{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:VOONYQKRNGKGDEUYKAURQ6DEB2","short_pith_number":"pith:VOONYQKR","canonical_record":{"source":{"id":"1108.4117","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-08-20T14:06:01Z","cross_cats_sorted":[],"title_canon_sha256":"0c018a824fc249f4c01c7637c4624c0849dc40bad20bcca29420864b706f333c","abstract_canon_sha256":"5267c5b248a32e6a99838250059acd95426e7b79aa167712d4df1900255e92de"},"schema_version":"1.0"},"canonical_sha256":"ab9cdc4151699461929850291878640eb09984d18f799f411ccd8a4614b82310","source":{"kind":"arxiv","id":"1108.4117","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1108.4117","created_at":"2026-05-18T03:58:39Z"},{"alias_kind":"arxiv_version","alias_value":"1108.4117v1","created_at":"2026-05-18T03:58:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1108.4117","created_at":"2026-05-18T03:58:39Z"},{"alias_kind":"pith_short_12","alias_value":"VOONYQKRNGKG","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_16","alias_value":"VOONYQKRNGKGDEUY","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_8","alias_value":"VOONYQKR","created_at":"2026-05-18T12:26:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:VOONYQKRNGKGDEUYKAURQ6DEB2","target":"record","payload":{"canonical_record":{"source":{"id":"1108.4117","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-08-20T14:06:01Z","cross_cats_sorted":[],"title_canon_sha256":"0c018a824fc249f4c01c7637c4624c0849dc40bad20bcca29420864b706f333c","abstract_canon_sha256":"5267c5b248a32e6a99838250059acd95426e7b79aa167712d4df1900255e92de"},"schema_version":"1.0"},"canonical_sha256":"ab9cdc4151699461929850291878640eb09984d18f799f411ccd8a4614b82310","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:58:39.562323Z","signature_b64":"f2qhuGVl0RIBPLJ4DGD3GLveZ32aWu/EMsXZbo2rZelyeR6JLWzjD2HK9N+5kUwP1YC5sQoMtJH+n7+7N9JfCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ab9cdc4151699461929850291878640eb09984d18f799f411ccd8a4614b82310","last_reissued_at":"2026-05-18T03:58:39.561697Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:58:39.561697Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1108.4117","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":"2026-05-18T03:58:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LeuIEBm1ovvlv8Sf8baLiaVOFFZNLCrFgZHRCVHbYBZAuarA2t8xv6Tp/3xY2cw7ABiPjhnwK/yWX5j4KNdCCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T12:27:17.708581Z"},"content_sha256":"c5e238042fab06222928a786c8f26f4b2d2577b9cb53026670c507a8639f3fca","schema_version":"1.0","event_id":"sha256:c5e238042fab06222928a786c8f26f4b2d2577b9cb53026670c507a8639f3fca"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:VOONYQKRNGKGDEUYKAURQ6DEB2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"First order antiferro-ferromagnetic transition in Fe49(Rh0.93Pd0.07)51 under simultaneous application of magnetic field and external pressure","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Pallab Bag, Pallavi Kushwaha, P Chaddah, R Rawat","submitted_at":"2011-08-20T14:06:01Z","abstract_excerpt":"The magnetic field-pressure-temperature (H-P-T) phase diagram for first order antiferromagnetic (AFM) to ferromagnetic (FM) transition in Fe49(Rh0.93Pd0.07)51 has been constructed using resistivity measurements under simultaneous application of magnetic field (up to 8 Tesla) and pressure (up to 20 kbar). Temperature dependence of resistivity ({\\rho}-T) shows that with increasing pressure, the width of the transition and the extent of hysteresis decreases whereas with the application of magnetic field it increases. Consistent with existing literature the first order transition temperature (TN) "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1108.4117","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":"2026-05-18T03:58:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sExHLkkNsjM8zRllkZIo8rbpXnMwTVVTuUtp4X8aC+/vi7YBTgexKSxdUEQWf5HDYiJSsesyI//yArcXnGpWDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T12:27:17.708921Z"},"content_sha256":"7bd6466b4755c5ec00848fa4a2bc53eab228965fdd59bfe43b3993cdd365ffce","schema_version":"1.0","event_id":"sha256:7bd6466b4755c5ec00848fa4a2bc53eab228965fdd59bfe43b3993cdd365ffce"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VOONYQKRNGKGDEUYKAURQ6DEB2/bundle.json","state_url":"https://pith.science