quartic equations
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1: 1.11 Zeros of Polynomials
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Quartic Equations
…2: 22.19 Physical Applications
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§22.19(ii) Classical Dynamics: The Quartic Oscillator
►Classical motion in one dimension is described by Newton’s equation … ►§22.19(iii) Nonlinear ODEs and PDEs
… ►These include the time dependent, and time independent, nonlinear Schrödinger equations (NLSE) (Drazin and Johnson (1993, Chapter 2), Ablowitz and Clarkson (1991, pp. 42, 99)), the Korteweg–de Vries (KdV) equation (Kruskal (1974), Li and Olver (2000)), the sine-Gordon equation, and others; see Drazin and Johnson (1993, Chapter 2) for an overview. … …3: 23.21 Physical Applications
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►In §22.19(ii) it is noted that Jacobian elliptic functions provide a natural basis of solutions for problems in Newtonian classical dynamics with quartic potentials in canonical form .
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§23.21(ii) Nonlinear Evolution Equations
►Airault et al. (1977) applies the function to an integrable classical many-body problem, and relates the solutions to nonlinear partial differential equations. For applications to soliton solutions of the Korteweg–de Vries (KdV) equation see McKean and Moll (1999, p. 91), Deconinck and Segur (2000), and Walker (1996, §8.1). …4: Bibliography R
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Composite approximations to the solutions of the Orr-Sommerfeld equation.
Studies in Appl. Math. 51, pp. 341–368.
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Uniform asymptotic approximations to the solutions of the Orr-Sommerfeld equation. I. Plane Couette flow.
Studies in Appl. Math. 53, pp. 91–110.
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Uniform asymptotic approximations to the solutions of the Orr-Sommerfeld equation. II. The general theory.
Studies in Appl. Math. 53, pp. 217–224.
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Integral representations for products of Airy functions. III. Quartic products.
Z. Angew. Math. Phys. 48 (4), pp. 656–664.
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Asymptotics and Bounds of the Roots of Equations (Russian).
Zinatne, Riga.
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5: 32.7 Bäcklund Transformations
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§32.7(ii) Second Painlevé Equation
… ►§32.7(iii) Third Painlevé Equation
… ► also has quadratic and quartic transformations. …The quartic transformation … …6: Bibliography B
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Integral equations and exact solutions for the fourth Painlevé equation.
Proc. Roy. Soc. London Ser. A 437, pp. 1–24.
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An Introduction to Linear Difference Equations.
Dover Publications Inc., New York.
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Avoided crossings of the quartic oscillator.
J. Phys. A 30 (9), pp. 3057–3067.
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Vortices in Ginzburg-Landau Equations.
In Proceedings of the International Congress of Mathematicians,
Vol. III (Berlin, 1998),
pp. 11–19.
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Ordinary differential equations.
Fourth edition, John Wiley & Sons, Inc., New York.
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7: 19.2 Definitions
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►Let be a cubic or quartic polynomial in with simple zeros, and let be a rational function of and containing at least one odd power of .
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19.2.8_1
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19.2.8_2
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19.2.11_5
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8: 18.39 Applications in the Physical Sciences
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►These eigenfunctions are the orthonormal eigenfunctions of the time-independent Schrödinger equation
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► b) The Morse Oscillator
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►c) A Rational SUSY Potential
►The Schrödinger equation with potential
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Other Analytically Solved Schrödinger Equations
…9: 19.29 Reduction of General Elliptic Integrals
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►These theorems reduce integrals over a real interval of certain integrands containing the square root of a quartic or cubic polynomial to symmetric integrals over containing the square root of a cubic polynomial (compare §19.16(i)).
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►In the quartic case () the basic integrals are
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►In the quartic case this recurrence relation has an extra term in , and hence , , is a basic integral.
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►If both square roots in (19.29.22) are 0, then the indeterminacy in the two preceding equations can be removed by using (19.27.8) to evaluate the integral as multiplied either by or by in the cases of (19.29.20) or (19.29.21), respectively.
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