{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:LZIX3TARIRRP3J4JIMEL2M52LJ","short_pith_number":"pith:LZIX3TAR","schema_version":"1.0","canonical_sha256":"5e517dcc114462fda7894308bd33ba5a5ef3263386c939c094ae3949fd72afba","source":{"kind":"arxiv","id":"2507.23108","version":1},"attestation_state":"computed","paper":{"title":"Quantification of the energy consumption of entanglement distribution","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Karol Horodecki, Leonard Sikorski, Marek Winczewski, Miko{\\l}aj Czechlewski, Pawe{\\l} Mazurek, Raja Yehia","submitted_at":"2025-07-30T21:21:19Z","abstract_excerpt":"Inspired by environmental sciences, we develop a framework to quantify the energy needed to generate quantum entanglement via noisy quantum channels, focusing on the hardware-independent, i.e. fundamental cost. Within this framework, we define a measure of the minimal fundamental energy consumption rate per distributed entanglement (expressed in Joule per ebit). We then derive a lower bound on the energy cost of distributing a maximally entangled state via a quantum channel, which yields a quantitative estimate of energy investment per entangled bit for future quantum networks. We thereby show"},"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":"2507.23108","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2025-07-30T21:21:19Z","cross_cats_sorted":[],"title_canon_sha256":"e5fcef31bd0a281f72bf529f3c24eef978c76965bb208fabb4f7f2f727f2e2b1","abstract_canon_sha256":"fef376b36864448cfd4b690b3cc0db3b03259e5a58e97d27cde804c997772e3e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:46:05.597662Z","signature_b64":"cA9nzsQeqoH7w7XCRSlVc+j/V+AP040V6DW05cp515uBnYTg50ocux99g0vLNwBd5aPpAMqsIewqOKRp5TEdCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5e517dcc114462fda7894308bd33ba5a5ef3263386c939c094ae3949fd72afba","last_reissued_at":"2026-07-05T11:46:05.597070Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:46:05.597070Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantification of the energy consumption of entanglement distribution","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Karol Horodecki, Leonard Sikorski, Marek Winczewski, Miko{\\l}aj Czechlewski, Pawe{\\l} Mazurek, Raja Yehia","submitted_at":"2025-07-30T21:21:19Z","abstract_excerpt":"Inspired by environmental sciences, we develop a framework to quantify the energy needed to generate quantum entanglement via noisy quantum channels, focusing on the hardware-independent, i.e. fundamental cost. Within this framework, we define a measure of the minimal fundamental energy consumption rate per distributed entanglement (expressed in Joule per ebit). We then derive a lower bound on the energy cost of distributing a maximally entangled state via a quantum channel, which yields a quantitative estimate of energy investment per entangled bit for future quantum networks. We thereby show"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2507.23108","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2507.23108/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2507.23108","created_at":"2026-07-05T11:46:05.597131+00:00"},{"alias_kind":"arxiv_version","alias_value":"2507.23108v1","created_at":"2026-07-05T11:46:05.597131+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2507.23108","created_at":"2026-07-05T11:46:05.597131+00:00"},{"alias_kind":"pith_short_12","alias_value":"LZIX3TARIRRP","created_at":"2026-07-05T11:46:05.597131+00:00"},{"alias_kind":"pith_short_16","alias_value":"LZIX3TARIRRP3J4J","created_at":"2026-07-05T11:46:05.597131+00:00"},{"alias_kind":"pith_short_8","alias_value":"LZIX3TAR","created_at":"2026-07-05T11:46:05.597131+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2511.05458","citing_title":"Trade-off between complexity and energy in quantum phase estimation","ref_index":98,"is_internal_anchor":false},{"citing_arxiv_id":"2603.16225","citing_title":"An Energetic Constraint for Qubit-Qubit Entanglement","ref_index":18,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LZIX3TARIRRP3J4JIMEL2M52LJ","json":"https://pith.science/pith/LZIX3TARIRRP3J4JIMEL2M52LJ.json","graph_json":"https://pith.science/api/pith-number/LZIX3TARIRRP3J4JIMEL2M52LJ/graph.json","events_json":"https://pith.science/api/pith-number/LZIX3TARIRRP3J4JIMEL2M52LJ/events.json","paper":"https://pith.science/paper/LZIX3TAR"},"agent_actions":{"view_html":"https://pith.science/pith/LZIX3TARIRRP3J4JIMEL2M52LJ","download_json":"https://pith.science/pith/LZIX3TARIRRP3J4JIMEL2M52LJ.json","view_paper":"https://pith.science/paper/LZIX3TAR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2507.23108&json=true","fetch_graph":"https://pith.science/api/pith-number/LZIX3TARIRRP3J4JIMEL2M52LJ/graph.json","fetch_events":"https://pith.science/api/pith-number/LZIX3TARIRRP3J4JIMEL2M52LJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LZIX3TARIRRP3J4JIMEL2M52LJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LZIX3TARIRRP3J4JIMEL2M52LJ/action/storage_attestation","attest_author":"https://pith.science/pith/LZIX3TARIRRP3J4JIMEL2M52LJ/action/author_attestation","sign_citation":"https://pith.science/pith/LZIX3TARIRRP3J4JIMEL2M52LJ/action/citation_signature","submit_replication":"https://pith.science/pith/LZIX3TARIRRP3J4JIMEL2M52LJ/action/replication_record"}},"created_at":"2026-07-05T11:46:05.597131+00:00","updated_at":"2026-07-05T11:46:05.597131+00:00"}