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| Format: | Preprint |
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2025
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| Online Access: | https://arxiv.org/abs/2503.04331 |
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| _version_ | 1866910946751938560 |
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| author | Sato, Masayoshi |
| author_facet | Sato, Masayoshi |
| contents | We analyze the correlation function in JT gravity using three approaches: by summing over all geodesics connecting boundary operators, integrating over the region of moduli space determined by the ``no-shortcut condition'' introduced by D.Stanford and Z.Yang, and using the formula for the universal spectral density correlation in the $τ$-scaling limit. We find that the behaviors of the three results coincide at late times: they all exhibit a ``ramp'' instead of permanent decay. Using the third approach we also confirm that the ``plateau'' appears after $T_H=2πe^{S_0}\hatρ_0(E)$. Overall, our results are consistent with the SFF analysis.
We also calculate the ERB length $\langle \ell(T) \rangle$ using the three approaches and find that the results are in good agreement with each other. We also find that the $\langle \ell(T) \rangle$ grows as a cubic function in $T$ due to the contribution from geometry including one observable baby universe, and converges to a constant after $T=T_H$. For the geometry with one baby universe, we compute the size $\langle b(T) \rangle$ of the baby universe and find that it is of the same order as $\langle \ell(T) \rangle$. This result is consistent with the baby universe emission mechanism claimed by P.Saad. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2503_04331 |
| institution | arXiv |
| publishDate | 2025 |
| record_format | arxiv |
| spellingShingle | What happens due to the baby universe effect in JT gravity? -Analysis of correlation functions and ERB length at late time using three approaches- Sato, Masayoshi High Energy Physics - Theory We analyze the correlation function in JT gravity using three approaches: by summing over all geodesics connecting boundary operators, integrating over the region of moduli space determined by the ``no-shortcut condition'' introduced by D.Stanford and Z.Yang, and using the formula for the universal spectral density correlation in the $τ$-scaling limit. We find that the behaviors of the three results coincide at late times: they all exhibit a ``ramp'' instead of permanent decay. Using the third approach we also confirm that the ``plateau'' appears after $T_H=2πe^{S_0}\hatρ_0(E)$. Overall, our results are consistent with the SFF analysis. We also calculate the ERB length $\langle \ell(T) \rangle$ using the three approaches and find that the results are in good agreement with each other. We also find that the $\langle \ell(T) \rangle$ grows as a cubic function in $T$ due to the contribution from geometry including one observable baby universe, and converges to a constant after $T=T_H$. For the geometry with one baby universe, we compute the size $\langle b(T) \rangle$ of the baby universe and find that it is of the same order as $\langle \ell(T) \rangle$. This result is consistent with the baby universe emission mechanism claimed by P.Saad. |
| title | What happens due to the baby universe effect in JT gravity? -Analysis of correlation functions and ERB length at late time using three approaches- |
| topic | High Energy Physics - Theory |
| url | https://arxiv.org/abs/2503.04331 |