{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:6CHVWWJKTCQ56INPN7KLSWPKI7","short_pith_number":"pith:6CHVWWJK","canonical_record":{"source":{"id":"1708.05434","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-08-17T20:44:32Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"c857000660cb7e1dabd6da1fb1689f822b0dfefb7ac730c39cdab24cedc44762","abstract_canon_sha256":"5a8e120c8d069f744f78dfba2a3338bc4f2a679ff758759a0243044a169ff274"},"schema_version":"1.0"},"canonical_sha256":"f08f5b592a98a1df21af6fd4b959ea47f353a944ec2182c5d2693c4d4ba1f72a","source":{"kind":"arxiv","id":"1708.05434","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.05434","created_at":"2026-05-17T23:50:47Z"},{"alias_kind":"arxiv_version","alias_value":"1708.05434v1","created_at":"2026-05-17T23:50:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.05434","created_at":"2026-05-17T23:50:47Z"},{"alias_kind":"pith_short_12","alias_value":"6CHVWWJKTCQ5","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_16","alias_value":"6CHVWWJKTCQ56INP","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_8","alias_value":"6CHVWWJK","created_at":"2026-05-18T12:31:03Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:6CHVWWJKTCQ56INPN7KLSWPKI7","target":"record","payload":{"canonical_record":{"source":{"id":"1708.05434","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-08-17T20:44:32Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"c857000660cb7e1dabd6da1fb1689f822b0dfefb7ac730c39cdab24cedc44762","abstract_canon_sha256":"5a8e120c8d069f744f78dfba2a3338bc4f2a679ff758759a0243044a169ff274"},"schema_version":"1.0"},"canonical_sha256":"f08f5b592a98a1df21af6fd4b959ea47f353a944ec2182c5d2693c4d4ba1f72a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:50:47.149581Z","signature_b64":"DKc5wtW6wDBuL2TuVsRynA39qqJSNALsx2bWReyjHVE5kGBYx8gHYuoGekX94RiHO9rxFDD1qUgXNHTZ+QGWCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f08f5b592a98a1df21af6fd4b959ea47f353a944ec2182c5d2693c4d4ba1f72a","last_reissued_at":"2026-05-17T23:50:47.148901Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:50:47.148901Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1708.05434","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":"2026-05-17T23:50:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"X/lgouyNLjmq5i/bsyGuUb75NJGOn4bU98WX3wxbkUgzVmkDIq80q68w7vyBenh8eYnBcmqjc228RcTpJl9iBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T17:22:34.509054Z"},"content_sha256":"9bf9abb4a28dee194e12fd4bfee46c8c0d6ec705c7a3135574b5e4275314f464","schema_version":"1.0","event_id":"sha256:9bf9abb4a28dee194e12fd4bfee46c8c0d6ec705c7a3135574b5e4275314f464"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:6CHVWWJKTCQ56INPN7KLSWPKI7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Biaxial magnetic field setup for angular magnetic measurements of thin films and spintronic nanodevices","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"physics.app-ph","authors_text":"Piotr Ogrodnik, Piotr Rzeszut, S{\\l}awomir Zi\\k{e}tek, Tomasz Stobiecki, Witold Skowro\\'nski","submitted_at":"2017-08-17T20:44:32Z","abstract_excerpt":"The biaxial magnetic-field setup for angular magnetic measurements of thin film and spintronic devices is designed and presented. The setup allows for application of the in-plane magnetic field using a quadrupole electromagnet, controlled by power supply units and integrated with an electromagnet biaxial magnetic field sensor. In addition, the probe station is equipped with a microwave circuitry, which enables angle-resolved spin torque oscillation measurements. The angular dependencies of magnetoresistance and spin diode effect in a giant magnetoresistance strip are shown as an operational