{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:ASLSQK5I7LVP6BZ5DNC3Y35JBB","short_pith_number":"pith:ASLSQK5I","canonical_record":{"source":{"id":"1303.4100","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-03-17T21:02:27Z","cross_cats_sorted":[],"title_canon_sha256":"8a1dd20614510aad1f73692fd8ab043b0069928dbc0cf754a0b7883446b9bbd6","abstract_canon_sha256":"c180adf800059d7f87849b4f019d5f8ee5736b9de722a4d2144a39799f1b47fa"},"schema_version":"1.0"},"canonical_sha256":"0497282ba8faeaff073d1b45bc6fa90874c925568840efc1aa0365a89a76c980","source":{"kind":"arxiv","id":"1303.4100","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.4100","created_at":"2026-05-18T03:30:39Z"},{"alias_kind":"arxiv_version","alias_value":"1303.4100v1","created_at":"2026-05-18T03:30:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.4100","created_at":"2026-05-18T03:30:39Z"},{"alias_kind":"pith_short_12","alias_value":"ASLSQK5I7LVP","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_16","alias_value":"ASLSQK5I7LVP6BZ5","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_8","alias_value":"ASLSQK5I","created_at":"2026-05-18T12:27:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:ASLSQK5I7LVP6BZ5DNC3Y35JBB","target":"record","payload":{"canonical_record":{"source":{"id":"1303.4100","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-03-17T21:02:27Z","cross_cats_sorted":[],"title_canon_sha256":"8a1dd20614510aad1f73692fd8ab043b0069928dbc0cf754a0b7883446b9bbd6","abstract_canon_sha256":"c180adf800059d7f87849b4f019d5f8ee5736b9de722a4d2144a39799f1b47fa"},"schema_version":"1.0"},"canonical_sha256":"0497282ba8faeaff073d1b45bc6fa90874c925568840efc1aa0365a89a76c980","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:30:39.852013Z","signature_b64":"RRfAFeiWAVhztV8EgSQNCC4j79CIAHlMsT0S2z+cvMhBouajOZcRImctm6wng39YAZ0gzTvt7BMeG5F4xp11Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0497282ba8faeaff073d1b45bc6fa90874c925568840efc1aa0365a89a76c980","last_reissued_at":"2026-05-18T03:30:39.851205Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:30:39.851205Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1303.4100","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":"2026-05-18T03:30:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oAyT6eFCoLJq4bwzDTnZkDZ/yRY3pLfhleIonrGJZ6Kjxm0jSI0z9qub/Lol0Xq2v4mFSWRTzfQOYRKOAym5Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T14:16:18.255823Z"},"content_sha256":"cb16c2775223e44afce2ea8508f81ea409c4c66a3fbcd06518e5773201a47b84","schema_version":"1.0","event_id":"sha256:cb16c2775223e44afce2ea8508f81ea409c4c66a3fbcd06518e5773201a47b84"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:ASLSQK5I7LVP6BZ5DNC3Y35JBB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On the ladder operators and nonclassicality of generalized coherent state associated with a particle in an infinite square well","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"H R Jalali, M K Tavassoly","submitted_at":"2013-03-17T21:02:27Z","abstract_excerpt":"In this paper the factorization method is used in order to obtain the eigenvalues and eigenfunctions of a quantum particle confined in a one-dimensional infinite well. The output results from the mentioned approach allows us to explore an appropriate new pair of raising and lowering operators corresponding to the physical system under consideration. From the symmetrical considerations, the connection between the obtained ladder operators with $su(1,1)$ Lie algebra is explicitly established. Next, after the construction of Barut-Girardello and Gilmore-Perelomov representations of coherent state"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.4100","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":"2026-05-18T03:30:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SzKF9+burePCHCSX1l1pht/aKVdu5mskF0iPj96rphGz0czNd14sYcLFJR85gvklewPWb8Xz4PnHNq4hEcgOCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T14:16:18.256243Z"},"content_sha256":"b635bcc2f9b92f3aea183f20d593b7f04aa4d3fb83097876255a1970e6331242","schema_version":"1.0","event_id":"sha256:b635bcc2f9b92f3aea183f20d593b7f04aa4d3fb83097876255a1970e6331242"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ASLSQK5I7LVP6BZ5DNC3Y35JBB/bundle.json","state_url":"https://pith.science