diff --git a/notes/conventions.md b/notes/conventions.md
index 2e8956d..632e1a3 100644
--- a/notes/conventions.md
+++ b/notes/conventions.md
@@ -2,24 +2,31 @@ VSWF conventions
 ================
 
 
-| Source	| VSWF definition  	| VSWF norm  	| CS Phase  	|  Field expansion 	|  Radiated power | Notes |
-|---	|---	|---	|---	|---	|---	|--- 	|
-| Kristensson I \cite kristensson_spherical_2014 	|  \f[ \wfkcreg, \wfkcout= \dots \f] 	|   	| Yes, in the spherical harmonics definition, cf. sect. D.2.  	| \f[ 
+| Source	| VSWF definition  	| E/M interrelations | VSWF norm  	| CS Phase  	|  Field expansion 	|  Radiated power | Notes |
+|---	|---	|---	|---	|---	|---	|--- 	|--- |
+| Kristensson I \cite kristensson_spherical_2014 	|  \f[ \wfkcreg, \wfkcout= \dots \f] 	| \f[
+	\wfkcreg_{1lm} = \frac{1}{k}\nabla\times\wfkcreg_{2lm}, \\
+	\wfkcreg_{2lm} = \frac{1}{k}\nabla\times\wfkcreg_{1lm},
+\f] and analogously for outgoing waves \f$ \wfkcout \f$, eq. (2.8) onwards. 	|  	| Yes, in the spherical harmonics definition, cf. sect. D.2.  	| \f[ 
 	\vect E = k \sqrt{\eta_0\eta} \sum_n \left( \wckcreg_n  \wfkcreg_n + \wckcout_n \wfkcout_n  \right), 
 	\\ 
 	\vect H =  \frac{k \sqrt{\eta_0\eta}}{i\eta_0\eta} \sum_n \left( \wckcreg_n  \wfkcreg_n + \wckcout_n \wfkcout_n  \right),
 \f] but for plane wave expansion \cite kristensson_spherical_2014 sect. 2.5 K. uses a different definition (same as in Kristensson II).  	| \f[
 	 P = \frac{1}{2} \sum_n \left( \abs{\wckcout_n}^2 +\Re \left(\wckcout_n\wckcreg_n^{*}\right)\right)
  \f]	| The \f$ \wckcreg, \wckcout \f$	coefficients have dimension \f$ \sqrt{\mathrm{W}} \f$. |
-| Kristensson II \cite kristensson_scattering_2016	| \f[ \wfkrreg, \wfkrout= \dots \f] 	|   	|   	| \f[ 
+| Kristensson II \cite kristensson_scattering_2016	| \f[ \wfkrreg, \wfkrout= \dots \f] 	|  \f[
+	\nabla\times\wfkrreg_{\tau n} = k\wfkrreg_{\overline{\tau} n},
+\f] eq. (7.7) and analogously for outgoing waves \f$ \wfkrout \f$. 	| 	|   	| \f[ 
 	\vect E = \sum_n \left( \wckrreg_n  \wfkrreg_n + \wckrout_n \wfkrout_n  \right), 
 	\\ 
 	\vect H =  \frac{1}{i\eta_0\eta} \sum_n \left( \wckrreg_n  \wfkrreg_n + \wckrout_n \wfkrout_n  \right)
 \f] 	| \f[
 	 P = \frac{1}{2k^2\eta_0\eta} \sum_n \left( \abs{\wckrout_n}^2 +\Re \left(\wckrout_n\wckrreg_n^{*}\right)\right)
  \f]	| The \f$ \wckrreg, \wckrout \f$ coefficients have dimension \f$ \mathrm{V/m} \f$. |
-| Reid \cite reid_electromagnetism_2016	|   |  	|   	|  \f[
-	\vect E = \sum_\alpha \pr{ \wcrreg_\alpha \wfrreg_\alpha + \wcrout_\alpha wfrout_\alpha }, \\
+| Reid \cite reid_electromagnetism_2016	|   | \f[
+	\nabla\times\wfr_{lmM} = -ik\wfr_{lmN}, \\ \nabla\times\wfr_{lmN} = +ik\wfr_{lmM}. 
+\f] 	|	|  |  \f[
+	\vect E = \sum_\alpha \pr{ \wcrreg_\alpha \wfrreg_\alpha + \wcrout_\alpha \wfrout_\alpha }, \\
 	\vect H = \frac{1}{Z_0Z^r} \sum_\alpha \pr{ \wcrreg_\alpha \sigma_\alpha\wfrreg_\overline{\alpha} +
 		 \wcrout_\alpha \sigma_\alpha\wfrout_\overline{\alpha}},
 \f] where \f$ \sigma_{lmM} = +1, \sigma_{lmN}=-1, \overline{lmM}=lmM, \overline{lmN}=lmM, \f$  cf. eq. (6). The notation is not extremely consistent throughout Reid's memo.	| 	| 	|
@@ -27,7 +34,7 @@ VSWF conventions
 	\wfet_{mn}^{(j)}	=	\frac{n(n+1)}{kr}\sqrt{\frac{2n+1}{4\pi}\frac{\left(n-m\right)!}{\left(n+m\right)!}}P_{n}^{m}\left(\cos\theta\right)e^{im\phi}z_{n}^{j}\left(kr\right)\uvec{r} \\
 		+\left[\tilde{\tau}_{mn}\left(\cos\theta\right)\uvec{\theta}+i\tilde{\pi}_{mn}\left(\cos\theta\right)\uvec{\phi}\right]e^{im\phi}\frac{1}{kr}\frac{\ud\left(kr\,z_{n}^{j}\left(kr\right)\right)}{\ud(kr)}, \\ 
 	\wfmt_{mn}^{(j)}	=	\left[i\tilde{\pi}_{mn}\left(\cos\theta\right)\uvec{\theta}-\tilde{\tau}_{mn}\left(\cos\theta\right)\uvec{\phi}\right]e^{im\phi}z_{n}^{j}\left(kr\right)
-\f]  | 	\f[
+\f]  	|	|	\f[
 	\int_{S(kr)} \wfmt_{mn}^{(j)} \wfmt_{m'n'}^{(j)}\,\ud S = n(n+1) \abs{z_n^{(j)}}^2 \delta_{m,m'}\delta_{n,n'} ,\\
 	\int_{S(kr)} \wfet_{mn}^{(j)} \wfet_{m'n'}^{(j)}\,\ud S =
            \pr{\pr{n(n+1)}^2 \abs{\frac{z_n^{(j)}}{kr}}^2 + n(n+1)\abs{\frac{1}{kr}\frac{\ud}{\ud(kr)}\pr{kr z_n^{(j)}}} } \delta_{m,m'}\delta_{n,n'} ,