{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:6ZKZ4YPSZAMZAPXC7DZJNWC6SZ","short_pith_number":"pith:6ZKZ4YPS","canonical_record":{"source":{"id":"1610.04225","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-10-13T06:32:13Z","cross_cats_sorted":[],"title_canon_sha256":"54a381a8da416f5da7cae437b859e2e3941f97c409fd07fd4a79ad8caec8e115","abstract_canon_sha256":"551eecd24463a992a86da949632488b1e9be67884403e7954a542d6061c4291b"},"schema_version":"1.0"},"canonical_sha256":"f6559e61f2c819903ee2f8f296d85e9675ee3f2174e20b238bc7ffe817ffdffd","source":{"kind":"arxiv","id":"1610.04225","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.04225","created_at":"2026-05-18T01:02:20Z"},{"alias_kind":"arxiv_version","alias_value":"1610.04225v1","created_at":"2026-05-18T01:02:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.04225","created_at":"2026-05-18T01:02:20Z"},{"alias_kind":"pith_short_12","alias_value":"6ZKZ4YPSZAMZ","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"6ZKZ4YPSZAMZAPXC","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"6ZKZ4YPS","created_at":"2026-05-18T12:30:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:6ZKZ4YPSZAMZAPXC7DZJNWC6SZ","target":"record","payload":{"canonical_record":{"source":{"id":"1610.04225","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-10-13T06:32:13Z","cross_cats_sorted":[],"title_canon_sha256":"54a381a8da416f5da7cae437b859e2e3941f97c409fd07fd4a79ad8caec8e115","abstract_canon_sha256":"551eecd24463a992a86da949632488b1e9be67884403e7954a542d6061c4291b"},"schema_version":"1.0"},"canonical_sha256":"f6559e61f2c819903ee2f8f296d85e9675ee3f2174e20b238bc7ffe817ffdffd","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:02:20.262088Z","signature_b64":"TgLcHHE+jXbvFNxNAT+/h54pDnb5FvKuPMKIHtIL7kSzoe3NzdGmwt2MUzl8/6+Kh9TAOHtjPj4AI5QTqsKKAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f6559e61f2c819903ee2f8f296d85e9675ee3f2174e20b238bc7ffe817ffdffd","last_reissued_at":"2026-05-18T01:02:20.261407Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:02:20.261407Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1610.04225","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":"2026-05-18T01:02:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"G6JUnhCwgQxfJOc3uMEW44C7myB6Okn5gBPhL60DghO85Edy7tIP96u9eqOc9WxiriPLlZQV0ubOHpwoNsQmCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T06:48:43.544180Z"},"content_sha256":"6f91ffc21d6bdb160bc905ca06ea4fcb4c01f899f6b26a72cab2041cb6f64b6e","schema_version":"1.0","event_id":"sha256:6f91ffc21d6bdb160bc905ca06ea4fcb4c01f899f6b26a72cab2041cb6f64b6e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:6ZKZ4YPSZAMZAPXC7DZJNWC6SZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Analytical approximate bound state solution of Schr\\\"odinger equation in $D$-dimensions with a new mixed class of potential for arbitrary $\\ell$-state via asymptotic iteration method","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Tapas Das","submitted_at":"2016-10-13T06:32:13Z","abstract_excerpt":"The bound state solutions of the $D$-dimensional Schr\\\"{o}dinger equation for new mixed class of potential, $V(r)=\\frac{V_1}{r^2}+\\frac{V_2e^{-\\alpha r}}{r}+V_3coth\\alpha r+V_4\\,,$ are studied within the framework of the Pekeris approximation for any arbitrary $\\ell$-state. Asymptotic iteration method (AIM) is used for the work. The energy spectrum are obtained as well as their corresponding normalized eigenfunctions are derived in terms of generalized hypergeometric functions $\\,_{2}F_{1}(a,b,c;z)$. It is shown that using the Pekeris approximation, present potential model is very much capable"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.04225","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":"2026-05-18T01:02:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VxdMN4x5n6V/Mn/KsivUJ1FoXkgrTpBy1tCcY2Y8oLkS4ZNCIaaDaghgfY0quzUvto7wTQ2CGIKJ0w7NyHxZBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T06:48:43.544542Z"},"content_sha256":"c059da1b03fa4bd3083b4101458d09349356bbc97e409381eb55e2520b239eb6","schema_version":"1.0","event_id":"sha256:c059da1b03fa4bd3083b4101458d09349356bbc97e409381eb55e2520b239eb6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6ZKZ4YPSZAMZAPXC7DZJNWC6SZ/bundle.json","state_url":"https://pith.science