\ln ^{2}}x},dx}  | N[int[0 a ∞] {1/Gamma(x)}] | T | A058655 | [2;1,4,4,1,18,5,1,3,4,1,5,3,6,1,1,1,5,1,1,1...] |
| 1.64872127070012814684865078781416357 | Raíz cuadrada del número e | e {\displaystyle {\sqrt {e}}  | ¡∑ n = 0 ∞ 1 2 n n ! ¡= ∑ n = 0 ∞ 1 ( 2 n ) ! ¡! = 1 1 + 1 2 + 1 8 + 1 48 + ⋯ {\displaystyle \\\Nsum _{n=0}^{{infty }{1}{2^{n}n!}}={sum _{n=0}^{{infty }{{1}{(2n)!!}}={{frac {1}{1}}+{frac {1}{2}}+{frac {1}{8}}+{frac {1}{48}}+\cdots }  | suma[n=0 a ∞]{1/(2^n n!)} | T | A019774 | [1;1,1,1,5,1,1,9,1,1,13,1,1,17,1,1,21,1,1,...] = [1;1,(1,1,4p+1)], p∈ℕ |
| i | Número imaginario | i {\displaystyle {i}  | - 1 = ln ( - 1 ) π e i π = - 1 {\displaystyle {\sqrt {-1}}={frac {\ln(-1)}{\pi }}qquad \qquad \mathrm {e}} ^{i,\pi }=-1}  | sqrt(-1) | C | | |
| 262537412640768743.999999999999250073 | Constante de Hermite-Ramanujan | R {\displaystyle {R}}  | e π 163 {\displaystyle e^{pi {\sqrt {163}}}}  | e^(π sqrt(163)) | T | A060295 | [262537412640768743;1,1333462407511,1,8,1,1,5,...] |
| 4.81047738096535165547303566670383313 | Juan constante | γ {\año de la pantalla \año de la pantalla \año \año}  | i i = i - i = i 1 i = ( i i ) - 1 = e π 2 {\displaystyle {\sqrt[{i}]{i}=i^{i}=i^{\frac {1}{i}=(i^{i})^{-1}=e^{\frac {\pi }{2}} ![{\displaystyle {\sqrt[{i}]{i}}=i^{-i}=i^{\frac {1}{i}}=(i^{i})^{-1}=e^{\frac {\pi }{2}}}](https://www.alegsaonline.com/image/904fff5ea95018fde18c45c94097a379edad291e.svg) | e^(π/2) | T | A042972 | [4;1,4,3,1,1,1,1,1,1,1,1,7,1,20,1,3,6,10,3,...] |
| 4.53236014182719380962768294571666681 | Constante de Van der Pauw | α {\año de la pantalla \año de la pantalla \año de la pantalla \año}  | π l n ( 2 ) = ∑ n = 0 ∞ 4 ( - 1 ) n 2 n + 1 ∑ n = 1 ∞ ( - 1 ) n + 1 n = 4 1 - 4 3 + 4 5 - 4 7 + 4 9 - ... 1 1 - 1 2 + 1 3 - 1 4 + 1 5 - ... {\frac {\pi }{ln(2)}}={frac {{suma _{n=0}^{infty}}{{frac {4(-1)^{n}}{2n+1}}{{suma _{n=1}^{infty}}{(-1)^{n+1}{n}}}}={frac {{4}{1}{-{{frac {4}{3}{+}{frac {4}{5}{-}{frac {4}{7}{+}{frac {4}{9}}-puntos}{frac {1}{1}{-}{frac {1}{2}{+}{frac {1}{3}{-}{frac {1}{4}{+}{puntos}}  | π/ln(2) | T | A163973 | [4;1,1,7,4,2,3,3,1,4,1,1,4,7,2,3,3,12,2,1,...] |
| 0.76159415595576488811945828260479359 | Tangente hiperbólica (1) | t h 1 {\diseño de la pantalla th\,1}  | e - 1 e e + 1 e = e 2 - 1 e 2 + 1 {\displaystyle {\frac {e-{\frac {1}{e}}{e+{\frac {1}{e}}}}={\frac {e^{2}-1}{e^{2}+1}}  | (e-1/e)/(e+1/e) | T | A073744 | [0;1,3,5,7,9,11,13,15,17,19,21,23,25,27,...] = [0;(2p+1)], p∈ℕ |
| 0.69777465796400798200679059255175260 | Constante de la fracción continua | C C F {\displaystyle {C}_{CF}}  | J 1 ( 2 ) J 0 ( 2 ) F u n c i ó n J k ( ) B e s e l = ∑ n = 0 ∞ n ! n ! ∑ n = 0 ∞ 1 n ! n ! = 0 1 + 1 1 + 2 4 + 3 36 + 4 576 + ... 1 1 + 1 1 + 1 4 + 1 36 + 1 576 + ... {{displaystyle}} {{conjunto de j_{k}()} {{Bessel}} {{conjunto de funciones}} {{frac {J_{1}(2)}{J_{0}(2)} }}}}={{frac {suma de límites _{n=0}^{{infty}} {{frac {n}{n!¡n!}}{{suma \N de los límites _{n=0}^{{infty}}{{1}{n!n!}}}}={{frac {0}{1}+{frac {1}{1}+{frac {2}{4}+{frac {3}{36}+{frac {4}{576}+puntos}{{frac {1}+{frac {1}{4}+{frac {1}{36}+{puntos}}  | (suma {n=0 a inf} n/(n!n!)) /(suma {n=0 a inf} 1/(n!n!)) | | A052119 | [0;1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,...] = [0;(p+1)], p∈ℕ |
