\newcommand{\advE}{\gamma_{1} \cdot \left(1 - e^{- 2 \cdot i \cdot \pi \cdot \phi}\right) + 1}
\newcommand{\advI}{\frac{1}{- \gamma_{1} \cdot \left(1 - e^{- 2 \cdot i \cdot \pi \cdot \phi}\right) + 1}}
\newcommand{\advA}{e^{2 \cdot i \cdot \pi \cdot \gamma_{1} \cdot \phi}}
\newcommand{\advH}{\theta_{0} \cdot e^{- 2 \cdot i \cdot \pi \cdot \phi} + \theta_{1}}
\newcommand{\advMagnitudeErrorE}{\cos{\left(\frac{1}{2} \cdot \operatorname{atan}_{2}{\left(0,4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1 \right)} \right)} \cdot \sqrt{\left|{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1}\right|} - 1}
\newcommand{\advMagnitudeErrorI}{-1 + \frac{1}{\sqrt{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} - 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1}}}
\newcommand{\advPhaseErrorE}{\left|{\frac{\arg{\left(\gamma_{1} - \gamma_{1} \cdot e^{- 2 \cdot i \cdot \pi \cdot \phi} + 1 \right)}}{\arg{\left(e^{2 \cdot i \cdot \pi \cdot \gamma_{1} \cdot \phi} \right)}}}\right| - 1}
\newcommand{\advPhaseErrorI}{\left|{\frac{\arg{\left(\frac{e^{2 \cdot i \cdot \pi \cdot \phi}}{- \gamma_{1} \cdot e^{2 \cdot i \cdot \pi \cdot \phi} + \gamma_{1} + e^{2 \cdot i \cdot \pi \cdot \phi}} \right)}}{\arg{\left(e^{2 \cdot i \cdot \pi \cdot \gamma_{1} \cdot \phi} \right)}}}\right| - 1}
\newcommand{\advISolTFirst}{- \frac{\gamma_{1}}{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} - 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1}}
\newcommand{\advISolTSecond}{\frac{- 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + \gamma_{1} + 1}{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} - 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1}}
\newcommand{\advASolTFirst}{- \frac{\sin{\left(2 \cdot \pi \cdot \gamma_{1} \cdot \psi \right)}}{\sin{\left(2 \cdot \pi \cdot \psi \right)}}}
\newcommand{\advASolTSecond}{\frac{\sin{\left(2 \cdot \pi \cdot \psi \cdot \left(\gamma_{1} + 1\right) \right)}}{\sin{\left(2 \cdot \pi \cdot \psi \right)}}}
\newcommand{\advESolTFirst}{- \gamma_{1}}
\newcommand{\advESolTSecond}{\gamma_{1} + 1}
\newcommand{\advHE}{\gamma_{1} - \gamma_{1} \cdot e^{- 2 \cdot i \cdot \pi \cdot \phi} + 1}
\newcommand{\advHA}{\frac{\left(e^{2 \cdot i \cdot \pi \cdot \phi} \cdot \sin{\left(2 \cdot \pi \cdot \psi \cdot \left(\gamma_{1} + 1\right) \right)} - \sin{\left(2 \cdot \pi \cdot \gamma_{1} \cdot \psi \right)}\right) \cdot e^{- 2 \cdot i \cdot \pi \cdot \phi}}{\sin{\left(2 \cdot \pi \cdot \psi \right)}}}
\newcommand{\advHI}{\frac{\left(- \gamma_{1} + \left(- 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + \gamma_{1} + 1\right) \cdot e^{2 \cdot i \cdot \pi \cdot \phi}\right) \cdot e^{- 2 \cdot i \cdot \pi \cdot \phi}}{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} - 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1}}
\newcommand{\advSupMagIIA}{\frac{\sqrt{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} - 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1} \cdot \left(- 4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + \cos{\left(\frac{1}{2} \cdot \operatorname{atan}_{2}{\left(0,- 16 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 16 \cdot \gamma_{1}^{2} \cdot \sin^{4}{\left(\pi \cdot \psi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} - 8 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1 \right)} \right)} \cdot \sqrt{\left|{- 16 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 16 \cdot \gamma_{1}^{2} \cdot \sin^{4}{\left(\pi \cdot \psi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} - 8 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1}\right|} - 1\right)}{\left(1 - \sqrt{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} - 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1}\right) \cdot \left(4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} - 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1\right)}}
