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contracting FLRW spacetimes<\/td><\/tr><\/td> <\/td><\/tr> 16:40\u201317:40<\/td> \u9ad8\u5742 \u826f\u53f2\uff08\u795e\u6238\u5927\u5b66\uff09<\/td><\/tr> <\/td> Willmore \u6d41\u306e\u95be\u5024\u578b\u8fd1\u4f3c\u30a2\u30eb\u30b4\u30ea\u30ba\u30e0\u306b\u3064\u3044\u3066<\/td><\/tr> <\/td> <\/td><\/tr> 18:00-20:00<\/td> \u4ea4\u6d41\u4f1a<\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n 10:00-11:00<\/td> \u5c0f\u91ce\u5bfa \u6804\u6cbb\uff08\u9ad8\u77e5\u5927\u5b66\uff09<\/td><\/tr> <\/td> Local well-posedness for a fourth-order nonlinear dispersive system
on the one-dimensional torus: from a viewpoint of geometric analysis<\/td><\/tr><\/td> <\/td><\/tr> 11:15-12:15<\/td> \u5185\u514d \u5927\u8f14\uff08\u5ba4\u862d\u5de5\u696d\u5927\u5b66\uff09<\/td><\/tr> <\/td> 2 \u6b21\u5143\u8d85\u81e8\u754c\u534a\u7dda\u5f62\u6955\u5186\u578b\u65b9\u7a0b\u5f0f\u306e\u7403\u5bfe\u79f0\u7206\u767a\u89e3\u306e\u7121\u9650\u96c6\u4e2d\u3068\u632f\u52d5\u73fe\u8c61\u306b\u3064\u3044\u3066<\/td><\/tr> <\/td> <\/td><\/tr> 12:15-<\/td> Closing<\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n
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