Difference between revisions of "Hankel H (2) in terms of csc and Bessel J"

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(Created page with "==Theorem== The following formula holds: $$H_{\nu}^{(2)}(z)=i\csc(\nu \pi) \left[ J_{-\nu}(z)-e^{\nu \pi i}J_{\nu}(z) \right],$$ where $H_{\nu}^{(2)}$ denotes the Hankel H (...")
 
 
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==References==
 
==References==
* {{BookReference|Handbook of mathematical functions|1964|Milton Abramowitz|author2=Irene A. Stegun|prev=Hankel H (2)|next=}}: 9.1.4
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* {{BookReference|Handbook of mathematical functions|1964|Milton Abramowitz|author2=Irene A. Stegun|prev=Hankel H (2)|next=Relationship between Bessel J sub n and Bessel J sub -n}}: 9.1.4
  
 
[[Category:Theorem]]
 
[[Category:Theorem]]
 
[[Category:Unproven]]
 
[[Category:Unproven]]

Latest revision as of 04:50, 11 June 2016

Theorem

The following formula holds: $$H_{\nu}^{(2)}(z)=i\csc(\nu \pi) \left[ J_{-\nu}(z)-e^{\nu \pi i}J_{\nu}(z) \right],$$ where $H_{\nu}^{(2)}$ denotes the Hankel function of the second kind, $i$ denotes the imaginary number, $\csc$ denotes the cosecant, $J_{-\nu}$ denotes the Bessel function of the first kind, and $e^{\nu \pi i}$ denotes the exponential.

Proof

References