{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:PCTI7MLUUY76AEDRIOPPYRLMS3","short_pith_number":"pith:PCTI7MLU","canonical_record":{"source":{"id":"1005.1776","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-05-11T09:32:24Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"da8538e5a0545706d52b39073fb8e527ec42f19ec65f6c529295f1ae02ca86d3","abstract_canon_sha256":"dd8cea0f7bf3964b34f6b76241d11389a76637b909a26f69c29b3f7c17d6de98"},"schema_version":"1.0"},"canonical_sha256":"78a68fb174a63fe01071439efc456c96dccc26075d6db70ff6f96ef9fdf72c60","source":{"kind":"arxiv","id":"1005.1776","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1005.1776","created_at":"2026-05-18T02:24:08Z"},{"alias_kind":"arxiv_version","alias_value":"1005.1776v2","created_at":"2026-05-18T02:24:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1005.1776","created_at":"2026-05-18T02:24:08Z"},{"alias_kind":"pith_short_12","alias_value":"PCTI7MLUUY76","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_16","alias_value":"PCTI7MLUUY76AEDR","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_8","alias_value":"PCTI7MLU","created_at":"2026-05-18T12:26:12Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:PCTI7MLUUY76AEDRIOPPYRLMS3","target":"record","payload":{"canonical_record":{"source":{"id":"1005.1776","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-05-11T09:32:24Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"da8538e5a0545706d52b39073fb8e527ec42f19ec65f6c529295f1ae02ca86d3","abstract_canon_sha256":"dd8cea0f7bf3964b34f6b76241d11389a76637b909a26f69c29b3f7c17d6de98"},"schema_version":"1.0"},"canonical_sha256":"78a68fb174a63fe01071439efc456c96dccc26075d6db70ff6f96ef9fdf72c60","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:24:08.462267Z","signature_b64":"Y505Dl0/ijosRV2jyyMPDYbwZHK9JJrVHAqNLsEo1JuAwMnvxpMfzyZsk3lMYxwQXQ6ukBFwtCF7aVYUK7nkCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"78a68fb174a63fe01071439efc456c96dccc26075d6db70ff6f96ef9fdf72c60","last_reissued_at":"2026-05-18T02:24:08.461748Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:24:08.461748Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1005.1776","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":"2026-05-18T02:24:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"p3IEy0awNjHzV/wcVfnEfubdTxrWun6l6kxSPx5U+Iz+KLPQYkjgUCKaJTjRHohrWUURcin5aUYOLA7Y0Xq5Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T12:12:35.880934Z"},"content_sha256":"feab18f84d748d24ff1171981610b8f8ef45b93ddf69c4d4ea0bf72b94dd0015","schema_version":"1.0","event_id":"sha256:feab18f84d748d24ff1171981610b8f8ef45b93ddf69c4d4ea0bf72b94dd0015"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:PCTI7MLUUY76AEDRIOPPYRLMS3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Emergent Gauge Fields in Holographic Superconductors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"hep-th","authors_text":"Alberto Salvio, Alex Pomarol, Marc Montull, Oriol Dom\\`enech, Pedro J. Silva","submitted_at":"2010-05-11T09:32:24Z","abstract_excerpt":"Holographic superconductors have been studied so far in the absence of dynamical electromagnetic fields, namely in the limit in which they coincide with holographic superfluids. It is possible, however, to introduce dynamical gauge fields if a Neumann-type boundary condition is imposed on the AdS-boundary. In 3+1 dimensions, the dual theory is a 2+1 dimensional CFT whose spectrum contains a massless gauge field, signaling the emergence of a gauge symmetry. We study the impact of a dynamical gauge field in vortex configurations where it is known to significantly affect the energetics and phase "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1005.1776","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":"2026-05-18T02:24:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"okdpWPfxqM9c8PKm26L2Zap2MrAW92gkbMGkSHjuFCS6pM0lLu6a6wa4SnEwiPjq7XOvpBwABs+62mlEZQ4gAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T12:12:35.881643Z"},"content_sha256":"bae6a33f44052cffba52d38f7db354dd7a85575003d5966dcfc776e8384e55a1","schema_version":"1.0","event_id":"sha256:bae6a33f44052cffba52d38f7db354dd7a85575003d5966dcfc776e8384e55a1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PCTI7MLUUY76AEDRIOPPYRLMS3/bundle.json","state_url":"https://pith.science/pith/PCTI7MLUUY76AEDRIOPPYRLMS3