{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:OIJVWAO4J3LBMDL6JVNDSYVFNG","short_pith_number":"pith:OIJVWAO4","canonical_record":{"source":{"id":"1407.1565","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2014-07-07T01:38:05Z","cross_cats_sorted":["cond-mat.soft","physics.flu-dyn"],"title_canon_sha256":"bdfa7143cb385a181f6cdc80c96f195b788ada3210587ce912dc190e7259225d","abstract_canon_sha256":"a3a1b0595c67b9311e8e3bd6c12bfa446dbdfa87539425067ed6310d7a869750"},"schema_version":"1.0"},"canonical_sha256":"72135b01dc4ed6160d7e4d5a3962a56991f9403ee301e63024f5d97dff58b71c","source":{"kind":"arxiv","id":"1407.1565","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.1565","created_at":"2026-05-18T02:29:32Z"},{"alias_kind":"arxiv_version","alias_value":"1407.1565v1","created_at":"2026-05-18T02:29:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.1565","created_at":"2026-05-18T02:29:32Z"},{"alias_kind":"pith_short_12","alias_value":"OIJVWAO4J3LB","created_at":"2026-05-18T12:28:41Z"},{"alias_kind":"pith_short_16","alias_value":"OIJVWAO4J3LBMDL6","created_at":"2026-05-18T12:28:41Z"},{"alias_kind":"pith_short_8","alias_value":"OIJVWAO4","created_at":"2026-05-18T12:28:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:OIJVWAO4J3LBMDL6JVNDSYVFNG","target":"record","payload":{"canonical_record":{"source":{"id":"1407.1565","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2014-07-07T01:38:05Z","cross_cats_sorted":["cond-mat.soft","physics.flu-dyn"],"title_canon_sha256":"bdfa7143cb385a181f6cdc80c96f195b788ada3210587ce912dc190e7259225d","abstract_canon_sha256":"a3a1b0595c67b9311e8e3bd6c12bfa446dbdfa87539425067ed6310d7a869750"},"schema_version":"1.0"},"canonical_sha256":"72135b01dc4ed6160d7e4d5a3962a56991f9403ee301e63024f5d97dff58b71c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:29:32.003411Z","signature_b64":"Xtk2g4Jhxp6WVXlyHZSoD3xyNhiLcNXFmgMj/gUVP3zRIyEQ8W4YS2wJveVkSp5FX9WZ2V6yBu1uOb0e8fIQAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"72135b01dc4ed6160d7e4d5a3962a56991f9403ee301e63024f5d97dff58b71c","last_reissued_at":"2026-05-18T02:29:32.002931Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:29:32.002931Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1407.1565","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:29:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pLBN+NFzE72RuSrWZkQyLtmGguSR+bWdPsyOfxO28/gcN9aARKhyPrWZ9Uv7HmBr0FEa2s1mgMZcJYvBWyrtBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T21:38:45.455182Z"},"content_sha256":"cbcaecee2b00a236a77175d0083e27b8ccfde5493ab842ea2544e60426e1eb1d","schema_version":"1.0","event_id":"sha256:cbcaecee2b00a236a77175d0083e27b8ccfde5493ab842ea2544e60426e1eb1d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:OIJVWAO4J3LBMDL6JVNDSYVFNG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Counterflow quantum turbulence in a square channel under the normal fluid with a Poiseuille flow","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft","physics.flu-dyn"],"primary_cat":"cond-mat.other","authors_text":"Makoto Tsubota, Satoshi Yui","submitted_at":"2014-07-07T01:38:05Z","abstract_excerpt":"We perform a numerical analysis of superfluid turbulence produced by thermal counterflow in He II by using the vortex filament model. Counterflow in a low aspect ratio channel is known to show the transition from laminar flow to the two turbulent states TI and TII. The present understanding is that the TI has the turbulent superfluid and the laminar normal fluid but both fluids are turbulent in the TII state. This work studies the vortex tangle in the TI state. Solid boundary condition is applied to walls of a square channel, and the velocity field of the normal fluid is prescribed to be a lam"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.1565","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":""},"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":"2026-05-18T02:29:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"To0PY/VxJbA34PLBoOQlJjuK/TfiICTCJXlN7Zqosen9DQOtPj6n88NL9Ylm/LSCRUmdSfL3TfFcCUUVPfzBBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T21:38:45.455540Z"},"content_sha256":"d8f2eb3369c6fdb52deeb0e157557abbb7de4092a967aef06ceca85951206c36","schema_version":"1.0","event_id":"sha256:d8f2eb3369c6fdb52deeb0e157557abbb7de4092a967aef06ceca85951206c36"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/OIJVWAO4J3LBMDL6JVNDSYVFNG/bundle.json","state_url":