Abstract
This publisher’s note contains corrections to Opt. Lett. 45, 2580 (2020). [CrossRef]
© 2020 Optical Society of
America
In Ref. [1], an equation was displayed
incorrectly. Equation (3) should have been
$$\begin{split}{\psi
_{LA}}\left({r,\theta} \right) &= - \frac{1}{{2a}}\ln
\left\{2a{{\left[{{a^2}{r^4} + \left({1 + 2a{d_1}} \right){r^2} + d_1^2}
\right]}^{\frac{1}{2}}}\right.\\&\quad + \left.\vphantom{
\frac{1}{{2a}}\ln \left\{2a{{\left[{{a^2}{r^4} + \left({1 + 2a{d_1}}
\right){r^2} + d_1^2} \right]}^{\frac{1}{2}}}\right.} 2{a^2}{r^2} + 1 +
2a{d_1} \right\} + {\rm const.}\end{split}$$
REFERENCE
1. Z. Y. Hu, Z. N. Tian, H. Fan, J. G. Hua, M. D. Qian, Q. D. Chen, and H. B. Sun, Opt. Lett. 45, 2580 (2020). [CrossRef]
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Equations (1)
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(1)