{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:WFL4EHUTGPPRTVNBQGLORUKBIA","short_pith_number":"pith:WFL4EHUT","canonical_record":{"source":{"id":"1106.3561","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2011-06-17T13:19:48Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"7e77b957c9d60ef285da518ea6d15120065cf7d4bca39dc35d2cf17a3e459714","abstract_canon_sha256":"0db1b4b22db8e49443809772844d92a782b7761cc4cb34304dddff71df15bb72"},"schema_version":"1.0"},"canonical_sha256":"b157c21e9333df19d5a18196e8d1414033ce009e8b9914bd738d3601a10f6988","source":{"kind":"arxiv","id":"1106.3561","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.3561","created_at":"2026-05-18T02:01:35Z"},{"alias_kind":"arxiv_version","alias_value":"1106.3561v2","created_at":"2026-05-18T02:01:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.3561","created_at":"2026-05-18T02:01:35Z"},{"alias_kind":"pith_short_12","alias_value":"WFL4EHUTGPPR","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_16","alias_value":"WFL4EHUTGPPRTVNB","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_8","alias_value":"WFL4EHUT","created_at":"2026-05-18T12:26:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:WFL4EHUTGPPRTVNBQGLORUKBIA","target":"record","payload":{"canonical_record":{"source":{"id":"1106.3561","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2011-06-17T13:19:48Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"7e77b957c9d60ef285da518ea6d15120065cf7d4bca39dc35d2cf17a3e459714","abstract_canon_sha256":"0db1b4b22db8e49443809772844d92a782b7761cc4cb34304dddff71df15bb72"},"schema_version":"1.0"},"canonical_sha256":"b157c21e9333df19d5a18196e8d1414033ce009e8b9914bd738d3601a10f6988","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:35.471729Z","signature_b64":"WE4PYU9WY+zykt2aVzxb42V6AvXPTJTRwg01UePDVK9pWjTW/SzAJj6aTHnxNwxiN/GVz/86H/145reSECbXAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b157c21e9333df19d5a18196e8d1414033ce009e8b9914bd738d3601a10f6988","last_reissued_at":"2026-05-18T02:01:35.470889Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:35.470889Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1106.3561","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":"2026-05-18T02:01:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xPtHs4AqSWOo/LVFWTxCZ7iHWsYi+aZh0YLDxfvunOtJViP4ZApRyxbg8DlHOpbKZAugGA7gR+LyyyAuXS0aDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T14:43:55.250557Z"},"content_sha256":"b0731a7219e0fcc6f723d124d4f1266e68dba36d1371f20e1d7b6bd19b35da77","schema_version":"1.0","event_id":"sha256:b0731a7219e0fcc6f723d124d4f1266e68dba36d1371f20e1d7b6bd19b35da77"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:WFL4EHUTGPPRTVNBQGLORUKBIA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The Effects of Tachyonic and Phantom Fields in the Intermediate and Logamediate Scenarios of the Anisotropic Universe","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"physics.gen-ph","authors_text":"Shuvendu Chakraborty, Ujjal Debnath","submitted_at":"2011-06-17T13:19:48Z","abstract_excerpt":"In this work, we have analyzed two scenarios namely, \"intermediate\" and \"logamadiate\" scenarios for closed, open and flat anisotropic universe in presence of phantom field, normal tachyonic field and phantom tachyonic field. We have assumed that there is no interaction between the above mentioned dark energy and dark matter. In these two types of the scenarios of the universe, the nature of the scalar fields and corresponding potentials have been investigated. In intermediate scenario, (i) the potential for normal tachyonic field decreases, (ii) the potentials for phantom tachyonic field and p"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.3561","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":"2026-05-18T02:01:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"U0jrRJVdSvQPQWbwqPxQXbtzKGDk4WSUL3TLJ7Mpb0vG9K3fxgt+6xdsqer5DJb7VcHhuPLElO6ovXhKuy+hCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T14:43:55.250906Z"},"content_sha256":"ec6f365ea6a822f9a50237ac352c42ea2b1fdbc0e06ef9fa861e805c6e3f3189","schema_version":"1.0","event_id":"sha256:ec6f365ea6a822f9a50237ac352c42ea2b1fdbc0e06ef9fa861e805c6e3f3189"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WFL4EHUTGPPRTVNBQGLORUKBIA/bundle.json","state_url":"https://