\newcommand{\advSupMagAIA}{\frac{\left(\cos{\left(\frac{1}{2} \cdot \operatorname{atan}_{2}{\left(0,\sin^{2}{\left(2 \cdot \pi \cdot \gamma_{1} \cdot \psi \right)} - 2 \cdot \sin{\left(2 \cdot \pi \cdot \gamma_{1} \cdot \psi \right)} \cdot \sin{\left(2 \cdot \pi \cdot \psi \cdot \left(\gamma_{1} + 1\right) \right)} \cdot \cos{\left(2 \cdot \pi \cdot \phi \right)} + \sin^{2}{\left(2 \cdot \pi \cdot \psi \cdot \left(\gamma_{1} + 1\right) \right)} \right)} \right)} \cdot \left|{\frac{\sqrt{\sin^{2}{\left(2 \cdot \pi \cdot \gamma_{1} \cdot \psi \right)} - 2 \cdot \sin{\left(2 \cdot \pi \cdot \gamma_{1} \cdot \psi \right)} \cdot \sin{\left(2 \cdot \pi \cdot \psi \cdot \left(\gamma_{1} + 1\right) \right)} \cdot \cos{\left(2 \cdot \pi \cdot \phi \right)} + \sin^{2}{\left(2 \cdot \pi \cdot \psi \cdot \left(\gamma_{1} + 1\right) \right)}}}{\sin{\left(2 \cdot \pi \cdot \psi \right)}}}\right| - 1\right) \cdot \sqrt{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} - 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1}}{1 - \sqrt{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} - 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1}}}
\newcommand{\advSupMagIEA}{\frac{- \left(\cos{\left(\frac{1}{2} \cdot \operatorname{atan}_{2}{\left(0,4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1 \right)} \right)} \cdot \sqrt{\left|{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1}\right|} - 1\right) \cdot \left(4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} - 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} - \cos{\left(\frac{1}{2} \cdot \operatorname{atan}_{2}{\left(0,- 16 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 16 \cdot \gamma_{1}^{2} \cdot \sin^{4}{\left(\pi \cdot \psi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} - 8 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1 \right)} \right)} \cdot \sqrt{\left|{- 16 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 16 \cdot \gamma_{1}^{2} \cdot \sin^{4}{\left(\pi \cdot \psi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} - 8 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1}\right|} + 1\right) + \sin{\left(\frac{1}{2} \cdot \operatorname{atan}_{2}{\left(0,4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1 \right)} \right)} \cdot \sin{\left(\frac{1}{2} \cdot \operatorname{atan}_{2}{\left(0,- 16 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 16 \cdot \gamma_{1}^{2} \cdot \sin^{4}{\left(\pi \cdot \psi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} - 8 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1 \right)} \right)} \cdot \left|{\sqrt{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1} \cdot \sqrt{- 16 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 16 \cdot \gamma_{1}^{2} \cdot \sin^{4}{\left(\pi \cdot \psi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} - 8 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1}}\right|}{\left(4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} - 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1\right) \cdot \left(- 2 \cdot \cos{\left(\frac{1}{2} \cdot \operatorname{atan}_{2}{\left(0,4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1 \right)} \right)} \cdot \sqrt{\left|{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1}\right|} + \left|{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1}\right| + 1\right)}}
