Incomplete Bessel Function
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mathematics Mathematics is a field of study that discovers and organizes methods, Mathematical theory, theories and theorems that are developed and Mathematical proof, proved for the needs of empirical sciences and mathematics itself. There are many ar ...
, the incomplete Bessel functions are types of
special function Special functions are particular mathematical functions that have more or less established names and notations due to their importance in mathematical analysis, functional analysis, geometry, physics, or other applications. The term is defined by ...
s which act as a type of extension from the complete-type of
Bessel functions Bessel functions, named after Friedrich Bessel who was the first to systematically study them in 1824, are canonical solutions of Bessel's differential equation x^2 \frac + x \frac + \left(x^2 - \alpha^2 \right)y = 0 for an arbitrary complex ...
.


Definition

The incomplete Bessel functions are defined as the same
delay differential equation In mathematics, delay differential equations (DDEs) are a type of differential equation in which the derivative of the unknown function at a certain time is given in terms of the values of the function at previous times. DDEs are also called tim ...
s of the complete-type
Bessel functions Bessel functions, named after Friedrich Bessel who was the first to systematically study them in 1824, are canonical solutions of Bessel's differential equation x^2 \frac + x \frac + \left(x^2 - \alpha^2 \right)y = 0 for an arbitrary complex ...
: :J_(z,w)-J_(z,w)=2\dfracJ_v(z,w) :Y_(z,w)-Y_(z,w)=2\dfracY_v(z,w) :I_(z,w)+I_(z,w)=2\dfracI_v(z,w) :K_(z,w)+K_(z,w)=-2\dfracK_v(z,w) :H_^(z,w)-H_^(z,w)=2\dfracH_v^(z,w) :H_^(z,w)-H_^(z,w)=2\dfracH_v^(z,w) And the following suitable extension forms of
delay differential equation In mathematics, delay differential equations (DDEs) are a type of differential equation in which the derivative of the unknown function at a certain time is given in terms of the values of the function at previous times. DDEs are also called tim ...
s from that of the complete-type
Bessel functions Bessel functions, named after Friedrich Bessel who was the first to systematically study them in 1824, are canonical solutions of Bessel's differential equation x^2 \frac + x \frac + \left(x^2 - \alpha^2 \right)y = 0 for an arbitrary complex ...
: :J_(z,w)+J_(z,w)=\dfracJ_v(z,w)-\dfrac\dfracJ_v(z,w) :Y_(z,w)+Y_(z,w)=\dfracY_v(z,w)-\dfrac\dfracY_v(z,w) :I_(z,w)-I_(z,w)=\dfracI_v(z,w)-\dfrac\dfracI_v(z,w) :K_(z,w)-K_(z,w)=-\dfracK_v(z,w)+\dfrac\dfracK_v(z,w) :H_^(z,w)+H_^(z,w)=\dfracH_v^(z,w)-\dfrac\dfracH_v^(z,w) :H_^(z,w)+H_^(z,w)=\dfracH_v^(z,w)-\dfrac\dfracH_v^(z,w) Where the new parameter w defines the integral bound of the upper-incomplete form and lower-incomplete form of the modified Bessel function of the second kind: :K_v(z,w)=\int_w^\infty e^\cosh vt~dt :J_v(z,w)=\int_0^we^\cosh vt~dt


Properties

:J_v(z,w)=J_v(z)+\dfrac :Y_v(z,w)=Y_v(z)+\dfrac :I_(z,w)=I_v(z,w) for integer v :I_(z,w)-I_v(z,w)=I_(z)-I_v(z)-\dfracJ(z,v,w) :I_v(z,w)=I_v(z)+\dfrac :I_v(z,w)=e^J_v(iz,w) :K_(z,w)=K_v(z,w) :K_v(z,w)=\dfrac\dfrac for non-integer v :H_v^(z,w)=J_v(z,w)+iY_v(z,w) :H_v^(z,w)=J_v(z,w)-iY_v(z,w) :H_^(z,w)=e^H_v^(z,w) :H_^(z,w)=e^H_v^(z,w) :H_v^(z,w)=\dfrac=\dfrac for non-integer v :H_v^(z,w)=\dfrac=\dfrac for non-integer v


