Table S2.

Field quantities of a propagating wave and an evanescent wave

Symbol	For a propagating wave $\mathbf{E}=\sqrt{\mu }{\mathbf{E}}_{\mathbf{0}}\exp \left(ikz\right)I={\left|{\mathbf{E}}_{\mathbf{0}}\right|}^2$	For an evanescent field $\mathbf{E}=\sqrt{\mu }{\mathbf{E}}_{\mathbf{0}}\exp \left(-\kappa x\right)\exp \left(i{k}_{\text{z}}z\right)I_{\text{e}}=\frac{{\left|{\mathbf{E}}_{\mathbf{0}}\right|}^2}{1+\tau {\left(\kappa /k_{\text{z}}\right)}^2}\exp \left(-2\kappa x\right)$	Quantity
$\mathbf{p}$	$\frac{g}{2\omega }I{k}_{\text{z}}\widehat{\mathbf{z}}$	$\frac{g}{2\omega }{I}_{\text{e}}\left(\sigma \frac{\kappa k}{k_{\text{z}}}\widehat{\mathbf{y}}+\frac{k^2}{k_{\text{z}}}\widehat{\mathbf{z}}\right)$	Poynting momentum density
${\mathbf{p}}^{″}$	0	$\frac{g}{2\omega }{I}_{\text{e}}\left(\tau \frac{\kappa k^2}{k_z^2}\widehat{\mathbf{x}}+\xi \frac{\kappa k}{k_z}\widehat{\mathbf{y}}\right)$	Value of the imaginary adjoint to the Poynting momentum density
${\mathbf{p}}^{\mathbf{o}}$	$\frac{g}{2\omega }I{k}_z\widehat{\mathbf{z}}$	$\frac{g}{2\omega }{I}_{\text{e}}{k}_z\widehat{\mathbf{z}}$	Orbital (or canonical) Poynting momentum density
${\mathbf{p}}_{\mathbf{e}}^{\mathbf{o}}$	$\frac{g}{4\omega }I{k}_z\widehat{\mathbf{z}}$	$\frac{g}{4\omega }{I}_{\text{e}}\left(1+\frac{{\kappa }^2}{k_z^2}\right)k_z\widehat{\mathbf{z}}$	Electric contribution to the orbital Poynting momentum density
${\mathbf{p}}_{\mathbf{m}}^{\mathbf{o}}$	$\frac{g}{4\omega }I{k}_z\widehat{\mathbf{z}}$	$\frac{g}{4\omega }{I}_{\text{e}}\left(1-\frac{{\kappa }^2}{k_z^2}\right)k_z\widehat{\mathbf{z}}$	Magnetic contribution to the orbital Poynting momentum density
${\mathbf{p}}^{\mathbf{s}}$	0	$\frac{g}{2\omega }{I}_{\text{e}}\left(-\frac{{\kappa }^2}{k_z^2}\widehat{\mathbf{z}}+\sigma \frac{\kappa k}{k_z}\widehat{\mathbf{y}}\right)$	Spin part of the Poynting momentum density [Belinfante’s momentum (17, 19)]
${\mathbf{p}}_{\mathbf{e}}^{\mathbf{s}}$	0	$\frac{g}{4\omega }{I}_{\text{e}}\left(-\left(1+\tau \right)\frac{{\kappa }^2}{k_z^2}\widehat{\mathbf{z}}+\sigma \frac{\kappa k}{k_z}\widehat{\mathbf{y}}\right)$	Electric contribution to the spin momentum density
${\mathbf{p}}_{\mathbf{m}}^{\mathbf{s}}$	0	$\frac{g}{4\omega }{I}_{\text{e}}\left(-\left(1-\tau \right)\frac{{\kappa }^2}{k_z^2}\widehat{\mathbf{z}}+\sigma \frac{\kappa k}{k_z}\widehat{\mathbf{y}}\right)$	Magnetic contribution to the spin momentum density
$\mathbf{s}$	$\frac{g}{2\omega }I\sigma \widehat{\mathbf{z}}$	$\frac{g}{2\omega }{I}_{\text{e}}\left(\sigma \frac{k}{k_z}\widehat{\mathbf{z}}+\frac{\kappa }{k_z}\widehat{\mathbf{y}}\right)$	SAM density
${\mathbf{s}}_{\mathbf{e}}$	$\frac{g}{4\omega }I\sigma \widehat{\mathbf{z}}$	$\frac{g}{4\omega }{I}_{\text{e}}\left(\sigma \frac{k}{k_z}\widehat{\mathbf{z}}+\left(1+\tau \right)\frac{\kappa }{k_z}\widehat{\mathbf{y}}+\xi \frac{\kappa k}{k_z^2}\widehat{\mathbf{x}}\right)$	Electric contribution to the SAM density
${\mathbf{s}}_{\mathbf{m}}$	$\frac{g}{4\omega }I\sigma \widehat{\mathbf{z}}$	$\frac{g}{4\omega }{I}_{\text{e}}\left(\sigma \frac{k}{k_z}\widehat{\mathbf{z}}+\left(1-\tau \right)\frac{\kappa }{k_z}\widehat{\mathbf{y}}-\xi \frac{\kappa k}{k_z^2}\widehat{\mathbf{x}}\right)$	Magnetic contribution to the SAM
h	$\frac{g}{2\omega }In\sigma$	$\frac{g}{2\omega }{I}_{\text{e}}{n}_2\sigma$	Helicity
$\nabla \times \mathbf{p}$	0	$\frac{g}{2\omega }{I}_{\text{e}}\left(2\frac{\kappa k^2}{k_z}\widehat{\mathbf{y}}-2\sigma \frac{{\kappa }^{2}k}{k_{\text{z}}}\widehat{\mathbf{z}}\right)$	Vorticity of the photon flow
$u_{\text{e}}$	$\frac{g{n}^2}{4}I$	$\frac{g{n}_2^2}{4}{I}_{\text{e}}\left(1+\tau \frac{{\kappa }^2}{k_{\text{z}}^2}\right)$	Electric contribution to energy density
$u_{\text{m}}$	$\frac{g{n}^2}{4}I$	$\frac{g{n}_2^2}{4}{I}_{\text{e}}\left(1-\tau \frac{{\kappa }^2}{k_{\text{z}}^2}\right)$	Magnetic contribution to energy density

Summary of the physical quantities involved in the force for a propagating plane wave and for an evanescent field. The magnetic and electric contributions to the orbital and spin angular momenta are listed explicitly.