{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2006:5TZJUICXINTLOKSX2SXU33OANE","short_pith_number":"pith:5TZJUICX","canonical_record":{"source":{"id":"physics/0601106","kind":"arxiv","version":4},"metadata":{"license":"","primary_cat":"physics.soc-ph","submitted_at":"2006-01-16T13:14:08Z","cross_cats_sorted":["q-fin.TR"],"title_canon_sha256":"a761f1661312a8e9b1431e9e44fd977bbaf17406c881bc58b096eb9d715e2fb7","abstract_canon_sha256":"a11fad4b7127c61520321032b0334afb16e8452398a92af9b96798812be29c6e"},"schema_version":"1.0"},"canonical_sha256":"ecf29a20574366b72a57d4af4dedc069185f49c32a6258eb07c6bf36a6f7fc47","source":{"kind":"arxiv","id":"physics/0601106","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"physics/0601106","created_at":"2026-05-18T03:13:43Z"},{"alias_kind":"arxiv_version","alias_value":"physics/0601106v4","created_at":"2026-05-18T03:13:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0601106","created_at":"2026-05-18T03:13:43Z"},{"alias_kind":"pith_short_12","alias_value":"5TZJUICXINTL","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_16","alias_value":"5TZJUICXINTLOKSX","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_8","alias_value":"5TZJUICX","created_at":"2026-05-18T12:25:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2006:5TZJUICXINTLOKSX2SXU33OANE","target":"record","payload":{"canonical_record":{"source":{"id":"physics/0601106","kind":"arxiv","version":4},"metadata":{"license":"","primary_cat":"physics.soc-ph","submitted_at":"2006-01-16T13:14:08Z","cross_cats_sorted":["q-fin.TR"],"title_canon_sha256":"a761f1661312a8e9b1431e9e44fd977bbaf17406c881bc58b096eb9d715e2fb7","abstract_canon_sha256":"a11fad4b7127c61520321032b0334afb16e8452398a92af9b96798812be29c6e"},"schema_version":"1.0"},"canonical_sha256":"ecf29a20574366b72a57d4af4dedc069185f49c32a6258eb07c6bf36a6f7fc47","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:13:43.913911Z","signature_b64":"AJL2PUnzceIXO2OGnU59qgKOsojd843vp+pI7tzjwtGw/nluAndCXfrSolHw+DICGwPvgtpvUJvv9AL2SHCGAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ecf29a20574366b72a57d4af4dedc069185f49c32a6258eb07c6bf36a6f7fc47","last_reissued_at":"2026-05-18T03:13:43.912924Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:13:43.912924Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"physics/0601106","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:13:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"E2HRKK2tyHF/N2vSffdJdKseqAZMl8uxmX6XGy8IVpDSA/RTe2DLTQmFbPf9pSJF6vZIzw2Nt3AgMyO5Sr49Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T22:32:22.659418Z"},"content_sha256":"533df46a8f509a677c6ac52bf9314afb4684f54d8f079c4127b8cae90c45e883","schema_version":"1.0","event_id":"sha256:533df46a8f509a677c6ac52bf9314afb4684f54d8f079c4127b8cae90c45e883"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2006:5TZJUICXINTLOKSX2SXU33OANE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"An interacting-agent model of financial markets from the viewpoint of nonextensive statistical mechanics","license":"","headline":"","cross_cats":["q-fin.TR"],"primary_cat":"physics.soc-ph","authors_text":"Taisei Kaizoji","submitted_at":"2006-01-16T13:14:08Z","abstract_excerpt":"In this paper we present an interacting-agent model of stock markets. We describe a stock market through an Ising-like model in order to formulate the tendency of traders getting to be influenced by the other traders' investment attitudes [1], and formulate the traders' decision-making regarding investment as the maximum entropy principle for nonextensive entropy. We demonstrate that the equilibrium probability distribution function of the traders' investment attitude is the {\\it q-exponential distribution}. We also show that the power-law distribution of the volatility of price fluctuations, "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0601106","kind":"arxiv","version":4},"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":"2026-05-18T03:13:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"w9kNCSaItdwG3uMn5U28HPCdBU8yJS4Ifd3rN9uerWivdSaYhykvkrYDYqJOshifkeb0ADT9c85hjCCLg16vDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T22:32:22.659754Z"},"content_sha256":"92edb3ad003b5a44f0481abe94e37e7d6c9cb8264edf15e2fd0b00d537d98cda","schema_version":"1.0","event_id":"sha256:92edb3ad003b5a44f0481abe94e37e7d6c9cb8264edf15e2fd0b00d537d98cda"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5TZJUICXINTLOKSX2SXU33OANE/bundle.json","state_url":