About the Project

degrees two, three, four

AdvancedHelp

(0.001 seconds)

5 matching pages

1: 1.11 Zeros of Polynomials
§1.11(iii) Polynomials of Degrees Two, Three, and Four
2: 18.19 Hahn Class: Definitions
The Askey scheme extends the three families of classical OP’s (Jacobi, Laguerre and Hermite) with eight further families of OP’s for which the role of the differentiation operator d d x in the case of the classical OP’s is played by a suitable difference operator. These eight further families can be grouped in two classes of OP’s:
  • 1.

    Hahn class (or linear lattice class). These are OP’s p n ( x ) where the role of d d x is played by Δ x or x or δ x (see §18.1(i) for the definition of these operators). The Hahn class consists of four discrete and two continuous families.

  • 2.

    Wilson class (or quadratic lattice class). These are OP’s p n ( x ) = p n ( λ ( y ) ) ( p n ( x ) of degree n in x , λ ( y ) quadratic in y ) where the role of the differentiation operator is played by Δ y Δ y ( λ ( y ) ) or y y ( λ ( y ) ) or δ y δ y ( λ ( y ) ) . The Wilson class consists of two discrete and two continuous families.

  • The Hahn class consists of four discrete families (Hahn, Krawtchouk, Meixner, and Charlier) and two continuous families (continuous Hahn and Meixner–Pollaczek). …
    3: Bille C. Carlson
    Carlson, in 1981, and is survived by his companion, Jody Stadler, two children, Marian Carlson and John Carlson, and four grandchildren. … After the war he returned to Harvard and completed Bachelor’s and Master’s degrees in physics and mathematics. He then went to Oxford as a Rhodes Scholar and completed a doctoral degree in physics. After four years in the Physics Department at Princeton, he went to the Ames Laboratory and Iowa State University in 1954, where he was a Professor in the Physics and Mathematics Departments. … This invariance usually replaces sets of twelve equations by sets of three equations and applies also to the relation between the first symmetric elliptic integral and the Jacobian functions. …
    4: 14.15 Uniform Asymptotic Approximations
    14.15.3 𝑸 ν μ ( x ) = 1 μ ν + ( 1 / 2 ) ( π u 2 ) 1 / 2 I ν + 1 2 ( μ u ) ( 1 + O ( 1 μ ) ) ,
    14.15.5 α = ν + 1 2 μ ( < 1 ) ,
    §14.15(iii) Large ν , Fixed μ
    14.15.19 α = μ ν + 1 2 ( < 1 ) ,
    5: 22.19 Physical Applications
    The periodicity and symmetry of the pendulum imply that the motion in each four intervals θ ( 0 , ± α ) and θ ( ± α , 0 ) have the same “quarter periods” K = K ( sin ( 1 2 α ) ) . … For β real and positive, three of the four possible combinations of signs give rise to bounded oscillatory motions. …The subsequent position as a function of time, x ( t ) , for the three cases is given with results expressed in terms of a and the dimensionless parameter η = 1 2 β a 2 . … Two types of oscillatory motion are possible. … Hyperelliptic functions u ( z ) are solutions of the equation z = 0 u ( f ( x ) ) 1 / 2 d x , where f ( x ) is a polynomial of degree higher than 4. …