{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:YL573PRPQQDCWUQAEB2RKL3D35","short_pith_number":"pith:YL573PRP","canonical_record":{"source":{"id":"1302.4898","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-02-20T13:16:45Z","cross_cats_sorted":["cond-mat.str-el","cond-mat.supr-con","gr-qc"],"title_canon_sha256":"2df9020a3efb7bd4561e65d820db82eb098568c274e03a89df9e51fa7c751309","abstract_canon_sha256":"63982fe4507bcb165c1ed32a72a7d8c8638e6eb29d612a8bb2995de2ed7e2771"},"schema_version":"1.0"},"canonical_sha256":"c2fbfdbe2f84062b52002075152f63df7e2e10b6429ac7b9e9479e87e6ea6b5f","source":{"kind":"arxiv","id":"1302.4898","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1302.4898","created_at":"2026-05-18T01:51:34Z"},{"alias_kind":"arxiv_version","alias_value":"1302.4898v2","created_at":"2026-05-18T01:51:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.4898","created_at":"2026-05-18T01:51:34Z"},{"alias_kind":"pith_short_12","alias_value":"YL573PRPQQDC","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_16","alias_value":"YL573PRPQQDCWUQA","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_8","alias_value":"YL573PRP","created_at":"2026-05-18T12:28:06Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:YL573PRPQQDCWUQAEB2RKL3D35","target":"record","payload":{"canonical_record":{"source":{"id":"1302.4898","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-02-20T13:16:45Z","cross_cats_sorted":["cond-mat.str-el","cond-mat.supr-con","gr-qc"],"title_canon_sha256":"2df9020a3efb7bd4561e65d820db82eb098568c274e03a89df9e51fa7c751309","abstract_canon_sha256":"63982fe4507bcb165c1ed32a72a7d8c8638e6eb29d612a8bb2995de2ed7e2771"},"schema_version":"1.0"},"canonical_sha256":"c2fbfdbe2f84062b52002075152f63df7e2e10b6429ac7b9e9479e87e6ea6b5f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:51:34.978875Z","signature_b64":"uqhYmxfFFMQIz2yGelgT5Rlh5Kas+0tjlk0s5rFVpnv645y1RXMKHxNxXEQVr5AW9D+7yaGiBQR4AZjtjjvnDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c2fbfdbe2f84062b52002075152f63df7e2e10b6429ac7b9e9479e87e6ea6b5f","last_reissued_at":"2026-05-18T01:51:34.978413Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:51:34.978413Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1302.4898","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:51:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zD3AwZX53FUPF7fI3FRLUuMiKXYaIa5LTefSa8jtWM6dnbObJnL9mCCRn89I368TCsZ2UCU6RPNtrqz4vk1XAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T10:18:18.846106Z"},"content_sha256":"df7afbbf91b90b47026915727346939a6841220f9f5eb9f00e42b749ae5fd6fe","schema_version":"1.0","event_id":"sha256:df7afbbf91b90b47026915727346939a6841220f9f5eb9f00e42b749ae5fd6fe"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:YL573PRPQQDCWUQAEB2RKL3D35","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Transitions in Dilaton Holography with Global or Local Symmetries","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","cond-mat.supr-con","gr-qc"],"primary_cat":"hep-th","authors_text":"Alberto Salvio","submitted_at":"2013-02-20T13:16:45Z","abstract_excerpt":"We study various transitions in dilaton holography, including those associated with the spontaneous breaking of a global (superfluid case) or local (superconductor case) U(1) symmetry in diverse dimensions d. By analyzing the thermodynamics of the dilaton-gravity system we find that scale invariance is broken at low temperatures, as shown by a nontrivial hyperscaling violation exponent in the infrared; increasing the temperature we recover scale symmetry in a d dependent way: while for d=2+1 a phase transition is found, for d=3+1 the transition is rather a crossover. This is the expected behav"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.4898","kind":"arxiv","version":2},"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":"2026-05-18T01:51:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"90ARUnf4BcMZoXCPHULfmKZpkX5VroPf3dvFSYGd/TAzstHji5CHjNxglftalE4p+X33gFOYHRkAea5BiLmcDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T10:18:18.846545Z"},"content_sha256":"d0760a159143fc469a2767edd69d0f8e033be1b74e66daf83f686fe5bcee64a0","schema_version":"1.0","event_id":"sha256:d0760a159143fc469a2767edd69d0f8e033be1b74e66daf83f686fe5bcee64a0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YL573PRPQQDCWUQAEB2RKL3D35/bundle.json","state_url":"https://pith.science/pith