| 0.36787944117144232159552377016146086 | Constante inversa de Napier | 1 e {\displaystyle {\frac {1}{e}}  | ¡∑ n = 0 ∞ ( - 1 ) n n ! ¡= 1 0 ! - ¡- 1 1 ! ¡+ 1 2 ! - ¡- 1 3 ! ¡+ 1 4 ! - ¡- 1 5 ! + ... {\displaystyle \ {{n=0}^{{infty}}={{1)^{n}} {{n!}}={frac {1}{0!}}-{frac {1}{1!}}+{frac {1}{2!}}-{frac {1}{3!}+{frac {1}{4!}}-{frac {1}{5!}+{puntos}}  | suma[n=2 a ∞]{(-1)^n/n!} | T | A068985 | [0;2,1,1,2,1,1,4,1,1,6,1,8,1,1,10,1,1,12,...] = [0;2,1,(1,2p,1)], p∈ℕ |
| 2.71828182845904523536028747135266250 | Constante de Napier | e {\diseño e}  | ¡∑ n = 0 ∞ 1 n ! ¡= 1 0 ! ¡+ 1 1 + 1 2 ! ¡+ 1 3 ! ¡+ 1 4 ! ¡+ 1 5 ! + ⋯ {\displaystyle \ {{n=0}^{infty}}={frac {1}{n!}}+{frac {1}{1}+{frac {1}{2!}+{frac {1}{3!}+{frac {1}{4!}+{frac {1}{5!}+{cdots }  | Suma[n=0 a ∞]{1/n!} | T | A001113 | [2;1,2,1,1,4,1,1,6,1,8,1,1,10,1,1,12,1,...] = [2;(1,2p,1)], p∈ℕ |
| 0.49801566811835604271369111746219809 - 0.15494982830181068512495513048388 i | Factorial de i | ¡i ! {\a6}*Estilo de visualización i\a6}*  | Γ ( 1 + i ) = i Γ ( i ) {\displaystyle \Gamma (1+i)=i,\Gamma (i)}  | Gamma(1+i) | C | A212877 A212878 | [0;6,2,4,1,8,1,46,2,2,3,5,1,10,7,5,1,7,2,...] - [0;2,125,2,18,1,2,1,1,19,1,1,1,2,3,34,...] i |
| 0.43828293672703211162697516355126482 + 0.36059247187138548595294052690600 i | Infinito Tetralogía de i | ∞ i {{displaystyle}}^{{infty}}  | lim n → ∞ n i = lim n → ∞ i i ⋅ i ⏟ n {\displaystyle \lim _{n a \infty }}^{n}i=lim _{n a \infty }\\\\bcipitaje {i^{cdot ^\cdot ^{i}}}}} _{n}}  | i^i^i^... | C | A077589 A077590 | [0;2,3,1,1,4,2,2,1,10,2,1,3,1,8,2,1,2,1, ...] + [0;2,1,3,2,2,3,1,5,5,1,2,1,10,10,6,1,1...] i |
| 0.56755516330695782538461314419245334 | Módulo del infinito Tetración de i | | ∞ i | {\displaystyle |{}^{\infty }i|}  | lim n → ∞ | n i | = | lim n → ∞ i i ⋅ ⋅ i ⏟ n | {\displaystyle \lim _{n\\\a \infty }left|{^{n}i\a derecha|=\left|\lim _{n\a \infty }{underbrace} {i^{{cdot ^{cdot ^{i}}}}} {{n}}Derecha}}  | Mod(i^i^i^...) | | A212479 | [0;1,1,3,4,1,58,12,1,51,1,4,12,1,1,2,2,3,...] |
| 0.26149721284764278375542683860869585 | Constante de Meissel-Mertens | M {\diseño M}  | lim n → ∞ ( ∑ p ≤ n 1 p - ln ( ln ( n ) ) ) {\displaystyle \lim _{n}flecha \infty }left(\sum _{p\leq n}{\frac {1}{p}}-\ln(\ln(n))\right)} ..... p: primos | | | A077761 | [0;3,1,4,1,2,5,2,1,1,1,1,13,4,2,4,2,1,33,...] |
| 1.9287800... | Constante de Wright | ω {\año de la pantalla \año de la pantalla \año de la pantalla \año \año \año \año}  | ⌊ 2 2 2 ⋅ ⋅ 2 ω ⌋ {\displaystyle \left\lfloor 2^{2^{cdot ^{cdot ^2^{omega }}}}}}\rfloor } = primos: ⌊ 2 ω ⌋ {\displaystyle \left\lfloor 2^{\omega }\right\rfloor } =3, ⌊ 2 2 ω ⌋ {\displaystyle \left\lfloor 2^{2^{\omega }\right\rfloor } =13, ⌊ 2 2 2 ω ⌋ {\displaystyle \left\lfloor 2^{2^{\omega }}\right\rfloor } =16381, ... {\displaystyle \dots }  | | | A086238 | [1; 1, 13, 24, 2, 1, 1, 3, 1, 1, 3] |
| 0.37395581361920228805472805434641641 | Artin constante | C A r t i n {\displaystyle C_{Artin}}  | ∏ n = 1 ∞ ( 1 - 1 p n ( p n - 1 ) ) {\displaystyle \{n=1}^{infty }\left(1-{frac {1}{p_{n}(p_{n}-1)}}right)} ...... pn : primo | | T | A005596 | [0;2,1,2,14,1,1,2,3,5,1,3,1,5,1,1,2,3,5,46,...] |
