{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:3CF2SXZVHEPKSFIYLVTOWET3ZA","short_pith_number":"pith:3CF2SXZV","canonical_record":{"source":{"id":"1312.6270","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-21T16:21:41Z","cross_cats_sorted":[],"title_canon_sha256":"c072f8effeae57e00c3544bd0be41e513a36d9eea77f6cd0da7680452494a02d","abstract_canon_sha256":"a211acf22f2183aa7b6a0e733123b996d27db8a4e1d2d929ecac6ac492a93336"},"schema_version":"1.0"},"canonical_sha256":"d88ba95f35391ea915185d66eb127bc815b1ba9e70a39e7a1dc32b3140c2c9f4","source":{"kind":"arxiv","id":"1312.6270","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.6270","created_at":"2026-05-18T01:45:42Z"},{"alias_kind":"arxiv_version","alias_value":"1312.6270v1","created_at":"2026-05-18T01:45:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.6270","created_at":"2026-05-18T01:45:42Z"},{"alias_kind":"pith_short_12","alias_value":"3CF2SXZVHEPK","created_at":"2026-05-18T12:27:32Z"},{"alias_kind":"pith_short_16","alias_value":"3CF2SXZVHEPKSFIY","created_at":"2026-05-18T12:27:32Z"},{"alias_kind":"pith_short_8","alias_value":"3CF2SXZV","created_at":"2026-05-18T12:27:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:3CF2SXZVHEPKSFIYLVTOWET3ZA","target":"record","payload":{"canonical_record":{"source":{"id":"1312.6270","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-21T16:21:41Z","cross_cats_sorted":[],"title_canon_sha256":"c072f8effeae57e00c3544bd0be41e513a36d9eea77f6cd0da7680452494a02d","abstract_canon_sha256":"a211acf22f2183aa7b6a0e733123b996d27db8a4e1d2d929ecac6ac492a93336"},"schema_version":"1.0"},"canonical_sha256":"d88ba95f35391ea915185d66eb127bc815b1ba9e70a39e7a1dc32b3140c2c9f4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:45:42.892264Z","signature_b64":"n/JNVkpORXsNyqV3KaOPaU4kHgjmsphUJhb8mtaeqY4/H8JCeRKzb+/0nZZytGdJdHBrUFG0Vlk41Vixrm5JDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d88ba95f35391ea915185d66eb127bc815b1ba9e70a39e7a1dc32b3140c2c9f4","last_reissued_at":"2026-05-18T01:45:42.891700Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:45:42.891700Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1312.6270","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":"2026-05-18T01:45:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0XqmfJ5CdhNkZzVc6zjQO2uKZ9O7CLwW8YuDtHBkDdFGs4WLnEP5cUtqt3Dr3KUEUeHO900fT3kaAMKdXEwXBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T21:03:15.181170Z"},"content_sha256":"2259dac1fcd5938a984b5e7fd283cec1a88bd5a5619d945fcb19ba5cac76bae0","schema_version":"1.0","event_id":"sha256:2259dac1fcd5938a984b5e7fd283cec1a88bd5a5619d945fcb19ba5cac76bae0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:3CF2SXZVHEPKSFIYLVTOWET3ZA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Deconfinement phase transition in the Hamiltonian approach to Yang-Mills theory in Coulomb gauge","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Davide R. Campagnari, Hugo Reinhardt, Jan Heffner","submitted_at":"2013-12-21T16:21:41Z","abstract_excerpt":"Recent results obtained for the deconfinement phase transition within the Hamiltonian approach to Yang-Mills theory are reviewed. Assuming a quasiparticle picture for the grand canonical gluon ensemble the thermal equilibrium state is found by minimizing the free energy with respect to the quasi-gluon energy. The deconfinement phase transition is accompanied by a drastic change of the infrared exponents of the ghost and gluon propagators. Above the phase transition the ghost form factor remains infrared divergent but its infrared exponent is approximately halved. The gluon energy being infrare"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.6270","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":"2026-05-18T01:45:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tmSFFXGZURi1YJZtj5Qks52Z8PZDCUi9ELRoedNrJON/HTL7yqQ14wKoF5ESwF3qb6tAv+s0dFcHZBPaTM6vBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T21:03:15.181800Z"},"content_sha256":"d86b8a78364991a2e30e2aa108dcf851349e6e2873e9f05d90fbe88e5f3599f5","schema_version":"1.0","event_id":"sha256:d86b8a78364991a2e30e2aa108dcf851349e6e2873e9f05d90fbe88e5f3599f5"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3CF2SXZVHEPKSFIYLVTOWET3ZA/bundle.json","state_url":"https://pith.science