\newcommand{\advSupMagAEA}{\frac{\left(\cos{\left(\frac{1}{2} \cdot \operatorname{atan}_{2}{\left(0,4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1 \right)} \right)} \cdot \sqrt{\left|{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1}\right|} - 1\right) \cdot \left(\cos{\left(\frac{1}{2} \cdot \operatorname{atan}_{2}{\left(0,\sin^{2}{\left(2 \cdot \pi \cdot \gamma_{1} \cdot \psi \right)} - 2 \cdot \sin{\left(2 \cdot \pi \cdot \gamma_{1} \cdot \psi \right)} \cdot \sin{\left(2 \cdot \pi \cdot \psi \cdot \left(\gamma_{1} + 1\right) \right)} \cdot \cos{\left(2 \cdot \pi \cdot \phi \right)} + \sin^{2}{\left(2 \cdot \pi \cdot \psi \cdot \left(\gamma_{1} + 1\right) \right)} \right)} \right)} \cdot \left|{\frac{\sqrt{\sin^{2}{\left(2 \cdot \pi \cdot \gamma_{1} \cdot \psi \right)} - 2 \cdot \sin{\left(2 \cdot \pi \cdot \gamma_{1} \cdot \psi \right)} \cdot \sin{\left(2 \cdot \pi \cdot \psi \cdot \left(\gamma_{1} + 1\right) \right)} \cdot \cos{\left(2 \cdot \pi \cdot \phi \right)} + \sin^{2}{\left(2 \cdot \pi \cdot \psi \cdot \left(\gamma_{1} + 1\right) \right)}}}{\sin{\left(2 \cdot \pi \cdot \psi \right)}}}\right| - 1\right) + \sin{\left(\frac{1}{2} \cdot \operatorname{atan}_{2}{\left(0,4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1 \right)} \right)} \cdot \sin{\left(\frac{1}{2} \cdot \operatorname{atan}_{2}{\left(0,\sin^{2}{\left(2 \cdot \pi \cdot \gamma_{1} \cdot \psi \right)} - 2 \cdot \sin{\left(2 \cdot \pi \cdot \gamma_{1} \cdot \psi \right)} \cdot \sin{\left(2 \cdot \pi \cdot \psi \cdot \left(\gamma_{1} + 1\right) \right)} \cdot \cos{\left(2 \cdot \pi \cdot \phi \right)} + \sin^{2}{\left(2 \cdot \pi \cdot \psi \cdot \left(\gamma_{1} + 1\right) \right)} \right)} \right)} \cdot \left|{\frac{\sqrt{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1}}{\sin{\left(2 \cdot \pi \cdot \psi \right)}} \cdot \sqrt{\sin^{2}{\left(2 \cdot \pi \cdot \gamma_{1} \cdot \psi \right)} - 2 \cdot \sin{\left(2 \cdot \pi \cdot \gamma_{1} \cdot \psi \right)} \cdot \sin{\left(2 \cdot \pi \cdot \psi \cdot \left(\gamma_{1} + 1\right) \right)} \cdot \cos{\left(2 \cdot \pi \cdot \phi \right)} + \sin^{2}{\left(2 \cdot \pi \cdot \psi \cdot \left(\gamma_{1} + 1\right) \right)}}}\right|}{- 2 \cdot \cos{\left(\frac{1}{2} \cdot \operatorname{atan}_{2}{\left(0,4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1 \right)} \right)} \cdot \sqrt{\left|{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1}\right|} + \left|{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1}\right| + 1}}
\newcommand{\advSupMagEIA}{\frac{\left(- \cos{\left(\frac{1}{2} \cdot \operatorname{atan}_{2}{\left(0,4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1 \right)} \right)} \cdot \sqrt{\left|{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1}\right|} + 1\right) \cdot \sqrt{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} - 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1}}{\sqrt{4 \cdot \gamma_{1}^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} - 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1} - 1}}
\newcommand{\advSupMagEAA}{\text{NaN}}
\newcommand{\advSupPhaseIIA}{\frac{\arg{\left(\left(- \gamma_{1} + \left(- 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + \gamma_{1} + 1\right) \cdot e^{2 \cdot i \cdot \pi \cdot \phi}\right) \cdot e^{- 2 \cdot i \cdot \pi \cdot \phi} \right)} - \arg{\left(e^{2 \cdot i \cdot \pi \cdot \gamma_{1} \cdot \phi} \right)}}{\arg{\left(\frac{e^{2 \cdot i \cdot \pi \cdot \phi}}{- \gamma_{1} \cdot e^{2 \cdot i \cdot \pi \cdot \phi} + \gamma_{1} + e^{2 \cdot i \cdot \pi \cdot \phi}} \right)} - \arg{\left(e^{2 \cdot i \cdot \pi \cdot \gamma_{1} \cdot \phi} \right)}}}