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PCTI7MLUUY76AEDRIOPPYRLMS3/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":"2026-05-31T12:12:35Z","links":{"resolver":"https://pith.science/pith/PCTI7MLUUY76AEDRIOPPYRLMS3","bundle":"https://pith.science/pith/PCTI7MLUUY76AEDRIOPPYRLMS3/bundle.json","state":"https://pith.science/pith/PCTI7MLUUY76AEDRIOPPYRLMS3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PCTI7MLUUY76AEDRIOPPYRLMS3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:PCTI7MLUUY76AEDRIOPPYRLMS3","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":"dd8cea0f7bf3964b34f6b76241d11389a76637b909a26f69c29b3f7c17d6de98","cross_cats_sorted":["cond-mat.supr-con"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-05-11T09:32:24Z","title_canon_sha256":"da8538e5a0545706d52b39073fb8e527ec42f19ec65f6c529295f1ae02ca86d3"},"schema_version":"1.0","source":{"id":"1005.1776","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1005.1776","created_at":"2026-05-18T02:24:08Z"},{"alias_kind":"arxiv_version","alias_value":"1005.1776v2","created_at":"2026-05-18T02:24:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1005.1776","created_at":"2026-05-18T02:24:08Z"},{"alias_kind":"pith_short_12","alias_value":"PCTI7MLUUY76","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_16","alias_value":"PCTI7MLUUY76AEDR","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_8","alias_value":"PCTI7MLU","created_at":"2026-05-18T12:26:12Z"}],"graph_snapshots":[{"event_id":"sha256:bae6a33f44052cffba52d38f7db354dd7a85575003d5966dcfc776e8384e55a1","target":"graph","created_at":"2026-05-18T02:24:08Z","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":"Holographic superconductors have been studied so far in the absence of dynamical electromagnetic fields, namely in the limit in which they coincide with holographic superfluids. It is possible, however, to introduce dynamical gauge fields if a Neumann-type boundary condition is imposed on the AdS-boundary. In 3+1 dimensions, the dual theory is a 2+1 dimensional CFT whose spectrum contains a massless gauge field, signaling the emergence of a gauge symmetry. We study the impact of a dynamical gauge field in vortex configurations where it is known to significantly affect the energetics and phase ","authors_text":"Alberto Salvio, Alex Pomarol, Marc Montull, Oriol Dom\\`enech, Pedro J. Silva","cross_cats":["cond-mat.supr-con"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-05-11T09:32:24Z","title":"Emergent Gauge Fields in Holographic Superconductors"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1005.1776","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:feab18f84d748d24ff1171981610b8f8ef45b93ddf69c4d4ea0bf72b94dd0015","target":"record","created_at":"2026-05-18T02:24:08Z","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":"dd8cea0f7bf3964b34f6b76241d11389a76637b909a26f69c29b3f7c17d6de98","cross_cats_sorted":["cond-mat.supr-con"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-05-11T09:32:24Z","title_canon_sha256":"da8538e5a0545706d52b39073fb8e527ec42f19ec65f6c529295f1ae02ca86d3"},"schema_version":"1.0","source":{"id":"1005.1776","kind":"arxiv","version":2}},"canonical_sha256":"78a68fb174a63fe01071439efc456c96dccc26075d6db70ff6f96ef9fdf72c60","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"78a68fb174a63fe01071439efc456c96dccc26075d6db70ff6f96ef9fdf72c60","first_computed_at":"2026-05-18T02:24:08.461748Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:24:08.461748Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Y505Dl0/ijosRV2jyyMPDYbwZHK9JJrVHAqNLsEo1JuAwMnvxpMfzyZsk3lMYxwQXQ6ukBFwtCF7aVYUK7nkCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:24:08.462267Z","signed_message":"canonical_sha256_bytes"},"source_id":"1005.1776","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:feab18f84d748d24ff1171981610b8f8ef45b93ddf69c4d4ea0bf72b94dd0015","sha256:bae6a33f44052cffba52d38f7db354dd7a85575003d5966dcfc776e8384e55a1"],"state_sha256":"3f60635d8251400cefd3acdd455d7660769f08552598c173a533ac3df966b695"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iiJVXmonoQovgOcFiCfJQsAGTT1Fz8SZTH4Xb21gnKg4ec/edPXgIE1sLmjZmi3CegKqxAana+fs0vRpI59rAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T12:12:35.885082Z","bundle_sha256":"3efaeb5f1661a2bdc68a517e07428bb7e09eee39521224b4b503fb39a09ae1b9"}}