Mingarelli Identity
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In the field of
ordinary differential equation In mathematics, an ordinary differential equation (ODE) is a differential equation (DE) dependent on only a single independent variable (mathematics), variable. As with any other DE, its unknown(s) consists of one (or more) Function (mathematic ...
s, the Mingarelli identityThe locution was coined by
Philip Hartman Philip Hartman (May 16, 1915 – August 28, 2015) was an American mathematician at Johns Hopkins University The Johns Hopkins University (often abbreviated as Johns Hopkins, Hopkins, or JHU) is a private university, private research u ...
, according to
is a theorem that provides criteria for the
oscillation Oscillation is the repetitive or periodic variation, typically in time, of some measure about a central value (often a point of equilibrium) or between two or more different states. Familiar examples of oscillation include a swinging pendulum ...
and non-oscillation of solutions of some
linear differential equation In mathematics, a linear differential equation is a differential equation that is linear equation, linear in the unknown function and its derivatives, so it can be written in the form a_0(x)y + a_1(x)y' + a_2(x)y'' \cdots + a_n(x)y^ = b(x) wher ...
s in the real domain. It extends the
Picone identity In the field of ordinary differential equations, the Picone identity, named after Mauro Picone, is a classical result about homogeneous linear second order differential equations. Since its inception in 1910 it has been used with tremendous success ...
from two to three or more differential equations of the second order.


The identity

Consider the solutions of the following (uncoupled) system of second order linear differential equations over the –interval : :(p_i(t) x_i^\prime)^\prime + q_i(t) x_i = 0, \,\,\,\,\,\,\,\,\,\, x_i(a)=1,\,\, x_i^\prime(a)=R_i where i=1,2, \ldots, n. Let \Delta denote the forward difference operator, i.e. :\Delta x_i = x_-x_i. The second order difference operator is found by iterating the first order operator as in :\Delta^2 (x_i) = \Delta(\Delta x_i) = x_-2x_+x_,, with a similar definition for the higher iterates. Leaving out the independent variable for convenience, and assuming the on , there holds the identity,. : \begin x_^2\Delta^(p_1r_1)]_a^b = &\int_a^b (x^\prime_)^2 \Delta^(p_1) - \int_a^b x_^2 \Delta^(q_1) \\ &- \sum_^ C(n-1,k)(-1)^\int_a^b p_ W^2(x_,x_)/x_^2, \end where *r_i = x^\prime_i/x_i is the
logarithmic derivative In mathematics, specifically in calculus and complex analysis, the logarithmic derivative of a function is defined by the formula \frac where is the derivative of . Intuitively, this is the infinitesimal relative change in ; that is, the in ...
, *W(x_i, x_j) = x^\prime_ix_j - x_ix^\prime_j, is the
Wronskian determinant In mathematics, the Wronskian of ''n'' differentiable functions is the determinant formed with the functions and their derivatives up to order . It was introduced in 1812 by the Polish mathematician Józef Wroński, and is used in the study of ...
, *C(n-1,k) are
binomial coefficients In mathematics, the binomial coefficients are the positive integers that occur as coefficients in the binomial theorem. Commonly, a binomial coefficient is indexed by a pair of integers and is written \tbinom. It is the coefficient of the te ...
. When this equality reduces to the
Picone identity In the field of ordinary differential equations, the Picone identity, named after Mauro Picone, is a classical result about homogeneous linear second order differential equations. Since its inception in 1910 it has been used with tremendous success ...
.


An application

The above identity leads quickly to the following comparison theorem for three linear differential equations,. which extends the classical
Sturm–Picone comparison theorem In mathematics, in the field of ordinary differential equations, the Sturm–Picone comparison theorem, named after Jacques Charles François Sturm and Mauro Picone, is a classical theorem which provides criteria for the oscillation and non-oscilla ...
. Let , , be real-valued continuous functions on the interval and let #(p_1(t) x_1^\prime)^\prime + q_1(t) x_1 = 0, \,\,\,\,\,\,\,\,\,\, x_1(a)=1,\,\, x_1^\prime(a)=R_1 #(p_2(t) x_2^\prime)^\prime + q_2(t) x_2 = 0, \,\,\,\,\,\,\,\,\,\, x_2(a)=1,\,\, x_2^\prime(a)=R_2 #(p_3(t) x_3^\prime)^\prime + q_3(t) x_3 = 0, \,\,\,\,\,\,\,\,\,\, x_3(a)=1,\,\, x_3^\prime(a)=R_3 be three homogeneous linear second order differential equations in
self-adjoint form In mathematics, an element of a *-algebra is called self-adjoint if it is the same as its adjoint (i.e. a = a^*). Definition Let \mathcal be a *-algebra. An element a \in \mathcal is called self-adjoint if The set of self-adjoint elements i ...
, where * for each and for all in , and *the are arbitrary real numbers. Assume that for all in we have, :\Delta^2(q_1) \ge 0 , :\Delta^2(p_1) \le 0 , :\Delta^2(p_1(a)R_1) \le 0 . Then, if on and , then any solution has at least one zero in .


Notes


References

* *{{cite journal , last=Mingarelli , first= Angelo B. , year=1979 , language= , title= Some extensions of the Sturm–Picone theorem , journal= Comptes Rendus Mathématique , series= , volume=1 , issue = 4 , pages=223–226 , location= Toronto, Ontario, Canada , publisher= The Royal Society of Canada , url= Ordinary differential equations Mathematical identities