/pith/ASLSQK5I7LVP6BZ5DNC3Y35JBB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ASLSQK5I7LVP6BZ5DNC3Y35JBB/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":"2026-06-08T14:16:18Z","links":{"resolver":"https://pith.science/pith/ASLSQK5I7LVP6BZ5DNC3Y35JBB","bundle":"https://pith.science/pith/ASLSQK5I7LVP6BZ5DNC3Y35JBB/bundle.json","state":"https://pith.science/pith/ASLSQK5I7LVP6BZ5DNC3Y35JBB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ASLSQK5I7LVP6BZ5DNC3Y35JBB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:ASLSQK5I7LVP6BZ5DNC3Y35JBB","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":"c180adf800059d7f87849b4f019d5f8ee5736b9de722a4d2144a39799f1b47fa","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-03-17T21:02:27Z","title_canon_sha256":"8a1dd20614510aad1f73692fd8ab043b0069928dbc0cf754a0b7883446b9bbd6"},"schema_version":"1.0","source":{"id":"1303.4100","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.4100","created_at":"2026-05-18T03:30:39Z"},{"alias_kind":"arxiv_version","alias_value":"1303.4100v1","created_at":"2026-05-18T03:30:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.4100","created_at":"2026-05-18T03:30:39Z"},{"alias_kind":"pith_short_12","alias_value":"ASLSQK5I7LVP","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_16","alias_value":"ASLSQK5I7LVP6BZ5","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_8","alias_value":"ASLSQK5I","created_at":"2026-05-18T12:27:38Z"}],"graph_snapshots":[{"event_id":"sha256:b635bcc2f9b92f3aea183f20d593b7f04aa4d3fb83097876255a1970e6331242","target":"graph","created_at":"2026-05-18T03:30:39Z","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":"In this paper the factorization method is used in order to obtain the eigenvalues and eigenfunctions of a quantum particle confined in a one-dimensional infinite well. The output results from the mentioned approach allows us to explore an appropriate new pair of raising and lowering operators corresponding to the physical system under consideration. From the symmetrical considerations, the connection between the obtained ladder operators with $su(1,1)$ Lie algebra is explicitly established. Next, after the construction of Barut-Girardello and Gilmore-Perelomov representations of coherent state","authors_text":"H R Jalali, M K Tavassoly","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-03-17T21:02:27Z","title":"On the ladder operators and nonclassicality of generalized coherent state associated with a particle in an infinite square well"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.4100","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:cb16c2775223e44afce2ea8508f81ea409c4c66a3fbcd06518e5773201a47b84","target":"record","created_at":"2026-05-18T03:30:39Z","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":"c180adf800059d7f87849b4f019d5f8ee5736b9de722a4d2144a39799f1b47fa","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-03-17T21:02:27Z","title_canon_sha256":"8a1dd20614510aad1f73692fd8ab043b0069928dbc0cf754a0b7883446b9bbd6"},"schema_version":"1.0","source":{"id":"1303.4100","kind":"arxiv","version":1}},"canonical_sha256":"0497282ba8faeaff073d1b45bc6fa90874c925568840efc1aa0365a89a76c980","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0497282ba8faeaff073d1b45bc6fa90874c925568840efc1aa0365a89a76c980","first_computed_at":"2026-05-18T03:30:39.851205Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:30:39.851205Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"RRfAFeiWAVhztV8EgSQNCC4j79CIAHlMsT0S2z+cvMhBouajOZcRImctm6wng39YAZ0gzTvt7BMeG5F4xp11Bw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:30:39.852013Z","signed_message":"canonical_sha256_bytes"},"source_id":"1303.4100","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cb16c2775223e44afce2ea8508f81ea409c4c66a3fbcd06518e5773201a47b84","sha256:b635bcc2f9b92f3aea183f20d593b7f04aa4d3fb83097876255a1970e6331242"],"state_sha256":"f09938653b827557232ee004ae0fc35fbf8a769544edbff0411a359cff306acd"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZKhHiqbrQR93+zpB8sc5Ju1SDk2Vr+1O3JTgvNYYazn8nKnj8j/St1aMNaOLPQUB2ZkSbJ5u+Aju1z/t2LflCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-08T14:16:18.259337Z","bundle_sha256":"50755c56bea93e31423f249dfbcf2003dadd6da1c91759873dbd8869f856cfb0"}}