{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:N7Q4EUF75ESP7JF2MECZQOCZVT","short_pith_number":"pith:N7Q4EUF7","canonical_record":{"source":{"id":"1707.09884","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-07-31T14:34:12Z","cross_cats_sorted":["cond-mat.other","quant-ph"],"title_canon_sha256":"9756aa421fa66958a26b0ff498bb0eefa541610885204fa54648069f1ec436cd","abstract_canon_sha256":"3b6ffc0a44fa92e3a22fbff57d80f171a96448b32a571a10053ae4e356330cf4"},"schema_version":"1.0"},"canonical_sha256":"6fe1c250bfe924ffa4ba6105983859acc9b459040da3f8c1133d00ce9f72cd82","source":{"kind":"arxiv","id":"1707.09884","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.09884","created_at":"2026-05-18T00:30:00Z"},{"alias_kind":"arxiv_version","alias_value":"1707.09884v2","created_at":"2026-05-18T00:30:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.09884","created_at":"2026-05-18T00:30:00Z"},{"alias_kind":"pith_short_12","alias_value":"N7Q4EUF75ESP","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_16","alias_value":"N7Q4EUF75ESP7JF2","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_8","alias_value":"N7Q4EUF7","created_at":"2026-05-18T12:31:31Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:N7Q4EUF75ESP7JF2MECZQOCZVT","target":"record","payload":{"canonical_record":{"source":{"id":"1707.09884","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-07-31T14:34:12Z","cross_cats_sorted":["cond-mat.other","quant-ph"],"title_canon_sha256":"9756aa421fa66958a26b0ff498bb0eefa541610885204fa54648069f1ec436cd","abstract_canon_sha256":"3b6ffc0a44fa92e3a22fbff57d80f171a96448b32a571a10053ae4e356330cf4"},"schema_version":"1.0"},"canonical_sha256":"6fe1c250bfe924ffa4ba6105983859acc9b459040da3f8c1133d00ce9f72cd82","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:30:00.955872Z","signature_b64":"Tz9FUwgK1AqQB92ZIsdhNcj0A1p2I4kkTmsx3MsXAmBQZeotnuJ6Tuiv/NjLwlIVQVv1m/PmDTO3SMJWqLYDAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6fe1c250bfe924ffa4ba6105983859acc9b459040da3f8c1133d00ce9f72cd82","last_reissued_at":"2026-05-18T00:30:00.955335Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:30:00.955335Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1707.09884","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":"2026-05-18T00:30:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pw/RyIA9LIDKVaT6p6QBHOEuTKhwqAYyh8gllQqfZvT9ZapsLipAzDzH/QHxEWDUdU4blvvFMBcDIu0RmtwVBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T13:53:12.747625Z"},"content_sha256":"4f70773dc83a4211c7c19234ac395caf22d5a682b0dfda2e34c55a952019e000","schema_version":"1.0","event_id":"sha256:4f70773dc83a4211c7c19234ac395caf22d5a682b0dfda2e34c55a952019e000"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:N7Q4EUF75ESP7JF2MECZQOCZVT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Spatial Kibble-Zurek mechanism through susceptibilities: the inhomogeneous quantum Ising model case","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other","quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Bogdan Damski, Mateusz {\\L}\\k{a}cki","submitted_at":"2017-07-31T14:34:12Z","abstract_excerpt":"We study the quantum Ising model in the transverse inhomogeneous magnetic field. Such a system can be approached numerically through exact diagonalization and analytically through the renormalization group techniques. Basic insights into its physics, however, can be obtained by adopting the Kibble-Zurek theory of non-equilibrium phase transitions to description of spatially inhomogeneous systems at equilibrium. We employ all these approaches and focus on derivatives of longitudinal and transverse magnetizations, which have extrema near the critical point. We discuss how these extrema can be