\newcommand{\advSupPhaseAIA}{\frac{\arg{\left(\frac{\left(e^{2 \cdot i \cdot \pi \cdot \phi} \cdot \sin{\left(2 \cdot \pi \cdot \psi \cdot \left(\gamma_{1} + 1\right) \right)} - \sin{\left(2 \cdot \pi \cdot \gamma_{1} \cdot \psi \right)}\right) \cdot e^{- 2 \cdot i \cdot \pi \cdot \phi}}{\sin{\left(2 \cdot \pi \cdot \psi \right)}} \right)} - \arg{\left(e^{2 \cdot i \cdot \pi \cdot \gamma_{1} \cdot \phi} \right)}}{\arg{\left(\frac{e^{2 \cdot i \cdot \pi \cdot \phi}}{- \gamma_{1} \cdot e^{2 \cdot i \cdot \pi \cdot \phi} + \gamma_{1} + e^{2 \cdot i \cdot \pi \cdot \phi}} \right)} - \arg{\left(e^{2 \cdot i \cdot \pi \cdot \gamma_{1} \cdot \phi} \right)}}}
\newcommand{\advSupPhaseIEA}{\frac{\arg{\left(\left(- \gamma_{1} + \left(- 4 \cdot \gamma_{1} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + \gamma_{1} + 1\right) \cdot e^{2 \cdot i \cdot \pi \cdot \phi}\right) \cdot e^{- 2 \cdot i \cdot \pi \cdot \phi} \right)} - \arg{\left(e^{2 \cdot i \cdot \pi \cdot \gamma_{1} \cdot \phi} \right)}}{\arg{\left(\gamma_{1} - \gamma_{1} \cdot e^{- 2 \cdot i \cdot \pi \cdot \phi} + 1 \right)} - \arg{\left(e^{2 \cdot i \cdot \pi \cdot \gamma_{1} \cdot \phi} \right)}}}
\newcommand{\advSupPhaseAEA}{\frac{\arg{\left(\frac{\left(e^{2 \cdot i \cdot \pi \cdot \phi} \cdot \sin{\left(2 \cdot \pi \cdot \psi \cdot \left(\gamma_{1} + 1\right) \right)} - \sin{\left(2 \cdot \pi \cdot \gamma_{1} \cdot \psi \right)}\right) \cdot e^{- 2 \cdot i \cdot \pi \cdot \phi}}{\sin{\left(2 \cdot \pi \cdot \psi \right)}} \right)} - \arg{\left(e^{2 \cdot i \cdot \pi \cdot \gamma_{1} \cdot \phi} \right)}}{\arg{\left(\gamma_{1} - \gamma_{1} \cdot e^{- 2 \cdot i \cdot \pi \cdot \phi} + 1 \right)} - \arg{\left(e^{2 \cdot i \cdot \pi \cdot \gamma_{1} \cdot \phi} \right)}}}
\newcommand{\advSupPhaseEIA}{\frac{\arg{\left(\gamma_{1} - \gamma_{1} \cdot e^{- 2 \cdot i \cdot \pi \cdot \phi} + 1 \right)} - \arg{\left(e^{2 \cdot i \cdot \pi \cdot \gamma_{1} \cdot \phi} \right)}}{\arg{\left(\frac{e^{2 \cdot i \cdot \pi \cdot \phi}}{- \gamma_{1} \cdot e^{2 \cdot i \cdot \pi \cdot \phi} + \gamma_{1} + e^{2 \cdot i \cdot \pi \cdot \phi}} \right)} - \arg{\left(e^{2 \cdot i \cdot \pi \cdot \gamma_{1} \cdot \phi} \right)}}}
\newcommand{\advSupPhaseEAA}{\tilde{\infty} \cdot \left(\arg{\left(\gamma_{1} - \gamma_{1} \cdot e^{- 2 \cdot i \cdot \pi \cdot \phi} + 1 \right)} - \arg{\left(e^{2 \cdot i \cdot \pi \cdot \gamma_{1} \cdot \phi} \right)}\right)}
\newcommand{\diffE}{\gamma_{2} \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) + 1}
\newcommand{\diffI}{\frac{1}{- \gamma_{2} \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) + 1}}
\newcommand{\diffA}{e^{- 2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \phi^{2}}}
\newcommand{\diffH}{\theta \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) + 1}
\newcommand{\diffMagnitudeErrorE}{\left(\gamma_{2} \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) + 1\right) \cdot e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \phi^{2}} - 1}
\newcommand{\diffMagnitudeErrorI}{\frac{- 2 \cdot \gamma_{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \phi^{2}} - 1}{2 \cdot \gamma_{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} + 1}}
\newcommand{\diffISol}{\frac{\gamma_{2}}{2 \cdot \gamma_{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1}}
\newcommand{\diffASol}{\frac{\left(1 - e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \psi^{2}}\right) \cdot e^{- 2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \psi^{2}}}{\cos{\left(2 \cdot \pi \cdot \psi \right)} - 1}}
\newcommand{\diffESol}{\gamma_{2}}
\newcommand{\diffHI}{\frac{\gamma_{2} \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) + 2 \cdot \gamma_{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1}{2 \cdot \gamma_{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1}}
