Cassini and Catalan identities

Cassini's formula was discovered in 1680 by Giovanni Domenico Cassini, then director of the Paris Observatory, and independently proven by Robert Simson (1753). Catalan's identity is named after Eugène Catalan (1814–1894). It can be found in one of his private research notes, entitled "Sur la série de Lamé" and dated October 1879. However, the identity did not appear in print until December 1886 as part of his collected works . This explains why some give 1879 and others 1886 as the date for Catalan's identity . The Hungarian-British mathematician Steven Vajda (1901–95) published a book on Fibonacci numbers (Fibonacci and Lucas Numbers, and the Golden Section: Theory and Applications, 1989) which contains the identity carrying his name. However, the identity had been published earlier in 1960 by Dustan Everman as problem 1396 in The American Mathematical Monthly, and in 1901 by Alberto Tagiuri in Periodico di Matematica. ==Proof of Cassini identity==

Proof by matrix theory A quick proof of Cassini's identity may be given by recognising the left side of the equation as a determinant of a 2×2 matrix of Fibonacci numbers. The result is almost immediate when the matrix is seen to be the th power of a matrix with determinant −1: :F_{n-1}F_{n+1} - F_n^2 =\det\left[\begin{matrix}F_{n+1}&F_n\\F_n&F_{n-1}\end{matrix}\right] =\det\left[\begin{matrix}1&1\\1&0\end{matrix}\right]^n =\left(\det\left[\begin{matrix}1&1\\1&0\end{matrix}\right]\right)^n =(-1)^n. Proof by induction Consider the induction statement: :F_{n-1}F_{n+1} - F_n^2 = (-1)^n The base case n=1 is true. Assume the statement is true for n. Then: :F_{n-1}F_{n+1} - F_n^2 + F_nF_{n+1} - F_nF_{n+1} = (-1)^n :F_{n-1}F_{n+1} + F_nF_{n+1} - F_n^2 - F_nF_{n+1} = (-1)^n :F_{n+1}(F_{n-1} + F_n) - F_n(F_n + F_{n+1}) = (-1)^n :F_{n+1}^2 - F_nF_{n+2} = (-1)^n :F_nF_{n+2} - F_{n+1}^2 = (-1)^{n+1} so the statement is true for all integers n>0. ==Proof of Catalan identity==

We use Binet's formula, that F_n=\frac{\phi^n-\psi^n}{\sqrt5}, where \phi=\frac{1+\sqrt5}{2} and \psi=\frac{1-\sqrt5}{2}. Hence, \phi+\psi=1 and \phi\psi=-1. So, :5(F_n^2 - F_{n-r}F_{n+r}) := (\phi^n-\psi^n)^2 - (\phi^{n-r}-\psi^{n-r})(\phi^{n+r}-\psi^{n+r}) := (\phi^{2n} - 2\phi^{n}\psi^{n} +\psi^{2n}) - (\phi^{2n} - \phi^{n}\psi^{n}(\phi^{-r}\psi^{r}+\phi^{r}\psi^{-r}) + \psi^{2n}) := - 2\phi^{n}\psi^{n} + \phi^{n}\psi^{n}(\phi^{-r}\psi^{r}+\phi^{r}\psi^{-r}) Using \phi\psi=-1, := -(-1)^n2 + (-1)^n(\phi^{-r}\psi^{r}+\phi^{r}\psi^{-r}) and again as \phi=\frac{-1}{\psi}, := -(-1)^n2 + (-1)^{n-r}(\psi^{2r}+\phi^{2r}) The Lucas number L_n is defined as L_n=\phi^n+\psi^n, so := -(-1)^n2 + (-1)^{n-r}L_{2r} Because L_{2n} = 5 F_n^2 + 2(-1)^n := -(-1)^n2 + (-1)^{n-r}(5 F_r^2 + 2(-1)^r) := -(-1)^n2 + (-1)^{n-r}2(-1)^r + (-1)^{n-r}5 F_r^2 := -(-1)^n2 + (-1)^n2 + (-1)^{n-r}5 F_r^2 := (-1)^{n-r}5 F_r^2 Cancelling the 5's gives the result. == Notes ==