--- title: Modular lambda function slug: modular-lambda-function qid: snapshot: enwiki-001365947878 content_hash: license: CC BY-SA 4.0 source: https://en.wikipedia.org/w/index.php?oldid=1365947878 tags: [129273668, 20477150, 23118434, 23603337, 29176311, 30525120, 63706574] --- # Modular lambda function > [!note] Provenance > Snapshot `enwiki-001365947878` · content root `…` > Derived from · Licensed CC BY-SA 4.0 In mathematics, the modular lambda function λ(τ) is a highly symmetric holomorphic function on the complex upper half-plane. It is invariant under the fractional linear action of the congruence group Γ(2), and generates the function field of the corresponding quotient, i.e., it is a Hauptmodul for the modular curve X(2). Over any point τ, its value can be described as a cross ratio of the branch points of a ramified double cover of the projective line by the elliptic curve \mathbb{C}/\langle 1, \tau \rangle , where the map is defined as the quotient by the [−1] involution. The q-expansion, where q = e^{\pi i \tau} is the nome, is given by: : \lambda(\tau) = 16q - 128q^2 + 704 q^3 - 3072q^4 + 11488q^5 - 38400q^6 + \dots . By symmetrizing the lambda function under the canonical action of the symmetric group S 3 on X(2), and then normalizing suitably, one obtains a function on the upper half-plane that is invariant under the full modular group \operatorname{SL}_2(\mathbb{Z}) , and it is in fact Klein's modular j-invariant. In mathematics, the modular lambda function λ(τ) is a highly symmetric holomorphic function on the complex upper half-plane. It is invariant under the fractional linear action of the congruence group Γ(2), and generates the function field of the corresponding quotient, i.e., it is a Hauptmodul for the modular curve X(2). Over any point τ, its value can be described as a cross ratio of the branch points of a ramified double cover of the projective line by the elliptic curve \mathbb{C}/\langle 1, \tau \rangle , where the map is defined as the quotient by the [−1] involution. The q-expansion, where q = e^{\pi i \tau} is the nome, is given by: \lambda(\tau) = 16q - 128q^2 + 704 q^3 - 3072q^4 + 11488q^5 - 38400q^6 + \dots . By symmetrizing the lambda function under the canonical action of the symmetric group S 3 on X(2), and then normalizing suitably, one obtains a function on the upper half-plane that is invariant under the full modular group \operatorname{SL}_2(\mathbb{Z}) , and it is in fact Klein's modular j-invariant. ==Modular properties== The function \lambda(\tau) is invariant under the group generated by \tau \mapsto \tau+2 \ ;\ \tau \mapsto \frac{\tau}{1-2\tau} \ . The generators of the modular group act by \tau \mapsto \tau+1 \ :\ \lambda \mapsto \frac{\lambda}{\lambda-1} \, ; \tau \mapsto -\frac{1}{\tau} \ :\ \lambda \mapsto 1 - \lambda \ . Consequently, the action of the modular group on \lambda(\tau) is that of the anharmonic group, giving the six values of the cross-ratio: \left\lbrace { \lambda, \frac{1}{1-\lambda}, \frac{\lambda-1}{\lambda}, \frac{1}{\lambda}, \frac{\lambda}{\lambda-1}, 1-\lambda } \right\rbrace \ . ==Relations to other functions== It is the square of the elliptic modulus, that is, \lambda(\tau)=k^2(\tau) . In terms of the Dedekind eta function \eta(\tau) and theta functions, \lambda(\tau) = \Bigg(\frac{\sqrt{2}\,\eta(\tfrac{\tau}{2})\eta^2(2\tau)}{\eta^3(\tau)}\Bigg)^8 = \frac{16}{\left(\frac{\eta(\tau/2)}{\eta(2\tau)}\right)^8 + 16} =\frac{\theta_2^4(\tau)}{\theta_3^4(\tau)} and, \frac{1}{\big(\lambda(\tau)\big)^{1/4}}-\big(\lambda(\tau)\big)^{1/4} = \frac{1}{2}\left(\frac{\eta(\tfrac{\tau}{4})}{\eta(\tau)}\right)^4 = 2\,\frac{\theta_4^2(\tfrac{\tau}{2})}{\theta_2^2(\tfrac{\tau}{2})} where \theta_2(\tau) =\sum_{n=-\infty}^\infty e^{\pi i\tau (n+1/2)^2} \theta_3(\tau) = \sum_{n=-\infty}^\infty e^{\pi i\tau n^2} \theta_4(\tau) = \sum_{n=-\infty}^\infty (-1)^n e^{\pi i\tau n^2} In terms of the half-periods of Weierstrass's elliptic functions, let [\omega_1,\omega_2] be a fundamental pair of periods with \tau=\frac{\omega_2}{\omega_1} . e_1 = \wp\left(\frac{\omega_1}{2}\right), \quad e_2 = \wp\left(\frac{\omega_2}{2}\right),\quad e_3 = \wp\left(\frac{\omega_1+\omega_2}{2}\right) we have \lambda = \frac{e_3-e_2}{e_1-e_2} \, . Since the three half-period values are distinct, this shows that \lambda does not take the value 0 or 1. The relation to the j-invariant is j(\tau) = \frac{256(1-\lambda(1-\lambda))^3}{(\lambda(1-\lambda))^2} = \frac{256(1-\lambda+\lambda^2)^3}{\lambda^2 (1-\lambda)^2} \ . which is the j-invariant of the elliptic curve of Legendre form y^2=x(x-1)(x-\lambda) Given m\in\mathbb{C}\setminus\{0,1\} , let \tau=i\frac{K\{1-m\}}{K\{m\}} where K is the complete elliptic integral of the first kind with parameter m=k^2 . Then \lambda (\tau)=m. ==Modular equations== The modular equation of degree p (where p is a prime number) is an algebraic equation in \lambda (p\tau) and \lambda (\tau) . If \lambda (p\tau)=u^8 and \lambda (\tau)=v^8 , the modular equations of degrees p=2,3,5,7 are, respectively, (1+u^4)^2v^8-4u^4=0, u^4-v^4+2uv(1-u^2v^2)=0, u^6-v^6+5u^2v^2(u^2-v^2)+4uv(1-u^4v^4)=0, (1-u^8)(1-v^8)-(1-uv)^8=0. The quantity v (and hence u ) can be thought of as a holomorphic function on the upper half-plane \operatorname{Im}\tau>0 : \begin{align}v&=\prod_{k=1}^\infty \tanh\frac{(k-1/2)\pi i}{\tau}=\sqrt{2}e^{\pi i\tau/8}\frac{\sum_{k\in\mathbb{Z}}e^{(2k^2+k)\pi i\tau}}{\sum_{k\in\mathbb{Z}}e^{k^2\pi i\tau}}\\ &=\cfrac{\sqrt{2}e^{\pi i\tau/8}}{1+\cfrac{e^{\pi