26,892 research outputs found

    Derivatives of tangent function and tangent numbers

    Full text link
    In the paper, by induction, the Fa\`a di Bruno formula, and some techniques in the theory of complex functions, the author finds explicit formulas for higher order derivatives of the tangent and cotangent functions as well as powers of the sine and cosine functions, obtains explicit formulas for two Bell polynomials of the second kind for successive derivatives of sine and cosine functions, presents curious identities for the sine function, discovers explicit formulas and recurrence relations for the tangent numbers, the Bernoulli numbers, the Genocchi numbers, special values of the Euler polynomials at zero, and special values of the Riemann zeta function at even numbers, and comments on five different forms of higher order derivatives for the tangent function and on derivative polynomials of the tangent, cotangent, secant, cosecant, hyperbolic tangent, and hyperbolic cotangent functions.Comment: 17 page

    An extension of an inequality for ratios of gamma functions

    Get PDF
    In this paper, we prove that for x+y>0x+y>0 and y+1>0y+1>0 the inequality {equation*} \frac{[\Gamma(x+y+1)/\Gamma(y+1)]^{1/x}}{[\Gamma(x+y+2)/\Gamma(y+1)]^{1/(x+1)}} 1andreversedif and reversed if x<1andthatthepower and that the power \frac12isthebestpossible,where is the best possible, where \Gamma(x)$ is the Euler gamma function. This extends the result in [Y. Yu, \textit{An inequality for ratios of gamma functions}, J. Math. Anal. Appl. \textbf{352} (2009), no.~2, 967\nobreakdash--970.] and resolves an open problem posed in [B.-N. Guo and F. Qi, \emph{Inequalities and monotonicity for the ratio of gamma functions}, Taiwanese J. Math. \textbf{7} (2003), no.~2, 239\nobreakdash--247.].Comment: 8 page

    Eight interesting identities involving the exponential function, derivatives, and Stirling numbers of the second kind

    Full text link
    In the paper, the author establishes some identities which show that the functions 1(1−e±t)k\frac1{(1-e^{\pm t})^k} and the derivatives (1e±t−1)(i)\bigl(\frac1{e^{\pm t}-1}\bigr)^{(i)} can be expressed each other by linear combinations with coefficients involving the combinatorial numbers and the Stirling numbers of the second kind, where t≠0t\ne0 and i,k∈Ni,k\in\mathbb{N}.Comment: 9 page

    Disk Sizes in a LCDM Universe

    Full text link
    We introduce a model which uses semi-analytic techniques to trace formation and evolution of galaxy disks in their cosmological context. For the first time we model the growth of gas and stellar disks separately. In contrast to previous work we follow in detail the angular momentum accumulation history through the gas cooling, merging and star formation processes. Our model successfully reproduces the stellar mass--radius distribution and gas-to-stellar disk size ratio distribution observed locally. We also investigate the dependence of clustering on galaxy size and find qualitative agreement with observation. There is still some discrepancy at small scale for less massive galaxies, indicating that our treatment of satellite galaxies needs to be improved.Comment: 6 pages, 3 figures, Proceedings of IAU Symposium 254 "The Galaxy disk in a cosmological context", Copenhagen, June 200

    Note on a Class of Completely Monotonic Functions Involving the Polygamma Functions

    Get PDF
    • …
    corecore