Singularities

List of finite values corresponding to the singularities (poles) of well-known functions.

H_n denotes the n-th harmonic number (with H_0 = 0 ).

G_n denotes the n-th Gregory number or coefficient.

\gamma = \zeta(1)  \approx 0.57721566490153286\ldots denotes the Euler-Mascheroni constant.

Poles of Order 0 (Removeable Singularities)

Function sinc( )

The unnormalized and normalized function sinc(z) \; (z\in\mathbb{C}) has one removable singularity at z=0 . Its finite value at its pole z=0 is:

sinc(0) = \dfrac{\sin(0)}{0} = 1 \qquad \, (unnormalized)

sinc(0) = \dfrac{\sin(0\pi)}{0\pi} = 1 \qquad \, (normalized)

Tangent function tan( )

The tangent function \tan(z) \; (z\in\mathbb{C}) has removable singularities at every odd multiple of ~\dfrac{\pi}{2} . Its finite value at its poles is:

\tan\left(\dfrac{(2n+1)\pi}{2}\right) = -\dfrac{1}{2\pi} \qquad (n\in\mathbb{N})

\tan\left(-\dfrac{(2n+1)\pi}{2}\right) = -\tan\left(\dfrac{(2n+1)\pi}{2}\right) = \dfrac{1}{2\pi} \qquad (n\in\mathbb{N})

In particular, \tan\left(\dfrac{\pi}{2}\right) = -\dfrac{1}{2\pi} .

Cotangent function cot( )

The cotangent function \cot(z) \; (z\in\mathbb{C}) has removable singularities at every multiple of \pi . Its finite value at its poles is:

\cot\left(\dfrac{\pi n}{2}\right) = 0 \qquad (n\in\mathbb{Z})

In particular, \cot(\pi) = \cot(0) = 0 .

Natural log of the sine function ln(sin( ))

The natural log of sine function \ln(\sin z)  \; (z\in\mathbb{C}) has removable singularities at every multiple of \pi . Its finite value at its poles is:

\ln(\sin \pi n) = -(\gamma+\ln2)

Natural log of the cosine function ln(cos( ))

The natural log of cosine function \ln(\cos z)  \; (z\in\mathbb{C}) has removable singularities at every odd multiple of \dfrac{\pi}{2} . Its finite value at its poles is:

\ln\left(\cos\pi\left(n+\dfrac{1}{2}\right)\right) = -(\gamma+\ln2)

Natural log of the tangent function ln(tan( ))

The natural log of the tangent function \ln(\tan z) \; (z\in\mathbb{C}) has removable singularities at every odd multiple of \dfrac{\pi}{2} . Its finite value at its poles is:

\ln\left(\tan\pi\left(n+\dfrac{1}{2}\right)\right) = \gamma+\ln2