/pith/6ZKZ4YPSZAMZAPXC7DZJNWC6SZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6ZKZ4YPSZAMZAPXC7DZJNWC6SZ/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":"2026-06-04T06:48:43Z","links":{"resolver":"https://pith.science/pith/6ZKZ4YPSZAMZAPXC7DZJNWC6SZ","bundle":"https://pith.science/pith/6ZKZ4YPSZAMZAPXC7DZJNWC6SZ/bundle.json","state":"https://pith.science/pith/6ZKZ4YPSZAMZAPXC7DZJNWC6SZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6ZKZ4YPSZAMZAPXC7DZJNWC6SZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:6ZKZ4YPSZAMZAPXC7DZJNWC6SZ","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":"551eecd24463a992a86da949632488b1e9be67884403e7954a542d6061c4291b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-10-13T06:32:13Z","title_canon_sha256":"54a381a8da416f5da7cae437b859e2e3941f97c409fd07fd4a79ad8caec8e115"},"schema_version":"1.0","source":{"id":"1610.04225","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.04225","created_at":"2026-05-18T01:02:20Z"},{"alias_kind":"arxiv_version","alias_value":"1610.04225v1","created_at":"2026-05-18T01:02:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.04225","created_at":"2026-05-18T01:02:20Z"},{"alias_kind":"pith_short_12","alias_value":"6ZKZ4YPSZAMZ","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"6ZKZ4YPSZAMZAPXC","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"6ZKZ4YPS","created_at":"2026-05-18T12:30:04Z"}],"graph_snapshots":[{"event_id":"sha256:c059da1b03fa4bd3083b4101458d09349356bbc97e409381eb55e2520b239eb6","target":"graph","created_at":"2026-05-18T01:02:20Z","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 bound state solutions of the $D$-dimensional Schr\\\"{o}dinger equation for new mixed class of potential, $V(r)=\\frac{V_1}{r^2}+\\frac{V_2e^{-\\alpha r}}{r}+V_3coth\\alpha r+V_4\\,,$ are studied within the framework of the Pekeris approximation for any arbitrary $\\ell$-state. Asymptotic iteration method (AIM) is used for the work. The energy spectrum are obtained as well as their corresponding normalized eigenfunctions are derived in terms of generalized hypergeometric functions $\\,_{2}F_{1}(a,b,c;z)$. It is shown that using the Pekeris approximation, present potential model is very much capable","authors_text":"Tapas Das","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-10-13T06:32:13Z","title":"Analytical approximate bound state solution of Schr\\\"odinger equation in $D$-dimensions with a new mixed class of potential for arbitrary $\\ell$-state via asymptotic iteration method"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.04225","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":"sha256:6f91ffc21d6bdb160bc905ca06ea4fcb4c01f899f6b26a72cab2041cb6f64b6e","target":"record","created_at":"2026-05-18T01:02:20Z","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":"551eecd24463a992a86da949632488b1e9be67884403e7954a542d6061c4291b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-10-13T06:32:13Z","title_canon_sha256":"54a381a8da416f5da7cae437b859e2e3941f97c409fd07fd4a79ad8caec8e115"},"schema_version":"1.0","source":{"id":"1610.04225","kind":"arxiv","version":1}},"canonical_sha256":"f6559e61f2c819903ee2f8f296d85e9675ee3f2174e20b238bc7ffe817ffdffd","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f6559e61f2c819903ee2f8f296d85e9675ee3f2174e20b238bc7ffe817ffdffd","first_computed_at":"2026-05-18T01:02:20.261407Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:02:20.261407Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TgLcHHE+jXbvFNxNAT+/h54pDnb5FvKuPMKIHtIL7kSzoe3NzdGmwt2MUzl8/6+Kh9TAOHtjPj4AI5QTqsKKAw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:02:20.262088Z","signed_message":"canonical_sha256_bytes"},"source_id":"1610.04225","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6f91ffc21d6bdb160bc905ca06ea4fcb4c01f899f6b26a72cab2041cb6f64b6e","sha256:c059da1b03fa4bd3083b4101458d09349356bbc97e409381eb55e2520b239eb6"],"state_sha256":"6eb6a5eac2831a5ccc527cbd5d046b0a59b18db689cbab07c90015b1ffec5ffc"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UaLWNyatXoPcI2LQNrdLBJyPleUppLGODHAsHWsHhowVa3TRu33BdXT2z60HbB0aOMXobLF0wblYiU3r/G65BQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-04T06:48:43.546929Z","bundle_sha256":"3e7a39f83429b554ff15c5b946e39fd677997f096f2866e75656bb7b4e080a24"}}