ve"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.05434","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":"2026-05-17T23:50:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"n/ReroSJEVQ4cV3lAYJGcrvJ7pBEjJ1qw/o99eF9y6ZedEIaMmNLQXT633nkZ0ZbuEmoHNB1ThZLFUD8cIchAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T17:22:34.509706Z"},"content_sha256":"45e8a1b5393bf4af8f07953923a31b31926c23cc9311cc8988c08870c9191849","schema_version":"1.0","event_id":"sha256:45e8a1b5393bf4af8f07953923a31b31926c23cc9311cc8988c08870c9191849"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6CHVWWJKTCQ56INPN7KLSWPKI7/bundle.json","state_url":"https://pith.science/pith/6CHVWWJKTCQ56INPN7KLSWPKI7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6CHVWWJKTCQ56INPN7KLSWPKI7/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":"2026-05-28T17:22:34Z","links":{"resolver":"https://pith.science/pith/6CHVWWJKTCQ56INPN7KLSWPKI7","bundle":"https://pith.science/pith/6CHVWWJKTCQ56INPN7KLSWPKI7/bundle.json","state":"https://pith.science/pith/6CHVWWJKTCQ56INPN7KLSWPKI7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6CHVWWJKTCQ56INPN7KLSWPKI7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:6CHVWWJKTCQ56INPN7KLSWPKI7","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":"5a8e120c8d069f744f78dfba2a3338bc4f2a679ff758759a0243044a169ff274","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-08-17T20:44:32Z","title_canon_sha256":"c857000660cb7e1dabd6da1fb1689f822b0dfefb7ac730c39cdab24cedc44762"},"schema_version":"1.0","source":{"id":"1708.05434","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.05434","created_at":"2026-05-17T23:50:47Z"},{"alias_kind":"arxiv_version","alias_value":"1708.05434v1","created_at":"2026-05-17T23:50:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.05434","created_at":"2026-05-17T23:50:47Z"},{"alias_kind":"pith_short_12","alias_value":"6CHVWWJKTCQ5","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_16","alias_value":"6CHVWWJKTCQ56INP","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_8","alias_value":"6CHVWWJK","created_at":"2026-05-18T12:31:03Z"}],"graph_snapshots":[{"event_id":"sha256:45e8a1b5393bf4af8f07953923a31b31926c23cc9311cc8988c08870c9191849","target":"graph","created_at":"2026-05-17T23:50:47Z","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 biaxial magnetic-field setup for angular magnetic measurements of thin film and spintronic devices is designed and presented. The setup allows for application of the in-plane magnetic field using a quadrupole electromagnet, controlled by power supply units and integrated with an electromagnet biaxial magnetic field sensor. In addition, the probe station is equipped with a microwave circuitry, which enables angle-resolved spin torque oscillation measurements. The angular dependencies of magnetoresistance and spin diode effect in a giant magnetoresistance strip are shown as an operational ve","authors_text":"Piotr Ogrodnik, Piotr Rzeszut, S{\\l}awomir Zi\\k{e}tek, Tomasz Stobiecki, Witold Skowro\\'nski","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-08-17T20:44:32Z","title":"Biaxial magnetic field setup for angular magnetic measurements of thin films and spintronic nanodevices"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.05434","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":"sha256:9bf9abb4a28dee194e12fd4bfee46c8c0d6ec705c7a3135574b5e4275314f464","target":"record","created_at":"2026-05-17T23:50:47Z","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":"5a8e120c8d069f744f78dfba2a3338bc4f2a679ff758759a0243044a169ff274","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-08-17T20:44:32Z","title_canon_sha256":"c857000660cb7e1dabd6da1fb1689f822b0dfefb7ac730c39cdab24cedc44762"},"schema_version":"1.0","source":{"id":"1708.05434","kind":"arxiv","version":1}},"canonical_sha256":"f08f5b592a98a1df21af6fd4b959ea47f353a944ec2182c5d2693c4d4ba1f72a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f08f5b592a98a1df21af6fd4b959ea47f353a944ec2182c5d2693c4d4ba1f72a","first_computed_at":"2026-05-17T23:50:47.148901Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:50:47.148901Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"DKc5wtW6wDBuL2TuVsRynA39qqJSNALsx2bWReyjHVE5kGBYx8gHYuoGekX94RiHO9rxFDD1qUgXNHTZ+QGWCw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:50:47.149581Z","signed_message":"canonical_sha256_bytes"},"source_id":"1708.05434","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9bf9abb4a28dee194e12fd4bfee46c8c0d6ec705c7a3135574b5e4275314f464","sha256:45e8a1b5393bf4af8f07953923a31b31926c23cc9311cc8988c08870c9191849"],"state_sha256":"0d0cac208b94ca15ba32281cdb4a7536e806e45e37292e78c8873d7bbe08f636"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rAdLiybXdqIBZ/be915l7uWRhdGKip6qfUZ0P9+Y4XbxZMPZ+pmWJDRz6FDSe1nHABYNl1YKsxa3293fFF69Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T17:22:34.512928Z","bundle_sha256":"8885fde91d48ebe0bf3524c7bc912d028bdc549f16c87d1b94559b190e4252af"}}