Table 2 The dynamical and topological properties of generic EM wave, linear polarized surface EM wave, deep-water gravity wave, and acoustic wave fields.
From: Dynamical and topological properties of the spin angular momenta in general electromagnetic fields
Generic EM wave | Linear polarized surface EM wave | Gravity water wave | Acoustic wave | |
|---|---|---|---|---|
Field components | Electric field E; Magnetic field H; | Electric or magnetic Hertz potential Ψ; | In-plane velocity V; Normal velocity W; | Velocity v; Pressure p; |
Kinetic momentum | \({{{{{\mathbf{\Pi }}}}}}=\frac{1}{2{c}^{2}}{{{{\mathrm{Re}}}}}\{{{{{{{\bf{E}}}}}}}^{\ast }\times {{{{{\bf{H}}}}}}\}\) | \({{{{{\mathbf{\Pi }}}}}}=\frac{\varepsilon {k}^{2}{k}_{p}^{2}}{2\omega }{{\mbox{Im}}}\{{\varPsi }^{\ast }\nabla \varPsi \}\) | \({{{{{{\mathbf{\Pi }}}}}}}_{G}=\frac{{\rho }_{G}{k}_{G}}{{\omega }_{G}}{{\mbox{Im}}}\{{W}^{\ast }{{{{{\bf{V}}}}}}\}\) | \({{{{{{\mathbf{\Pi }}}}}}}_{A}=\frac{1}{2{c}_{A}^{2}}{{{{\mathrm{Re}}}}}\{{p}^{\ast }{{{{{\bf{v}}}}}}\}\) |
Spin angular momenum | \({{{{{\bf{S}}}}}}=\frac{1}{4\omega }{{\mbox{Im}}}\{\begin{array}{c}\varepsilon {{{{{{\bf{E}}}}}}}^{\ast }\times {{{{{\bf{E}}}}}}\\ +\mu {{{{{{\bf{H}}}}}}}^{\ast }\times {{{{{\bf{H}}}}}}\end{array}\}\) | \({{{{{\bf{S}}}}}}=\frac{\varepsilon {k}_{p}^{2}}{4\omega }{{\mbox{Im}}}\{\nabla {\varPsi }^{\ast }\times \nabla \varPsi \}\) | \({{{{{{\bf{S}}}}}}}_{G}=\frac{{\rho }_{G}}{2{\omega }_{G}}{{\mbox{Im}}}\{{{{{{{\bf{V}}}}}}}^{\ast }\times {{{{{\bf{V}}}}}}\}\) | \({{{{{{\bf{S}}}}}}}_{A}=\frac{{\rho }_{A}}{2{\omega }_{A}}{{\mbox{Im}}}\{{{{{{{\bf{v}}}}}}}^{\ast }\times {{{{{\bf{v}}}}}}\}\) |
Helicity | Spin-1 photon σ = ±1 | Spin-1 photon σ = ±1 | Spin-0 phonon σG = 0 | Spin-0 phonon σA = 0 |
Spin-momentum locking | \(\begin{array}{c}{{{{{{\bf{S}}}}}}}_{t}=\frac{1}{2{k}^{2}}\nabla \times {{{{{\mathbf{\Pi }}}}}}\\ {{{{{{\bf{S}}}}}}}_{l}=\mathop{\sum}\limits_{i}\hslash {\sigma }_{i}{\hat{{{{{{\bf{k}}}}}}}}_{i}+\mathop{\sum}\limits_{i\ne j}\hslash {\sigma }_{ij}{\hat{{{{{{\bf{k}}}}}}}}_{ij}\end{array}\) | \(\begin{array}{c}{{{{{{\bf{S}}}}}}}_{t}=\frac{1}{2{k}^{2}}\nabla \times {{{{{\mathbf{\Pi }}}}}}\\ {{{{{{\bf{S}}}}}}}_{l}=0\end{array}\) | \({{{{{{\bf{S}}}}}}}_{G}=\frac{1}{2{k}_{G}^{2}}{\nabla }_{2}\times {{{{{{\mathbf{\Pi }}}}}}}_{G}\) | \({{{{{{\bf{S}}}}}}}_{A}=\frac{1}{{k}_{A}^{2}}\nabla \times {{{{{{\mathbf{\Pi }}}}}}}_{A}\) |