{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2001:Y3A7Y4OGXHYLY27R4CP57JLDYD","short_pith_number":"pith:Y3A7Y4OG","canonical_record":{"source":{"id":"hep-lat/0110103","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2001-10-15T16:29:15Z","cross_cats_sorted":[],"title_canon_sha256":"ce17ead10ba4876b34af3fe7b8d4b3588e950c566cac0dfec4f3326690918d10","abstract_canon_sha256":"5faf2e91b6c0aa0c1717cdba5933a90edf0f4695d8b497648ec3e61c8addf5de"},"schema_version":"1.0"},"canonical_sha256":"c6c1fc71c6b9f0bc6bf1e09fdfa563c0d32a473d3e29733bce658544a4b5cf16","source":{"kind":"arxiv","id":"hep-lat/0110103","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0110103","created_at":"2026-05-18T01:39:14Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0110103v1","created_at":"2026-05-18T01:39:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0110103","created_at":"2026-05-18T01:39:14Z"},{"alias_kind":"pith_short_12","alias_value":"Y3A7Y4OGXHYL","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"Y3A7Y4OGXHYLY27R","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"Y3A7Y4OG","created_at":"2026-05-18T12:25:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2001:Y3A7Y4OGXHYLY27R4CP57JLDYD","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/0110103","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2001-10-15T16:29:15Z","cross_cats_sorted":[],"title_canon_sha256":"ce17ead10ba4876b34af3fe7b8d4b3588e950c566cac0dfec4f3326690918d10","abstract_canon_sha256":"5faf2e91b6c0aa0c1717cdba5933a90edf0f4695d8b497648ec3e61c8addf5de"},"schema_version":"1.0"},"canonical_sha256":"c6c1fc71c6b9f0bc6bf1e09fdfa563c0d32a473d3e29733bce658544a4b5cf16","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:14.855843Z","signature_b64":"IYvIj14UC4SfuFcqBJcquEXk6zG9/qD+3WC6vqnX7MjYveNMdnZ3rsDpkBaQHqkivewehx5hqDbzvRjgfD+gBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c6c1fc71c6b9f0bc6bf1e09fdfa563c0d32a473d3e29733bce658544a4b5cf16","last_reissued_at":"2026-05-18T01:39:14.855297Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:14.855297Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/0110103","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":"2026-05-18T01:39:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kfTJCnMyp11n9eSil9VVThlxtosv0nyCK2R+8dCvqhErCyWQb5GolQKIdxdKHVWHxZHe5a+HfZk9dC5ykh2BBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T18:05:39.061442Z"},"content_sha256":"b36a63b1594b1fdf85ec2713e6a98fdb9b6badc859dc6d044cfb5231a41d151e","schema_version":"1.0","event_id":"sha256:b36a63b1594b1fdf85ec2713e6a98fdb9b6badc859dc6d044cfb5231a41d151e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2001:Y3A7Y4OGXHYLY27R4CP57JLDYD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Short distance physics with heavy quark potentials","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"F. Karsch, F. Zantow, O. Kaczmarek, P. Petreczky","submitted_at":"2001-10-15T16:29:15Z","abstract_excerpt":"We present lattice studies of heavy quark potentials in the quenched approximation of QCD at finite temperatures. Both, the color singlet and color averaged potentials are calculated. While the potentials are well known at large distances, we give a detailed analysis of their short distance behavior (from 0.015 fm to 1 fm) near the critical temperature. At these distances we expect that the T-dependent potentials go over into the zero temperature potential. Indeed, we find evidences that the temperature influence gets suppressed and the potentials starts to become a unique function of the unde"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0110103","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":"2026-05-18T01:39:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AR6ZmG8NUdpUWRh0O8Ied/XdQNoR/em44Pl39o6um3T3m76BUoJYKvkqOJ0P0/X+6PsD6x3e2BoYXjrjT3gmBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T18:05:39.062094Z"},"content_sha256":"4c17b534a3e6fb7eaa94ce288361af080982fde65bbbfbbd9e9358bdb65044af","schema_version":"1.0","event_id":"sha256:4c17b534a3e6fb7eaa94ce288361af080982fde65bbbfbbd9e9358bdb65044af"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/Y3A7Y4OGXHYLY27R4CP57JLDYD/bundle.json","state_url":"https://pith.science/pith/Y