{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:DQ2TT6BFU42T6ACQHP5Z2GO56Q","short_pith_number":"pith:DQ2TT6BF","canonical_record":{"source":{"id":"1608.00183","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2016-07-31T03:58:27Z","cross_cats_sorted":[],"title_canon_sha256":"c8e813c7fe26e90ab74698bac42000ef435b2f4a6c905f63af3bc880d3e2a3e1","abstract_canon_sha256":"773a65c6dbbd79ed7f9f37ae30cba7868d7edd433e1f1e5731ad42982bf5eb30"},"schema_version":"1.0"},"canonical_sha256":"1c3539f825a7353f00503bfb9d19ddf42f49e9564f79a45b4c69cbc5c0413432","source":{"kind":"arxiv","id":"1608.00183","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.00183","created_at":"2026-05-18T00:53:24Z"},{"alias_kind":"arxiv_version","alias_value":"1608.00183v2","created_at":"2026-05-18T00:53:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.00183","created_at":"2026-05-18T00:53:24Z"},{"alias_kind":"pith_short_12","alias_value":"DQ2TT6BFU42T","created_at":"2026-05-18T12:30:12Z"},{"alias_kind":"pith_short_16","alias_value":"DQ2TT6BFU42T6ACQ","created_at":"2026-05-18T12:30:12Z"},{"alias_kind":"pith_short_8","alias_value":"DQ2TT6BF","created_at":"2026-05-18T12:30:12Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:DQ2TT6BFU42T6ACQHP5Z2GO56Q","target":"record","payload":{"canonical_record":{"source":{"id":"1608.00183","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2016-07-31T03:58:27Z","cross_cats_sorted":[],"title_canon_sha256":"c8e813c7fe26e90ab74698bac42000ef435b2f4a6c905f63af3bc880d3e2a3e1","abstract_canon_sha256":"773a65c6dbbd79ed7f9f37ae30cba7868d7edd433e1f1e5731ad42982bf5eb30"},"schema_version":"1.0"},"canonical_sha256":"1c3539f825a7353f00503bfb9d19ddf42f49e9564f79a45b4c69cbc5c0413432","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:53:24.330105Z","signature_b64":"aBXZy8BaPP/BmpLXSOwlWCB5SVBP7Ho7z97HebktkFLDstywu26HeeK2k7ag5wGrdojaEFbtamYhToB4mF+hBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1c3539f825a7353f00503bfb9d19ddf42f49e9564f79a45b4c69cbc5c0413432","last_reissued_at":"2026-05-18T00:53:24.329647Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:53:24.329647Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1608.00183","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":"2026-05-18T00:53:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZhOIxliVumoQ9R0rQYHj2oTtiQ0Q/UHcUGG3AwicaTaC2L88L8QebqYByEwMu6CQLAnu+QtxKG1bYcN3Ti9KBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T23:20:21.790076Z"},"content_sha256":"fc759c06178768026efc8b0c93514dee6c53335469597ae8c35f14b1cace8388","schema_version":"1.0","event_id":"sha256:fc759c06178768026efc8b0c93514dee6c53335469597ae8c35f14b1cace8388"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:DQ2TT6BFU42T6ACQHP5Z2GO56Q","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"High-momentum distribution with subleading $k^{-3}$ tail in the odd-wave interacting one-dimensional Fermi gases","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"Huifang Dong, Xiaoling Cui","submitted_at":"2016-07-31T03:58:27Z","abstract_excerpt":"We study the odd-wave interacting identical fermions in one-dimension with finite effective range. We show that to fully describe the high-momentum distribution $\\rho(k)$ up to $k^{-4}$, one needs four parameters characterizing the properties when two particles {\\it contact} with each other. Two parameters are related to the variation of energy with respect to the odd-wave scattering length and the effective range, respectively, determining the $k^{-2}$ tail and part of $k^{-4}$ tail in $\\rho(k)$. The other two parameters are related to the center-of-mass motion of the system, respectively det"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.00183","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":"2026-05-18T00:53:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JYYnMa0o68sIUI3YgglQIPfe8sb1Q629gbp8Uz2sBo/0r/h7ZxnGVECe7A3Ka/9qil600SBJqdkC4qDmscJuDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T23:20:21.790734Z"},"content_sha256":"03c8399c54378f2d4c9cceb144215a56dad88ba570ca04554364ff6f794893b2","schema_version":"1.0","event_id":"sha256:03c8399c54378f2d4c9cceb144215a56dad88ba570ca04554364ff6f794893b2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DQ2TT6BFU42T6ACQHP5Z2GO56Q/bundle.json","state_url":"https://pith.