{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2001:35AAI35E3JF6XF5BI4ODSUCSS5","short_pith_number":"pith:35AAI35E","canonical_record":{"source":{"id":"nucl-th/0109071","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2001-09-24T15:15:54Z","cross_cats_sorted":[],"title_canon_sha256":"7d4f2a9fc92b5bfd6f2dac6f79610329a2fd0ce40d65b6c138ae42cfa7abda8a","abstract_canon_sha256":"c3632b5bc48b6101c24d23535cf65c800d8a7098c75bb133ed4f8002c7197eab"},"schema_version":"1.0"},"canonical_sha256":"df40046fa4da4beb97a1471c395052974d1bf4932ceea6a36796631f9594f562","source":{"kind":"arxiv","id":"nucl-th/0109071","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0109071","created_at":"2026-07-04T16:28:41Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0109071v1","created_at":"2026-07-04T16:28:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0109071","created_at":"2026-07-04T16:28:41Z"},{"alias_kind":"pith_short_12","alias_value":"35AAI35E3JF6","created_at":"2026-07-04T16:28:41Z"},{"alias_kind":"pith_short_16","alias_value":"35AAI35E3JF6XF5B","created_at":"2026-07-04T16:28:41Z"},{"alias_kind":"pith_short_8","alias_value":"35AAI35E","created_at":"2026-07-04T16:28:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2001:35AAI35E3JF6XF5BI4ODSUCSS5","target":"record","payload":{"canonical_record":{"source":{"id":"nucl-th/0109071","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2001-09-24T15:15:54Z","cross_cats_sorted":[],"title_canon_sha256":"7d4f2a9fc92b5bfd6f2dac6f79610329a2fd0ce40d65b6c138ae42cfa7abda8a","abstract_canon_sha256":"c3632b5bc48b6101c24d23535cf65c800d8a7098c75bb133ed4f8002c7197eab"},"schema_version":"1.0"},"canonical_sha256":"df40046fa4da4beb97a1471c395052974d1bf4932ceea6a36796631f9594f562","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:28:41.219746Z","signature_b64":"jf9ujEiFqG6Pedqe+X1ibgnphOopwZ6ZkTMeOldfskaLIHOBzKfpLftxwylla2ggcgIwwVbZx/t40Ko5WJarDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"df40046fa4da4beb97a1471c395052974d1bf4932ceea6a36796631f9594f562","last_reissued_at":"2026-07-04T16:28:41.219407Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:28:41.219407Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"nucl-th/0109071","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":"2026-07-04T16:28:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7iw5aLAoml9cp2Lq9wbUOwru6AkA02/JD763BgVsgrd7gjRHk08tDNNnNeTb9MMfXboAO0tMPUKBPtMgDXA/Bw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T00:47:31.203827Z"},"content_sha256":"50f5a4a0ef002007f6530c8162a39adcd37573a79410b3879225f866eb54f45c","schema_version":"1.0","event_id":"sha256:50f5a4a0ef002007f6530c8162a39adcd37573a79410b3879225f866eb54f45c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2001:35AAI35E3JF6XF5BI4ODSUCSS5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Chiral 2$\\pi$-exchange NN-potentials: Relativistic $1/M^2$-Corrections","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"N. Kaiser","submitted_at":"2001-09-24T15:15:54Z","abstract_excerpt":"We calculate in baryon chiral perturbation theory the relativistic $1/M^2$-corrections to the leading order two-pion exchange diagrams. We give explicit expressions for the corresponding one-loop NN-amplitudes in momentum space. The resulting isovector central and isoscalar spin-spin and tensor NN-amplitudes involve non-static terms proportional to the squared nucleon center-of-mass momentum $p^2$. From the two-pion exchange box diagrams we obtain an isoscalar quadratic spin-orbit NN-amplitude. We give also analytical expressions for the corresponding NN-potentials in coordinate space. The dia"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0109071","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/nucl-th/0109071/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-04T16:28:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tQaME1/JfNaxOdVloru3MKXjStqv3+B5mYugXPA0CXa0OQibuWzRAzdUWQ2sQ+LVMZi0KyVgw0/zQo9O4nHLDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T00:47:31.204425Z"},"content_sha256":"c1d72187218dab16662136c75d2c3ad074cbc15f959a961aa8889069bc2d1f30","schema_version":"1.0","event_id":"sha256:c1d72187218dab16662136c75d2c3ad074cbc15f959a961aa8889069bc2d1f30"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/35AAI35E3JF6XF5BI4ODSUCSS5/bundle.json","state_url":"https://pith.science/pith/35AAI35E3JF6XF5BI4ODSUCSS5