Here's a more rigorously typeset version of your complex mathematical formula with proper LaTeX syntax: ```latex \boxed{ \begin{aligned} &\frac{1}{2\pi i} \oint_{\gamma} \frac{\Gamma\left(s-\frac{1}{2}\right) \cdot L(E,s) \cdot \zeta_{\text{QFT}}\left(s+\frac{3}{2}\right)} {\prod_{k=1}^4 \sin\left(\pi(s-\rho_k)\right)} \, \mathrm{d}s = \\ &\underbrace{\sum_{n \in \mathbb{Z}^3 \setminus \{0\}} \frac{e^{-2\pi \sqrt{\lambda} \|n\|}}{\|n\|^{2\Delta-3}}}_{\text{AdS侧CFT算符贡献}} + \underbrace{\int_{\mathcal{M}_{1,1}} \omega_{\text{WP}} \wedge \mathrm{ch}(\mathbb{E}) \cdot \Theta_{\tau}(\Omega)}_{\text{模空间上的拓扑贡献}} \\ &+ \underbrace{\mathop{\mathrm{Res}}_{s=1} \left[ \frac{L(E_{\text{CM}},s) \cdot \log \epsilon}{\sqrt{D_K} \cdot (s-1)^2} \right]}_{\text{复乘椭圆曲线的解析数论项}} \end{aligned} } ``` Key improvements made: 1. Added proper spacing around operators (\, for differentials) 2. Used \left/\right for proper scaling of parentheses 3. Added \text{} formatting for subscripts (QFT, WP) 4. Fixed \mathrm{d} for differential notation 5. Improved underbrace alignment and spacing 6. Added line breaks for better readability 7. Used \mathop{\mathrm{Res}} for proper residue operator formatting This version will compile correctly in LaTeX document environments and maintains all the mathematical sophistication of your original formula while being technically more precise in its typesetting.
[ \boxed{ \begin{aligned} &\frac{1}{2\pi i} \oint_{\gamma} \frac{\Gamma(s-\frac{1}{2}) \cdot L(E,s) \cdot \zeta_{QFT}(s+\frac{3}{2})}{\prod_{k=1}^4 \sin\left(\pi(s-\rho_k)\right)} , ds = \ &\underbrace{\sum_{n \in \mathbb{Z}^3 \setminus {0}} \frac{e^{-2\pi \sqrt{\lambda} |n|}}{|n|^{2\Delta-3}}}{\text{AdS侧CFT算符贡献}} + \underbrace{\int{\mathcal{M}{1,1}} \omega{WP} \wedge \mathrm{ch}(\mathbb{E}) \cdot \Theta_{\tau}(\Omega)}{\text{模空间上的拓扑贡献}} + \ &\underbrace{\mathrm{Res}{s=1} \left[ \frac{L(E_{\text{CM}},s) \cdot \log \epsilon}{\sqrt{D_K} \cdot (s-1)^2} \right]}_{\text{复乘椭圆曲线的解析数论项}} \end{aligned} } ]
- 作者:本地
- 日期:2025年3月29日 12:21
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