{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:3C6D2PZPMB26UFZUPOF2XLOOAZ","short_pith_number":"pith:3C6D2PZP","canonical_record":{"source":{"id":"1204.2673","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2012-04-12T10:17:37Z","cross_cats_sorted":[],"title_canon_sha256":"69545e141a4ea749513dc78fbe7cc1acc9c2fb198a714f038f3b065b6c6274dd","abstract_canon_sha256":"1fa0fb5a569c337aec5afc25b1a2eccb70a2d73741df719ec6b86e13df976d0e"},"schema_version":"1.0"},"canonical_sha256":"d8bc3d3f2f6075ea17347b8babadce0667e5d1302e647c799c73d44268550575","source":{"kind":"arxiv","id":"1204.2673","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1204.2673","created_at":"2026-05-18T01:57:53Z"},{"alias_kind":"arxiv_version","alias_value":"1204.2673v1","created_at":"2026-05-18T01:57:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1204.2673","created_at":"2026-05-18T01:57:53Z"},{"alias_kind":"pith_short_12","alias_value":"3C6D2PZPMB26","created_at":"2026-05-18T12:26:50Z"},{"alias_kind":"pith_short_16","alias_value":"3C6D2PZPMB26UFZU","created_at":"2026-05-18T12:26:50Z"},{"alias_kind":"pith_short_8","alias_value":"3C6D2PZP","created_at":"2026-05-18T12:26:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:3C6D2PZPMB26UFZUPOF2XLOOAZ","target":"record","payload":{"canonical_record":{"source":{"id":"1204.2673","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2012-04-12T10:17:37Z","cross_cats_sorted":[],"title_canon_sha256":"69545e141a4ea749513dc78fbe7cc1acc9c2fb198a714f038f3b065b6c6274dd","abstract_canon_sha256":"1fa0fb5a569c337aec5afc25b1a2eccb70a2d73741df719ec6b86e13df976d0e"},"schema_version":"1.0"},"canonical_sha256":"d8bc3d3f2f6075ea17347b8babadce0667e5d1302e647c799c73d44268550575","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:57:53.185571Z","signature_b64":"yr13iwZuCq5FdywUZ99/u2wal6rZQAO2ZvyvW6L5gta2QU7ryw/OvObPaZgpb/bVEL1jFO1fWoSfNsFXt3a2Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d8bc3d3f2f6075ea17347b8babadce0667e5d1302e647c799c73d44268550575","last_reissued_at":"2026-05-18T01:57:53.184989Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:57:53.184989Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1204.2673","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":"2026-05-18T01:57:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dQfr+BJA5WkgG2e91oQinDoTcH1DX22vkCP4bcxcsPLK7LZYo4xE0g3vJNbSvF7BB4auzeb4gQB2k3z7TCnVAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T18:49:32.733666Z"},"content_sha256":"91e2bded3a4f2905896efefc12bb6ffd8e171a3dd2483dd43a220f2977db2026","schema_version":"1.0","event_id":"sha256:91e2bded3a4f2905896efefc12bb6ffd8e171a3dd2483dd43a220f2977db2026"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:3C6D2PZPMB26UFZUPOF2XLOOAZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A new class of $f$-deformed charge coherent states and their nonclassical properties","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"M K Tavassoly, M Mortazavi","submitted_at":"2012-04-12T10:17:37Z","abstract_excerpt":"Two-mode charge (pair) coherent states has been introduced previously by using $<\\eta|$ representation. In the present paper we reobtain these states by a rather different method. Then, using the nonlinear coherent states approach and based on a simple manner by which the representation of two-mode charge coherent states is introduced, we generalize the bosonic creation and annihilation operators to the $f$-deformed ladder operators and construct a new class of $f$-deformed charge coherent states. Unlike the (linear) pair coherent states, our presented structure has the potentiality to generat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1204.2673","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":"2026-05-18T01:57:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/lPGAo6Yicwgq0hK8uLydxLC8Q+XLTsHiDIxOH7gC4kWcgz2ZOR5LTyPOXiWvnC67iePl6stTib5gUFeH9CLAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T18:49:32.734365Z"},"content_sha256":"5fa1dbd7d0fe3e60084b8b396dce1c8c584ba75dd57d4f1b732df3984a5acff5","schema_version":"1.0","event_id":"sha256:5fa1dbd7d0fe3e60084b8b396dce1c8c584ba75dd57d4f1b732df3984a5acff5"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3C6D2PZPMB26UFZUPOF2XLOOAZ/bundle.json","state_url":"https://pith.science/pith/3C6D2PZPMB26UFZUPOF2XLOOAZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3C6D2PZPMB26UFZUPOF2XLOOAZ/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":"2026-06-07T18:49:32Z","links":{"resolver":"https://pith.science/pith/3C6D2PZPMB26UFZUPOF2XLOOAZ","bundle":"https://pith.science/pith/3C6D2PZPMB26UFZUPOF2XLOOAZ/bundle.json","state":"https://pith.science/pith/3C6D2PZPMB26UFZUPOF2XLOOAZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3C6D2PZPMB26UFZUPOF2XLOOAZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:3C6D2PZPMB26UFZUPOF2XLOOAZ","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":"1fa0fb5a569c337aec5afc25b1a2eccb70a2d73741df719ec6b86e13df976d0e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2012-04-12T10:17:37Z","title_canon_sha256":"69545e141a4ea749513dc78fbe7cc1acc9c2fb198a714f038f3b065b6c6274dd"},"schema_version":"1.0","source":{"id":"1204.2673","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1204.2673","created_at":"2026-05-18T01:57:53Z"},{"alias_kind":"arxiv_version","alias_value":"1204.2673v1","created_at":"2026-05-18T01:57:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1204.2673","created_at":"2026-05-18T01:57:53Z"},{"alias_kind":"pith_short_12","alias_value":"3C6D2PZPMB26","created_at":"2026-05-18T12:26:50Z"},{"alias_kind":"pith_short_16","alias_value":"3C6D2PZPMB26UFZU","created_at":"2026-05-18T12:26:50Z"},{"alias_kind":"pith_short_8","alias_value":"3C6D2PZP","created_at":"2026-05-18T12:26:50Z"}],"graph_snapshots":[{"event_id":"sha256:5fa1dbd7d0fe3e60084b8b396dce1c8c584ba75dd57d4f1b732df3984a5acff5","target":"graph","created_at":"2026-05-18T01:57:53Z","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":"Two-mode charge (pair) coherent states has been introduced previously by using $<\\eta|$ representation. In the present paper we reobtain these states by a rather different method. Then, using the nonlinear coherent states approach and based on a simple manner by which the representation of two-mode charge coherent states is introduced, we generalize the bosonic creation and annihilation operators to the $f$-deformed ladder operators and construct a new class of $f$-deformed charge coherent states. Unlike the (linear) pair coherent states, our presented structure has the potentiality to generat","authors_text":"M K Tavassoly, M Mortazavi","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2012-04-12T10:17:37Z","title":"A new class of $f$-deformed charge coherent states and their nonclassical properties"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1204.2673","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":"sha256:91e2bded3a4f2905896efefc12bb6ffd8e171a3dd2483dd43a220f2977db2026","target":"record","created_at":"2026-05-18T01:57:53Z","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":"1fa0fb5a569c337aec5afc25b1a2eccb70a2d73741df719ec6b86e13df976d0e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2012-04-12T10:17:37Z","title_canon_sha256":"69545e141a4ea749513dc78fbe7cc1acc9c2fb198a714f038f3b065b6c6274dd"},"schema_version":"1.0","source":{"id":"1204.2673","kind":"arxiv","version":1}},"canonical_sha256":"d8bc3d3f2f6075ea17347b8babadce0667e5d1302e647c799c73d44268550575","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d8bc3d3f2f6075ea17347b8babadce0667e5d1302e647c799c73d44268550575","first_computed_at":"2026-05-18T01:57:53.184989Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:57:53.184989Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"yr13iwZuCq5FdywUZ99/u2wal6rZQAO2ZvyvW6L5gta2QU7ryw/OvObPaZgpb/bVEL1jFO1fWoSfNsFXt3a2Bg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:57:53.185571Z","signed_message":"canonical_sha256_bytes"},"source_id":"1204.2673","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:91e2bded3a4f2905896efefc12bb6ffd8e171a3dd2483dd43a220f2977db2026","sha256:5fa1dbd7d0fe3e60084b8b396dce1c8c584ba75dd57d4f1b732df3984a5acff5"],"state_sha256":"6fdc71a7f869b31590252a40b4ff46506e483fd0d65607832a7b2e6894e1e982"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bJceVCPoThGCP22a48GsYwPvawHljlq1g4NC3qG/4cAGtQCkbbiWvZSAyUZnwgaLIvSWoTNbrl+XJSbOaQulAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-07T18:49:32.738222Z","bundle_sha256":"7278b236723f8481084983bd690b04aa33dcc0ab970ed30dcc3e68588f5826c4"}}