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Transactions of the American Mathematical Society

Published by the American Mathematical Society since 1900, Transactions of the American Mathematical Society is devoted to longer research articles in all areas of pure and applied mathematics.

ISSN 1088-6850 (online) ISSN 0002-9947 (print)

The 2020 MCQ for Transactions of the American Mathematical Society is 1.48.

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A fixed point theorem, a perturbed differential equation, and a multivariable Volterra integral equation
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by David Lowell Lovelady PDF
Trans. Amer. Math. Soc. 182 (1973), 71-83 Request permission

Abstract:

A fixed point theorem is obtained for an equation of the form $u = T[p,f + G[u]]$. This theorem is then applied to a functionally perturbed ordinary differential equation of the form $u’(t) = f(t) + A(t,u(t)) + G[u](t);u(0) = p$, and, as a consequence of this, Fredholm integrodifferential equations of the form $z’(t) = f(t) + \phi (t,z(t)) + \int _0^\infty {\alpha (t,s)\omega (z(s))ds,z(0) = p}$. Applications are also made to a multivariable Volterra integral system \[ \begin {array}{*{20}{c}} {{u_1}(s,t) = {g_1}(s,t) + \int _0^s {\int _0^t {F\left [ {{u_1}(x,y),{u_2}(x,y),{u_3}(x,y)} \right ]dy\;dx} } } \hfill \\ {{u_2}(s,t) = {g_2}(s,t) + \int _0^t {F\left [ {{u_1}(s,y),{u_2}(s,y),{u_3}(s,y)} \right ]} \;dy} \hfill \\ {{u_3}(s,t) = {g_3}(s,t) + \int _0^s {F\left [ {{u_1}(x,t),{u_2}(x,t),{u_3}(x,t)} \right ]} \;dx,} \hfill \\ \end {array} \] and, as a corollary to this, a differential equation of the form \[ \begin {array}{*{20}{c}} \hfill {\frac {{{\partial ^2}}}{{\partial s\partial t}}u(s,t) = f(s,t) + F\left [ {u(s,t),\frac {\partial }{{\partial s}}u(s,t),\frac {\partial }{{\partial t}}u(s,t)} \right ],} \\ \hfill {u(s,0) = \phi (s),u(0,t) = \psi (t).} \\ \end {array} \] These last two equations are set in a Banach space so as to allow applications to integrodifferential equations such as \[ \begin {array}{*{20}{c}} {\frac {{{\partial ^2}}}{{\partial s\partial t}}u(s,t,z) = f(s,t,z) + H\left ( {z,u(s,t,z),\frac {\partial }{{\partial s}}u(s,t,z),\frac {\partial }{{\partial t}}u(s,t,z)} \right )} \\ { + \int _0^1 {K\left ( {z,r,u(s,t,r),\frac {\partial }{{\partial s}}u(s,t,r),\frac {\partial }{{\partial t}}u(s,t,r)} \right )} \;dr,} \\ {u(s,0,z) = \sigma (s,z),u(0,t,z) = \tau (t,z).} \\ \end {array} \]
References
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Additional Information
  • © Copyright 1973 American Mathematical Society
  • Journal: Trans. Amer. Math. Soc. 182 (1973), 71-83
  • MSC: Primary 45J05; Secondary 34K10, 47H10
  • DOI: https://doi.org/10.1090/S0002-9947-1973-0336263-9
  • MathSciNet review: 0336263