/pith/VOONYQKRNGKGDEUYKAURQ6DEB2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VOONYQKRNGKGDEUYKAURQ6DEB2/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":"2026-06-04T12:27:17Z","links":{"resolver":"https://pith.science/pith/VOONYQKRNGKGDEUYKAURQ6DEB2","bundle":"https://pith.science/pith/VOONYQKRNGKGDEUYKAURQ6DEB2/bundle.json","state":"https://pith.science/pith/VOONYQKRNGKGDEUYKAURQ6DEB2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VOONYQKRNGKGDEUYKAURQ6DEB2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:VOONYQKRNGKGDEUYKAURQ6DEB2","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":"5267c5b248a32e6a99838250059acd95426e7b79aa167712d4df1900255e92de","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-08-20T14:06:01Z","title_canon_sha256":"0c018a824fc249f4c01c7637c4624c0849dc40bad20bcca29420864b706f333c"},"schema_version":"1.0","source":{"id":"1108.4117","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1108.4117","created_at":"2026-05-18T03:58:39Z"},{"alias_kind":"arxiv_version","alias_value":"1108.4117v1","created_at":"2026-05-18T03:58:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1108.4117","created_at":"2026-05-18T03:58:39Z"},{"alias_kind":"pith_short_12","alias_value":"VOONYQKRNGKG","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_16","alias_value":"VOONYQKRNGKGDEUY","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_8","alias_value":"VOONYQKR","created_at":"2026-05-18T12:26:44Z"}],"graph_snapshots":[{"event_id":"sha256:7bd6466b4755c5ec00848fa4a2bc53eab228965fdd59bfe43b3993cdd365ffce","target":"graph","created_at":"2026-05-18T03:58:39Z","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":"The magnetic field-pressure-temperature (H-P-T) phase diagram for first order antiferromagnetic (AFM) to ferromagnetic (FM) transition in Fe49(Rh0.93Pd0.07)51 has been constructed using resistivity measurements under simultaneous application of magnetic field (up to 8 Tesla) and pressure (up to 20 kbar). Temperature dependence of resistivity ({\\rho}-T) shows that with increasing pressure, the width of the transition and the extent of hysteresis decreases whereas with the application of magnetic field it increases. Consistent with existing literature the first order transition temperature (TN) ","authors_text":"Pallab Bag, Pallavi Kushwaha, P Chaddah, R Rawat","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-08-20T14:06:01Z","title":"First order antiferro-ferromagnetic transition in Fe49(Rh0.93Pd0.07)51 under simultaneous application of magnetic field and external pressure"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1108.4117","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:c5e238042fab06222928a786c8f26f4b2d2577b9cb53026670c507a8639f3fca","target":"record","created_at":"2026-05-18T03:58:39Z","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":"5267c5b248a32e6a99838250059acd95426e7b79aa167712d4df1900255e92de","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-08-20T14:06:01Z","title_canon_sha256":"0c018a824fc249f4c01c7637c4624c0849dc40bad20bcca29420864b706f333c"},"schema_version":"1.0","source":{"id":"1108.4117","kind":"arxiv","version":1}},"canonical_sha256":"ab9cdc4151699461929850291878640eb09984d18f799f411ccd8a4614b82310","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ab9cdc4151699461929850291878640eb09984d18f799f411ccd8a4614b82310","first_computed_at":"2026-05-18T03:58:39.561697Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:58:39.561697Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"f2qhuGVl0RIBPLJ4DGD3GLveZ32aWu/EMsXZbo2rZelyeR6JLWzjD2HK9N+5kUwP1YC5sQoMtJH+n7+7N9JfCg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:58:39.562323Z","signed_message":"canonical_sha256_bytes"},"source_id":"1108.4117","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c5e238042fab06222928a786c8f26f4b2d2577b9cb53026670c507a8639f3fca","sha256:7bd6466b4755c5ec00848fa4a2bc53eab228965fdd59bfe43b3993cdd365ffce"],"state_sha256":"5b70288d52958bf48111dcfabb4d428592d57be0ee3443c6561965bade908344"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"S7hWaU0ls2KR5YSZL1HNSIiwFvcYmYHivV4m63xDZLEg8UeKA8eN/K28FU8bWFZ9rfZZipyaRbwMMoEOFMXZCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-04T12:27:17.711019Z","bundle_sha256":"0ecf67ee232ddbcdaf1c45267ddbcfcbf6f886b42b8c90950e2f65d41812dd61"}}