summaryrefslogtreecommitdiff
diff options
context:
space:
mode:
authorJaron Kent-Dobias <jaron@kent-dobias.com>2024-10-29 10:24:54 +0100
committerJaron Kent-Dobias <jaron@kent-dobias.com>2024-10-29 10:24:54 +0100
commitf824dea3df7492fecfa95d34b33900a533bfd699 (patch)
tree74560807522c9f2ba7f973a29b2ad9b39cf0ac8b
parent568324cd4bc0cf2dd6a81464b1c4c700ee7ebfa5 (diff)
downloadmarginal-f824dea3df7492fecfa95d34b33900a533bfd699.tar.gz
marginal-f824dea3df7492fecfa95d34b33900a533bfd699.tar.bz2
marginal-f824dea3df7492fecfa95d34b33900a533bfd699.zip
Changed also convention for superbasis in R^N|4
-rw-r--r--marginal.tex13
1 files changed, 11 insertions, 2 deletions
diff --git a/marginal.tex b/marginal.tex
index 88809d2..85743c3 100644
--- a/marginal.tex
+++ b/marginal.tex
@@ -1843,8 +1843,17 @@ The same method can be used to calculate the
superdeterminant and supertrace in arbitrary superspaces, where for $\mathbb R^{N|2D}$ each
basis has $2^{2D-1}$ elements. For instance, for $\mathbb R^{N|4}$ we have
\begin{align}
- &\mathbf e(1,2)=\{1,i\bar\theta_1\theta_1,i\bar\theta_2\theta_2,i\bar\theta_1\theta_2,i\bar\theta_2\theta_1,i\bar\theta_1\bar\theta_2,i\theta_1\theta_2,\bar\theta_1\theta_1\bar\theta_2\theta_2\}\notag \\
- &\mathbf f(1,2)=\{i\bar\theta_1,i\theta_1,i\bar\theta_2,i\theta_2,\bar\theta_1\theta_1\bar\theta_2,\bar\theta_2\theta_2\theta_1,\bar\theta_1\theta_1\theta_2,\bar\theta_2\theta_2\theta_1\}
+ &\mathbf e(1,2)=\{
+ 1,\bar\theta_1\theta_1,\bar\theta_2\theta_2,
+ \bar\theta_1\theta_2,\bar\theta_2\theta_1,
+ \bar\theta_1\bar\theta_2,\theta_1\theta_2,
+ \bar\theta_1\theta_1\bar\theta_2\theta_2
+ \}\notag \\
+ &\mathbf f(1,2)=\{
+ \bar\theta_1,\theta_1,\bar\theta_2,\theta_2,
+ \bar\theta_1\theta_1\bar\theta_2,\bar\theta_2\theta_2\theta_1,
+ \bar\theta_1\theta_1\theta_2,\bar\theta_2\theta_2\theta_1
+ \}
\end{align}
with the dual bases defined analogously to those above.