{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:AM4U5V2S337CX3RIZ3D7UCYTME","short_pith_number":"pith:AM4U5V2S","canonical_record":{"source":{"id":"1509.09163","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-09-30T13:09:10Z","cross_cats_sorted":[],"title_canon_sha256":"cf610d2b29356dbc634379e916689a1d88fbd2c41ee05facaa58502d378b12d4","abstract_canon_sha256":"e6ec7c8f5a9a82ef53bb661e316093e8bc01466b6ca1fdaa10b9f19465da2d10"},"schema_version":"1.0"},"canonical_sha256":"03394ed752defe2bee28cec7fa0b13610ecb03694696bcdcd7a5c01350755aeb","source":{"kind":"arxiv","id":"1509.09163","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1509.09163","created_at":"2026-05-18T01:25:26Z"},{"alias_kind":"arxiv_version","alias_value":"1509.09163v4","created_at":"2026-05-18T01:25:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.09163","created_at":"2026-05-18T01:25:26Z"},{"alias_kind":"pith_short_12","alias_value":"AM4U5V2S337C","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_16","alias_value":"AM4U5V2S337CX3RI","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_8","alias_value":"AM4U5V2S","created_at":"2026-05-18T12:29:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:AM4U5V2S337CX3RIZ3D7UCYTME","target":"record","payload":{"canonical_record":{"source":{"id":"1509.09163","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-09-30T13:09:10Z","cross_cats_sorted":[],"title_canon_sha256":"cf610d2b29356dbc634379e916689a1d88fbd2c41ee05facaa58502d378b12d4","abstract_canon_sha256":"e6ec7c8f5a9a82ef53bb661e316093e8bc01466b6ca1fdaa10b9f19465da2d10"},"schema_version":"1.0"},"canonical_sha256":"03394ed752defe2bee28cec7fa0b13610ecb03694696bcdcd7a5c01350755aeb","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:25:26.062354Z","signature_b64":"kX5Hnm2N/cRs/NB5XQ1WU+DOgNgMXvVWxypuDJX0YUJx3SsK3Uh/gqvqPJs4+8Xrkm4wnuzIR9ksZi+QRUKZDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"03394ed752defe2bee28cec7fa0b13610ecb03694696bcdcd7a5c01350755aeb","last_reissued_at":"2026-05-18T01:25:26.061889Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:25:26.061889Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1509.09163","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:25:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vDks47yi4eFklRlF1TSB0bgmMZzXRARwGOXvNfWdwc6H8Hq93tpxfyGeedlvbg6fLBRtoM80XT/PA52S/di1BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T17:35:25.652627Z"},"content_sha256":"b01cca0692abfe0651652713a2457514dfe929b1e1a3e4ef367c878e45270ba6","schema_version":"1.0","event_id":"sha256:b01cca0692abfe0651652713a2457514dfe929b1e1a3e4ef367c878e45270ba6"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:AM4U5V2S337CX3RIZ3D7UCYTME","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum critical dynamics of a magnetic impurity in a semiconducting host","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. Taraphder, Juana Moreno, Mark Jarrell, Nagamalleswararao Dasari, N. S. Vidhyadhiraja, Swagata Acharya","submitted_at":"2015-09-30T13:09:10Z","abstract_excerpt":"We have investigated the finite temperature dynamics of the singlet to doublet continuous quantum phase transition in the gapped Anderson impurity model using hybridization expansion continuous time quantum Monte-Carlo. Using the self-energy and the longitudinal static susceptibility, we obtain a phase diagram in the temperature-gap plane. The separatrix between the low temperature local moment phase and the high temperature generalized Fermi liquid phase of this phase diagram is shown to be the lower bound of the critical scaling region of the zero gap quantum critical point of interacting ty"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.09163","kind":"arxiv","version":4},"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":"2026-05-18T01:25:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"K0w5KZXmw1m/ML8LPwzSCv9uSqKdRpCq6yL1m8Lq0QYJBKLInyYZYKmoGmFRETHyyQBGiXI664Ipi61vhvzFBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T17:35:25.653352Z"},"content_sha256":"c918fc65d48da5eb312805f3f29d773fca932e0ad9466b0fb93f46ed61a6f7ee","schema_version":"1.0","event_id":"sha256:c918fc65d48da5eb312805f3f29d773fca932e0ad9466b0fb93f46ed61a6f7ee"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AM4U5V2S337CX3RIZ3D7UCYTME/bundle.json","state_url":"https://pith.science/pith