"https://pith.science/pith/OIJVWAO4J3LBMDL6JVNDSYVFNG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/OIJVWAO4J3LBMDL6JVNDSYVFNG/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":"2026-06-01T21:38:45Z","links":{"resolver":"https://pith.science/pith/OIJVWAO4J3LBMDL6JVNDSYVFNG","bundle":"https://pith.science/pith/OIJVWAO4J3LBMDL6JVNDSYVFNG/bundle.json","state":"https://pith.science/pith/OIJVWAO4J3LBMDL6JVNDSYVFNG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/OIJVWAO4J3LBMDL6JVNDSYVFNG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:OIJVWAO4J3LBMDL6JVNDSYVFNG","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":"a3a1b0595c67b9311e8e3bd6c12bfa446dbdfa87539425067ed6310d7a869750","cross_cats_sorted":["cond-mat.soft","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2014-07-07T01:38:05Z","title_canon_sha256":"bdfa7143cb385a181f6cdc80c96f195b788ada3210587ce912dc190e7259225d"},"schema_version":"1.0","source":{"id":"1407.1565","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.1565","created_at":"2026-05-18T02:29:32Z"},{"alias_kind":"arxiv_version","alias_value":"1407.1565v1","created_at":"2026-05-18T02:29:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.1565","created_at":"2026-05-18T02:29:32Z"},{"alias_kind":"pith_short_12","alias_value":"OIJVWAO4J3LB","created_at":"2026-05-18T12:28:41Z"},{"alias_kind":"pith_short_16","alias_value":"OIJVWAO4J3LBMDL6","created_at":"2026-05-18T12:28:41Z"},{"alias_kind":"pith_short_8","alias_value":"OIJVWAO4","created_at":"2026-05-18T12:28:41Z"}],"graph_snapshots":[{"event_id":"sha256:d8f2eb3369c6fdb52deeb0e157557abbb7de4092a967aef06ceca85951206c36","target":"graph","created_at":"2026-05-18T02:29:32Z","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 perform a numerical analysis of superfluid turbulence produced by thermal counterflow in He II by using the vortex filament model. Counterflow in a low aspect ratio channel is known to show the transition from laminar flow to the two turbulent states TI and TII. The present understanding is that the TI has the turbulent superfluid and the laminar normal fluid but both fluids are turbulent in the TII state. This work studies the vortex tangle in the TI state. Solid boundary condition is applied to walls of a square channel, and the velocity field of the normal fluid is prescribed to be a lam","authors_text":"Makoto Tsubota, Satoshi Yui","cross_cats":["cond-mat.soft","physics.flu-dyn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2014-07-07T01:38:05Z","title":"Counterflow quantum turbulence in a square channel under the normal fluid with a Poiseuille flow"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.1565","kind":"arxiv","version":1},"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:cbcaecee2b00a236a77175d0083e27b8ccfde5493ab842ea2544e60426e1eb1d","target":"record","created_at":"2026-05-18T02:29:32Z","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":"a3a1b0595c67b9311e8e3bd6c12bfa446dbdfa87539425067ed6310d7a869750","cross_cats_sorted":["cond-mat.soft","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2014-07-07T01:38:05Z","title_canon_sha256":"bdfa7143cb385a181f6cdc80c96f195b788ada3210587ce912dc190e7259225d"},"schema_version":"1.0","source":{"id":"1407.1565","kind":"arxiv","version":1}},"canonical_sha256":"72135b01dc4ed6160d7e4d5a3962a56991f9403ee301e63024f5d97dff58b71c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"72135b01dc4ed6160d7e4d5a3962a56991f9403ee301e63024f5d97dff58b71c","first_computed_at":"2026-05-18T02:29:32.002931Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:29:32.002931Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Xtk2g4Jhxp6WVXlyHZSoD3xyNhiLcNXFmgMj/gUVP3zRIyEQ8W4YS2wJveVkSp5FX9WZ2V6yBu1uOb0e8fIQAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:29:32.003411Z","signed_message":"canonical_sha256_bytes"},"source_id":"1407.1565","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cbcaecee2b00a236a77175d0083e27b8ccfde5493ab842ea2544e60426e1eb1d","sha256:d8f2eb3369c6fdb52deeb0e157557abbb7de4092a967aef06ceca85951206c36"],"state_sha256":"f21ec3664c713a19fbad7884ad907a7cda2e3ffdf35f57e09af2f4a3cd7f7258"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ks52PLsvuXSjK1L1oJjvniSLrCgeyoi2NpqolIGmYgmEkYiFGdMOwTJzDAVuJy+0REoyf3cMZU0NIHNS9Y+gDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T21:38:45.457513Z","bundle_sha256":"8a3137d5d35c7c09ea20de509ba3045dd57bc01fac1d8cd3decfa83af11cc787"}}