{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:RLAX4QV2TWQI4EGV4T3LZEIYT4","short_pith_number":"pith:RLAX4QV2","schema_version":"1.0","canonical_sha256":"8ac17e42ba9da08e10d5e4f6bc91189f2dfac3a5712c26b5a8890cfb0e779e02","source":{"kind":"arxiv","id":"1402.6954","version":1},"attestation_state":"computed","paper":{"title":"Composition of Two Potentials","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math.MP"],"primary_cat":"math-ph","authors_text":"Khosrow Chadan, Reido Kobayashi, Ryu Sasaki","submitted_at":"2014-02-27T16:21:53Z","abstract_excerpt":"Given two potentials V0 and V1 together with a certain nodeless solution {\\phi}0 of V0, we form a composition of these two potentials. If V1 is exactly solvable, the composition is exactly solvable, too. By combining various solvable potentials in one-dimensional quantum mechanics, a huge variety of solvable compositions can be made."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1402.6954","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2014-02-27T16:21:53Z","cross_cats_sorted":["math.MP"],"title_canon_sha256":"47a1751e4ac7f91d6baf315dc56c4c8fb738ef03659abca4928ee8711f8fa384","abstract_canon_sha256":"15b6abaa9517a9e6ee764de7c71e4ccb473a90b349bfc062aadeee4f19b568fc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:57:36.530691Z","signature_b64":"weOBwlIOkrdsm8VRPGjVkJSwcM6pr0YB2XTXin7wiBvUbkJwK+KkSFJg78FtgzsIPxXloPa6tVJEtuAVtNtnBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8ac17e42ba9da08e10d5e4f6bc91189f2dfac3a5712c26b5a8890cfb0e779e02","last_reissued_at":"2026-05-18T02:57:36.530166Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:57:36.530166Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Composition of Two Potentials","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math.MP"],"primary_cat":"math-ph","authors_text":"Khosrow Chadan, Reido Kobayashi, Ryu Sasaki","submitted_at":"2014-02-27T16:21:53Z","abstract_excerpt":"Given two potentials V0 and V1 together with a certain nodeless solution {\\phi}0 of V0, we form a composition of these two potentials. If V1 is exactly solvable, the composition is exactly solvable, too. By combining various solvable potentials in one-dimensional quantum mechanics, a huge variety of solvable compositions can be made."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.6954","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1402.6954","created_at":"2026-05-18T02:57:36.530242+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.6954v1","created_at":"2026-05-18T02:57:36.530242+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.6954","created_at":"2026-05-18T02:57:36.530242+00:00"},{"alias_kind":"pith_short_12","alias_value":"RLAX4QV2TWQI","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_16","alias_value":"RLAX4QV2TWQI4EGV","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_8","alias_value":"RLAX4QV2","created_at":"2026-05-18T12:28:46.137349+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RLAX4QV2TWQI4EGV4T3LZEIYT4","json":"https://pith.science/pith/RLAX4QV2TWQI4EGV4T3LZEIYT4.json","graph_json":"https://pith.science/api/pith-number/RLAX4QV2TWQI4EGV4T3LZEIYT4/graph.json","events_json":"https://pith.science/api/pith-number/RLAX4QV2TWQI4EGV4T3LZEIYT4/events.json","paper":"https://pith.science/paper/RLAX4QV2"},"agent_actions":{"view_html":"https://pith.science/pith/RLAX4QV2TWQI4EGV4T3LZEIYT4","download_json":"https://pith.science/pith/RLAX4QV2TWQI4EGV4T3LZEIYT4.json","view_paper":"https://pith.science/paper/RLAX4QV2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.6954&json=true","fetch_graph":"https://pith.science/api/pith-number/RLAX4QV2TWQI4EGV4T3LZEIYT4/graph.json","fetch_events":"https://pith.science/api/pith-number/RLAX4QV2TWQI4EGV4T3LZEIYT4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RLAX4QV2TWQI4EGV4T3LZEIYT4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RLAX4QV2TWQI4EGV4T3LZEIYT4/action/storage_attestation","attest_author":"https://pith.science/pith/RLAX4QV2TWQI4EGV4T3LZEIYT4/action/author_attestation","sign_citation":"https://pith.science/pith/RLAX4QV2TWQI4EGV4T3LZEIYT4/action/citation_signature","submit_replication":"https://pith.science/pith/RLAX4QV2TWQI4EGV4T3LZEIYT4/action/replication_record"}},"created_at":"2026-05-18T02:57:36.530242+00:00","updated_at":"2026-05-18T02:57:36.530242+00:00"}