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/35AAI35E3JF6XF5BI4ODSUCSS5/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":"2026-08-06T00:47:31Z","links":{"resolver":"https://pith.science/pith/35AAI35E3JF6XF5BI4ODSUCSS5","bundle":"https://pith.science/pith/35AAI35E3JF6XF5BI4ODSUCSS5/bundle.json","state":"https://pith.science/pith/35AAI35E3JF6XF5BI4ODSUCSS5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/35AAI35E3JF6XF5BI4ODSUCSS5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2001:35AAI35E3JF6XF5BI4ODSUCSS5","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":"c3632b5bc48b6101c24d23535cf65c800d8a7098c75bb133ed4f8002c7197eab","cross_cats_sorted":[],"license":"","primary_cat":"nucl-th","submitted_at":"2001-09-24T15:15:54Z","title_canon_sha256":"7d4f2a9fc92b5bfd6f2dac6f79610329a2fd0ce40d65b6c138ae42cfa7abda8a"},"schema_version":"1.0","source":{"id":"nucl-th/0109071","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0109071","created_at":"2026-07-04T16:28:41Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0109071v1","created_at":"2026-07-04T16:28:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0109071","created_at":"2026-07-04T16:28:41Z"},{"alias_kind":"pith_short_12","alias_value":"35AAI35E3JF6","created_at":"2026-07-04T16:28:41Z"},{"alias_kind":"pith_short_16","alias_value":"35AAI35E3JF6XF5B","created_at":"2026-07-04T16:28:41Z"},{"alias_kind":"pith_short_8","alias_value":"35AAI35E","created_at":"2026-07-04T16:28:41Z"}],"graph_snapshots":[{"event_id":"sha256:c1d72187218dab16662136c75d2c3ad074cbc15f959a961aa8889069bc2d1f30","target":"graph","created_at":"2026-07-04T16:28:41Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/nucl-th/0109071/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We calculate in baryon chiral perturbation theory the relativistic $1/M^2$-corrections to the leading order two-pion exchange diagrams. We give explicit expressions for the corresponding one-loop NN-amplitudes in momentum space. The resulting isovector central and isoscalar spin-spin and tensor NN-amplitudes involve non-static terms proportional to the squared nucleon center-of-mass momentum $p^2$. From the two-pion exchange box diagrams we obtain an isoscalar quadratic spin-orbit NN-amplitude. We give also analytical expressions for the corresponding NN-potentials in coordinate space. The dia","authors_text":"N. Kaiser","cross_cats":[],"headline":"","license":"","primary_cat":"nucl-th","submitted_at":"2001-09-24T15:15:54Z","title":"Chiral 2$\\pi$-exchange NN-potentials: Relativistic $1/M^2$-Corrections"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0109071","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":"sha256:50f5a4a0ef002007f6530c8162a39adcd37573a79410b3879225f866eb54f45c","target":"record","created_at":"2026-07-04T16:28:41Z","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":"c3632b5bc48b6101c24d23535cf65c800d8a7098c75bb133ed4f8002c7197eab","cross_cats_sorted":[],"license":"","primary_cat":"nucl-th","submitted_at":"2001-09-24T15:15:54Z","title_canon_sha256":"7d4f2a9fc92b5bfd6f2dac6f79610329a2fd0ce40d65b6c138ae42cfa7abda8a"},"schema_version":"1.0","source":{"id":"nucl-th/0109071","kind":"arxiv","version":1}},"canonical_sha256":"df40046fa4da4beb97a1471c395052974d1bf4932ceea6a36796631f9594f562","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"df40046fa4da4beb97a1471c395052974d1bf4932ceea6a36796631f9594f562","first_computed_at":"2026-07-04T16:28:41.219407Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:28:41.219407Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jf9ujEiFqG6Pedqe+X1ibgnphOopwZ6ZkTMeOldfskaLIHOBzKfpLftxwylla2ggcgIwwVbZx/t40Ko5WJarDA==","signature_status":"signed_v1","signed_at":"2026-07-04T16:28:41.219746Z","signed_message":"canonical_sha256_bytes"},"source_id":"nucl-th/0109071","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:50f5a4a0ef002007f6530c8162a39adcd37573a79410b3879225f866eb54f45c","sha256:c1d72187218dab16662136c75d2c3ad074cbc15f959a961aa8889069bc2d1f30"],"state_sha256":"b5f390c7ec6581465323583bdce48fadf69de6d16d9109d251d456b15a5608b1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ApPWrmHsP3nJb658QS3pyqwE3l8hFYIZksbvvzJ1u0a/3w7xiSuWEIoYLlqXyVQTK/2ePiy5PxCzGDjAH9IaAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-06T00:47:31.210724Z","bundle_sha256":"03f7d6820ab9e100fe3fddc09c8b7d608544ae489b155ea88ccf14dee86d749f"}}