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author | Ian Jauslin <ian.jauslin@roma1.infn.it> | 2016-01-10 19:07:32 +0000 |
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committer | Ian Jauslin <ian.jauslin@roma1.infn.it> | 2016-01-10 19:07:32 +0000 |
commit | 071adcecbb11817660e42a9354a42cbbdd367722 (patch) | |
tree | 988d9a005b990f27ac25f68e8f16311d5c2f8c07 | |
parent | c6a2b9ffb580c4f50f416fe4c673322875dd6ded (diff) |
Fix typov0.1.4
-rw-r--r-- | Giuliani_Jauslin_2015.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/Giuliani_Jauslin_2015.tex b/Giuliani_Jauslin_2015.tex index 334f3a1..3af7797 100644 --- a/Giuliani_Jauslin_2015.tex +++ b/Giuliani_Jauslin_2015.tex @@ -1772,7 +1772,7 @@ Therefore, using the bound~(\ref{boundGt}), the change of variables defined abov \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} |