us"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.09884","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":"2026-05-18T00:30:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"g+aFg7PFCTB3xsBsR91xGGO2mLc+CCZI+O2+dkz5NqUsK0jJttsTF4lG7qswBgybEOMSLrrEYDl97kMaRA3NBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T13:53:12.747978Z"},"content_sha256":"09a5b5ccb4545f11a52a2744be741badf972c42e3db8c103c09d94bf5de1a5e8","schema_version":"1.0","event_id":"sha256:09a5b5ccb4545f11a52a2744be741badf972c42e3db8c103c09d94bf5de1a5e8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/N7Q4EUF75ESP7JF2MECZQOCZVT/bundle.json","state_url":"https://pith.science/pith/N7Q4EUF75ESP7JF2MECZQOCZVT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/N7Q4EUF75ESP7JF2MECZQOCZVT/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":"2026-05-27T13:53:12Z","links":{"resolver":"https://pith.science/pith/N7Q4EUF75ESP7JF2MECZQOCZVT","bundle":"https://pith.science/pith/N7Q4EUF75ESP7JF2MECZQOCZVT/bundle.json","state":"https://pith.science/pith/N7Q4EUF75ESP7JF2MECZQOCZVT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/N7Q4EUF75ESP7JF2MECZQOCZVT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:N7Q4EUF75ESP7JF2MECZQOCZVT","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":"3b6ffc0a44fa92e3a22fbff57d80f171a96448b32a571a10053ae4e356330cf4","cross_cats_sorted":["cond-mat.other","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-07-31T14:34:12Z","title_canon_sha256":"9756aa421fa66958a26b0ff498bb0eefa541610885204fa54648069f1ec436cd"},"schema_version":"1.0","source":{"id":"1707.09884","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.09884","created_at":"2026-05-18T00:30:00Z"},{"alias_kind":"arxiv_version","alias_value":"1707.09884v2","created_at":"2026-05-18T00:30:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.09884","created_at":"2026-05-18T00:30:00Z"},{"alias_kind":"pith_short_12","alias_value":"N7Q4EUF75ESP","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_16","alias_value":"N7Q4EUF75ESP7JF2","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_8","alias_value":"N7Q4EUF7","created_at":"2026-05-18T12:31:31Z"}],"graph_snapshots":[{"event_id":"sha256:09a5b5ccb4545f11a52a2744be741badf972c42e3db8c103c09d94bf5de1a5e8","target":"graph","created_at":"2026-05-18T00:30:00Z","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 quantum Ising model in the transverse inhomogeneous magnetic field. Such a system can be approached numerically through exact diagonalization and analytically through the renormalization group techniques. Basic insights into its physics, however, can be obtained by adopting the Kibble-Zurek theory of non-equilibrium phase transitions to description of spatially inhomogeneous systems at equilibrium. We employ all these approaches and focus on derivatives of longitudinal and transverse magnetizations, which have extrema near the critical point. We discuss how these extrema can be us","authors_text":"Bogdan Damski, Mateusz {\\L}\\k{a}cki","cross_cats":["cond-mat.other","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-07-31T14:34:12Z","title":"Spatial Kibble-Zurek mechanism through susceptibilities: the inhomogeneous quantum Ising model case"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.09884","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":"sha256:4f70773dc83a4211c7c19234ac395caf22d5a682b0dfda2e34c55a952019e000","target":"record","created_at":"2026-05-18T00:30:00Z","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":"3b6ffc0a44fa92e3a22fbff57d80f171a96448b32a571a10053ae4e356330cf4","cross_cats_sorted":["cond-mat.other","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-07-31T14:34:12Z","title_canon_sha256":"9756aa421fa66958a26b0ff498bb0eefa541610885204fa54648069f1ec436cd"},"schema_version":"1.0","source":{"id":"1707.09884","kind":"arxiv","version":2}},"canonical_sha256":"6fe1c250bfe924ffa4ba6105983859acc9b459040da3f8c1133d00ce9f72cd82","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6fe1c250bfe924ffa4ba6105983859acc9b459040da3f8c1133d00ce9f72cd82","first_computed_at":"2026-05-18T00:30:00.955335Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:30:00.955335Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Tz9FUwgK1AqQB92ZIsdhNcj0A1p2I4kkTmsx3MsXAmBQZeotnuJ6Tuiv/NjLwlIVQVv1m/PmDTO3SMJWqLYDAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:30:00.955872Z","signed_message":"canonical_sha256_bytes"},"source_id":"1707.09884","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4f70773dc83a4211c7c19234ac395caf22d5a682b0dfda2e34c55a952019e000","sha256:09a5b5ccb4545f11a52a2744be741badf972c42e3db8c103c09d94bf5de1a5e8"],"state_sha256":"4cd35770e3cec57578e1ac31308b15df46bcd1e03083e65614f4fa2521768064"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"k2WgZj5e69+C5kkVXyqIoYpRsz1+UWWSLSSJipNlz0cx0RYtev0OYKzvJjuBWGrX9/mq0fX1oE4wP4ZZRmCRDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T13:53:12.750374Z","bundle_sha256":"621cb4acff1cc42491c5b48a0d5d0ead3b1da1fc8e12e4d38e516708f66ce64e"}}