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Commit 13537135 authored by Luke Naylor's avatar Luke Naylor
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Find good alt expression for hyp term of bgmlv3

parent 8f631ac0
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...@@ -571,17 +571,19 @@ bgmlv3_d_upperbound_exp_term = ( ...@@ -571,17 +571,19 @@ bgmlv3_d_upperbound_exp_term = (
# Verify the simplified forms of the terms that will be mentioned in text # Verify the simplified forms of the terms that will be mentioned in text
var("chbv",domain="real") # symbol to represent ch_1^\beta(v) var("chb1v chb2v",domain="real") # symbol to represent ch_1^\beta(v)
var("psi phi", domain="real") # symbol to represent ch_1^\beta(v) and
# ch_2^\beta(v)
assert bgmlv3_d_upperbound_const_term == ( assert bgmlv3_d_upperbound_const_term == (
( (
# keep hold of this alternative expression: # keep hold of this alternative expression:
bgmlv3_d_upperbound_const_term_alt := ( bgmlv3_d_upperbound_const_term_alt := (
chbv phi
+ beta*q + beta*q
) )
) )
.subs(chbv == v.twist(beta).ch[2]) # subs real val of ch_1^\beta(v) .subs(phi == v.twist(beta).ch[2]) # subs real val of ch_1^\beta(v)
.expand() .expand()
) )
...@@ -590,13 +592,25 @@ assert bgmlv3_d_upperbound_exp_term == ( ...@@ -590,13 +592,25 @@ assert bgmlv3_d_upperbound_exp_term == (
# Keep hold of this alternative expression: # Keep hold of this alternative expression:
bgmlv3_d_upperbound_exp_term_alt := bgmlv3_d_upperbound_exp_term_alt :=
( (
R*chbv R*phi
+ (C - q)^2/2 + (C - q)^2/2
+ R*beta*q + R*beta*q
- D*R - D*R
)/(r-R) )/(r-R)
) )
.subs(chbv == v.twist(beta).ch[2]) # subs real val of ch_1^\beta(v) .subs(phi == v.twist(beta).ch[2]) # subs real val of ch_1^\beta(v)
.expand()
)
assert bgmlv3_d_upperbound_exp_term == (
(
# Keep hold of this alternative expression:
bgmlv3_d_upperbound_exp_term_alt2 :=
(
(psi - q)^2/2/(r-R)
)
)
.subs(psi == v.twist(beta).ch[1]) # subs real val of ch_1^\beta(v)
.expand() .expand()
) )
\end{sagesilent} \end{sagesilent}
...@@ -611,7 +625,10 @@ The linear term in $r$ is ...@@ -611,7 +625,10 @@ The linear term in $r$ is
$\sage{bgmlv3_d_upperbound_linear_term}$. $\sage{bgmlv3_d_upperbound_linear_term}$.
Finally, there's an hyperbolic term in $r$ which tends to 0 as $r \to \infty$, Finally, there's an hyperbolic term in $r$ which tends to 0 as $r \to \infty$,
and can be written: and can be written:
$\frac{R\chern^{\beta}_2(F) + (C-q)^2/2 + R\beta q - DR}{r-R}$. \bgroup
\def\psi{\chern_1^{\beta}(F)}
$\sage{bgmlv3_d_upperbound_exp_term_alt2}$.
\egroup
In the case $\beta = \beta_{-}$ (or $\beta_{+}$) we have In the case $\beta = \beta_{-}$ (or $\beta_{+}$) we have
$\chern^{\beta}_2(F) = 0$, $\chern^{\beta}_2(F) = 0$,
so some of these expressions simplify, and in particular, the constant and so some of these expressions simplify, and in particular, the constant and
......
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