{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:4IFPDMLSFW5EU7ZP25IOAVR6KS","short_pith_number":"pith:4IFPDMLS","canonical_record":{"source":{"id":"1506.04895","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-06-16T09:50:44Z","cross_cats_sorted":["cond-mat.quant-gas"],"title_canon_sha256":"062ffa3e2e484f942a223e30259697df0593b20258a0069a649d165fa5fc8867","abstract_canon_sha256":"f09700c6002f3c71b621866ca6525b3ae3a3148110326f06cf84649d04bb8b9d"},"schema_version":"1.0"},"canonical_sha256":"e20af1b1722dba4a7f2fd750e0563e54b67712f2213974973dfdd5f9f689dfbb","source":{"kind":"arxiv","id":"1506.04895","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1506.04895","created_at":"2026-05-18T01:28:54Z"},{"alias_kind":"arxiv_version","alias_value":"1506.04895v1","created_at":"2026-05-18T01:28:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1506.04895","created_at":"2026-05-18T01:28:54Z"},{"alias_kind":"pith_short_12","alias_value":"4IFPDMLSFW5E","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_16","alias_value":"4IFPDMLSFW5EU7ZP","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_8","alias_value":"4IFPDMLS","created_at":"2026-05-18T12:29:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:4IFPDMLSFW5EU7ZP25IOAVR6KS","target":"record","payload":{"canonical_record":{"source":{"id":"1506.04895","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-06-16T09:50:44Z","cross_cats_sorted":["cond-mat.quant-gas"],"title_canon_sha256":"062ffa3e2e484f942a223e30259697df0593b20258a0069a649d165fa5fc8867","abstract_canon_sha256":"f09700c6002f3c71b621866ca6525b3ae3a3148110326f06cf84649d04bb8b9d"},"schema_version":"1.0"},"canonical_sha256":"e20af1b1722dba4a7f2fd750e0563e54b67712f2213974973dfdd5f9f689dfbb","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:28:54.991729Z","signature_b64":"xjS8w5yn8yp1SUxSQ6BSI/IBcFpzzNLuGnEf+qRBhCllynG+sycoCh+SmIPXJOz9BShnwDqqCnq23ge/uPmsCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e20af1b1722dba4a7f2fd750e0563e54b67712f2213974973dfdd5f9f689dfbb","last_reissued_at":"2026-05-18T01:28:54.991045Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:28:54.991045Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1506.04895","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:28:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vvC0F8ow6Y6UWwuCCEh5DV6uisKh8KB9T+JLfiOuWn65mRMnHK9DO7nVTFddAvlf26DpNYbceiWYqRNKuyJGAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T17:19:15.696633Z"},"content_sha256":"802a8376d2cd7abd5ff9f395e916784c9155d17655ac6b56d42ee31227f69c5c","schema_version":"1.0","event_id":"sha256:802a8376d2cd7abd5ff9f395e916784c9155d17655ac6b56d42ee31227f69c5c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:4IFPDMLSFW5EU7ZP25IOAVR6KS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Bose-Einstein condensation and critical behavior of two-component bosonic gases","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas"],"primary_cat":"cond-mat.stat-mech","authors_text":"Andrea Pelissetto, Ettore Vicari, Giacomo Ceccarelli, Jacopo Nespolo","submitted_at":"2015-06-16T09:50:44Z","abstract_excerpt":"We study Bose-Einstein condensation (BEC) in three-dimensional two-component bosonic gases, characterizing the universal behaviors of the critical modes arising at the BEC transitions. For this purpose, we use field-theoretical (FT) renormalization-group (RG) methods and perform mean-field and numerical calculations. The FT RG analysis is based on the Landau-Ginzburg-Wilson Phi4 theory with two complex scalar fields which has the same symmetry as the bosonic system. In particular, for identical bosons with exchange Z_2,e symmetry, coupled by effective density-density interactions, the global s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1506.04895","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:28:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UkEPw5Dsx/bBA1+YnC3TJnkr1OSeYxO6YTc0nWByTu5m65X0J8my3NRdUfE5ggBG62iP51NlMrLmGa3HI0blCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T17:19:15.697292Z"},"content_sha256":"f30ff5bf295d135f961287801563fc3ef0d7381908e52643d28104dbfa41bdf3","schema_version":"1.0","event_id":"sha256:f30ff5bf295d135f961287801563fc3ef0d7381908e52643d28104dbfa41bdf3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4IFPDMLSFW5EU7ZP25IOAVR6KS/bundle.json","state_url":"https://pith.science/pith/4IFPDMLSFW5EU7ZP25IOAVR6KS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4IFPDMLSFW5EU7ZP25IOAVR6KS/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-27T17:19:15Z","links":{"resolver":"https://pith.science/pith/4IFPDMLSFW5EU7ZP25IOAVR6KS","bundle":"https://pith.science/pith/4IFPDMLSFW5EU7ZP25IOAVR6KS/bundle.json","state":"https://pith.science/pith/4IFPDMLSFW5EU7ZP25IOAVR6KS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4IFPDMLSFW5EU7ZP25IOAVR6KS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:4IFPDMLSFW5EU7ZP25IOAVR6KS","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"f09700c6002f3c71b621866ca6525b3ae3a3148110326f06cf84649d04bb8b9d","cross_cats_sorted":["cond-mat.quant-gas"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-06-16T09:50:44Z","title_canon_sha256":"062ffa3e2e484f942a223e30259697df0593b20258a0069a649d165fa5fc8867"},"schema_version":"1.0","source":{"id":"1506.04895","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1506.04895","created_at":"2026-05-18T01:28:54Z"},{"alias_kind":"arxiv_version","alias_value":"1506.04895v1","created_at":"2026-05-18T01:28:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1506.04895","created_at":"2026-05-18T01:28:54Z"},{"alias_kind":"pith_short_12","alias_value":"4IFPDMLSFW5E","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_16","alias_value":"4IFPDMLSFW5EU7ZP","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_8","alias_value":"4IFPDMLS","created_at":"2026-05-18T12:29:05Z"}],"graph_snapshots":[{"event_id":"sha256:f30ff5bf295d135f961287801563fc3ef0d7381908e52643d28104dbfa41bdf3","target":"graph","created_at":"2026-05-18T01:28:54Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We study Bose-Einstein condensation (BEC) in three-dimensional two-component bosonic gases, characterizing the universal behaviors of the critical modes arising at the BEC transitions. For this purpose, we use field-theoretical (FT) renormalization-group (RG) methods and perform mean-field and numerical calculations. The FT RG analysis is based on the Landau-Ginzburg-Wilson Phi4 theory with two complex scalar fields which has the same symmetry as the bosonic system. In particular, for identical bosons with exchange Z_2,e symmetry, coupled by effective density-density interactions, the global s","authors_text":"Andrea Pelissetto, Ettore Vicari, Giacomo Ceccarelli, Jacopo Nespolo","cross_cats":["cond-mat.quant-gas"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-06-16T09:50:44Z","title":"Bose-Einstein condensation and critical behavior of two-component bosonic gases"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1506.04895","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:802a8376d2cd7abd5ff9f395e916784c9155d17655ac6b56d42ee31227f69c5c","target":"record","created_at":"2026-05-18T01:28:54Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"f09700c6002f3c71b621866ca6525b3ae3a3148110326f06cf84649d04bb8b9d","cross_cats_sorted":["cond-mat.quant-gas"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-06-16T09:50:44Z","title_canon_sha256":"062ffa3e2e484f942a223e30259697df0593b20258a0069a649d165fa5fc8867"},"schema_version":"1.0","source":{"id":"1506.04895","kind":"arxiv","version":1}},"canonical_sha256":"e20af1b1722dba4a7f2fd750e0563e54b67712f2213974973dfdd5f9f689dfbb","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e20af1b1722dba4a7f2fd750e0563e54b67712f2213974973dfdd5f9f689dfbb","first_computed_at":"2026-05-18T01:28:54.991045Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:28:54.991045Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xjS8w5yn8yp1SUxSQ6BSI/IBcFpzzNLuGnEf+qRBhCllynG+sycoCh+SmIPXJOz9BShnwDqqCnq23ge/uPmsCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:28:54.991729Z","signed_message":"canonical_sha256_bytes"},"source_id":"1506.04895","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:802a8376d2cd7abd5ff9f395e916784c9155d17655ac6b56d42ee31227f69c5c","sha256:f30ff5bf295d135f961287801563fc3ef0d7381908e52643d28104dbfa41bdf3"],"state_sha256":"a0d8217bd505add63874c23ee56557d9b4d922f183f4ce48fd9bfbe2c556587f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WDSy+8MLn5wjdoEUNvTqwuPWn9/mHp1TH0oYUza9wjMCuefvUJR8255ZwMh88f3RTAuaym6SZMwi5smUFtgUAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T17:19:15.700939Z","bundle_sha256":"e5314106f870d3865674c947b533ff7e6640e885cfb0f43b76d0800cd2cbd526"}}