Differential equations

K_v(z,w) satisfies the inhomogeneous
Bessel's differential equation Bessel functions, named after Friedrich Bessel who was the first to systematically study them in 1824, are canonical solutions of Bessel's differential equation x^2 \frac + x \frac + \left(x^2 - \alpha^2 \right)y = 0 for an arbitrary complex ...
:z^2\dfrac+z\dfrac-(x^2+v^2)y=(v\sinh vw+z\cosh vw\sinh w)e^ Both J_v(z,w) , Y_v(z,w) , H_v^(z,w) and H_v^(z,w) satisfy the
partial differential equation In mathematics, a partial differential equation (PDE) is an equation which involves a multivariable function and one or more of its partial derivatives. The function is often thought of as an "unknown" that solves the equation, similar to ho ...
:z^2\dfrac+z\dfrac+(z^2-v^2)y-\dfrac+2v\tanh vw\dfrac=0 Both I_v(z,w) and K_v(z,w) satisfy the
partial differential equation In mathematics, a partial differential equation (PDE) is an equation which involves a multivariable function and one or more of its partial derivatives. The function is often thought of as an "unknown" that solves the equation, similar to ho ...
:z^2\dfrac+z\dfrac-(z^2+v^2)y-\dfrac+2v\tanh vw\dfrac=0


Integral representations

Base on the preliminary definitions above, one would derive directly the following integral forms of J_v(z,w) , Y_v(z,w): :\begin J_v(z,w)&=J_v(z)+\dfrac\left(\int_0^we^\cosh vt~dt-\int_0^we^\cosh vt~dt\right) \\&=J_v(z)+\dfrac\left(\int_0^w\cos\left(z\cosh t-\dfrac\right)\cosh vt~dt-i\int_0^w\sin\left(z\cosh t-\dfrac\right)\cosh vt~dt\right.\\ &\quad\quad\quad\quad\quad\quad\left.-\int_0^w\cos\left(z\cosh t-\dfrac\right)\cosh vt~dt-i\int_0^w\sin\left(z\cosh t-\dfrac\right)\cosh vt~dt\right) \\&=J_v(z)+\dfrac\left(-2i\int_0^w\sin\left(z\cosh t-\dfrac\right)\cosh vt~dt\right) \\&=J_v(z)-\dfrac\int_0^w\sin\left(z\cosh t-\dfrac\right)\cosh vt~dt\end :\begin Y_v(z,w)&=Y_v(z)+\dfrac\left(\int_0^we^\cosh vt~dt+\int_0^we^\cosh vt~dt\right) \\&=Y_v(z)+\dfrac\left(\int_0^w\cos\left(z\cosh t-\dfrac\right)\cosh vt~dt-i\int_0^w\sin\left(z\cosh t-\dfrac\right)\cosh vt~dt\right.\\ &\quad\quad\quad\quad\quad\quad\left.+\int_0^w\cos\left(z\cosh t-\dfrac\right)\cosh vt~dt+i\int_0^w\sin\left(z\cosh t-\dfrac\right)\cosh vt~dt\right) \\&=Y_v(z)+\dfrac\int_0^w\cos\left(z\cosh t-\dfrac\right)\cosh vt~dt\end With the Mehler–Sonine integral expressions of J_v(z)=\dfrac\int_0^\infty\sin\left(z\cosh t-\dfrac\right)\cosh vt~dt and Y_v(z)=-\dfrac\int_0^\infty\cos\left(z\cosh t-\dfrac\right)\cosh vt~dt mentioned in
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, we can further simplify to J_v(z,w)=\dfrac\int_w^\infty\sin\left(z\cosh t-\dfrac\right)\cosh vt~dt and Y_v(z,w)=-\dfrac\int_w^\infty\cos\left(z\cosh t-\dfrac\right)\cosh vt~dt , but the issue is not quite good since the convergence range will reduce greatly to , v, <1.


References


External links

* * *{{cite journal , last1=Jones , first1=D. S. , title=Incomplete Bessel functions. II. Asymptotic expansions for large argument , journal=Proceedings of the Edinburgh Mathematical Society , date=October 2007 , volume=50 , issue=3 , pages=711–723 , doi=10.1017/S0013091505000908, doi-access=free Special hypergeometric functions