{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2009:4FFIZH3RSZ7AUQTDHBBB6AIASS","short_pith_number":"pith:4FFIZH3R","canonical_record":{"source":{"id":"0901.4216","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-01-27T10:28:57Z","cross_cats_sorted":[],"title_canon_sha256":"36c17f8f4a372cf58714faac19ded627bbd48a3c7842d425cac94bd2bbc3ebf1","abstract_canon_sha256":"4002a2a77f979f317ce165577014b8ad26573acbd9f3bcf29c56f65f9765e699"},"schema_version":"1.0"},"canonical_sha256":"e14a8c9f71967e0a426338421f0100949753f747a89a40745d7a9672d5020ffe","source":{"kind":"arxiv","id":"0901.4216","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0901.4216","created_at":"2026-05-18T02:35:06Z"},{"alias_kind":"arxiv_version","alias_value":"0901.4216v1","created_at":"2026-05-18T02:35:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0901.4216","created_at":"2026-05-18T02:35:06Z"},{"alias_kind":"pith_short_12","alias_value":"4FFIZH3RSZ7A","created_at":"2026-05-18T12:25:58Z"},{"alias_kind":"pith_short_16","alias_value":"4FFIZH3RSZ7AUQTD","created_at":"2026-05-18T12:25:58Z"},{"alias_kind":"pith_short_8","alias_value":"4FFIZH3R","created_at":"2026-05-18T12:25:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2009:4FFIZH3RSZ7AUQTDHBBB6AIASS","target":"record","payload":{"canonical_record":{"source":{"id":"0901.4216","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-01-27T10:28:57Z","cross_cats_sorted":[],"title_canon_sha256":"36c17f8f4a372cf58714faac19ded627bbd48a3c7842d425cac94bd2bbc3ebf1","abstract_canon_sha256":"4002a2a77f979f317ce165577014b8ad26573acbd9f3bcf29c56f65f9765e699"},"schema_version":"1.0"},"canonical_sha256":"e14a8c9f71967e0a426338421f0100949753f747a89a40745d7a9672d5020ffe","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:35:06.198441Z","signature_b64":"leqjLRgW4DwbNybAB2DqIIdVLG8jS5HoF/yod/H3MA9sHGsg1Si139QgEMK31ICOzLjro4yEBNUXN7jfOsD9Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e14a8c9f71967e0a426338421f0100949753f747a89a40745d7a9672d5020ffe","last_reissued_at":"2026-05-18T02:35:06.198021Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:35:06.198021Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0901.4216","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":"2026-05-18T02:35:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3TzVQNB1hzxJUIFnJXq87BOkdFfSYTfxJeyM1Txbj4hUKkFgLXPMLolkcmOQO8DTndy//F76qzHkx7NCbd5tDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T12:20:43.743255Z"},"content_sha256":"44820fe0a700ed15d68a59dbd0ff76c5cff5ef8b7465ed3e4fab661f57ae1284","schema_version":"1.0","event_id":"sha256:44820fe0a700ed15d68a59dbd0ff76c5cff5ef8b7465ed3e4fab661f57ae1284"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2009:4FFIZH3RSZ7AUQTDHBBB6AIASS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Do 1/r potentials require massless particles ?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M. Consoli","submitted_at":"2009-01-27T10:28:57Z","abstract_excerpt":"Long-range 1/r potentials play a fundamental role in physics. Their ultimate origin is usually traced back to the existence of genuine massless particles as photons or gravitons related to fundamental properties of continuum quantum field theories such as gauge invariance. In this Letter, it is argued that, in principle, an asymptotic, infinitesimally weak 1/r potential might also occur in the cutoff version of a simple, one-component spontaneously broken \\Phi^4 theory, after taking into account the peculiar nature of the zero-momentum limit of the connected scalar propagator. Physical interpr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0901.4216","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":"2026-05-18T02:35:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IwQuWOStPY0JKNMhGnw6VrYwDEPCepiWX7uxWsrLSe1OV7SeKhZdICnWqZ+dZGD/7FF9Hg8328JkWsX1fJtKDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T12:20:43.743832Z"},"content_sha256":"4f3cdb5567aadb83fdf287db0c12b34113beb1715d74eb406fabebe38b29c428","schema_version":"1.0","event_id":"sha256:4f3cdb5567aadb83fdf287db0c12b34113beb1715d74eb406fabebe38b29c428"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4FFIZH3RSZ7AUQTDHBBB6AIASS/bundle.json","state_url":"https://pith.science/pith/4FFIZH3RSZ7AUQTDHBBB6AIASS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4FFIZH3RSZ7AUQTDHBBB6AIASS/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":"2026-05-31T12:20:43Z","links":{"resolver":"https://pith.science/pith/4FFIZH3RSZ7AUQTDHBBB6AIASS","bundle":"https://pith.science/pith/4FFIZH3RSZ7AUQTDHBBB6AIASS/bundle.json","state":"https://pith.science/pith/4FFIZH3RSZ7AUQTDHBBB6AIASS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4FFIZH3RSZ7AUQTDHBBB6AIASS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:4FFIZH3RSZ7AUQTDHBBB6AIASS","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":"4002a2a77f979f317ce165577014b8ad26573acbd9f3bcf29c56f65f9765e699","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-01-27T10:28:57Z","title_canon_sha256":"36c17f8f4a372cf58714faac19ded627bbd48a3c7842d425cac94bd2bbc3ebf1"},"schema_version":"1.0","source":{"id":"0901.4216","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0901.4216","created_at":"2026-05-18T02:35:06Z"},{"alias_kind":"arxiv_version","alias_value":"0901.4216v1","created_at":"2026-05-18T02:35:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0901.4216","created_at":"2026-05-18T02:35:06Z"},{"alias_kind":"pith_short_12","alias_value":"4FFIZH3RSZ7A","created_at":"2026-05-18T12:25:58Z"},{"alias_kind":"pith_short_16","alias_value":"4FFIZH3RSZ7AUQTD","created_at":"2026-05-18T12:25:58Z"},{"alias_kind":"pith_short_8","alias_value":"4FFIZH3R","created_at":"2026-05-18T12:25:58Z"}],"graph_snapshots":[{"event_id":"sha256:4f3cdb5567aadb83fdf287db0c12b34113beb1715d74eb406fabebe38b29c428","target":"graph","created_at":"2026-05-18T02:35:06Z","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":"Long-range 1/r potentials play a fundamental role in physics. Their ultimate origin is usually traced back to the existence of genuine massless particles as photons or gravitons related to fundamental properties of continuum quantum field theories such as gauge invariance. In this Letter, it is argued that, in principle, an asymptotic, infinitesimally weak 1/r potential might also occur in the cutoff version of a simple, one-component spontaneously broken \\Phi^4 theory, after taking into account the peculiar nature of the zero-momentum limit of the connected scalar propagator. Physical interpr","authors_text":"M. Consoli","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-01-27T10:28:57Z","title":"Do 1/r potentials require massless particles ?"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0901.4216","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":"sha256:44820fe0a700ed15d68a59dbd0ff76c5cff5ef8b7465ed3e4fab661f57ae1284","target":"record","created_at":"2026-05-18T02:35:06Z","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":"4002a2a77f979f317ce165577014b8ad26573acbd9f3bcf29c56f65f9765e699","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-01-27T10:28:57Z","title_canon_sha256":"36c17f8f4a372cf58714faac19ded627bbd48a3c7842d425cac94bd2bbc3ebf1"},"schema_version":"1.0","source":{"id":"0901.4216","kind":"arxiv","version":1}},"canonical_sha256":"e14a8c9f71967e0a426338421f0100949753f747a89a40745d7a9672d5020ffe","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e14a8c9f71967e0a426338421f0100949753f747a89a40745d7a9672d5020ffe","first_computed_at":"2026-05-18T02:35:06.198021Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:35:06.198021Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"leqjLRgW4DwbNybAB2DqIIdVLG8jS5HoF/yod/H3MA9sHGsg1Si139QgEMK31ICOzLjro4yEBNUXN7jfOsD9Ag==","signature_status":"signed_v1","signed_at":"2026-05-18T02:35:06.198441Z","signed_message":"canonical_sha256_bytes"},"source_id":"0901.4216","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:44820fe0a700ed15d68a59dbd0ff76c5cff5ef8b7465ed3e4fab661f57ae1284","sha256:4f3cdb5567aadb83fdf287db0c12b34113beb1715d74eb406fabebe38b29c428"],"state_sha256":"11b59f25fca0544b626aa8ef8a86fb968e441b597b40cfd545c32aa96d8ba2b9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SjyluQW+ynVS2VH9VXBEazw+1WxjbY21cyzdI42rsqd5hbd3WnU0mTM0obeCxR9CCYJ8l2ZSab9ZAF5XaxPgAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T12:20:43.746710Z","bundle_sha256":"0e06e62cc56e1a8f9daf3a17619cbfad189fa44a39496183d21cd90c842ef717"}}