{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:GP2CXULK7HX54GK34O365L2MXF","short_pith_number":"pith:GP2CXULK","canonical_record":{"source":{"id":"1810.09135","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2018-10-22T08:28:55Z","cross_cats_sorted":["math.MP"],"title_canon_sha256":"83578ec499bfbb16cd715dfa8d87ca10c0099f0bda2fec46f5db00f6aa381ba9","abstract_canon_sha256":"7417ed9a0bbcfee5baddf43f88bd8c7c3bb084ef6e08d21b33f622bd180929d2"},"schema_version":"1.0"},"canonical_sha256":"33f42bd16af9efde195be3b7eeaf4cb95b45a71e74232c46abf30db380179b4d","source":{"kind":"arxiv","id":"1810.09135","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1810.09135","created_at":"2026-05-17T23:46:36Z"},{"alias_kind":"arxiv_version","alias_value":"1810.09135v3","created_at":"2026-05-17T23:46:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.09135","created_at":"2026-05-17T23:46:36Z"},{"alias_kind":"pith_short_12","alias_value":"GP2CXULK7HX5","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_16","alias_value":"GP2CXULK7HX54GK3","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_8","alias_value":"GP2CXULK","created_at":"2026-05-18T12:32:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:GP2CXULK7HX54GK34O365L2MXF","target":"record","payload":{"canonical_record":{"source":{"id":"1810.09135","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2018-10-22T08:28:55Z","cross_cats_sorted":["math.MP"],"title_canon_sha256":"83578ec499bfbb16cd715dfa8d87ca10c0099f0bda2fec46f5db00f6aa381ba9","abstract_canon_sha256":"7417ed9a0bbcfee5baddf43f88bd8c7c3bb084ef6e08d21b33f622bd180929d2"},"schema_version":"1.0"},"canonical_sha256":"33f42bd16af9efde195be3b7eeaf4cb95b45a71e74232c46abf30db380179b4d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:46:36.079896Z","signature_b64":"3X5lr5+rW9p6gPKyi2/4cjfV5HgX58gEjWOXCiWXeiw3Lx1mqcO4vXpXMMJUKCE/Tc2O5BbNPAifkTN30qqTDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"33f42bd16af9efde195be3b7eeaf4cb95b45a71e74232c46abf30db380179b4d","last_reissued_at":"2026-05-17T23:46:36.079284Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:46:36.079284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1810.09135","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:46:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OV1KkQiAnPEcrdV+dtF+nftOVD/yZD/TwWvMbiIy9Ft7MU0obGZ000FL2OZGISc5guNvxQ0X2/QsiqbAQGfQAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T11:27:12.331569Z"},"content_sha256":"26c1951c1e5781f873dd9b63a9882942ec666c1a44efe2ba168d6450c7bb4fce","schema_version":"1.0","event_id":"sha256:26c1951c1e5781f873dd9b63a9882942ec666c1a44efe2ba168d6450c7bb4fce"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:GP2CXULK7HX54GK34O365L2MXF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"One-Boson Scattering Processes in the massive Spin-Boson Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math.MP"],"primary_cat":"math-ph","authors_text":"Dirk-Andr\\'e Deckert, Felix H\\\"anle, J\\'er\\'emy Faupin, Miguel Ballesteros","submitted_at":"2018-10-22T08:28:55Z","abstract_excerpt":"The Spin-Boson model describes a two-level quantum system that interacts with a second-quantized boson scalar field. Recently the relation between the integral kernel of the scattering matrix and the resonance in this model has been established in [14] for the case of massless bosons. In the present work, we treat the massive case. On the one hand, one might rightfully expect that the massive case is easier to handle since, in contrast to the massless case, the corresponding Hamiltonian features a spectral gap. On the other hand, it turns out that the non-zero boson mass introduces a new compl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.09135","kind":"arxiv","version":3},"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":"2026-05-17T23:46:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bWt6XW+pPyFznGL6QWJeDNQ68CiAPq9MAPPvTAH2SV6y/cuRGu0H8m+MSWK+IEkfVr1Y800XB1BUbPEwoL/vBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T11:27:12.332216Z"},"content_sha256":"be29f200f85adaeecbd52d120584461f4316b8ce8398fa3d2c933e158a482561","schema_version":"1.0","event_id":"sha256:be29f200f85adaeecbd52d120584461f4316b8ce8398fa3d2c933e158a482561"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GP2CXULK7HX54GK34O365L2MXF/bundle.json","state_url":"https://pith.science/pith/GP2CXULK7HX54GK34O365L2MXF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GP2CXULK7HX54GK34O365L2MXF/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":"2026-06-02T11:27:12Z","links":{"resolver":"https://pith.science/pith/GP2CXULK7HX54GK34O365L2MXF","bundle":"https://pith.science/pith/GP2CXULK7HX54GK34O365L2MXF/bundle.json","state":"https://pith.science/pith/GP2CXULK7HX54GK34O365L2MXF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GP2CXULK7HX54GK34O365L2MXF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:GP2CXULK7HX54GK34O365L2MXF","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":"7417ed9a0bbcfee5baddf43f88bd8c7c3bb084ef6e08d21b33f622bd180929d2","cross_cats_sorted":["math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2018-10-22T08:28:55Z","title_canon_sha256":"83578ec499bfbb16cd715dfa8d87ca10c0099f0bda2fec46f5db00f6aa381ba9"},"schema_version":"1.0","source":{"id":"1810.09135","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1810.09135","created_at":"2026-05-17T23:46:36Z"},{"alias_kind":"arxiv_version","alias_value":"1810.09135v3","created_at":"2026-05-17T23:46:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.09135","created_at":"2026-05-17T23:46:36Z"},{"alias_kind":"pith_short_12","alias_value":"GP2CXULK7HX5","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_16","alias_value":"GP2CXULK7HX54GK3","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_8","alias_value":"GP2CXULK","created_at":"2026-05-18T12:32:25Z"}],"graph_snapshots":[{"event_id":"sha256:be29f200f85adaeecbd52d120584461f4316b8ce8398fa3d2c933e158a482561","target":"graph","created_at":"2026-05-17T23:46:36Z","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 Spin-Boson model describes a two-level quantum system that interacts with a second-quantized boson scalar field. Recently the relation between the integral kernel of the scattering matrix and the resonance in this model has been established in [14] for the case of massless bosons. In the present work, we treat the massive case. On the one hand, one might rightfully expect that the massive case is easier to handle since, in contrast to the massless case, the corresponding Hamiltonian features a spectral gap. On the other hand, it turns out that the non-zero boson mass introduces a new compl","authors_text":"Dirk-Andr\\'e Deckert, Felix H\\\"anle, J\\'er\\'emy Faupin, Miguel Ballesteros","cross_cats":["math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2018-10-22T08:28:55Z","title":"One-Boson Scattering Processes in the massive Spin-Boson Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.09135","kind":"arxiv","version":3},"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":"sha256:26c1951c1e5781f873dd9b63a9882942ec666c1a44efe2ba168d6450c7bb4fce","target":"record","created_at":"2026-05-17T23:46:36Z","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":"7417ed9a0bbcfee5baddf43f88bd8c7c3bb084ef6e08d21b33f622bd180929d2","cross_cats_sorted":["math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2018-10-22T08:28:55Z","title_canon_sha256":"83578ec499bfbb16cd715dfa8d87ca10c0099f0bda2fec46f5db00f6aa381ba9"},"schema_version":"1.0","source":{"id":"1810.09135","kind":"arxiv","version":3}},"canonical_sha256":"33f42bd16af9efde195be3b7eeaf4cb95b45a71e74232c46abf30db380179b4d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"33f42bd16af9efde195be3b7eeaf4cb95b45a71e74232c46abf30db380179b4d","first_computed_at":"2026-05-17T23:46:36.079284Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:46:36.079284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"3X5lr5+rW9p6gPKyi2/4cjfV5HgX58gEjWOXCiWXeiw3Lx1mqcO4vXpXMMJUKCE/Tc2O5BbNPAifkTN30qqTDg==","signature_status":"signed_v1","signed_at":"2026-05-17T23:46:36.079896Z","signed_message":"canonical_sha256_bytes"},"source_id":"1810.09135","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:26c1951c1e5781f873dd9b63a9882942ec666c1a44efe2ba168d6450c7bb4fce","sha256:be29f200f85adaeecbd52d120584461f4316b8ce8398fa3d2c933e158a482561"],"state_sha256":"f55606a3c0342a3af1632b5c76e91147cf701f6ff9b30114adf8e6572d7b3c58"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/kwgGfIdopuJR/Fk0fKAYN7nB4pm/NjZZpYP7aa7H2cgC8J2+0WU4ol5qeQHrEIyK6YRN8SVc562TpSmgUDzBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T11:27:12.335575Z","bundle_sha256":"62224f5c1ed25e0c166ec40c7cfe58c112bf54cf0f1f10382155594ade41ed3e"}}