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| -rw-r--r-- | Figs/sd_susc_0_28.pdf | bin | 28107 -> 34718 bytes | |||
| -rw-r--r-- | Figs/sd_susc_plot.pdf | bin | 48379 -> 48687 bytes | |||
| -rw-r--r-- | Jauslin_2015-PhD.tex | 2 |
3 files changed, 1 insertions, 1 deletions
diff --git a/Figs/sd_susc_0_28.pdf b/Figs/sd_susc_0_28.pdf Binary files differindex c1aff16..834df05 100644 --- a/Figs/sd_susc_0_28.pdf +++ b/Figs/sd_susc_0_28.pdf diff --git a/Figs/sd_susc_plot.pdf b/Figs/sd_susc_plot.pdf Binary files differindex ff8c4ce..602a3c3 100644 --- a/Figs/sd_susc_plot.pdf +++ b/Figs/sd_susc_plot.pdf diff --git a/Jauslin_2015-PhD.tex b/Jauslin_2015-PhD.tex index bddec82..841aee2 100644 --- a/Jauslin_2015-PhD.tex +++ b/Jauslin_2015-PhD.tex @@ -1932,7 +1932,7 @@ Therefore, using the bound~(\ref{bilayerboundGt}), the change of variables defin \begin{equation} \begin{array}{>{\displaystyle}r@{\ }>{\displaystyle}l} \frac{1}{\beta|\Lambda|}\int d\underline{\mathbf x}\ \left|(\underline{\mathbf x}-\mathbf x_{2l})^mB_{2l,\underline\varpi}^{(h)}(\underline{\mathbf x})\right| -\leqslant&\sum_{N=1}^\infty\sum_{\tau\in\mathcal T_N^{(h)}}\sum_{T\in\mathbf T(\tau)}\sum_{\underline l_\tau}\sum_{\displaystyle\mathop{\scriptstyle \mathbf P\in\tilde{\mathcal P}_{\tau,\underline l_\tau,\ell_0}}_{|P_{v_0}|=2l}}c_1^N\mathfrak F_h(\underline m)\cdot\\[0.5cm] +\leqslant&\sum_{N=1}^\infty\sum_{\tau\in\mathcal T_N^{(h)}}\sum_{T\in\mathbf T(\tau)}\sum_{\underline l_\tau}\sum_{\displaystyle\mathop{\scriptstyle \mathbf P\in\tilde{\mathcal P}_{\tau,\underline l_\tau,\ell_0}}_{|P_{v_0}|=2l}}C_1^N\mathfrak F_h(\underline m)\cdot\\[0.5cm] &\cdot\prod_{v\in\mathfrak V(\tau)}\frac{1}{s_v!}C_G^{n_v-s_v+1}C_g^{s_v-1}2^{h_v((c_k-c_g)n_v-c_k(s_v-1))}\cdot\\[0.5cm] &\cdot\prod_{v\in\mathfrak E(\tau)}c_2^{2l_v}\mathfrak C_{2l_v}|U|^{\max(1,l_v-1)}2^{(h_v-1)(c_k-(c_k-c_g)l_v)} \end{array} |