\newcommand{\diffHA}{\frac{\left(\left(1 - e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \psi^{2}}\right) \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) + \left(\cos{\left(2 \cdot \pi \cdot \psi \right)} - 1\right) \cdot e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \psi^{2}}\right) \cdot e^{- 2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \psi^{2}}}{\cos{\left(2 \cdot \pi \cdot \psi \right)} - 1}}
\newcommand{\diffHE}{\gamma_{2} \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) + 1}
\newcommand{\diffSupMagIIA}{\frac{\left(\gamma_{2} \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) - 1\right) \cdot \left(2 \cdot \gamma_{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + \left(2 \cdot \gamma_{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)} - 2 \cdot \gamma_{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} - 1\right) \cdot e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \phi^{2}} + 1\right)}{\left(2 \cdot \gamma_{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1\right) \cdot \left(\gamma_{2} \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) + e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \phi^{2}} - 1\right)}}
\newcommand{\diffSupMagAIA}{- \frac{\left(\gamma_{2} \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) - 1\right) \cdot \left(- \left(\left(e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \psi^{2}} - 1\right) \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) - \left(\cos{\left(2 \cdot \pi \cdot \psi \right)} - 1\right) \cdot e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \psi^{2}}\right) \cdot e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \phi^{2}} + 2 \cdot e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \psi^{2}} \cdot \sin^{2}{\left(\pi \cdot \psi \right)}\right) \cdot e^{- 2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \psi^{2}}}{\left(\cos{\left(2 \cdot \pi \cdot \psi \right)} - 1\right) \cdot \left(\gamma_{2} \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) + e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \phi^{2}} - 1\right)}}
\newcommand{\diffSupMagIEA}{\frac{- 2 \cdot \gamma_{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + \left(\gamma_{2} \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) + 2 \cdot \gamma_{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1\right) \cdot e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \phi^{2}} - 1}{\left(2 \cdot \gamma_{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} + 1\right) \cdot \left(\left(\gamma_{2} \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) + 1\right) \cdot e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \phi^{2}} - 1\right)}}
\newcommand{\diffSupMagAEA}{\frac{\left(\left(\left(1 - e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \psi^{2}}\right) \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) + \left(\cos{\left(2 \cdot \pi \cdot \psi \right)} - 1\right) \cdot e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \psi^{2}}\right) \cdot e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \phi^{2}} + 2 \cdot e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \psi^{2}} \cdot \sin^{2}{\left(\pi \cdot \psi \right)}\right) \cdot e^{- 2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \psi^{2}}}{\left(\left(\gamma_{2} \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) + 1\right) \cdot e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \phi^{2}} - 1\right) \cdot \left(\cos{\left(2 \cdot \pi \cdot \psi \right)} - 1\right)}}
\newcommand{\diffSupMagEIA}{- \frac{\left(\gamma_{2} \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) - 1\right) \cdot \left(\left(\gamma_{2} \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) + 1\right) \cdot e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \phi^{2}} - 1\right)}{\gamma_{2} \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right) + e^{2 \cdot \pi^{2} \cdot \gamma_{2} \cdot \phi^{2}} - 1}}