science/pith/DQ2TT6BFU42T6ACQHP5Z2GO56Q/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DQ2TT6BFU42T6ACQHP5Z2GO56Q/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":"2026-06-10T23:20:21Z","links":{"resolver":"https://pith.science/pith/DQ2TT6BFU42T6ACQHP5Z2GO56Q","bundle":"https://pith.science/pith/DQ2TT6BFU42T6ACQHP5Z2GO56Q/bundle.json","state":"https://pith.science/pith/DQ2TT6BFU42T6ACQHP5Z2GO56Q/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DQ2TT6BFU42T6ACQHP5Z2GO56Q/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:DQ2TT6BFU42T6ACQHP5Z2GO56Q","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":"773a65c6dbbd79ed7f9f37ae30cba7868d7edd433e1f1e5731ad42982bf5eb30","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2016-07-31T03:58:27Z","title_canon_sha256":"c8e813c7fe26e90ab74698bac42000ef435b2f4a6c905f63af3bc880d3e2a3e1"},"schema_version":"1.0","source":{"id":"1608.00183","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.00183","created_at":"2026-05-18T00:53:24Z"},{"alias_kind":"arxiv_version","alias_value":"1608.00183v2","created_at":"2026-05-18T00:53:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.00183","created_at":"2026-05-18T00:53:24Z"},{"alias_kind":"pith_short_12","alias_value":"DQ2TT6BFU42T","created_at":"2026-05-18T12:30:12Z"},{"alias_kind":"pith_short_16","alias_value":"DQ2TT6BFU42T6ACQ","created_at":"2026-05-18T12:30:12Z"},{"alias_kind":"pith_short_8","alias_value":"DQ2TT6BF","created_at":"2026-05-18T12:30:12Z"}],"graph_snapshots":[{"event_id":"sha256:03c8399c54378f2d4c9cceb144215a56dad88ba570ca04554364ff6f794893b2","target":"graph","created_at":"2026-05-18T00:53:24Z","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 the odd-wave interacting identical fermions in one-dimension with finite effective range. We show that to fully describe the high-momentum distribution $\\rho(k)$ up to $k^{-4}$, one needs four parameters characterizing the properties when two particles {\\it contact} with each other. Two parameters are related to the variation of energy with respect to the odd-wave scattering length and the effective range, respectively, determining the $k^{-2}$ tail and part of $k^{-4}$ tail in $\\rho(k)$. The other two parameters are related to the center-of-mass motion of the system, respectively det","authors_text":"Huifang Dong, Xiaoling Cui","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2016-07-31T03:58:27Z","title":"High-momentum distribution with subleading $k^{-3}$ tail in the odd-wave interacting one-dimensional Fermi gases"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.00183","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:fc759c06178768026efc8b0c93514dee6c53335469597ae8c35f14b1cace8388","target":"record","created_at":"2026-05-18T00:53:24Z","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":"773a65c6dbbd79ed7f9f37ae30cba7868d7edd433e1f1e5731ad42982bf5eb30","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2016-07-31T03:58:27Z","title_canon_sha256":"c8e813c7fe26e90ab74698bac42000ef435b2f4a6c905f63af3bc880d3e2a3e1"},"schema_version":"1.0","source":{"id":"1608.00183","kind":"arxiv","version":2}},"canonical_sha256":"1c3539f825a7353f00503bfb9d19ddf42f49e9564f79a45b4c69cbc5c0413432","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1c3539f825a7353f00503bfb9d19ddf42f49e9564f79a45b4c69cbc5c0413432","first_computed_at":"2026-05-18T00:53:24.329647Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:53:24.329647Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"aBXZy8BaPP/BmpLXSOwlWCB5SVBP7Ho7z97HebktkFLDstywu26HeeK2k7ag5wGrdojaEFbtamYhToB4mF+hBg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:53:24.330105Z","signed_message":"canonical_sha256_bytes"},"source_id":"1608.00183","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fc759c06178768026efc8b0c93514dee6c53335469597ae8c35f14b1cace8388","sha256:03c8399c54378f2d4c9cceb144215a56dad88ba570ca04554364ff6f794893b2"],"state_sha256":"fc5f5b8d88d023018c8e41eb62934a8badc34fdbad3c2a3ed55afd9730464f13"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/xneOIv0RQOLM/bj2kxgWUDg+5zI3DYojjEk8bunuW8ZrMKX23mS09gyGqTySWMjxGZFS+6Egmdw6IXDfZ16Dw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-10T23:20:21.794197Z","bundle_sha256":"351a0e30a6bda3dcf54482dc1db00ec4c54072c49c0bc1a969872d1af7dd0caa"}}