{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1996:PYB73XKNVSI3EET5VGSMR4VU7E","short_pith_number":"pith:PYB73XKN","canonical_record":{"source":{"id":"quant-ph/9604012","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"quant-ph","submitted_at":"1996-04-15T15:20:57Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"d6ffd067c9c469ab2ccccc40e7d793a8051caa3ec6cc2b0c819a87b965d3fdb7","abstract_canon_sha256":"299ebe805e5428fc13badf3623a3ef59e09cdcd7af8259916b5e9758343e1145"},"schema_version":"1.0"},"canonical_sha256":"7e03fddd4dac91b2127da9a4c8f2b4f939cb8bad92324e82c7c4bbc60a2179fc","source":{"kind":"arxiv","id":"quant-ph/9604012","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"quant-ph/9604012","created_at":"2026-05-18T01:37:53Z"},{"alias_kind":"arxiv_version","alias_value":"quant-ph/9604012v1","created_at":"2026-05-18T01:37:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.quant-ph/9604012","created_at":"2026-05-18T01:37:53Z"},{"alias_kind":"pith_short_12","alias_value":"PYB73XKNVSI3","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_16","alias_value":"PYB73XKNVSI3EET5","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_8","alias_value":"PYB73XKN","created_at":"2026-05-18T12:25:48Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1996:PYB73XKNVSI3EET5VGSMR4VU7E","target":"record","payload":{"canonical_record":{"source":{"id":"quant-ph/9604012","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"quant-ph","submitted_at":"1996-04-15T15:20:57Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"d6ffd067c9c469ab2ccccc40e7d793a8051caa3ec6cc2b0c819a87b965d3fdb7","abstract_canon_sha256":"299ebe805e5428fc13badf3623a3ef59e09cdcd7af8259916b5e9758343e1145"},"schema_version":"1.0"},"canonical_sha256":"7e03fddd4dac91b2127da9a4c8f2b4f939cb8bad92324e82c7c4bbc60a2179fc","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:37:53.393539Z","signature_b64":"SSz+uYAo3skbXKNLMvdX0x/fpiwNIa2/JQt7KX4yEVZgP/JoxDucoZmvWCT+pXV0YnegDGgCeXjBQN0pypnWCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7e03fddd4dac91b2127da9a4c8f2b4f939cb8bad92324e82c7c4bbc60a2179fc","last_reissued_at":"2026-05-18T01:37:53.392948Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:37:53.392948Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"quant-ph/9604012","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":"2026-05-18T01:37:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zTNtTCZTTTXxDDulFCwGHWDJ4TvCz4dwNXd/APODZfQ8fncnHYYUgjngBmDzQA2hMslysM3tUWkQnha/7VJwBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-28T19:15:26.821606Z"},"content_sha256":"d22ca7d25bba8d41a1b82d5bfae261fe640f2138f6817c74fc8140d382fe64b6","schema_version":"1.0","event_id":"sha256:d22ca7d25bba8d41a1b82d5bfae261fe640f2138f6817c74fc8140d382fe64b6"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1996:PYB73XKNVSI3EET5VGSMR4VU7E","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Small-angle scattering on a system of magnetic and electric charges","license":"","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"quant-ph","authors_text":"M. Penttinen","submitted_at":"1996-04-15T15:20:57Z","abstract_excerpt":"The generalization of the conformal scattering method for small-angle scattering processes involving magnetic monopoles and ordinary charges is constructed. Using this generalization we show that introducing of magnetic charges corresponds to analytical continuation of the eikonal amplitude in the complex charge plane (the imaginary part is proportional to the magnetic charge). We calculate explicitly the eikonal amplitude for scattering on a dyon and two monopoles in terms of confluent hypergeometric functions. The singularities of the corresponding amplitudes (focal points) are studied in de"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"quant-ph/9604012","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":"2026-05-18T01:37:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PUQzf28u2jUiQ+atfS60i40zIkufxOXZ7mj4pU9gNXAQ5/ori7RIqRyWzhUhbSy4nL4Fz576Okek9Ms2CvjuBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-28T19:15:26.821947Z"},"content_sha256":"2e8fde3d244e062f9d1ad154c65a74cfce655339c3370dab0fca3f04726b5aca","schema_version":"1.0","event_id":"sha256:2e8fde3d244e062f9d1ad154c65a74cfce655339c3370dab0fca3f04726b5aca"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PYB73XKNVSI3EET5VGSMR4VU7E/bundle.json","state_url":"https://pith.science