| 4.66920160910299067185320382046620161 | Constante de Feigenbaum δ | δ {\displaystyle {\delta }}  | lim n → ∞ x n + 1 - x n x n + 2 - x n + 1 x ∈ ( 3 , 8284 ; 3 , 8495 ) {{displaystyle }lim _{n\a \infty }{frac {x_{n+1}-x_{n}}{x_{n+2}-x_{n+1}}qquad \scriptstyle x\in (3,8284;\a,3,8495)}  x n + 1 = a x n ( 1 - x n ) o x n + 1 = a sin ( x n ) {\displaystyle \scriptstyle x_{n+1}=,ax_{n}(1-x_{n})\quad {o}quad x_{n+1}=,a\sin(x_{n})}  | | T | A006890 | [4;1,2,43,2,163,2,3,1,1,2,5,1,2,3,80,2,5,...] |
| 2.50290787509589282228390287321821578 | Constante de Feigenbaum α | α {\año de la pantalla \año de la pantalla \año de la pantalla \año}  | lim n → ∞ d n d n + 1 {\displaystyle \lim _{n\to \infty }{frac {d_{n}}{d_{n+1}}}}  | | T | A006891 | [2;1,1,85,2,8,1,10,16,3,8,9,2,1,40,1,2,3,...] |
| 5.97798681217834912266905331933922774 | Constante de Madelung hexagonal 2 | H 2 ( 2 ) {\displaystyle H_{2}(2)}  | π ln ( 3 ) 3 {\displaystyle \pi \ln(3){\aqrt {3}}  | Pi Log[3]Sqrt[3] | T | A086055 | [5;1,44,2,2,1,15,1,1,12,1,65,11,1,3,1,1,...] |
| 0.96894614625936938048363484584691860 | Beta(3) | β ( 3 ) {\N-estilo de la pantalla \N-beta (3)}  | π 3 32 = ∑ n = 1 ∞ - 1 n + 1 ( - 1 + 2 n ) 3 = 1 1 3 - 1 3 3 + 1 5 3 - 1 7 3 + ... {{displaystyle}} {\frac {\pi ^{3}}{32}}=suma _{n=1}^{{infty}}}{{1^{n+1}}(-1+2n)^{3}}={frac {1}{1^{3}}{-}{frac {1}{3^{3}}{+}{frac {1}{5^{3}}{-}{frac {1}{7^{3}}{+}{puntos}}  | Suma[n=1 a ∞]{(-1)^(n+1)/(-1+2n)^3} | T | A153071 | [0;1,31,4,1,18,21,1,1,2,1,2,1,3,6,3,28,1,...] |
| 1.902160583104 | Constante de Brun2 = Σ primos gemelos inversos | B 2 {\displaystyle B_{\\2}  | ∑ ( 1 p + 1 p + 2 ) p , p + 2 : p r i m o s = ( 1 3 + 1 5 ) + ( 1 5 + 1 7 ) + ( 1 11 + 1 13 ) + ... {\displaystyle \textstyle \sum {\underset {p,\2:\{{primos}}({\frac {1}{p}+{\frac {1}{p+2}})}}=({\frac {1}{3}{+}{\frac {1}{5}})+({\tfrac {1}{5}{+}{\tfrac {1}{7}})+({\tfrac {1}{11}{+}{\tfrac {1}{13}})+\dots }  | | | A065421 | [1; 1, 9, 4, 1, 1, 8, 3, 4, 4, 2, 2] |
| 0.870588379975 | Constante de Brun4 = Σ inversa del primo gemelo | B 4 {\displaystyle B_{,4}}  | ( 1 5 + 1 7 + 1 11 + 1 13 ) p , p + 2 , p + 4 , p + 6 : p r i m e s + ( 1 11 + 1 13 + 1 17 + 1 19 ) + ... {\displaystyle {\underset {p,\2,\4,\6:\{{primas}} {Izquierda({tfrac {1}{5}}+{tfrac {1}{7}}+{tfrac {1}{11}}+{tfrac {1}{13}}Derecha)}+Izquierda({tfrac {1}{11}+{tfrac {1}{13}}+{tfrac {1}{17}+{tfrac {1}{19}}Derecha)+{puntos}}  | | | A213007 | [0; 1, 6, 1, 2, 1, 2, 956, 3, 1, 1] |
| 22.4591577183610454734271522045437350 | pi^e | π e {\displaystyle \pi ^{e}}  | π e {\displaystyle \pi ^{e}}  | pi^e | | A059850 | [22;2,5,1,1,1,1,1,3,2,1,1,3,9,15,25,1,1,5,...] |
| 3.14159265358979323846264338327950288 | Pi, constante de Arquímedes | π {\año de la pantalla \año de la pantalla \año de la pantalla \año}  | lim n → ∞ 2 n 2 - 2 + 2 + ⋯ + 2 ⏟ n {\displaystyle \lim _{n\a \infty },2^{n}{sqrt} {2-{sqrt} {2+{sqrt} +{\a} {2+{puntos} {{sqrt} {2}}}}}}}} _{n}}  | Sum[n=0 a ∞]{(-1)^n 4/(2n+1)} | T | A000796 | [3;7,15,1,292,1,1,1,2,1,3,1,14,...] |
| 0.06598803584531253707679018759684642 | | e - e {\displaystyle e^{-e}}  | e - e {\displaystyle e^{-e}} ... Límite inferior de la Tetración | | T | A073230 | [0;15,6,2,13,1,3,6,2,1,1,5,1,1,1,9,4,1,1,1,...] |
| 0.20787957635076190854695561983497877 | i^i | i i i {desde el estilo i^{i}}  | e - π 2 {\displaystyle e^\frac {-\pi }{2}}  | e^(-pi/2) | T | A049006 | [0;4,1,4,3,1,1,1,1,1,1,1,1,7,1,20,1,3,6,10,...] |
