Coshc function

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The cardinal hyperbolic cosine function coshc(z) plotted in the complex plane from -2-2i to 2+2i
The cardinal hyperbolic cosine function coshc(z) plotted in the complex plane from -2-2i to 2+2i

In mathematics, the coshc function appears frequently in papers about optical scattering,[1] Heisenberg spacetime[2] and hyperbolic geometry.[3][better source needed] For [math]\displaystyle{ z \neq 0 }[/math], it is defined as[4] [math]\displaystyle{ \operatorname{coshc}(z)=\frac {\cosh(z) }{z} }[/math]

It is a solution of the following differential equation: [math]\displaystyle{ w( z) z-2\frac {d}{dz} w (z) -z \frac {d^2}{dz^2} w (z) =0 }[/math]

Coshc 2D plot
Coshc'(z) 2D plot

Properties

The first-order derivative is given by

[math]\displaystyle{ \frac {\sinh(z)}{z} - \frac {\cosh(z)}{z^2} }[/math]

The Taylor series expansion is[math]\displaystyle{ \operatorname{coshc} z \approx \left(z^{-1}+\frac {1}{2}z+\frac {1}{24}z^3+\frac {1}{720}z^5+\frac {1}{40320}z^7+\frac {1}{3628800}z^9+\frac {1}{479001600}z^{11}+\frac {1}{87178291200}z^{13}+O(z^{15}) \right) }[/math]

The Padé approximant is[math]\displaystyle{ \operatorname{Coshc} \left( z \right) ={\frac {23594700729600+11275015752000\,{ z}^{2}+727718024880\,{z}^{4}+13853547000\,{z}^{6}+80737373\,{z}^{8}}{ 147173\,{z}^{9}-39328920\,{z}^{7}+5772800880\,{z}^{5}-522334612800\,{z }^{3}+23594700729600\,z}} }[/math]

In terms of other special functions

  • [math]\displaystyle{ \operatorname{coshc}(z) = \frac {( iz+1/2\,\pi) {\rm M}(1,2,i\pi -2z)}{e^{(i/2)\pi -z} z} }[/math], where [math]\displaystyle{ {\rm{M}}(a,b,z) }[/math] is Kummer's confluent hypergeometric function.
  • [math]\displaystyle{ \operatorname{coshc}(z)=\frac{1}{2}\,\frac {(2\,iz+\pi) \operatorname{HeunB} \left( 2,0,0,0,\sqrt {2}\sqrt {1/2\,i\pi -z} \right) } {e^{1/2\,i\pi -z}z} }[/math], where [math]\displaystyle{ {\rm{HeunB}}(q, \alpha, \gamma, \delta, \epsilon ,z) }[/math] is the biconfluent Heun function.
  • [math]\displaystyle{ \operatorname{coshc}(z)= \frac {-i(2\,iz+\pi) {{\rm \mathbf WhittakerM}(0,\,1/2,\,i\pi -2z)}}{(4iz+2\pi) z} }[/math], where [math]\displaystyle{ {\rm{WhittakerM}}(a,b,z) }[/math] is a Whittaker function.

Gallery

Coshc abs complex 3D
Coshc Im complex 3D plot
Coshc Re complex 3D plot
Coshc'(z) Im complex 3D plot
Coshc'(z) Re complex 3D plot
Coshc'(z) abs complex 3D plot
Coshc'(x) abs density plot
Coshc'(x) Im density plot
Coshc'(x) Re density plot

See also

References

  1. den Outer, P. N.; Lagendijk, Ad; Nieuwenhuizen, Th. M. (1993-06-01). "Location of objects in multiple-scattering media" (in en). Journal of the Optical Society of America A 10 (6): 1209. doi:10.1364/JOSAA.10.001209. ISSN 1084-7529. Bibcode1993JOSAA..10.1209D. https://opg.optica.org/abstract.cfm?URI=josaa-10-6-1209. 
  2. Körpinar, Talat (2014). "New Characterizations for Minimizing Energy of Biharmonic Particles in Heisenberg Spacetime" (in en). International Journal of Theoretical Physics 53 (9): 3208–3218. doi:10.1007/s10773-014-2118-5. ISSN 0020-7748. Bibcode2014IJTP...53.3208K. http://link.springer.com/10.1007/s10773-014-2118-5. 
  3. Nilgün Sönmez, A Trigonometric Proof of the Euler Theorem in Hyperbolic Geometry, International Mathematical Forum, 4, 2009, no. 38, 1877–1881
  4. ten Thije Boonkkamp, J. H. M.; van Dijk, J.; Liu, L.; Peerenboom, K. S. C. (2012). "Extension of the Complete Flux Scheme to Systems of Conservation Laws" (in en). Journal of Scientific Computing 53 (3): 552–568. doi:10.1007/s10915-012-9588-5. ISSN 0885-7474.