Alternative Equation Formats

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MathML

γ_{z} (h) = {\begin{cases} 0 & if ∣ h ∣= 0 \\ c_{n} + {σ_{0}}^{2} [1 - \frac{2}{Γ (ν)} {(\frac{∣ h ∣ \sqrt{ν}}{a_{0}})}^{ν} K_{ν} (2 \frac{∣ h ∣ \sqrt{ν}}{a_{0}})] & if 0 <∣ h ∣, ν > 0 \end{cases}

MathML rendered with MathJax

γ_{z} (h) = {\begin{cases} 0 & if ∣ h ∣= 0 \\ c_{n} + {σ_{0}}^{2} [1 - \frac{2}{Γ (ν)} {(\frac{∣ h ∣ \sqrt{ν}}{a_{0}})}^{ν} K_{ν} (2 \frac{∣ h ∣ \sqrt{ν}}{a_{0}})] & if 0 <∣ h ∣, ν > 0 \end{cases}

Math as LaTeX Source

$ \gamma _ z(\bm {h}) = \left\{ \begin{array}{ll} 0 & \mbox{if $\mid \bm {h} \mid = 0$} \\ c_ n + {\sigma _0}^2\left[1 - \frac{ 2 }{ \Gamma (\nu ) } \left( \frac{ \mid \bm {h} \mid \sqrt {\nu } }{ a_0 } \right)^{\nu } K_{\nu } \left( 2 \frac{ \mid \bm {h} \mid \sqrt {\nu } }{ a_0 } \right) \right] & \mbox{if $0 < \mid \bm {h} \mid $, $\nu > 0$} \end{array} \right. $