| 0.28016949902386913303643649123067200 | Constante de Bernstein | β {\año de la pantalla \año de la pantalla \año}  | 1 2 π {\frac {1}{2}{\fracción cuadrática {\pi }}}}}  | | T | A073001 | [0;3,1,1,3,9,6,3,1,3,13,1,16,3,3,4,…] |
| 0.28878809508660242127889972192923078 | Flajolet y Richmond | Q {\diseño Q}  | ∏ n = 1 ∞ ( 1 - 1 2 n ) = ( 1 - 1 2 1 ) ( 1 - 1 2 2 ) ( 1 - 1 2 3 ) ... {\displaystyle \\\n=1}^{infty }\left(1-{\frac {1}{2^{n}}}right)=\left(1{-}{\frac {1}{2^{1}}right)\left(1{-}{\frac {1}{2^{2}}right)\left(1{-}{\frac {1}{2^{3}{right)\n}  | prod[n=1 a ∞]{1-1/2^n} | | A048651 | |
| 0.31830988618379067153776752674502872 | Inversa de Pi, Ramanujan | 1 π {\displaystyle {\frac {1}{pi }}  | ¡2 2 9801 ∑ n = 0 ∞ ( 4 n ) ! ( 1103 + 26390 n ) ( n ! ) 4 396 4 n {{displaystyle {\frac {2{cuadrado {2}}{9801}} {{suma _{n=0}^{{infty }{{{4n}}  | | T | A049541 | [0;3,7,15,292,1,1,1,2,1,3,1,14,2,1,1,...] |
| 0.47494937998792065033250463632798297 | Constante de Weierstraß | W W E {{displaystyle W_{WE}}  | e π 8 π 4 ∗ 2 3 / 4 ( 1 4 ! ) 2 {\displaystyle {\frac {e^{frac {\pi }{8}} {\sqrt {\pi }} 4*2^{3/4}{{{1}{4}})^2}}}}}  | (E^(Pi/8) Sqrt[Pi])/(4 2^(3/4) (1/4)!^2) | T | A094692 | [0;2,9,2,11,1,6,1,4,6,3,19,9,217,1,2,...] |
| 0.56714329040978387299996866221035555 | Constante Omega | Ω {\año de la pantalla \año de la pantalla \año}  | ¡W ( 1 ) = ∑ n = 1 ∞ ( - n ) n - 1 n ! = 1 - 1 + 3 2 - 8 3 + 125 24 - ... {\displaystyle W(1)={suma _{n=1}^{{infty }{{frac {(-n)^{n-1}}{n!}}=1{-}1{+}{frac {3}{2}}{{}{frac {8}{3}}{+}{{frac {125}{24}}-puntos }  | suma[n=1 a ∞]{(-n)^(n-1)/n!} | T | A030178 | [0;1,1,3,4,2,10,4,1,1,1,1,2,7,306,1,5,1,...] |
| 0.57721566490153286060651209008240243 | El número de Euler | γ {\año de la pantalla \año de la pantalla \año \año}  | - ψ ( 1 ) = ∑ n = 1 ∞ ∑ k = 0 ∞ ( - 1 ) k 2 n + k {\displaystyle -\psi (1)=suma _{n=1}^{\infty }{suma _{k=0}^{\infty }{frac {(-1)^{k}{2^{n}+k}}  | suma[n=1 a ∞]|suma[k=0 a ∞]{((-1)^k)/(2^n+k)} | ? | A001620 | [0;1,1,2,1,2,1,4,3,13,5,1,1,8,1,2,...] |
| 0.60459978807807261686469275254738524 | Serie de Dirichlet | π 3 3 {\displaystyle {\frac {\pi }{3{sqrt {3}}}}}  | ∑ n = 1 ∞ 1 n ( 2 n n ) = 1 - 1 2 + 1 4 - 1 5 + 1 7 - 1 8 + ⋯ {{displaystyle \\\\}sum _{n=1}^{\infty }{\frac {1}{2n{elegir n}}=1-{{frac {1}{2}}+{frac {1}{4}}-{frac {1}{5}}+{frac {1}{7}}-{frac {1}{8}}+{cdots }  | Sum[1/(n Binomio[2 n, n]), {n, 1, ∞}] | T | A073010 | [0;1,1,1,1,8,10,2,2,3,3,1,9,2,5,4,1,27,27,...] |
| 0.63661977236758134307553505349005745 | 2/Pi, François Viète | 2 π {\displaystyle {\frac {2}{pi }}  | 2 2 ⋅ 2 + 2 2 ⋅ 2 + 2 + 2 ⋯ {\displaystyle {\frac {\sqrt {2}{2}{cdot} {\frac {\sqrt {2+{2}{cdot} {\frac {\sqrt {2+{2}{cdot}}  | | T | A060294 | [0;1,1,1,3,31,1,145,1,4,2,8,1,6,1,2,3,1,4,...] |
| 0.66016181584686957392781211001455577 | Constante prima gemela | C 2 {\displaystyle C_{2}}  | ∏ p = 3 ∞ p ( p - 2 ) ( p - 1 ) 2 {\displaystyle \{prod _{p=3}^{\infty }{\frac {p(p-2)}{(p-1)^{2}}}}  | prod[p=3 a ∞]{p(p-2)/(p-1)^2 | | A005597 | [0;1,1,1,16,2,2,2,2,1,18,2,2,11,1,1,2,4,1,...] |
| 0.66274341934918158097474209710925290 | Constante de límite de Laplace | λ {\año de la pantalla \año de la cámara}  | | | | A033259 | [0;1,1,1,27,1,1,1,8,2,154,2,4,1,5,...] |