3A7Y4OGXHYLY27R4CP57JLDYD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/Y3A7Y4OGXHYLY27R4CP57JLDYD/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":"2026-05-29T18:05:39Z","links":{"resolver":"https://pith.science/pith/Y3A7Y4OGXHYLY27R4CP57JLDYD","bundle":"https://pith.science/pith/Y3A7Y4OGXHYLY27R4CP57JLDYD/bundle.json","state":"https://pith.science/pith/Y3A7Y4OGXHYLY27R4CP57JLDYD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/Y3A7Y4OGXHYLY27R4CP57JLDYD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2001:Y3A7Y4OGXHYLY27R4CP57JLDYD","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":"5faf2e91b6c0aa0c1717cdba5933a90edf0f4695d8b497648ec3e61c8addf5de","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"2001-10-15T16:29:15Z","title_canon_sha256":"ce17ead10ba4876b34af3fe7b8d4b3588e950c566cac0dfec4f3326690918d10"},"schema_version":"1.0","source":{"id":"hep-lat/0110103","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0110103","created_at":"2026-05-18T01:39:14Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0110103v1","created_at":"2026-05-18T01:39:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0110103","created_at":"2026-05-18T01:39:14Z"},{"alias_kind":"pith_short_12","alias_value":"Y3A7Y4OGXHYL","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"Y3A7Y4OGXHYLY27R","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"Y3A7Y4OG","created_at":"2026-05-18T12:25:50Z"}],"graph_snapshots":[{"event_id":"sha256:4c17b534a3e6fb7eaa94ce288361af080982fde65bbbfbbd9e9358bdb65044af","target":"graph","created_at":"2026-05-18T01:39:14Z","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 present lattice studies of heavy quark potentials in the quenched approximation of QCD at finite temperatures. Both, the color singlet and color averaged potentials are calculated. While the potentials are well known at large distances, we give a detailed analysis of their short distance behavior (from 0.015 fm to 1 fm) near the critical temperature. At these distances we expect that the T-dependent potentials go over into the zero temperature potential. Indeed, we find evidences that the temperature influence gets suppressed and the potentials starts to become a unique function of the unde","authors_text":"F. Karsch, F. Zantow, O. Kaczmarek, P. Petreczky","cross_cats":[],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"2001-10-15T16:29:15Z","title":"Short distance physics with heavy quark potentials"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0110103","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:b36a63b1594b1fdf85ec2713e6a98fdb9b6badc859dc6d044cfb5231a41d151e","target":"record","created_at":"2026-05-18T01:39:14Z","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":"5faf2e91b6c0aa0c1717cdba5933a90edf0f4695d8b497648ec3e61c8addf5de","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"2001-10-15T16:29:15Z","title_canon_sha256":"ce17ead10ba4876b34af3fe7b8d4b3588e950c566cac0dfec4f3326690918d10"},"schema_version":"1.0","source":{"id":"hep-lat/0110103","kind":"arxiv","version":1}},"canonical_sha256":"c6c1fc71c6b9f0bc6bf1e09fdfa563c0d32a473d3e29733bce658544a4b5cf16","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c6c1fc71c6b9f0bc6bf1e09fdfa563c0d32a473d3e29733bce658544a4b5cf16","first_computed_at":"2026-05-18T01:39:14.855297Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:39:14.855297Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"IYvIj14UC4SfuFcqBJcquEXk6zG9/qD+3WC6vqnX7MjYveNMdnZ3rsDpkBaQHqkivewehx5hqDbzvRjgfD+gBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:39:14.855843Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/0110103","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b36a63b1594b1fdf85ec2713e6a98fdb9b6badc859dc6d044cfb5231a41d151e","sha256:4c17b534a3e6fb7eaa94ce288361af080982fde65bbbfbbd9e9358bdb65044af"],"state_sha256":"c55e70f2178dcc71577962bd0a5dbec6c0dd8a05eb450e665b0b1811e5b1e7ea"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3t9PRqfkOwVrbQ//b58oSu/TmupEx/cZe818YfzTz+8ywd1BTvA/0I2dXj1pSkxezDZ8pbPMThywalXnOYfnBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T18:05:39.065669Z","bundle_sha256":"2a289ffd82358099b2ef3eded7b7c6178ec57ceae4563ddf3f58681a6add8a79"}}