i\tau}}{1+e^{\pi i\tau}+\cfrac{e^{2\pi i\tau}}{1+e^{2\pi i\tau}+\cfrac{e^{3\pi i\tau}}{1+e^{3\pi i\tau}+\ddots}}}}\end{align} Since \lambda(i)=1/2 , the modular equations can be used to give algebraic values of \lambda(pi) for any prime p . The algebraic values of \lambda(ni) are also given by \lambda (ni)=\prod_{k=1}^{n/2} \operatorname{sl}^8\frac{(2k-1)\varpi}{2n}\quad (n\,\text{even}) \lambda (ni)=\frac{1}{2^n}\prod_{k=1}^{n-1} \left(1-\operatorname{sl}^2\frac{k\varpi}{n}\right)^2\quad (n\,\text{odd}) where \operatorname{sl} is the lemniscate sine and \varpi is the lemniscate constant. ==Lambda-star== ===Definition and computation of lambda-star=== The function \lambda^*(x) (where x\in\mathbb{R}^+ ) gives the value of the elliptic modulus k , for which the complete elliptic integral of the first kind K(k) and its complementary counterpart K(\sqrt{1-k^2}) are related by following expression: \frac{K\left[\sqrt{1-\lambda^*(x)^2}\right]}{K[\lambda^*(x)]} = \sqrt{x} The values of \lambda^*(x) can be computed as follows: \lambda^*(x) = \frac{\theta^2_2(i\sqrt{x})}{\theta^2_3(i\sqrt{x})} \lambda^*(x) = \left[\sum_{a=-\infty}^\infty\exp[-(a+1/2)^2\pi\sqrt{x}]\right]^2\left[\sum_{a=-\infty}^\infty\exp(-a^2\pi\sqrt{x})\right]^{-2} \lambda^*(x) = \left[\sum_{a=-\infty}^\infty\operatorname{sech}[(a+1/2)\pi\sqrt{x}]\right]\left[\sum_{a=-\infty}^\infty\operatorname{sech}(a\pi\sqrt{x})\right]^{-1} The functions \lambda^* and \lambda are related to each other in this way: \lambda^*(x) = \sqrt{\lambda(i\sqrt{x})} ===Properties of lambda-star=== Every \lambda^* value of a positive rational number is a positive algebraic number: \lambda^*(x) \in \overline{\mathbb{Q}}_+ \quad \forall x\in\mathbb{Q}^+. K(\lambda^*(x)) and E(\lambda^*(x)) (the complete elliptic integral of the second kind) can be expressed in closed form in terms of the gamma function for any x\in\mathbb{Q}^+ , as Selberg and Chowla proved in 1949. The following expression is valid for all n \in \mathbb{N} : \sqrt{n} = \sum_{a = 1}^{n} \operatorname{dn}\left[\frac{2a}{n}K\left[\lambda^*\left(\frac{1}{n}\right)\right];\lambda^*\left(\frac{1}{n}\right)\right] where \operatorname{dn} is the Jacobi elliptic function delta amplitudinis with modulus k . By knowing one \lambda^* value, this formula can be used to compute related \lambda^* values: \lambda^*(n^2x) = \lambda^*(x)^n\prod_{a=1}^{n}\operatorname{sn}\left\{\frac{2a-1}{n}K[\lambda^*(x)];\lambda^*(x)\right\}^2 where n\in\mathbb{N} and \operatorname{sn} is the Jacobi elliptic function sinus amplitudinis with modulus k . Further relations: \lambda^*(x)^2 + \lambda^*(1/x)^2 = 1 [\lambda^*(x)+1][\lambda^*(4/x)+1] = 2 \lambda^*(4x) = \frac{1-\sqrt{1-\lambda^*(x)^2}}{1+\sqrt{1-\lambda^*(x)^2}} = \tan\left\{\frac{1}{2}\arcsin[\lambda^*(x)]\right\}^2 \lambda^*(x) - \lambda^*(9x) = 2[\lambda^*(x)\lambda^*(9x)]^{1/4} - 2[\lambda^*(x)\lambda^*(9x)]^{3/4} \begin{align} & a^{6}-f^{6} = 2af +2a^5f^5\, &\left(a = \left[\frac{2\lambda^*(x)}{1-\lambda^*(x)^2}\right]^{1/12}\right) &\left(f = \left[\frac{2\lambda^*(25x)}{1-\lambda^*(25x)^2}\right]^{1/12}\right) \\ &a^{8}+b^{8}-7a^4b^4 = 2\sqrt{2}ab+2\sqrt{2}a^7b^7\, &\left(a = \left[\frac{2\lambda^*(x)}{1-\lambda^*(x)^2}\right]^{1/12}\right) &\left(b = \left[\frac{2\lambda^*(49x)}{1-\lambda^*(49x)^2}\right]^{1/12}\right) \\ & a^{12}-c^{12} = 2\sqrt{2}(ac+a^3c^3)(1+3a^2c^2+a^4c^4)(2+3a^2c^2+2a^4c^4)\, &\left(a = \left[\frac{2\lambda^*(x)}{1-\lambda^*(x)^2}\right]^{1/12}\right) &\left(c = \left[\frac{2\lambda^*(121x)}{1-\lambda^*(121x)^2}\right]^{1/12}\right) \\ & (a^2-d^2)(a^4+d^4-7a^2d^2)[(a^2-d^2)^4-a^2d^2(a^2+d^2)^2] = 8ad+8a^{13}d^{13}\, &\left(a = \left[\frac{2\lambda^*(x)}{1-\lambda^*(x)^2}\right]^{1/12}\right) &\left(d = \left[\frac{2\lambda^*(169x)}{1-\lambda^*(169x)^2}\right]^{1/12}\right) \end{align} Lambda-star values of integer numbers of 4n-3-type: \lambda^*(1) = \frac{1}{\sqrt{2}} \lambda^*(5) = \sin\left[\frac{1}{2}\arcsin\left(\sqrt{5}-2\right)\right] \lambda^*(9) = \frac{1}{2}(\sqrt{3}-1)(\sqrt{2}-\sqrt[4]{3}) \lambda^*(13) = \sin\left[\frac{1}{2}\arcsin(5\sqrt{13}-18)\right] \lambda^*(17) = \sin\left\{\frac{1}{2}\arcsin\left[\frac{1}{64}\left(5+\sqrt{17}-\sqrt{10\sqrt{17}+26}\right)^3\right]\right\} \lambda^*(21) = \sin\left\{\frac{1}{2}\arcsin[(8-3\sqrt{7})(2\sqrt{7}-3\sqrt{3})]\right\} \lambda^*(25) = \frac{1}{\sqrt{2}}(\sqrt{5}-2)(3-2\sqrt[4]{5}) \lambda^*(33) = \sin\left\{\frac{1}{2}\arcsin[(10-3\sqrt{11})(2-\sqrt{3})^3]\right\} \lambda^*(37) = \sin\left\{\frac{1}{2}\arcsin[(\sqrt{37}-6)^3]\right\} \lambda^*(45) = \sin\left\{\frac{1}{2}\arcsin[(4-\sqrt{15})^2(\sqrt{5}-2)^3]\right\} \lambda^*(49) = \frac{1}{4}(8+3\sqrt{7})(5-\sqrt{7}-\sqrt[4]{28})\left(\sqrt{14}-\sqrt{2}-\sqrt[8]{28}\sqrt{5-\sqrt{7}}\right) \lambda^*(57) = \sin\left\{\frac{1}{2}\arcsin[(170-39\sqrt{19})(2-\sqrt{3})^3]\right\} \lambda^*(73) = \sin\left\{\frac{1}{2}\arcsin\left[\frac{1}{64}\left(45+5\sqrt{73}-3\sqrt{50\sqrt{73}+426}\right)^3\right]\right\} Lambda-star values of integer numbers of 4n-2-type: \lambda^*(2) = \sqrt{2}-1 \lambda^*(6) = (2-\sqrt{3})(\sqrt{3}-\sqrt{2}) \lambda^*(10) = (\sqrt{10}-3)(\sqrt{2}-1)^2 \lambda^*(14) = \tan\left\{\frac{1}{2}\arctan\left[\frac{1}{8}\left(2\sqrt{2}+1-\sqrt{4\sqrt{2}+5}\right)^3\right]\right\} \lambda^*(18) = (\sqrt{2}-1)^3(2-\sqrt{3})^2 \lambda^*(22) = (10-3\sqrt{11})(3\sqrt{11}-7\sqrt{2}) \lambda^*(30) = \tan\left\{\frac{1}{2}\arctan[(\sqrt{10}-3)^2(\sqrt{5}-2)^2]\right\} \lambda^*(34) = \tan\left\{\frac{1}{4}\arcsin\left[\frac{1}{9}(\sqrt{17}-4)^2\right]\right\} \lambda^*(42) = \tan\left\{\frac{1}{2}\arctan[(2\sqrt{7}-3\sqrt{3})^2(2\sqrt{2}-\sqrt{7})^2]\right\} \lambda^*(46) = \tan\left\{\frac{1}{2}\arctan\left[\frac{1}{64}\left(3+\sqrt{2}-\sqrt{6\sqrt{2}+7}\right)^6\right]\right\} \lambda^*(58) = (13\sqrt{58}-99)(\sqrt{2}-1)^6 \lambda^*(70) = \tan\left\{\frac{1}{2}\arctan[(\sqrt{5}-2)^4(\sqrt{2}-1)^6]\right\} \lambda^*(78) = \tan\left\{\frac{1}{2}\arctan[(5\sqrt{13}-18)^2(\sqrt{26}-5)^2]\right\} \lambda^*(82) = \tan\left\{\frac{1}{4}\arcsin\left[\frac{1}{4761}(8\sqrt{41}-51)^2\right]\right\} Lambda-star values of integer numbers of 4n-1-type: \lambda^*(3) = \frac{1}{2\sqrt{2}}(\sqrt{3}-1) \lambda^*(7) = \frac{1}{4\sqrt{2}}(3-\sqrt{7}) \lambda^*(11) = \frac{1}{8\sqrt{2}}(\sqrt{11}+3)\left(\frac{1}{3}\sqrt[3]{6\sqrt{3}+2\sqrt{11}}-\frac{1}{3}\sqrt[3]{6\sqrt{3}-2\sqrt{11}}+\frac{1}{3}\sqrt{11}-1\right)^4 \lambda^*(15) = \frac{1}{8\sqrt{2}}(3-\sqrt{5})(\sqrt{5}-\sqrt{3})(2-\sqrt{3}) \lambda^*(19) = \frac{1}{8\sqrt{2}}(3\sqrt{19}+13)\left[\frac{1}{6}(\sqrt{19}-2+\sqrt{3})\sqrt[3]{3\sqrt{3}-\sqrt{19}}-\frac{1}{6}(\sqrt{19}-2-\sqrt{3})\sqrt[3]{3\sqrt{3}+\sqrt{19}}-\frac{1}{3}(5-\sqrt{19})\right]^4 \lambda^*(23) = \frac{1}{16\sqrt{2}}(5+\sqrt{23})\left[\frac{1}{6}(\sqrt{3}+1)\sqrt[3]{100-12\sqrt{69}}-\frac{1}{6}(\sqrt{3}-1)\sqrt[3]{100+12\sqrt{69}}+\frac{2}{3}\right]^4 \lambda^*(27) = \frac{1}{16\sqrt{2}}(\sqrt{3}-1)^3\left[\frac{1}{3}\sqrt{3}(\sqrt[3]{4}-\sqrt[3]{2}+1)-\sqrt[3]{2}+1\right]^4 \lambda^*(39) = \sin\left\{\frac{1}{2}\arcsin\left[\frac{1}{16}\left(6-\sqrt{13}-3\sqrt{6\sqrt{13}-21}\right)\right]\right\} \lambda^*(55) = \sin\left\{\frac{1}{2}\arcsin\left[\frac{1}{512}\left(3\sqrt{5}-3-\sqrt{6\sqrt{5}-2}\right)^3\right]\right\} Lambda-star values of integer numbers of 4n-type: \lambda^*(4) = (\sqrt{2}-1)^2 \lambda^*(8) = \left(\sqrt{2}+1-\sqrt{2\sqrt{2}+2}\right)^2 \lambda^*(12) = (\sqrt{3}-\sqrt{2})^2(\sqrt{2}-1)^2 \lambda^*(16) = (\sqrt{2}+1)^2(\sqrt[4]{2}-1)^4 \lambda^*(20) = \tan\left[\frac{1}{4}\arcsin(\sqrt{5}-2)\right]^2 \lambda^*(24) = \tan\left\{\frac{1}{2}\arcsin[(2-\sqrt{3})(\sqrt{3}-\sqrt{2})]\right\}^2 \lambda^*(28) = (2\sqrt{2}-\sqrt{7})^2(\sqrt{2}-1)^4 \lambda^*(32) = \tan\left\{\frac{1}{2}\arcsin\left[\left(\sqrt{2}+1-\sqrt{2\sqrt{2}+2}\right)^2\right]\right\}^2 Lambda-star values of rational fractions: \lambda^*\left(\frac{1}{2}\right) = \sqrt{2\sqrt{2}-2} \lambda^*\left(\frac{1}{3}\right) = \frac{1}{2\sqrt{2}}(\sqrt{3}+1) \lambda^*\left(\frac{2}{3}\right) = (2-\sqrt{3})(\sqrt{3}+\sqrt{2}) \lambda^*\left(\frac{1}{4}\right) = 2\sqrt[4]{2}(\sqrt{2}-1) \lambda^*\left(\frac{3}{4}\right) = \sqrt[4]{8}(\sqrt{3}-\sqrt{2})(\sqrt{2}+1)\sqrt{(\sqrt{3}-1)^3} \lambda^*\left(\frac{1}{5}\right) = \frac{1}{2\sqrt{2}}\left(\sqrt{2\sqrt{5}-2}+\sqrt{5}-1\right) \lambda^*\left(\frac{2}{5}\right) = (\sqrt{10}-3)(\sqrt{2}+1)^2 \lambda^*\left(\frac{3}{5}\right) = \frac{1}{8\sqrt{2}}(3+\sqrt{5})(\sqrt{5}-\sqrt{3})(2+\sqrt{3}) \lambda^*\left(\frac{4}{5}\right) = \tan\left[\frac{\pi}{4}-\frac{1}{4}\arcsin(\sqrt{5}-2)\right]^2 ===Ramanujan's class invariants=== Ramanujan's class invariants G_n and g_n are defined as G_n=2^{-1/4}e^{\pi\sqrt{n}/24}\prod_{k=0}^\infty \left(1+e^{-(2k+1)\pi\sqrt{n}}\right), g_n=2^{-1/4}e^{\pi\sqrt{n}/24}\prod_{k=0}^\infty \left(1-e^{-(2k+1)\pi\sqrt{n}}\right), where n\in\mathbb{Q}^+ . For such n , the class invariants are algebraic numbers. For example g_{58}=\sqrt{\frac{5+\sqrt{29}}{2}}, \quad g_{190}=\sqrt{(\sqrt{5}+2)(\sqrt{10}+3)}. Identities with the class invariants include G_n=G_{1/n},\quad g_{n}=\frac{1}{g_{4/n}},\quad g_{4n}=2^{1/4}g_nG_n. The class invariants are very closely related to the Weber modular functions \mathfrak{f} and \mathfrak{f}_1 . These are the relations between lambda-star and the class invariants: G_n = \sin\{2\arcsin[\lambda^*(n)]\}^{-1/12} = 1\Big /\left[\sqrt[12]{2\lambda^*(n)}\sqrt[24]{1-\lambda^*(n)^2}\right] g_n = \tan\{2\arctan[\lambda^*(n)]\}^{-1/12} = \sqrt[12]{[1-\lambda^*(n)^2]/[2\lambda^*(n)]} \lambda^*(n) = \tan\left\{ \frac{1}{2}\arctan[g_n^{-12}]\right\} = \sqrt{g_n^{24}+1}-g_n^{12} ===Little Picard theorem=== The lambda function is used in the original proof of the Little Picard theorem, that an entire non-constant function on the complex plane cannot omit more than one value. This theorem was proved by Picard in 1879. Suppose if possible that f is entire and does not take the values 0 and 1. Since λ is holomorphic, it has a local holomorphic inverse ω defined away from 0,1,∞. Consider the function z → ω(f(z)). By the Monodromy theorem this is holomorphic and maps the complex plane C to the upper half plane. From this it is easy to construct a holomorphic function from C to the unit disc, which by Liouville's theorem must be constant. ===Moonshine=== The function \tau\mapsto 16/\lambda(2\tau) - 8 is the normalized Hauptmodul for the group \Gamma_0(4) , and its q-expansion q^{-1} + 20q - 62q^3 + \dots , where q=e^{2\pi i\tau } , is the graded character of any element in conjugacy class 4C of the monster group acting on the monster vertex algebra. ==Footnotes== ==References== ===Notes=== ===Other=== Borwein, J. M. and Borwein, P. B. Pi & the AGM: A Study in Analytic Number Theory and Computational Complexity. New York: Wiley, pp. 139 and 298, 1987. Conway, J. H. and Norton, S. P. "Monstrous Moonshine." Bull. London Math. Soc. 11, 308-339, 1979. Selberg, A. and Chowla, S. "On Epstein's Zeta-Function." J. reine angew. Math. 227, 86-110, 1967. ==External links== Modular lambda function at Fungrim