| 0.69314718055994530941723212145817657 | Logaritmo de 2 | L n ( 2 ) {\Ndirección Ln(2)}  | ∑ n = 1 ∞ ( - 1 ) n + 1 n = 1 1 - 1 2 + 1 3 - 1 4 + 1 5 - ⋯ {{displaystyle \\\_sum _{n=1}^{\infty }{{frac {(-1)^{n+1}}{n}={frac {1}}-{frac {1}{2}}+{frac {1}{3}}-{frac {1}{4}}+{frac {1}{5}}{cdots }  | Suma[n=1 a ∞]{(-1)^(n+1)/n} | T | A002162 | [0;1,2,3,1,6,3,1,1,2,1,1,1,1,3,10,...] |
| 0.78343051071213440705926438652697546 | El sueño de un estudiante de segundo año1 J.Bernoulli | I 1 {\displaystyle I_{1}  | ∑ n = 1 ∞ ( - 1 ) n + 1 n = 1 - 1 2 2 + 1 3 3 - 1 4 4 + 1 5 5 + ... {\displaystyle \{sum _{n=1}^{{infty }{{{1)^{n+1}{n^{n}}=1-{{frac {1}{2^{2}}+{{frac {1}{3^{3}}+{{frac {1}{4^{4}}+{{frac {1}{5^{5}}+{puntos}  | Suma[ -(-1)^n /n^n] | T | A083648 | [0;1,3,1,1,1,1,1,1,2,4,7,2,1,2,1,1,1,...] |
| 0.78539816339744830961566084581987572 | Dirichlet beta(1) | β ( 1 ) {\N-estilo de la pantalla \N-beta (1)}  | π 4 = ∑ n = 0 ∞ ( - 1 ) n 2 n + 1 = 1 1 - 1 3 + 1 5 - 1 7 + 1 9 - ⋯ {\frac {\pi }{4}}={suma _{n=0}^{\infty }{{frac {(-1)^{n}}{2n+1}}={frac {1}}-{frac {1}{3}}+{frac {1}{5}}-{frac {1}{7}}+{frac {1}{9}}-{cdots }  | Sum[n=0 a ∞]{(-1)^n/(2n+1)} | T | A003881 | [0; 1,3,1,1,1,15,2,72,1,9,1,17,1,2,1,5,...] |
| 0.82246703342411321823620758332301259 | Vendedor ambulante Nielsen-Ramanujan | ζ ( 2 ) 2 {\displaystyle {\frac {\zeta (2)}{2}}  | π 2 12 = ∑ n = 1 ∞ ( - 1 ) n + 1 n 2 = 1 2 - 1 2 2 + 1 3 2 - 1 4 2 + 1 5 2 - ... {\frac {\pi ^{2}}{12}=suma _{n=1}^{infty }{{{1}^{n+1}}{n^{2}}={frac {1}{1^{2}}{-{frac {1}{2^{2}}{+}{frac {1}{3^{2}}{-{frac {1}{4^{2}}{+}{{puntos}}  | Suma[n=1 a ∞]{((-1)^(k+1))/n^2} | T | A072691 | [0;1,4,1,1,1,2,1,1,1,1,3,2,2,4,1,1,1,...] |
| 0.91596559417721901505460351493238411 | Constante catalana | C {\año C}  | ∑ n = 0 ∞ ( - 1 ) n ( 2 n + 1 ) 2 = 1 1 2 - 1 3 2 + 1 5 2 - 1 7 2 + ⋯ {\displaystyle \sum _{n=0}^{\infty }{{frac {(-1)^{n}}(2n+1)^{2}}={frac {1}{1^{2}}-{frac {1}{3^{2}}+{frac {1}{5^{2}}-{frac {1}{7^{2}}+{cdots }  | Sum[n=0 a ∞]{(-1)^n/(2n+1)^2} | I | A006752 | [0;1,10,1,8,1,88,4,1,1,7,22,1,2,...] |
| 1.05946309435929526456182529494634170 | Relación de la distancia entre semitonos | 2 12 {\displaystyle {\sqrt[{12}]{2}} ![{\displaystyle {\sqrt[{12}]{2}}}](https://www.alegsaonline.com/image/bc835f27425fb3140e1f75a5faa35b1e8b9efc35.svg) | 2 12 {\displaystyle {\sqrt[{12}]{2}} ![{\displaystyle {\sqrt[{12}]{2}}}](https://www.alegsaonline.com/image/bc835f27425fb3140e1f75a5faa35b1e8b9efc35.svg) | 2^(1/12) | I | A010774 | [1;16,1,4,2,7,1,1,2,2,7,4,1,2,1,60,1,3,1,2,...] |
| 1,.08232323371113819151600369654116790 | Zeta(04) | ζ 4 {\a6}  | π 4 90 = ∑ n = 1 ∞ 1 n 4 = 1 1 4 + 1 2 4 + 1 3 4 + 1 4 4 + 1 5 4 + ... {\frac {\pi ^{4}{90}=suma _{n=1}^{infty}}={frac {1}{n^{4}}={frac {1}{4}+{frac {1}{2^{4}+{frac {1}{3^{4}}+{frac {1}{4^{4}}+{frac {1}{5^{4}}+{puntos}  | Suma[n=1 a ∞]{1/n^4} | T | A013662 | [1;12,6,1,3,1,4,183,1,1,2,1,3,1,1,5,4,2,7,...] |
| 1.1319882487943 ... | Viswanaths Archivado 2013-04-13 en la Wayback Machine constante | C V i {\displaystyle C_{Vi}}  | lim n → ∞ | a n | 1 n {\displaystyle \lim _{n a \infty }|a_{n}|^{frac {1}{n}}  | | | A078416 | [1;7,1,1,2,1,3,2,1,2,1,8,1,5,1,1,1,9,1,...] |
| 1.20205690315959428539973816151144999 | Apéry constante | ζ ( 3 ) {\a6)  | ∑ n = 1 ∞ 1 n 3 = 1 1 3 + 1 2 3 + 1 3 3 + 1 4 3 + 1 5 3 + ⋯ {{displaystyle \\\_sum _{n=1}^{\infty }{\frac {{1}{n^{3}}={{refrac}{1}{1^{3}}+{refrac}{1}{2^{3}}+{refrac}{1}{3^{3}}+{refrac}{4^{3}}+{refrac}{5^{3}}+{cdots},¡\!}  | Suma[n=1 a ∞]{1/n^3} | I | A010774 | [1;4,1,18,1,1,1,4,1,9,9,2,1,1,1,2,...] |
| 1.22541670246517764512909830336289053 | Gamma(3/4) | Γ ( 3 4 ) {\displaystyle \Gamma ({\tfrac {3}{4})}  | ¡( - 1 + 3 4 ) ! {\displaystyle \left(-1+{{frac {3}{4}}\right)!}  | ¡(-1+3/4)! | T | A068465 | [1;4,2,3,2,2,1,1,1,2,1,4,7,1,171,3,2,3,1,1,...] |
| 1.23370055013616982735431137498451889 | Constante de Favard | 3 4 ζ ( 2 ) {\displaystyle {\tfrac {3}{4} {zeta (2)}  | π 2 8 = ∑ n = 0 ∞ 1 ( 2 n - 1 ) 2 = 1 2 + 1 3 2 + 1 5 2 + 1 7 2 + ... {\displaystyle {\frac {\pi ^{2}}{8}=suma _{n=0}^{{infty }{{1}(2n-1)^{2}}={frac {1}{1^{2}}+{frac {1}{3^{2}}+{frac {1}{5^{2}}+{frac {1}{7^{2}}+{puntos}  | suma[n=1 a ∞]{1/((2n-1)^2)} | T | A111003 | [1;4,3,1,1,2,2,5,1,1,1,1,2,1,2,1,10,4,3,1,1,...] |
| 1.25992104989487316476721060727822835 | Raíz cúbica de 2, constante Delian | 2 3 {\displaystyle {\sqrt[{3}]{2}} ![{\displaystyle {\sqrt[{3}]{2}}}](https://www.alegsaonline.com/image/9ca071ab504481c2bb76081aacb03f5519930710.svg) | 2 3 {\displaystyle {\sqrt[{3}]{2}} ![{\displaystyle {\sqrt[{3}]{2}}}](https://www.alegsaonline.com/image/9ca071ab504481c2bb76081aacb03f5519930710.svg) | 2^(1/3) | I | A002580 | [1;3,1,5,1,1,4,1,1,8,1,14,1,10,...] |
| 1.29128599706266354040728259059560054 | El sueño de un estudiante de segundo año2 J.Bernoulli | I 2 {\displaystyle I_{2}  | ∑ n = 1 ∞ 1 n = 1 + 1 2 2 + 1 3 3 + 1 4 4 + 1 5 5 + 1 6 6 + ... {\displaystyle \\\Nsuma _{n=1}^{infty }{{1}{n^{n}}=1+{frac {1}{2^{2}}+{frac {1}{3^{3}}+{frac {1}{4^{4}}+{frac {1}{5^{5}}+{frac {1}{6^{6}}+{puntos}  | Sum[1/(n^n]), {n, 1, ∞}] | | A073009 | [1;3,2,3,4,3,1,2,1,1,6,7,2,5,3,1,2,1,8,1,...] |
| 1.32471795724474602596090885447809734 | Número de plástico | ρ {\año de la pantalla \año de la pantalla \año}  | 1 + 1 + 1 + ⋯ 3 3 3 {\displaystyle {{sqrt[{3}]{1+{{sqrt[{3}]{1+{sqrt[{3}]{1+{{sqrt[{3}]{1+{cdots }}}}}}}}} ![{\displaystyle {\sqrt[{3}]{1+{\sqrt[{3}]{1+{\sqrt[{3}]{1+{\sqrt[{3}]{1+\cdots }}}}}}}}}](https://www.alegsaonline.com/image/fe5c1cba04372927a214a2ce1b1d6b213bb12ee3.svg) | | I | A060006 | [1;3,12,1,1,3,2,3,2,4,2,141,80,2,5,1,2,8,...] |
| 1.41421356237309504880168872420969808 | Raíz cuadrada de 2, constante de Pitágoras | 2 {\displaystyle {\sqrt {2}}  | ∏ n = 1 ∞ 1 + ( - 1 ) n + 1 2 n - 1 = ( 1 + 1 1 ) ( 1 - 1 3 ) ( 1 + 1 5 ) . . . {\displaystyle \\\n=1}^{\infty }1+{\frac {(-1)^{n+1}{2n-1}}={{{}}Izquierda(1{+}{\frac {1}{1}}Derecha)}{{{}Izquierda(1{}{3}{Derecha)}{{{{1}{5}{Derecha)...}  | prod[n=1 a ∞]{1+(-1)^(n+1)/(2n-1)} | I | A002193 | [1;2,2,2,2,2,2,2,2,2,2,2,2,2,2,2,2,2,2,2,2,...] = [1;(2),...] |
| 1.44466786100976613365833910859643022 | Número de Steiner | e 1 e {\displaystyle e^\frac {1}{e}}  | e 1 / e {\displaystyle e^{1/e}} ... Límite superior de la tetralogía | | | A073229 | [1;2,4,55,27,1,1,16,9,3,2,8,3,2,1,1,4,1,9,...] |