/pith/3CF2SXZVHEPKSFIYLVTOWET3ZA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3CF2SXZVHEPKSFIYLVTOWET3ZA/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":"2026-05-26T21:03:15Z","links":{"resolver":"https://pith.science/pith/3CF2SXZVHEPKSFIYLVTOWET3ZA","bundle":"https://pith.science/pith/3CF2SXZVHEPKSFIYLVTOWET3ZA/bundle.json","state":"https://pith.science/pith/3CF2SXZVHEPKSFIYLVTOWET3ZA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3CF2SXZVHEPKSFIYLVTOWET3ZA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:3CF2SXZVHEPKSFIYLVTOWET3ZA","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":"a211acf22f2183aa7b6a0e733123b996d27db8a4e1d2d929ecac6ac492a93336","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-21T16:21:41Z","title_canon_sha256":"c072f8effeae57e00c3544bd0be41e513a36d9eea77f6cd0da7680452494a02d"},"schema_version":"1.0","source":{"id":"1312.6270","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.6270","created_at":"2026-05-18T01:45:42Z"},{"alias_kind":"arxiv_version","alias_value":"1312.6270v1","created_at":"2026-05-18T01:45:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.6270","created_at":"2026-05-18T01:45:42Z"},{"alias_kind":"pith_short_12","alias_value":"3CF2SXZVHEPK","created_at":"2026-05-18T12:27:32Z"},{"alias_kind":"pith_short_16","alias_value":"3CF2SXZVHEPKSFIY","created_at":"2026-05-18T12:27:32Z"},{"alias_kind":"pith_short_8","alias_value":"3CF2SXZV","created_at":"2026-05-18T12:27:32Z"}],"graph_snapshots":[{"event_id":"sha256:d86b8a78364991a2e30e2aa108dcf851349e6e2873e9f05d90fbe88e5f3599f5","target":"graph","created_at":"2026-05-18T01:45:42Z","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":"Recent results obtained for the deconfinement phase transition within the Hamiltonian approach to Yang-Mills theory are reviewed. Assuming a quasiparticle picture for the grand canonical gluon ensemble the thermal equilibrium state is found by minimizing the free energy with respect to the quasi-gluon energy. The deconfinement phase transition is accompanied by a drastic change of the infrared exponents of the ghost and gluon propagators. Above the phase transition the ghost form factor remains infrared divergent but its infrared exponent is approximately halved. The gluon energy being infrare","authors_text":"Davide R. Campagnari, Hugo Reinhardt, Jan Heffner","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-21T16:21:41Z","title":"Deconfinement phase transition in the Hamiltonian approach to Yang-Mills theory in Coulomb gauge"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.6270","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":"sha256:2259dac1fcd5938a984b5e7fd283cec1a88bd5a5619d945fcb19ba5cac76bae0","target":"record","created_at":"2026-05-18T01:45:42Z","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":"a211acf22f2183aa7b6a0e733123b996d27db8a4e1d2d929ecac6ac492a93336","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-21T16:21:41Z","title_canon_sha256":"c072f8effeae57e00c3544bd0be41e513a36d9eea77f6cd0da7680452494a02d"},"schema_version":"1.0","source":{"id":"1312.6270","kind":"arxiv","version":1}},"canonical_sha256":"d88ba95f35391ea915185d66eb127bc815b1ba9e70a39e7a1dc32b3140c2c9f4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d88ba95f35391ea915185d66eb127bc815b1ba9e70a39e7a1dc32b3140c2c9f4","first_computed_at":"2026-05-18T01:45:42.891700Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:45:42.891700Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"n/JNVkpORXsNyqV3KaOPaU4kHgjmsphUJhb8mtaeqY4/H8JCeRKzb+/0nZZytGdJdHBrUFG0Vlk41Vixrm5JDA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:45:42.892264Z","signed_message":"canonical_sha256_bytes"},"source_id":"1312.6270","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2259dac1fcd5938a984b5e7fd283cec1a88bd5a5619d945fcb19ba5cac76bae0","sha256:d86b8a78364991a2e30e2aa108dcf851349e6e2873e9f05d90fbe88e5f3599f5"],"state_sha256":"fefb7bdc3bd53a856507c16b7af30ae11f11777fdf16149625cb763112b7c135"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vHeUwsMlr3ol5H7tglCa1fn2YQIPOsuJ6gtanAWz1vjzRwNz1EF05ZwOGdsDLgJl6sbSd9XqX5F7JvH3V2HcBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T21:03:15.185255Z","bundle_sha256":"eb5f92026981eb990f8a7ac8f003983750053c34d8f9aab96d22b58e6fe0a45f"}}