{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:Z2S3AQYRHLDFO2JZIJNMSXARTJ","short_pith_number":"pith:Z2S3AQYR","schema_version":"1.0","canonical_sha256":"cea5b043113ac6576939425ac95c119a42e8ae62358a226c14a4f5fcd559c383","source":{"kind":"arxiv","id":"1411.1744","version":2},"attestation_state":"computed","paper":{"title":"Weak Field Collapse in AdS: Introducing a Charge Density","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","gr-qc","nucl-th"],"primary_cat":"hep-th","authors_text":"Arnab Kundu, Di-Lun Yang, Elena Caceres, Juan F. Pedraza","submitted_at":"2014-11-06T20:54:27Z","abstract_excerpt":"We study the effect of a non-vanishing chemical potential on the thermalization time of a strongly coupled large $N_c$ gauge theory in $(2+1)$-dimensions, using a specific bottom-up gravity model in asymptotically AdS space. We first construct a perturbative solution to the gravity-equations, which dynamically interpolates between two AdS black hole backgrounds with different temperatures and chemical potentials, in a perturbative expansion of a bulk neutral scalar field. In the dual field theory, this corresponds to a quench dynamics by a marginal operator, where the corresponding coupling se"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1411.1744","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-11-06T20:54:27Z","cross_cats_sorted":["cond-mat.str-el","gr-qc","nucl-th"],"title_canon_sha256":"7d301ab4f07914e48a7c847c0c345957157fd798a42c87ab9cd34375824da35d","abstract_canon_sha256":"52884c5e3815c7827b0dba356ebd99f328e83b332c2e05976cfa5935d6ec8e72"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:05:09.879798Z","signature_b64":"A5iasT/ca7U9FdF14px/xN0jQFaQ6co6/NbbvVm3+2VOLtwoMY9Okki+aUbDv+30S0uXTaR6zGJlvGIYLNujBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cea5b043113ac6576939425ac95c119a42e8ae62358a226c14a4f5fcd559c383","last_reissued_at":"2026-05-18T00:05:09.879362Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:05:09.879362Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Weak Field Collapse in AdS: Introducing a Charge Density","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","gr-qc","nucl-th"],"primary_cat":"hep-th","authors_text":"Arnab Kundu, Di-Lun Yang, Elena Caceres, Juan F. Pedraza","submitted_at":"2014-11-06T20:54:27Z","abstract_excerpt":"We study the effect of a non-vanishing chemical potential on the thermalization time of a strongly coupled large $N_c$ gauge theory in $(2+1)$-dimensions, using a specific bottom-up gravity model in asymptotically AdS space. We first construct a perturbative solution to the gravity-equations, which dynamically interpolates between two AdS black hole backgrounds with different temperatures and chemical potentials, in a perturbative expansion of a bulk neutral scalar field. In the dual field theory, this corresponds to a quench dynamics by a marginal operator, where the corresponding coupling se"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.1744","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1411.1744","created_at":"2026-05-18T00:05:09.879435+00:00"},{"alias_kind":"arxiv_version","alias_value":"1411.1744v2","created_at":"2026-05-18T00:05:09.879435+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.1744","created_at":"2026-05-18T00:05:09.879435+00:00"},{"alias_kind":"pith_short_12","alias_value":"Z2S3AQYRHLDF","created_at":"2026-05-18T12:28:59.999130+00:00"},{"alias_kind":"pith_short_16","alias_value":"Z2S3AQYRHLDFO2JZ","created_at":"2026-05-18T12:28:59.999130+00:00"},{"alias_kind":"pith_short_8","alias_value":"Z2S3AQYR","created_at":"2026-05-18T12:28:59.999130+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Z2S3AQYRHLDFO2JZIJNMSXARTJ","json":"https://pith.science/pith/Z2S3AQYRHLDFO2JZIJNMSXARTJ.json","graph_json":"https://pith.science/api/pith-number/Z2S3AQYRHLDFO2JZIJNMSXARTJ/graph.json","events_json":"https://pith.science/api/pith-number/Z2S3AQYRHLDFO2JZIJNMSXARTJ/events.json","paper":"https://pith.science/paper/Z2S3AQYR"},"agent_actions":{"view_html":"https://pith.science/pith/Z2S3AQYRHLDFO2JZIJNMSXARTJ","download_json":"https://pith.science/pith/Z2S3AQYRHLDFO2JZIJNMSXARTJ.json","view_paper":"https://pith.science/paper/Z2S3AQYR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1411.1744&json=true","fetch_graph":"https://pith.science/api/pith-number/Z2S3AQYRHLDFO2JZIJNMSXARTJ/graph.json","fetch_events":"https://pith.science/api/pith-number/Z2S3AQYRHLDFO2JZIJNMSXARTJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Z2S3AQYRHLDFO2JZIJNMSXARTJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Z2S3AQYRHLDFO2JZIJNMSXARTJ/action/storage_attestation","attest_author":"https://pith.science/pith/Z2S3AQYRHLDFO2JZIJNMSXARTJ/action/author_attestation","sign_citation":"https://pith.science/pith/Z2S3AQYRHLDFO2JZIJNMSXARTJ/action/citation_signature","submit_replication":"https://pith.science/pith/Z2S3AQYRHLDFO2JZIJNMSXARTJ/action/replication_record"}},"created_at":"2026-05-18T00:05:09.879435+00:00","updated_at":"2026-05-18T00:05:09.879435+00:00"}