{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:436TFLO7ZZD2AY4WFLTEGZ6XGO","short_pith_number":"pith:436TFLO7","canonical_record":{"source":{"id":"1407.6687","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"hep-ph","submitted_at":"2014-07-24T18:48:12Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"92cd853615751612245d0e673d7f44e3dfa0eb1becb73980a7d1c87f9c0fe7e7","abstract_canon_sha256":"fa8b4c2c8153431de85bbdf15bc8f661804f776bd70ca7e3cf927067d74b463e"},"schema_version":"1.0"},"canonical_sha256":"e6fd32addfce47a063962ae64367d73380399b66ae8855dc4925cadfa8e32cc1","source":{"kind":"arxiv","id":"1407.6687","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.6687","created_at":"2026-05-18T01:28:39Z"},{"alias_kind":"arxiv_version","alias_value":"1407.6687v3","created_at":"2026-05-18T01:28:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.6687","created_at":"2026-05-18T01:28:39Z"},{"alias_kind":"pith_short_12","alias_value":"436TFLO7ZZD2","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"436TFLO7ZZD2AY4W","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"436TFLO7","created_at":"2026-05-18T12:28:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:436TFLO7ZZD2AY4WFLTEGZ6XGO","target":"record","payload":{"canonical_record":{"source":{"id":"1407.6687","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"hep-ph","submitted_at":"2014-07-24T18:48:12Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"92cd853615751612245d0e673d7f44e3dfa0eb1becb73980a7d1c87f9c0fe7e7","abstract_canon_sha256":"fa8b4c2c8153431de85bbdf15bc8f661804f776bd70ca7e3cf927067d74b463e"},"schema_version":"1.0"},"canonical_sha256":"e6fd32addfce47a063962ae64367d73380399b66ae8855dc4925cadfa8e32cc1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:28:39.301792Z","signature_b64":"75CW4RtaZ3RfU1dzSIXXByZX0hB1qwj0Xfq9XyiUnyY/X3grXvrKWQGQk4rs51ULFi5IdHB406Y0zTlDLUqGDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e6fd32addfce47a063962ae64367d73380399b66ae8855dc4925cadfa8e32cc1","last_reissued_at":"2026-05-18T01:28:39.301201Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:28:39.301201Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1407.6687","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:28:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RHU+o26GLwNeCGCRgitPnL/WTQS4ML+OMZ4jnVRtzvlbYwtIl/M6wPNop2Degzvj08gx0x5xVApYQDx8xCjXBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-01T23:52:08.211492Z"},"content_sha256":"2dc670a6cbfbfaa8a7a58c2d0da86fe2e64d418e7bdc817efd6e1ff52ddf33ab","schema_version":"1.0","event_id":"sha256:2dc670a6cbfbfaa8a7a58c2d0da86fe2e64d418e7bdc817efd6e1ff52ddf33ab"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:436TFLO7ZZD2AY4WFLTEGZ6XGO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Geometrical Scaling and the Dependence of the Average Transverse Momentum on the Multiplicity and Energy for the ALICE Experiment","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Larry McLerran, Michal Praszalowicz","submitted_at":"2014-07-24T18:48:12Z","abstract_excerpt":"We review the recent ALICE data on charged particle multiplicity in p-p collisions, and show that it exhibits Geometrical Scaling (GS) with energy dependence given with characteristic exponent $\\lambda=0.22$. Next, starting from the GS hypothesis and using results of the Color Glass Condensate effective theory, we calculate $< p_{\\text{T}}>$ as a function $N_{\\rm ch}$ including dependence on the scattering energy $W$. We show that $< p_{\\text{T}}>$ both in p-p and p-Pb collisions scales in terms of scaling variable $(W/W_{0})^{\\lambda/(2+\\lambda)}% \\sqrt{N_{\\mathrm{ch}}/S_{\\bot}}$ where $S_{\\b"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.6687","kind":"arxiv","version":3},"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":"2026-05-18T01:28:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QBB1V/6+eWViUVNd+Xtxr+xANvOM9v9Wx2PdR8iDr3S9zpuqDUNTYqTENcCEb8eXUV3KMEK6GtAONvl5HnsSDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-01T23:52:08.212065Z"},"content_sha256":"3f4be2c187b18f962b2ab666d7ae8e8f09e2ba8d597a374eeb196c51917e781b","schema_version":"1.0","event_id":"sha256:3f4be2c187b18f962b2ab666d7ae8e8f09e2ba8d597a374eeb196c51917e781b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/436TFLO7ZZD2AY4WFLTEGZ6XGO/bundle.json","state_url":"https://pith.science/pith/436TFLO7ZZD2AY4WFLTEGZ6XGO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