/YL573PRPQQDCWUQAEB2RKL3D35/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YL573PRPQQDCWUQAEB2RKL3D35/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":"2026-08-04T10:18:18Z","links":{"resolver":"https://pith.science/pith/YL573PRPQQDCWUQAEB2RKL3D35","bundle":"https://pith.science/pith/YL573PRPQQDCWUQAEB2RKL3D35/bundle.json","state":"https://pith.science/pith/YL573PRPQQDCWUQAEB2RKL3D35/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YL573PRPQQDCWUQAEB2RKL3D35/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:YL573PRPQQDCWUQAEB2RKL3D35","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":"63982fe4507bcb165c1ed32a72a7d8c8638e6eb29d612a8bb2995de2ed7e2771","cross_cats_sorted":["cond-mat.str-el","cond-mat.supr-con","gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-02-20T13:16:45Z","title_canon_sha256":"2df9020a3efb7bd4561e65d820db82eb098568c274e03a89df9e51fa7c751309"},"schema_version":"1.0","source":{"id":"1302.4898","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1302.4898","created_at":"2026-05-18T01:51:34Z"},{"alias_kind":"arxiv_version","alias_value":"1302.4898v2","created_at":"2026-05-18T01:51:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.4898","created_at":"2026-05-18T01:51:34Z"},{"alias_kind":"pith_short_12","alias_value":"YL573PRPQQDC","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_16","alias_value":"YL573PRPQQDCWUQA","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_8","alias_value":"YL573PRP","created_at":"2026-05-18T12:28:06Z"}],"graph_snapshots":[{"event_id":"sha256:d0760a159143fc469a2767edd69d0f8e033be1b74e66daf83f686fe5bcee64a0","target":"graph","created_at":"2026-05-18T01:51:34Z","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 various transitions in dilaton holography, including those associated with the spontaneous breaking of a global (superfluid case) or local (superconductor case) U(1) symmetry in diverse dimensions d. By analyzing the thermodynamics of the dilaton-gravity system we find that scale invariance is broken at low temperatures, as shown by a nontrivial hyperscaling violation exponent in the infrared; increasing the temperature we recover scale symmetry in a d dependent way: while for d=2+1 a phase transition is found, for d=3+1 the transition is rather a crossover. This is the expected behav","authors_text":"Alberto Salvio","cross_cats":["cond-mat.str-el","cond-mat.supr-con","gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-02-20T13:16:45Z","title":"Transitions in Dilaton Holography with Global or Local Symmetries"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.4898","kind":"arxiv","version":2},"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:df7afbbf91b90b47026915727346939a6841220f9f5eb9f00e42b749ae5fd6fe","target":"record","created_at":"2026-05-18T01:51:34Z","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":"63982fe4507bcb165c1ed32a72a7d8c8638e6eb29d612a8bb2995de2ed7e2771","cross_cats_sorted":["cond-mat.str-el","cond-mat.supr-con","gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-02-20T13:16:45Z","title_canon_sha256":"2df9020a3efb7bd4561e65d820db82eb098568c274e03a89df9e51fa7c751309"},"schema_version":"1.0","source":{"id":"1302.4898","kind":"arxiv","version":2}},"canonical_sha256":"c2fbfdbe2f84062b52002075152f63df7e2e10b6429ac7b9e9479e87e6ea6b5f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c2fbfdbe2f84062b52002075152f63df7e2e10b6429ac7b9e9479e87e6ea6b5f","first_computed_at":"2026-05-18T01:51:34.978413Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:51:34.978413Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"uqhYmxfFFMQIz2yGelgT5Rlh5Kas+0tjlk0s5rFVpnv645y1RXMKHxNxXEQVr5AW9D+7yaGiBQR4AZjtjjvnDA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:51:34.978875Z","signed_message":"canonical_sha256_bytes"},"source_id":"1302.4898","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:df7afbbf91b90b47026915727346939a6841220f9f5eb9f00e42b749ae5fd6fe","sha256:d0760a159143fc469a2767edd69d0f8e033be1b74e66daf83f686fe5bcee64a0"],"state_sha256":"bd96dcb748435620d4f0346c826423f83da3674428d095c97e624685b224c5e6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dxa+QKoJPlZtoMzIDOx3e+CmsYXAcXvVWeF6CnmYWSz2Mz7QWDeSbxJfftaRrFP6Ca69hEBZrJdbgCaNrOVJAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T10:18:18.886539Z","bundle_sha256":"05c0fe19e9a44aa674fa6d2d3069ffde8473c001b0208533bdd2a8755576093d"}}