| 1.53960071783900203869106341467188655 | Constante de hielo cuadrado de Lieb | W 2 D {\displaystyle W_{2D}}  | lim n → ∞ ( f ( n ) ) n - 2 = ( 4 3 ) 3 2 {\displaystyle \lim _{n\to \infty }(f(n))^{n^-2}=left({\frac {4}{3}}right)^{\frac {3}{2}}  | (4/3)^(3/2) | I | A118273 | [1;1,1,5,1,4,2,1,6,1,6,1,2,4,1,5,1,1,2,...] |
| 1.57079632679489661923132169163975144 | Producto Wallis | π / 2 {\desde el punto de vista de la visualización \pi /2}  | ∏ n = 1 ∞ ( 4 n 2 4 n 2 - 1 ) = 2 1 ⋅ 2 3 ⋅ 4 3 ⋅ 4 5 ⋅ 6 5 ⋅ 6 7 ⋅ 8 7 ⋅ 8 9 ⋯ {\displaystyle \prod _{n=1}^{infty }\left({\frac {4n^{2}{4n^{2}- | | T | A019669 | [1;1,1,3,31,1,145,1,4,2,8,1,6,1,2,3,1...] |
| 1.60669515241529176378330152319092458 | Constante de Erdős-Borwein | E B {\displaystyle E_{\\\\año,B}}  | ∑ n = 1 ∞ 1 2 n - 1 = 1 1 + 1 3 + 1 7 + 1 15 + ⋯ {{displaystyle}{{suma}{n=1}^{infty}}{{frac {1}{2^{n}-1}}={frac {1}{3}+{frac {1}{7}+{frac {1}{15}}+{cdots{,\}}  | suma[n=1 a ∞]{1/(2^n-1)} | I | A065442 | [1;1,1,1,1,5,2,1,2,29,4,1,2,2,2,2,6,1,7,1,...] |
| 1.61803398874989484820458633436563812 | Phi, proporción áurea | φ {\\Ndejar de ver el estilo \N de la pantalla }  | 1 + 5 2 = 1 + 1 + 1 + ⋯ {\displaystyle {\frac {1+{cuadrado}}}{2}}={cuadrado}{1+{cuadrado}{1+{cuadrado}{1+{cuadrado}{1+cuadrado}{1+cuadrado}{2}}.  | (1+5^(1/2))/2 | I | A001622 | [0;1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,...] = [0;(1),...] |
| 1.64493406684822643647241516664602519 | Zeta(2) | ζ ( 2 ) {\año de la pantalla \año de la pantalla (\año,2)}  | π 2 6 = ∑ n = 1 ∞ 1 n 2 = 1 1 2 + 1 2 2 + 1 3 2 + 1 4 2 + ⋯ {\displaystyle {\frac {\pi ^{2}}{6}=\suma {{n=1}^{infty }{{1}{n^2}}={frac {1}{1^2}}+{frac {1}{2^2}}+{frac {1}{3^2}}+{frac {1}{4^2}}+{cdots }  | Suma[n=1 a ∞]{1/n^2} | T | A013661 | [1;1,1,1,4,2,4,7,1,4,2,3,4,10 1,2,1,1,1,15,...] |
| 1.66168794963359412129581892274995074 | La constante de recurrencia cuadrática de Somos | σ {\año de la pantalla \año de la pantalla \año}  | 1 2 3 ⋯ = 1 1 / 2 ; 2 1 / 4 ; 3 1 / 8 ⋯ {\displaystyle {{sqrt} {2{sqrt} {3\cdots }}}}}}=1^{1/2};2^{1/4};3^{1/8}\cdots }  | | T | A065481 | [1;1,1,1,21,1,1,1,6,4,2,1,1,2,1,3,1,13,13,...] |
| 1.73205080756887729352744634150587237 | Constante de Teodoro | 3 {\displaystyle {\sqrt {3}}  | 3 {\displaystyle {\sqrt {3}}  | 3^(1/2) | I | A002194 | [1;1,2,1,2,1,2,1,2,1,2,1,2,1,2,1,2,1,2,1,2,...] = [1;(1,2),...] |
| 1.75793275661800453270881963821813852 | Número de Kasner | R {\diseño de R}  | 1 + 2 + 3 + 4 + ⋯ {\displaystyle {\sqrt {1+\sqrt {2+\sqrt {3+\sqrt {4+\cdots }}}}}}}}}  | | | A072449 | [1;1,3,7,1,1,1,2,3,1,4,1,1,2,1,2,20,1,2,2,...] |
| 1.77245385090551602729816748334114518 | Constante Carlson-Levin | Γ ( 1 2 ) {\displaystyle \Gamma ({\tfrac {1}{2}})}  | ¡π = ( - 1 2 ) ! {\displaystyle {\sqrt {\pi }}=\left(-{{frac {1}{2}}right)!}  | sqrt (pi) | T | A002161 | [1;1,3,2,1,1,6,1,28,13,1,1,2,18,1,1,1,83,1,...] |
| 2.29558714939263807403429804918949038 | Constante parabólica universal | P 2 {\displaystyle P_{{2}}  | ln ( 1 + 2 ) + 2 {\displaystyle \ln(1+{cuadrado {2}})+{cuadrado {2}}  | ln(1+sqrt 2)+sqrt 2 | T | A103710 | [2;3,2,1,1,1,1,3,3,1,1,4,2,3,2,7,1,6,1,8,...] |
| 2.30277563773199464655961063373524797 | Número de bronce | σ R r {{desde el punto de vista de la visualización}}  | 3 + 13 2 = 1 + 3 + 3 + 3 + ⋯ {\displaystyle {\frac {3+{cuadrado}}}{2}}=1+{cuadrado}{3+{cuadrado}{3+cuadrado}{3+cuadrado}{3+cuadrado}{3+cuadrado}{2}}  | (3+sqrt 13)/2 | I | A098316 | [3;3,3,3,3,3,3,3,3,3,3,3,3,3,3,3,3,3,3,...] = [3;(3),...] |
| 2.37313822083125090564344595189447424 | Constante de Lévy2 | 2 ln γ {\Ndice 2,\ln \Ngamma }  | π 2 6 ln ( 2 ) {\frac {\pi ^{2}}{6\ln(2)}}  | Pi^(2)/(6*ln(2)) | T | A174606 | [2;2,1,2,8,57,9,32,1,1,2,1,2,1,2,1,2,1,3,2,...] |
| 2.50662827463100050241576528481104525 | raíz cuadrada de 2 pi | 2 π {\displaystyle {\sqrt {2\pi }}  | 2 π = lim n → ∞ n ! e n n n n {\displaystyle {{sqrt {2\pi }}={lim _{n\to \infty }} {{frac {n!\\};e^{n}}{{sqrt {n}}}}}  | sqrt (2*pi) | T | A019727 | [2;1,1,37,4,1,1,1,1,9,1,1,2,8,6,1,2,2,1,3,...] |
| 2.66514414269022518865029724987313985 | Constante de Gelfond-Schneider | G G S {\displaystyle G_{\\\\\\Nde la GS}}  | 2 2 {\displaystyle 2^{\\\c al cuadrado {2}}  | 2^sqrt{2} | T | A007507 | [2;1,1,1,72,3,4,1,3,2,1,1,1,14,1,2,1,1,3,1,...] |
| 2.68545200106530644530971483548179569 | Constante de Khintchin | K 0 {\displaystyle K_{{0}}  | ∏ n = 1 ∞ [ 1 + 1 n ( n + 2 ) ] ln n / ln 2 {\displaystyle \{prod _{n=1}^{\infty }left[{1+{1 \over n(n+2)}\ right]^{ln n/\ln 2}}. ![{\displaystyle \prod _{n=1}^{\infty }\left[{1+{1 \over n(n+2)}}\right]^{\ln n/\ln 2}}](https://www.alegsaonline.com/image/cbfef25fcd2817842f1c50956dc798248c418be6.svg) | prod[n=1 a ∞]{(1+1/(n(n+2)))^((ln(n)/ln(2))} | ? | A002210 | [2;1,2,5,1,1,2,1,1,3,10,2,1,3,2,24,1,3,2,...] |
| 3.27582291872181115978768188245384386 | Constante de Khinchin-Lévy | γ {\año de la pantalla \año de la pantalla \año \año}  | e π 2 / ( 12 ln 2 ) {\displaystyle e^{pi ^{2}/(12\ln 2)}}  | e^(\pi^2/(12 ln(2)) | | A086702 | [3;3,1,1,1,2,29,1,130,1,12,3,8,2,4,1,3,55,...] |
| 3.35988566624317755317201130291892717 | Constante recíproca de Fibonacci | Ψ {\\Ndice el estilo \N de la pantalla}  | ∑ n = 1 ∞ 1 F n = 1 1 + 1 1 + 1 2 + 1 3 + 1 5 + 1 8 + 1 13 + ⋯ {{displaystyle \\\\_sum _{n=1}^{{infty }{{frac {1}{F_{n}}={{frac}{1}}+{frac}{1}{1}}+{frac}{2}}+{frac}{3}}+{frac}{5}+{frac}{8}+{frac}{13}+{cdots}}  | | | A079586 | [3;2,1,3,1,1,13,2,3,3,2,1,1,6,3,2,4,362,...] |
| 4.13273135412249293846939188429985264 | Raíz de 2 e pi | 2 e π {\displaystyle {\sqrt {2e\pi }}  | 2 e π {\displaystyle {\sqrt {2e\pi }}  | sqrt(2e pi) | T | A019633 | [4;7,1,1,6,1,5,1,1,1,8,3,1,2,2,15,2,1,1,2,4,...] |
| 6.58088599101792097085154240388648649 | Constante de Froda | 2 e {\displaystyle 2^{\\\\\}}  | 2 e {\displaystyle 2^{e}}  | 2^e | | | [6;1,1,2,1,1,2,3,1,14,11,4,3,1,1,7,5,5,2,7,...] |
| 9.86960440108935861883449099987615114 | Pi al cuadrado | π 2 {\displaystyle \pi ^{2}}  | 6 ∑ n = 1 ∞ 1 n 2 = 6 1 2 + 6 2 2 + 6 3 2 + 6 4 2 + ⋯ {{displaystyle 6{suma _{n=1}^{infty }}={{frac {1}{n^2}}+{frac {6}{1^2}}+{frac {6}{3^2}}+{frac {6}{4^2}}+{cdots }  | 6 Suma[n=1 a ∞]{1/n^2} | T | A002388 | [9;1,6,1,2,47,1,8,1,1,2,2,1,1,8,3,1,10,5,...] |
| 23.1406926327792690057290863679485474 | Constante de Gelfond | e π {\displaystyle e^{\pi }}  | ¡∑ n = 0 ∞ π n n ! ¡= π 1 1 + π 2 2 ! ¡+ π 3 3 ! ¡+ π 4 4 ! + ⋯ {\displaystyle \{n=0}^{{infty }{{frac {\pi ^{n}{n!}}={frac {\pi ^{1}{1}+{frac {\pi ^{2}{2!}+{frac {\pi ^{3}{3!}+{frac {\pi ^{4}{4!}+{cdots }  | Sum[n=0 a ∞]{(pi^n)/n!} | T | A039661 | [23;7,9,3,1,1,591,2,9,1,2,34,1,16,1,30,1,...] |