Fig. 1.
Behaviors of $ \Lambda_0$ ($ x$ ) and $ F$ ($ x$ ,$ \theta_{\rm H}$ ) for $ \theta_{\rm H} =$ 0 and $ \pi/2$ [see equations (47)-(51)]. Note that $ \Lambda$ ($ x$ ,$ \theta_{\rm H}; h^2$ ) is obtained by adding $ F$ ($ x,\theta_{\rm H}$ ) multiplied by factor $ h^2$ to $ \Lambda_0$ ($ x$ ), and $ x_{\rm N}$ is given by adding $-h^2$ (2$ ^{1/3}$ )$ F$ (2$ ^{1/3}$ ,$ \theta_{\rm H}$ ) to 2$ ^{1/3}$ , as seen in equation (52). $ f_{\rm H} = f$ (1) $ =$ 0.5676. (Color online)

Behaviors of |$ \Lambda_0$| (⁠|$ x$| ) and |$ F$| (⁠|$ x$| ,|$ \theta_{\rm H}$| ) for |$ \theta_{\rm H} =$| 0 and |$ \pi/2$| [see equations (47)-(51)]. Note that |$ \Lambda$| (⁠|$ x$| ,|$ \theta_{\rm H}; h^2$| ) is obtained by adding |$ F$| (⁠|$ x,\theta_{\rm H}$| ) multiplied by factor |$ h^2$| to |$ \Lambda_0$| (⁠|$ x$| ), and |$ x_{\rm N}$| is given by adding |$-h^2$| (2|$ ^{1/3}$| )|$ F$| (2|$ ^{1/3}$| ,|$ \theta_{\rm H}$| ) to 2|$ ^{1/3}$| , as seen in equation (52). |$ f_{\rm H} = f$| (1) |$ =$| 0.5676. (Color online)

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