{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:R6KSUP7N4USNUUCXHBFLPZYDYG","short_pith_number":"pith:R6KSUP7N","canonical_record":{"source":{"id":"1001.2904","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-01-17T16:40:10Z","cross_cats_sorted":[],"title_canon_sha256":"511daff6ce6fecb994e79e32d2d05b223fabdb30ba10246fa91bc4ccaa68dc2b","abstract_canon_sha256":"967936868ea4321e2aeeaea9658ae33e4ad64c0e8ede44faf57e0ecbbbd62fc5"},"schema_version":"1.0"},"canonical_sha256":"8f952a3fede524da5057384ab7e703c18f199f06ad713a2790e36c6ffbf6c724","source":{"kind":"arxiv","id":"1001.2904","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1001.2904","created_at":"2026-05-18T02:24:45Z"},{"alias_kind":"arxiv_version","alias_value":"1001.2904v4","created_at":"2026-05-18T02:24:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1001.2904","created_at":"2026-05-18T02:24:45Z"},{"alias_kind":"pith_short_12","alias_value":"R6KSUP7N4USN","created_at":"2026-05-18T12:26:13Z"},{"alias_kind":"pith_short_16","alias_value":"R6KSUP7N4USNUUCX","created_at":"2026-05-18T12:26:13Z"},{"alias_kind":"pith_short_8","alias_value":"R6KSUP7N","created_at":"2026-05-18T12:26:13Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:R6KSUP7N4USNUUCXHBFLPZYDYG","target":"record","payload":{"canonical_record":{"source":{"id":"1001.2904","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-01-17T16:40:10Z","cross_cats_sorted":[],"title_canon_sha256":"511daff6ce6fecb994e79e32d2d05b223fabdb30ba10246fa91bc4ccaa68dc2b","abstract_canon_sha256":"967936868ea4321e2aeeaea9658ae33e4ad64c0e8ede44faf57e0ecbbbd62fc5"},"schema_version":"1.0"},"canonical_sha256":"8f952a3fede524da5057384ab7e703c18f199f06ad713a2790e36c6ffbf6c724","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:24:45.025136Z","signature_b64":"P2Z+57n3/q7QVeKDyKq+egGoPkAjp0ucBw6kZAsGlWinUIpD49vS2L9j92cI0LvqARVbfDF0TF/3MN62XuykBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8f952a3fede524da5057384ab7e703c18f199f06ad713a2790e36c6ffbf6c724","last_reissued_at":"2026-05-18T02:24:45.024662Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:24:45.024662Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1001.2904","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":"2026-05-18T02:24:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qKwZyI6Fn8EhUZRom4/zPMn0mE96FoXgvV9KxewCo5dSwoqhLomfPWywC7hf2TBYh5xuvAf1fRkX9waJ3weWAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T15:51:55.816967Z"},"content_sha256":"2ffc7523e309eee77dd81765a49ff30eb46280b8d63c669a282e4a2692ca4edd","schema_version":"1.0","event_id":"sha256:2ffc7523e309eee77dd81765a49ff30eb46280b8d63c669a282e4a2692ca4edd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:R6KSUP7N4USNUUCXHBFLPZYDYG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Drag force in a hot non-relativistic, non-commutative Yang-Mills plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Kamal L. Panigrahi, Shibaji Roy","submitted_at":"2010-01-17T16:40:10Z","abstract_excerpt":"We apply the standard technique of Null Melvin Twist to the non-extremal (D1, D3) bound state configuration of type IIB string theory. Under a particular decoupling limit, such configuration represents the gravity dual of the non-relativistic, non-commutative Yang-Mills theory at a finite temperature. We then use the AdS/CFT and the string probe approach to compute the drag force on an external quark moving through such a hot non-relativistic, non-commutative YM plasma. We discuss various limiting cases to show the interplay between the non-relativistic as well as the non-commutative effect of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1001.2904","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":"2026-05-18T02:24:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xE8d8c/inMHOxCEDAChXLq5YnKD+E/Hn/JoQby4EYJQSD3UpU05B18EPgcWtg70h4oZoFJIY8QNIuubV5kTDDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T15:51:55.817374Z"},"content_sha256":"9498b99cd21f654fc50873864917b0a8efef49f7c892909d49bfa293d174db02","schema_version":"1.0","event_id":"sha256:9498b99cd21f654fc50873864917b0a8efef49f7c892909d49bfa293d174db02"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/R6KSUP7N4USNUUCXHBFLPZYDYG/bundle.json","state_url":"https://pith.science