"https://pith.science/pith/5TZJUICXINTLOKSX2SXU33OANE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5TZJUICXINTLOKSX2SXU33OANE/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":"2026-06-08T22:32:22Z","links":{"resolver":"https://pith.science/pith/5TZJUICXINTLOKSX2SXU33OANE","bundle":"https://pith.science/pith/5TZJUICXINTLOKSX2SXU33OANE/bundle.json","state":"https://pith.science/pith/5TZJUICXINTLOKSX2SXU33OANE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5TZJUICXINTLOKSX2SXU33OANE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2006:5TZJUICXINTLOKSX2SXU33OANE","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":"a11fad4b7127c61520321032b0334afb16e8452398a92af9b96798812be29c6e","cross_cats_sorted":["q-fin.TR"],"license":"","primary_cat":"physics.soc-ph","submitted_at":"2006-01-16T13:14:08Z","title_canon_sha256":"a761f1661312a8e9b1431e9e44fd977bbaf17406c881bc58b096eb9d715e2fb7"},"schema_version":"1.0","source":{"id":"physics/0601106","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"physics/0601106","created_at":"2026-05-18T03:13:43Z"},{"alias_kind":"arxiv_version","alias_value":"physics/0601106v4","created_at":"2026-05-18T03:13:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0601106","created_at":"2026-05-18T03:13:43Z"},{"alias_kind":"pith_short_12","alias_value":"5TZJUICXINTL","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_16","alias_value":"5TZJUICXINTLOKSX","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_8","alias_value":"5TZJUICX","created_at":"2026-05-18T12:25:53Z"}],"graph_snapshots":[{"event_id":"sha256:92edb3ad003b5a44f0481abe94e37e7d6c9cb8264edf15e2fd0b00d537d98cda","target":"graph","created_at":"2026-05-18T03:13:43Z","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 we present an interacting-agent model of stock markets. We describe a stock market through an Ising-like model in order to formulate the tendency of traders getting to be influenced by the other traders' investment attitudes [1], and formulate the traders' decision-making regarding investment as the maximum entropy principle for nonextensive entropy. We demonstrate that the equilibrium probability distribution function of the traders' investment attitude is the {\\it q-exponential distribution}. We also show that the power-law distribution of the volatility of price fluctuations, ","authors_text":"Taisei Kaizoji","cross_cats":["q-fin.TR"],"headline":"","license":"","primary_cat":"physics.soc-ph","submitted_at":"2006-01-16T13:14:08Z","title":"An interacting-agent model of financial markets from the viewpoint of nonextensive statistical mechanics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0601106","kind":"arxiv","version":4},"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":"sha256:533df46a8f509a677c6ac52bf9314afb4684f54d8f079c4127b8cae90c45e883","target":"record","created_at":"2026-05-18T03:13:43Z","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":"a11fad4b7127c61520321032b0334afb16e8452398a92af9b96798812be29c6e","cross_cats_sorted":["q-fin.TR"],"license":"","primary_cat":"physics.soc-ph","submitted_at":"2006-01-16T13:14:08Z","title_canon_sha256":"a761f1661312a8e9b1431e9e44fd977bbaf17406c881bc58b096eb9d715e2fb7"},"schema_version":"1.0","source":{"id":"physics/0601106","kind":"arxiv","version":4}},"canonical_sha256":"ecf29a20574366b72a57d4af4dedc069185f49c32a6258eb07c6bf36a6f7fc47","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ecf29a20574366b72a57d4af4dedc069185f49c32a6258eb07c6bf36a6f7fc47","first_computed_at":"2026-05-18T03:13:43.912924Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:13:43.912924Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AJL2PUnzceIXO2OGnU59qgKOsojd843vp+pI7tzjwtGw/nluAndCXfrSolHw+DICGwPvgtpvUJvv9AL2SHCGAg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:13:43.913911Z","signed_message":"canonical_sha256_bytes"},"source_id":"physics/0601106","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:533df46a8f509a677c6ac52bf9314afb4684f54d8f079c4127b8cae90c45e883","sha256:92edb3ad003b5a44f0481abe94e37e7d6c9cb8264edf15e2fd0b00d537d98cda"],"state_sha256":"c4f9eb7f8c80ef28b318d330d911aba0bd671b1c3db94bd6849d7e0396917f4e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HoUMMtV8T/Rtfg/OrQWsh63fWTFRCF+5Tj21nLrlZSuYy4QPVxRTZVmaVU09sN7X5YHwruHpj/1wCrToSKOXDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-08T22:32:22.661498Z","bundle_sha256":"cd5ff789afd987cb3394ab4e40a24dbdd450f91bd26da526a81d44cb04ad9bea"}}