\newcommand{\poissFD}{\frac{1}{2 - 2 \cdot \cos{\left(2 \cdot \pi \cdot \phi \right)}}}
\newcommand{\poissA}{\frac{1}{4 \cdot \pi^{2} \cdot \phi^{2}}}
\newcommand{\poissIter}{\frac{0.5 - 0.5 \cdot \cos^{q}{\left(2 \cdot \pi \cdot \phi \right)}}{1 - \cos{\left(2 \cdot \pi \cdot \phi \right)}}}
\newcommand{\poissH}{\frac{\theta}{2 - 2 \cdot \cos{\left(2 \cdot \pi \cdot \phi \right)}}}
\newcommand{\poissMagnitudeErrorFD}{\frac{\pi^{2} \cdot \phi^{2}}{\sin^{2}{\left(\pi \cdot \phi \right)}} - 1}
\newcommand{\poissMagnitudeErrorIter}{2.0 \cdot \pi^{2} \cdot \phi^{2} \cdot \left|{\frac{\cos^{q}{\left(2 \cdot \pi \cdot \phi \right)} - 1}{\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1}}\right| - 1.0}
\newcommand{\poissMagnitudeErrorIterAgainstFD}{2.0 \cdot \sin^{2}{\left(\pi \cdot \phi \right)} \cdot \left|{\frac{\cos^{q}{\left(2 \cdot \pi \cdot \phi \right)} - 1}{\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1}}\right| - 1}
\newcommand{\poissIterSol}{1.0 - \cos^{q}{\left(6.28318530717959 \cdot \psi \right)}}
\newcommand{\poissFDSol}{1}
\newcommand{\poissASol}{\frac{\sin^{2}{\left(\pi \cdot \psi \right)}}{\pi^{2} \cdot \psi^{2}}}
\newcommand{\poissHIter}{\frac{\cos^{q}{\left(6.28318530717959 \cdot \psi \right)} - 1.0}{2 \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right)}}
\newcommand{\poissHFD}{- \frac{1}{2 \cdot \cos{\left(2 \cdot \pi \cdot \phi \right)} - 2}}
\newcommand{\poissHA}{- \frac{\sin^{2}{\left(\pi \cdot \psi \right)}}{2 \cdot \pi^{2} \cdot \psi^{2} \cdot \left(\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right)}}
\newcommand{\poissSupMagIterFDA}{\frac{2 \cdot \left(\pi^{2} \cdot \phi^{2} \cdot \left|{\frac{\cos^{q}{\left(6.28318530717959 \cdot \psi \right)} - 1.0}{\sin^{2}{\left(\pi \cdot \phi \right)}}}\right| - 1\right) \cdot \sin^{2}{\left(\pi \cdot \phi \right)}}{2 \cdot \pi^{2} \cdot \phi^{2} + \cos{\left(2 \cdot \pi \cdot \phi \right)} - 1}}
\newcommand{\poissSupMagIterIterA}{\frac{\pi^{2} \cdot \phi^{2} \cdot \left|{\frac{\cos^{q}{\left(6.28318530717959 \cdot \psi \right)} - 1.0}{\sin^{2}{\left(\pi \cdot \phi \right)}}}\right| - 1}{2.0 \cdot \pi^{2} \cdot \phi^{2} \cdot \left|{\frac{\cos^{q}{\left(2 \cdot \pi \cdot \phi \right)} - 1}{\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1}}\right| - 1.0}}
\newcommand{\poissSupMagFDIterA}{\frac{1.0 \cdot \left(\frac{\pi^{2} \cdot \phi^{2}}{\sin^{2}{\left(\pi \cdot \phi \right)}} - 1\right)}{\pi^{2} \cdot \phi^{2} \cdot \left|{\frac{\left(- (2 \cdot \sin^{2}{\left(\pi \cdot \phi \right)} - 1)\right)^{q} - 1}{\sin^{2}{\left(\pi \cdot \phi \right)}}}\right| - 1}}
\newcommand{\poissSupMagFDFDA}{1}
\newcommand{\poissSupMagIterIterFD}{\frac{1.0 \cdot \left(\sin^{2}{\left(\pi \cdot \phi \right)} \cdot \left|{\frac{\cos^{q}{\left(6.28318530717959 \cdot \psi \right)} - 1.0}{\sin^{2}{\left(\pi \cdot \phi \right)}}}\right| - 1\right)}{2 \cdot \sin^{2}{\left(\pi \cdot \phi \right)} \cdot \left|{\frac{\cos^{q}{\left(2 \cdot \pi \cdot \phi \right)} - 1}{\cos{\left(2 \cdot \pi \cdot \phi \right)} - 1}}\right| - 1}}
\newcommand{\poissSupMagAIterA}{\frac{1.0 \cdot \left(\frac{\phi^{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)}}{\sin^{2}{\left(\pi \cdot \phi \right)}} - \psi^{2}\right)}{\psi^{2} \cdot \left(\pi^{2} \cdot \phi^{2} \cdot \left|{\frac{\left(- (2 \cdot \sin^{2}{\left(\pi \cdot \phi \right)} - 1)\right)^{q} - 1}{\sin^{2}{\left(\pi \cdot \phi \right)}}}\right| - 1\right)}}
\newcommand{\poissSupMagAFD2A}{\frac{2 \cdot \left(\phi^{2} \cdot \sin^{2}{\left(\pi \cdot \psi \right)} - \psi^{2} \cdot \sin^{2}{\left(\pi \cdot \phi \right)}\right)}{\psi^{2} \cdot \left(2 \cdot \pi^{2} \cdot \phi^{2} + \cos{\left(2 \cdot \pi \cdot \phi \right)} - 1\right)}}