/436TFLO7ZZD2AY4WFLTEGZ6XGO/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":"2026-07-01T23:52:08Z","links":{"resolver":"https://pith.science/pith/436TFLO7ZZD2AY4WFLTEGZ6XGO","bundle":"https://pith.science/pith/436TFLO7ZZD2AY4WFLTEGZ6XGO/bundle.json","state":"https://pith.science/pith/436TFLO7ZZD2AY4WFLTEGZ6XGO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/436TFLO7ZZD2AY4WFLTEGZ6XGO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:436TFLO7ZZD2AY4WFLTEGZ6XGO","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":"fa8b4c2c8153431de85bbdf15bc8f661804f776bd70ca7e3cf927067d74b463e","cross_cats_sorted":["nucl-th"],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"hep-ph","submitted_at":"2014-07-24T18:48:12Z","title_canon_sha256":"92cd853615751612245d0e673d7f44e3dfa0eb1becb73980a7d1c87f9c0fe7e7"},"schema_version":"1.0","source":{"id":"1407.6687","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.6687","created_at":"2026-05-18T01:28:39Z"},{"alias_kind":"arxiv_version","alias_value":"1407.6687v3","created_at":"2026-05-18T01:28:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.6687","created_at":"2026-05-18T01:28:39Z"},{"alias_kind":"pith_short_12","alias_value":"436TFLO7ZZD2","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"436TFLO7ZZD2AY4W","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"436TFLO7","created_at":"2026-05-18T12:28:11Z"}],"graph_snapshots":[{"event_id":"sha256:3f4be2c187b18f962b2ab666d7ae8e8f09e2ba8d597a374eeb196c51917e781b","target":"graph","created_at":"2026-05-18T01:28:39Z","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":"We review the recent ALICE data on charged particle multiplicity in p-p collisions, and show that it exhibits Geometrical Scaling (GS) with energy dependence given with characteristic exponent $\\lambda=0.22$. Next, starting from the GS hypothesis and using results of the Color Glass Condensate effective theory, we calculate $< p_{\\text{T}}>$ as a function $N_{\\rm ch}$ including dependence on the scattering energy $W$. We show that $< p_{\\text{T}}>$ both in p-p and p-Pb collisions scales in terms of scaling variable $(W/W_{0})^{\\lambda/(2+\\lambda)}% \\sqrt{N_{\\mathrm{ch}}/S_{\\bot}}$ where $S_{\\b","authors_text":"Larry McLerran, Michal Praszalowicz","cross_cats":["nucl-th"],"headline":"","license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"hep-ph","submitted_at":"2014-07-24T18:48:12Z","title":"Geometrical Scaling and the Dependence of the Average Transverse Momentum on the Multiplicity and Energy for the ALICE Experiment"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.6687","kind":"arxiv","version":3},"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":"sha256:2dc670a6cbfbfaa8a7a58c2d0da86fe2e64d418e7bdc817efd6e1ff52ddf33ab","target":"record","created_at":"2026-05-18T01:28:39Z","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":"fa8b4c2c8153431de85bbdf15bc8f661804f776bd70ca7e3cf927067d74b463e","cross_cats_sorted":["nucl-th"],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"hep-ph","submitted_at":"2014-07-24T18:48:12Z","title_canon_sha256":"92cd853615751612245d0e673d7f44e3dfa0eb1becb73980a7d1c87f9c0fe7e7"},"schema_version":"1.0","source":{"id":"1407.6687","kind":"arxiv","version":3}},"canonical_sha256":"e6fd32addfce47a063962ae64367d73380399b66ae8855dc4925cadfa8e32cc1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e6fd32addfce47a063962ae64367d73380399b66ae8855dc4925cadfa8e32cc1","first_computed_at":"2026-05-18T01:28:39.301201Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:28:39.301201Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"75CW4RtaZ3RfU1dzSIXXByZX0hB1qwj0Xfq9XyiUnyY/X3grXvrKWQGQk4rs51ULFi5IdHB406Y0zTlDLUqGDA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:28:39.301792Z","signed_message":"canonical_sha256_bytes"},"source_id":"1407.6687","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2dc670a6cbfbfaa8a7a58c2d0da86fe2e64d418e7bdc817efd6e1ff52ddf33ab","sha256:3f4be2c187b18f962b2ab666d7ae8e8f09e2ba8d597a374eeb196c51917e781b"],"state_sha256":"412d8d9965a5ee785faf991968247688dfa092844272425deff247d681e6733b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KJJywFWK3pfTI4X/MP/h0fVlIhAE38Vs9/jY3MAGmwi/VwHFsuFaqJ+cRSVfEJsEtnkyzODKDxOrcwDuZvp2DA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-01T23:52:08.215621Z","bundle_sha256":"443aea8b64cf230d73c2b4462c724e8f6581386d69d5a416a2b8ec230c63c7ad"}}