/pith/PYB73XKNVSI3EET5VGSMR4VU7E/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PYB73XKNVSI3EET5VGSMR4VU7E/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":"2026-06-28T19:15:26Z","links":{"resolver":"https://pith.science/pith/PYB73XKNVSI3EET5VGSMR4VU7E","bundle":"https://pith.science/pith/PYB73XKNVSI3EET5VGSMR4VU7E/bundle.json","state":"https://pith.science/pith/PYB73XKNVSI3EET5VGSMR4VU7E/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PYB73XKNVSI3EET5VGSMR4VU7E/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1996:PYB73XKNVSI3EET5VGSMR4VU7E","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":"299ebe805e5428fc13badf3623a3ef59e09cdcd7af8259916b5e9758343e1145","cross_cats_sorted":["hep-ph","hep-th"],"license":"","primary_cat":"quant-ph","submitted_at":"1996-04-15T15:20:57Z","title_canon_sha256":"d6ffd067c9c469ab2ccccc40e7d793a8051caa3ec6cc2b0c819a87b965d3fdb7"},"schema_version":"1.0","source":{"id":"quant-ph/9604012","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"quant-ph/9604012","created_at":"2026-05-18T01:37:53Z"},{"alias_kind":"arxiv_version","alias_value":"quant-ph/9604012v1","created_at":"2026-05-18T01:37:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.quant-ph/9604012","created_at":"2026-05-18T01:37:53Z"},{"alias_kind":"pith_short_12","alias_value":"PYB73XKNVSI3","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_16","alias_value":"PYB73XKNVSI3EET5","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_8","alias_value":"PYB73XKN","created_at":"2026-05-18T12:25:48Z"}],"graph_snapshots":[{"event_id":"sha256:2e8fde3d244e062f9d1ad154c65a74cfce655339c3370dab0fca3f04726b5aca","target":"graph","created_at":"2026-05-18T01:37:53Z","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 generalization of the conformal scattering method for small-angle scattering processes involving magnetic monopoles and ordinary charges is constructed. Using this generalization we show that introducing of magnetic charges corresponds to analytical continuation of the eikonal amplitude in the complex charge plane (the imaginary part is proportional to the magnetic charge). We calculate explicitly the eikonal amplitude for scattering on a dyon and two monopoles in terms of confluent hypergeometric functions. The singularities of the corresponding amplitudes (focal points) are studied in de","authors_text":"M. Penttinen","cross_cats":["hep-ph","hep-th"],"headline":"","license":"","primary_cat":"quant-ph","submitted_at":"1996-04-15T15:20:57Z","title":"Small-angle scattering on a system of magnetic and electric charges"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"quant-ph/9604012","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:d22ca7d25bba8d41a1b82d5bfae261fe640f2138f6817c74fc8140d382fe64b6","target":"record","created_at":"2026-05-18T01:37:53Z","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":"299ebe805e5428fc13badf3623a3ef59e09cdcd7af8259916b5e9758343e1145","cross_cats_sorted":["hep-ph","hep-th"],"license":"","primary_cat":"quant-ph","submitted_at":"1996-04-15T15:20:57Z","title_canon_sha256":"d6ffd067c9c469ab2ccccc40e7d793a8051caa3ec6cc2b0c819a87b965d3fdb7"},"schema_version":"1.0","source":{"id":"quant-ph/9604012","kind":"arxiv","version":1}},"canonical_sha256":"7e03fddd4dac91b2127da9a4c8f2b4f939cb8bad92324e82c7c4bbc60a2179fc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7e03fddd4dac91b2127da9a4c8f2b4f939cb8bad92324e82c7c4bbc60a2179fc","first_computed_at":"2026-05-18T01:37:53.392948Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:37:53.392948Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"SSz+uYAo3skbXKNLMvdX0x/fpiwNIa2/JQt7KX4yEVZgP/JoxDucoZmvWCT+pXV0YnegDGgCeXjBQN0pypnWCA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:37:53.393539Z","signed_message":"canonical_sha256_bytes"},"source_id":"quant-ph/9604012","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d22ca7d25bba8d41a1b82d5bfae261fe640f2138f6817c74fc8140d382fe64b6","sha256:2e8fde3d244e062f9d1ad154c65a74cfce655339c3370dab0fca3f04726b5aca"],"state_sha256":"7e289bafa44b8a6e148a5d353f2c925bf46355f3eadd92cf14de390634fef543"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"R0NyR+gAyrlzKdUziLxoL7qfhDL8aqFPCWhglrAk8kL4aT04DKtuw6swcWP3KOCcJUtnTh6fxvwR4FAzBSXRDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-28T19:15:26.823861Z","bundle_sha256":"6dc475093ae13ecc348d319a047f64410e658320976039a1448e8d977d6149b0"}}