{"id":3459,"date":"2025-12-15T10:34:19","date_gmt":"2025-12-15T01:34:19","guid":{"rendered":"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/?post_type=seminar&#038;p=3459"},"modified":"2025-12-15T10:44:16","modified_gmt":"2025-12-15T01:44:16","slug":"the-trichotomy-of-primordial-black-holes-initial-conditions","status":"publish","type":"seminar","link":"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/seminar\/3459\/","title":{"rendered":"The trichotomy of Primordial Black Holes initial conditions"},"content":{"rendered":"<p>In this talk, I will show that the formation of primordial black holes, in an asymptotically flat and radiation dominated Friedman-Robertson-Walker (FRW) Universe, is not mainly determined by the behaviour of the smoothed linear over-density at its maximum, as earlier thought, but also by the three-dimensional curvature at smaller (but super-horizon) scales, which is called \u201cthe core\u201d.<br \/>\nI will present three classes of initial condition characterised by an open, closed or flat FRW core. I will motivate the use of the three-dimensional curvature as the key parameter to determine the threshold of PBH formation.<\/p>\n<hr>\n<p>\u672c\u30bb\u30df\u30ca\u30fc\u3067\u306f\u3001\u6f38\u8fd1\u7684\u306b\u5e73\u5766\u3067\u653e\u5c04\u512a\u52e2\u306e\u30d5\u30ea\u30fc\u30c9\u30de\u30f3\uff1d\u30ed\u30d0\u30fc\u30c8\u30bd\u30f3\uff1d\u30a6\u30a9\u30fc\u30ab\u30fc\uff08FRW\uff09\u5b87\u5b99\u306b\u304a\u3051\u308b\u539f\u59cb\u30d6\u30e9\u30c3\u30af\u30db\u30fc\u30eb\uff08PBH\uff09\u306e\u5f62\u6210\u304c\u3001\u3053\u308c\u307e\u3067\u8003\u3048\u3089\u308c\u3066\u3044\u305f\u3088\u3046\u306b\u5e73\u6ed1\u5316\u3055\u308c\u305f\u7dda\u5f62\u904e\u5bc6\u5ea6\u306e\u6700\u5927\u5024\u306e\u6319\u52d5\u3060\u3051\u3067\u6c7a\u307e\u308b\u306e\u3067\u306f\u306a\u304f\u3001\u3088\u308a\u5c0f\u3055\u3044\uff08\u305f\u3060\u3057\u8d85\u5730\u5e73\u7dda\uff09\u30b9\u30b1\u30fc\u30eb\u306b\u304a\u3051\u308b\u4e09\u6b21\u5143\u66f2\u7387\u3001\u3059\u306a\u308f\u3061\u300c\u30b3\u30a2\u300d\u306b\u3082\u4f9d\u5b58\u3059\u308b\u3053\u3068\u3092\u793a\u3057\u307e\u3059\u3002<br \/>\n\u305d\u3057\u3066\u3001\u958b\u3044\u305f\u30fb\u9589\u3058\u305f\u30fb\u5e73\u5766\u3068\u3044\u3046FRW\u30b3\u30a2\u306b\u3088\u3063\u3066\u7279\u5fb4\u3065\u3051\u3089\u308c\u308b3\u3064\u306e\u521d\u671f\u6761\u4ef6\u3092\u89e3\u8aac\u3057\u3001PBH\u5f62\u6210\u306e\u30b9\u30ec\u30c3\u30b7\u30e7\u30eb\u30c9\u3092\u6c7a\u5b9a\u3059\u308b\u305f\u3081\u306e\u4e3b\u8981\u306a\u30d1\u30e9\u30e1\u30fc\u30bf\u30fc\u3068\u3057\u3066\u4e09\u6b21\u5143\u66f2\u7387\u3092\u3082\u3061\u3044\u308b\u3053\u3068\u306e\u59a5\u5f53\u6027\u3092\u8aac\u660e\u3057\u307e\u3059\u3002<\/p>\n","protected":false},"featured_media":0,"template":"","tags":[],"seminar_category":[154],"acf":{"s_now_accepting":true,"s_date_order":"2025-12-16 10:30:00","s_date_end":"2025-12-16 11:30:00","s_date_text":"10:30 - 11:30","s_text":"Laia Montell\u00e0 Manuel (Universitat de Barcelona, ICCUB)","s_place":"ES635","s_place_other":"","s_categoryother":"","s_poster":"","s_poster2":"","s_slide":""},"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v23.5 - https:\/\/yoast.com\/wordpress\/plugins\/seo\/ -->\n<title>The trichotomy of Primordial Black Holes initial conditions - KMI - Nagoya University<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/seminar\/3459\/\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"The trichotomy of Primordial Black Holes initial conditions - KMI - Nagoya University\" \/>\n<meta property=\"og:description\" content=\"In this talk, I will show that the formation of primordial black holes, in an asymptotically flat and radiation dominated Friedman-Robertson-Walker (FRW) Universe, is not mainly determined by the behaviour of the smoothed linear over-density at its maximum, as earlier thought, but also by the three-dimensional curvature at smaller (but super-horizon) scales, which is called \u201cthe core\u201d. 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