/pith/R6KSUP7N4USNUUCXHBFLPZYDYG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/R6KSUP7N4USNUUCXHBFLPZYDYG/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":"2026-05-31T15:51:55Z","links":{"resolver":"https://pith.science/pith/R6KSUP7N4USNUUCXHBFLPZYDYG","bundle":"https://pith.science/pith/R6KSUP7N4USNUUCXHBFLPZYDYG/bundle.json","state":"https://pith.science/pith/R6KSUP7N4USNUUCXHBFLPZYDYG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/R6KSUP7N4USNUUCXHBFLPZYDYG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:R6KSUP7N4USNUUCXHBFLPZYDYG","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":"967936868ea4321e2aeeaea9658ae33e4ad64c0e8ede44faf57e0ecbbbd62fc5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-01-17T16:40:10Z","title_canon_sha256":"511daff6ce6fecb994e79e32d2d05b223fabdb30ba10246fa91bc4ccaa68dc2b"},"schema_version":"1.0","source":{"id":"1001.2904","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1001.2904","created_at":"2026-05-18T02:24:45Z"},{"alias_kind":"arxiv_version","alias_value":"1001.2904v4","created_at":"2026-05-18T02:24:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1001.2904","created_at":"2026-05-18T02:24:45Z"},{"alias_kind":"pith_short_12","alias_value":"R6KSUP7N4USN","created_at":"2026-05-18T12:26:13Z"},{"alias_kind":"pith_short_16","alias_value":"R6KSUP7N4USNUUCX","created_at":"2026-05-18T12:26:13Z"},{"alias_kind":"pith_short_8","alias_value":"R6KSUP7N","created_at":"2026-05-18T12:26:13Z"}],"graph_snapshots":[{"event_id":"sha256:9498b99cd21f654fc50873864917b0a8efef49f7c892909d49bfa293d174db02","target":"graph","created_at":"2026-05-18T02:24:45Z","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 apply the standard technique of Null Melvin Twist to the non-extremal (D1, D3) bound state configuration of type IIB string theory. Under a particular decoupling limit, such configuration represents the gravity dual of the non-relativistic, non-commutative Yang-Mills theory at a finite temperature. We then use the AdS/CFT and the string probe approach to compute the drag force on an external quark moving through such a hot non-relativistic, non-commutative YM plasma. We discuss various limiting cases to show the interplay between the non-relativistic as well as the non-commutative effect of","authors_text":"Kamal L. Panigrahi, Shibaji Roy","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-01-17T16:40:10Z","title":"Drag force in a hot non-relativistic, non-commutative Yang-Mills plasma"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1001.2904","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":"sha256:2ffc7523e309eee77dd81765a49ff30eb46280b8d63c669a282e4a2692ca4edd","target":"record","created_at":"2026-05-18T02:24:45Z","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":"967936868ea4321e2aeeaea9658ae33e4ad64c0e8ede44faf57e0ecbbbd62fc5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-01-17T16:40:10Z","title_canon_sha256":"511daff6ce6fecb994e79e32d2d05b223fabdb30ba10246fa91bc4ccaa68dc2b"},"schema_version":"1.0","source":{"id":"1001.2904","kind":"arxiv","version":4}},"canonical_sha256":"8f952a3fede524da5057384ab7e703c18f199f06ad713a2790e36c6ffbf6c724","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8f952a3fede524da5057384ab7e703c18f199f06ad713a2790e36c6ffbf6c724","first_computed_at":"2026-05-18T02:24:45.024662Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:24:45.024662Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"P2Z+57n3/q7QVeKDyKq+egGoPkAjp0ucBw6kZAsGlWinUIpD49vS2L9j92cI0LvqARVbfDF0TF/3MN62XuykBA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:24:45.025136Z","signed_message":"canonical_sha256_bytes"},"source_id":"1001.2904","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2ffc7523e309eee77dd81765a49ff30eb46280b8d63c669a282e4a2692ca4edd","sha256:9498b99cd21f654fc50873864917b0a8efef49f7c892909d49bfa293d174db02"],"state_sha256":"ed9eb7678cb649d7895665f83ceef9aeb63edd6c6435b2019767901f95c4a60e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"88xIcWz3Pnf3Hyyj/bSeUhz/jqtwrknBN6zfMuhCkIJ1HRoCgeVP5ncD8JgtYMJFz2cwySGiX2Dal8ODHVcmAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T15:51:55.821401Z","bundle_sha256":"ec15c2d508be63f678c0bf29ee94af93b3ce87e0efa7c6f099ffc230a3c24c9c"}}