pith.science/pith/WFL4EHUTGPPRTVNBQGLORUKBIA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WFL4EHUTGPPRTVNBQGLORUKBIA/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":"2026-06-26T14:43:55Z","links":{"resolver":"https://pith.science/pith/WFL4EHUTGPPRTVNBQGLORUKBIA","bundle":"https://pith.science/pith/WFL4EHUTGPPRTVNBQGLORUKBIA/bundle.json","state":"https://pith.science/pith/WFL4EHUTGPPRTVNBQGLORUKBIA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WFL4EHUTGPPRTVNBQGLORUKBIA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:WFL4EHUTGPPRTVNBQGLORUKBIA","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":"0db1b4b22db8e49443809772844d92a782b7761cc4cb34304dddff71df15bb72","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2011-06-17T13:19:48Z","title_canon_sha256":"7e77b957c9d60ef285da518ea6d15120065cf7d4bca39dc35d2cf17a3e459714"},"schema_version":"1.0","source":{"id":"1106.3561","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.3561","created_at":"2026-05-18T02:01:35Z"},{"alias_kind":"arxiv_version","alias_value":"1106.3561v2","created_at":"2026-05-18T02:01:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.3561","created_at":"2026-05-18T02:01:35Z"},{"alias_kind":"pith_short_12","alias_value":"WFL4EHUTGPPR","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_16","alias_value":"WFL4EHUTGPPRTVNB","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_8","alias_value":"WFL4EHUT","created_at":"2026-05-18T12:26:44Z"}],"graph_snapshots":[{"event_id":"sha256:ec6f365ea6a822f9a50237ac352c42ea2b1fdbc0e06ef9fa861e805c6e3f3189","target":"graph","created_at":"2026-05-18T02:01:35Z","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":"In this work, we have analyzed two scenarios namely, \"intermediate\" and \"logamadiate\" scenarios for closed, open and flat anisotropic universe in presence of phantom field, normal tachyonic field and phantom tachyonic field. We have assumed that there is no interaction between the above mentioned dark energy and dark matter. In these two types of the scenarios of the universe, the nature of the scalar fields and corresponding potentials have been investigated. In intermediate scenario, (i) the potential for normal tachyonic field decreases, (ii) the potentials for phantom tachyonic field and p","authors_text":"Shuvendu Chakraborty, Ujjal Debnath","cross_cats":["gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2011-06-17T13:19:48Z","title":"The Effects of Tachyonic and Phantom Fields in the Intermediate and Logamediate Scenarios of the Anisotropic Universe"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.3561","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:b0731a7219e0fcc6f723d124d4f1266e68dba36d1371f20e1d7b6bd19b35da77","target":"record","created_at":"2026-05-18T02:01:35Z","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":"0db1b4b22db8e49443809772844d92a782b7761cc4cb34304dddff71df15bb72","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2011-06-17T13:19:48Z","title_canon_sha256":"7e77b957c9d60ef285da518ea6d15120065cf7d4bca39dc35d2cf17a3e459714"},"schema_version":"1.0","source":{"id":"1106.3561","kind":"arxiv","version":2}},"canonical_sha256":"b157c21e9333df19d5a18196e8d1414033ce009e8b9914bd738d3601a10f6988","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b157c21e9333df19d5a18196e8d1414033ce009e8b9914bd738d3601a10f6988","first_computed_at":"2026-05-18T02:01:35.470889Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:01:35.470889Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"WE4PYU9WY+zykt2aVzxb42V6AvXPTJTRwg01UePDVK9pWjTW/SzAJj6aTHnxNwxiN/GVz/86H/145reSECbXAg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:01:35.471729Z","signed_message":"canonical_sha256_bytes"},"source_id":"1106.3561","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b0731a7219e0fcc6f723d124d4f1266e68dba36d1371f20e1d7b6bd19b35da77","sha256:ec6f365ea6a822f9a50237ac352c42ea2b1fdbc0e06ef9fa861e805c6e3f3189"],"state_sha256":"31fcf65f29888727eb32d8fe50d36d715e7c9cd10d502386b3656988dbfb8a54"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Sg9ylzqrD80M3CUsqMtNKKtPDkOIDp06wchqR0zpK1hXTFpAcWIBmtJsQ9uH6LSz+6gEbbL53xWOwHirYARICQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-26T14:43:55.252792Z","bundle_sha256":"64094b7225789d693243828309fe801a804987d92e37c83ba229869fa4f973f3"}}