{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:TTIA54LLAGCQ6BP4SVICSMTDS2","short_pith_number":"pith:TTIA54LL","canonical_record":{"source":{"id":"1212.1281","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-06T10:40:55Z","cross_cats_sorted":[],"title_canon_sha256":"4fca6a1eadb2bcc872a685c2c3306de60dbafc456672e947e661fcd207ea688a","abstract_canon_sha256":"5ed019c3a718f53b9232d2ff4b7c7d207b9282a3081743184e8369c1af6b1e22"},"schema_version":"1.0"},"canonical_sha256":"9cd00ef16b01850f05fc95502932639686b07cc7315b719a33ff6892f643f572","source":{"kind":"arxiv","id":"1212.1281","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1212.1281","created_at":"2026-05-18T02:19:44Z"},{"alias_kind":"arxiv_version","alias_value":"1212.1281v1","created_at":"2026-05-18T02:19:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.1281","created_at":"2026-05-18T02:19:44Z"},{"alias_kind":"pith_short_12","alias_value":"TTIA54LLAGCQ","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_16","alias_value":"TTIA54LLAGCQ6BP4","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_8","alias_value":"TTIA54LL","created_at":"2026-05-18T12:27:23Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:TTIA54LLAGCQ6BP4SVICSMTDS2","target":"record","payload":{"canonical_record":{"source":{"id":"1212.1281","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-06T10:40:55Z","cross_cats_sorted":[],"title_canon_sha256":"4fca6a1eadb2bcc872a685c2c3306de60dbafc456672e947e661fcd207ea688a","abstract_canon_sha256":"5ed019c3a718f53b9232d2ff4b7c7d207b9282a3081743184e8369c1af6b1e22"},"schema_version":"1.0"},"canonical_sha256":"9cd00ef16b01850f05fc95502932639686b07cc7315b719a33ff6892f643f572","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:19:44.001107Z","signature_b64":"15wB+6fSzFHICmHvExW/dl3QmeSGGzP4HVZTkgP+tHM8vfooRWqC+6lU5tv3/p8KzeEqa1NAJ/XThppUVy9dBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9cd00ef16b01850f05fc95502932639686b07cc7315b719a33ff6892f643f572","last_reissued_at":"2026-05-18T02:19:44.000715Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:19:44.000715Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1212.1281","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":"2026-05-18T02:19:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PCA/8IjCmXs7F0pcGi7pgEISmFSQ1qaDSHlcxRQTIYoSSVL7xQrw6avUmT8sL1DrX8asDGqraohcwe3f5wAGAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T16:06:48.088584Z"},"content_sha256":"4b41676fd41c8c3a0a08d2a53dd7bd039e8765c5db7889949ad3153c49fc7ba5","schema_version":"1.0","event_id":"sha256:4b41676fd41c8c3a0a08d2a53dd7bd039e8765c5db7889949ad3153c49fc7ba5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:TTIA54LLAGCQ6BP4SVICSMTDS2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Scaling behavior of transverse momenta distributions in hadronic and nuclear collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"G. Wilk, M. Rybczynski, Z. Wlodarczyk","submitted_at":"2012-12-06T10:40:55Z","abstract_excerpt":"It has been recently noticed that transverse momenta ($p_T$) distributions observed in high energy production processes exhibit remarkably universal scaling behavior. This is seen when they are in some suitable variable, replacing the usual $p_T$. On the other hand, it is also known that transverse momenta distributions in general follow a power-like Tsallis distribution, rather than an exponential Boltzmann-Gibbs, with a (generally energy dependent) nonextensivity parameter $q$. We now show that it is possible to choose a suitable variable such that $p_T$ distributions of particles produced i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.1281","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":"2026-05-18T02:19:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yKi5qUAbiV8X0dIIscIoC51WqK4U28EuniHQlXovfjY8sgAGNvD8QwInSeujE1D2fB/aZ9aInWXdfna+aTnuBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T16:06:48.089222Z"},"content_sha256":"73ca5e0fc022682b31f726c308d942f2b520f734545f8ab0fe96766edb5b7b20","schema_version":"1.0","event_id":"sha256:73ca5e0fc022682b31f726c308d942f2b520f734545f8ab0fe96766edb5b7b20"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TTIA54LLAGCQ6BP4SVICSMTDS2/bundle.json","state_url":"https://pith.science/pith/TTIA54LLAGCQ6BP4SVICSMTDS2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TTIA54LLAGCQ6BP4SVICSMTDS2/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":"2026-05-25T16:06:48Z","links":{"resolver":"https://pith.science/pith/TTIA54LLAGCQ6BP4SVICSMTDS2","bundle":"https://pith.science/pith/TTIA54LLAGCQ6BP4SVICSMTDS2/bundle.json","state":"https://pith.science/pith/TTIA54LLAGCQ6BP4SVICSMTDS2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TTIA54LLAGCQ6BP4SVICSMTDS2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:TTIA54LLAGCQ6BP4SVICSMTDS2","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":"5ed019c3a718f53b9232d2ff4b7c7d207b9282a3081743184e8369c1af6b1e22","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-06T10:40:55Z","title_canon_sha256":"4fca6a1eadb2bcc872a685c2c3306de60dbafc456672e947e661fcd207ea688a"},"schema_version":"1.0","source":{"id":"1212.1281","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1212.1281","created_at":"2026-05-18T02:19:44Z"},{"alias_kind":"arxiv_version","alias_value":"1212.1281v1","created_at":"2026-05-18T02:19:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.1281","created_at":"2026-05-18T02:19:44Z"},{"alias_kind":"pith_short_12","alias_value":"TTIA54LLAGCQ","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_16","alias_value":"TTIA54LLAGCQ6BP4","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_8","alias_value":"TTIA54LL","created_at":"2026-05-18T12:27:23Z"}],"graph_snapshots":[{"event_id":"sha256:73ca5e0fc022682b31f726c308d942f2b520f734545f8ab0fe96766edb5b7b20","target":"graph","created_at":"2026-05-18T02:19:44Z","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":"It has been recently noticed that transverse momenta ($p_T$) distributions observed in high energy production processes exhibit remarkably universal scaling behavior. This is seen when they are in some suitable variable, replacing the usual $p_T$. On the other hand, it is also known that transverse momenta distributions in general follow a power-like Tsallis distribution, rather than an exponential Boltzmann-Gibbs, with a (generally energy dependent) nonextensivity parameter $q$. We now show that it is possible to choose a suitable variable such that $p_T$ distributions of particles produced i","authors_text":"G. Wilk, M. Rybczynski, Z. Wlodarczyk","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-06T10:40:55Z","title":"Scaling behavior of transverse momenta distributions in hadronic and nuclear collisions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.1281","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":"sha256:4b41676fd41c8c3a0a08d2a53dd7bd039e8765c5db7889949ad3153c49fc7ba5","target":"record","created_at":"2026-05-18T02:19:44Z","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":"5ed019c3a718f53b9232d2ff4b7c7d207b9282a3081743184e8369c1af6b1e22","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-06T10:40:55Z","title_canon_sha256":"4fca6a1eadb2bcc872a685c2c3306de60dbafc456672e947e661fcd207ea688a"},"schema_version":"1.0","source":{"id":"1212.1281","kind":"arxiv","version":1}},"canonical_sha256":"9cd00ef16b01850f05fc95502932639686b07cc7315b719a33ff6892f643f572","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9cd00ef16b01850f05fc95502932639686b07cc7315b719a33ff6892f643f572","first_computed_at":"2026-05-18T02:19:44.000715Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:19:44.000715Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"15wB+6fSzFHICmHvExW/dl3QmeSGGzP4HVZTkgP+tHM8vfooRWqC+6lU5tv3/p8KzeEqa1NAJ/XThppUVy9dBw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:19:44.001107Z","signed_message":"canonical_sha256_bytes"},"source_id":"1212.1281","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4b41676fd41c8c3a0a08d2a53dd7bd039e8765c5db7889949ad3153c49fc7ba5","sha256:73ca5e0fc022682b31f726c308d942f2b520f734545f8ab0fe96766edb5b7b20"],"state_sha256":"2a95622bc7dff549aa8991858a33825731b6f0f5e8bb581ed5f7f930710c25e9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MyfDgpixAYN7EKIGdcEwQcjByC75EU9IsQiIwxa1yoVASkBGWSYFUsUeu2mX+l6KvAjxsKLKl5UfGrXmKnXHAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T16:06:48.092781Z","bundle_sha256":"1c53091cac4fadda28a47e7bf4362b0bab0d05d140fa86ca5bee20d92286ad54"}}