/AM4U5V2S337CX3RIZ3D7UCYTME/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AM4U5V2S337CX3RIZ3D7UCYTME/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":"2026-06-09T17:35:25Z","links":{"resolver":"https://pith.science/pith/AM4U5V2S337CX3RIZ3D7UCYTME","bundle":"https://pith.science/pith/AM4U5V2S337CX3RIZ3D7UCYTME/bundle.json","state":"https://pith.science/pith/AM4U5V2S337CX3RIZ3D7UCYTME/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AM4U5V2S337CX3RIZ3D7UCYTME/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:AM4U5V2S337CX3RIZ3D7UCYTME","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":"e6ec7c8f5a9a82ef53bb661e316093e8bc01466b6ca1fdaa10b9f19465da2d10","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-09-30T13:09:10Z","title_canon_sha256":"cf610d2b29356dbc634379e916689a1d88fbd2c41ee05facaa58502d378b12d4"},"schema_version":"1.0","source":{"id":"1509.09163","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1509.09163","created_at":"2026-05-18T01:25:26Z"},{"alias_kind":"arxiv_version","alias_value":"1509.09163v4","created_at":"2026-05-18T01:25:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.09163","created_at":"2026-05-18T01:25:26Z"},{"alias_kind":"pith_short_12","alias_value":"AM4U5V2S337C","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_16","alias_value":"AM4U5V2S337CX3RI","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_8","alias_value":"AM4U5V2S","created_at":"2026-05-18T12:29:10Z"}],"graph_snapshots":[{"event_id":"sha256:c918fc65d48da5eb312805f3f29d773fca932e0ad9466b0fb93f46ed61a6f7ee","target":"graph","created_at":"2026-05-18T01:25:26Z","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 have investigated the finite temperature dynamics of the singlet to doublet continuous quantum phase transition in the gapped Anderson impurity model using hybridization expansion continuous time quantum Monte-Carlo. Using the self-energy and the longitudinal static susceptibility, we obtain a phase diagram in the temperature-gap plane. The separatrix between the low temperature local moment phase and the high temperature generalized Fermi liquid phase of this phase diagram is shown to be the lower bound of the critical scaling region of the zero gap quantum critical point of interacting ty","authors_text":"A. Taraphder, Juana Moreno, Mark Jarrell, Nagamalleswararao Dasari, N. S. Vidhyadhiraja, Swagata Acharya","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-09-30T13:09:10Z","title":"Quantum critical dynamics of a magnetic impurity in a semiconducting host"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.09163","kind":"arxiv","version":4},"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:b01cca0692abfe0651652713a2457514dfe929b1e1a3e4ef367c878e45270ba6","target":"record","created_at":"2026-05-18T01:25:26Z","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":"e6ec7c8f5a9a82ef53bb661e316093e8bc01466b6ca1fdaa10b9f19465da2d10","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-09-30T13:09:10Z","title_canon_sha256":"cf610d2b29356dbc634379e916689a1d88fbd2c41ee05facaa58502d378b12d4"},"schema_version":"1.0","source":{"id":"1509.09163","kind":"arxiv","version":4}},"canonical_sha256":"03394ed752defe2bee28cec7fa0b13610ecb03694696bcdcd7a5c01350755aeb","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"03394ed752defe2bee28cec7fa0b13610ecb03694696bcdcd7a5c01350755aeb","first_computed_at":"2026-05-18T01:25:26.061889Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:25:26.061889Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"kX5Hnm2N/cRs/NB5XQ1WU+DOgNgMXvVWxypuDJX0YUJx3SsK3Uh/gqvqPJs4+8Xrkm4wnuzIR9ksZi+QRUKZDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:25:26.062354Z","signed_message":"canonical_sha256_bytes"},"source_id":"1509.09163","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b01cca0692abfe0651652713a2457514dfe929b1e1a3e4ef367c878e45270ba6","sha256:c918fc65d48da5eb312805f3f29d773fca932e0ad9466b0fb93f46ed61a6f7ee"],"state_sha256":"3bcab36055b18a850606549f9b5b5847b6426318e888e5b6032b1caadc2812a2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oaBQBiSko+TKl63I67Zfd7vducVYZuVq4rwAjrHq5ZgV4yZnN5/6yQA0LUIuQB4IEKQuiz2OEVvHL/d7GxlWDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T17:35:25.681442Z","bundle_sha256":"c8a71d43aca9a91d069edd75d9e528d223aaefadcfdec8b4fc49cb2dd4669795"}}