{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:FEM6JFA7USQMEXBG5SCJCM3EXO","short_pith_number":"pith:FEM6JFA7","canonical_record":{"source":{"id":"1305.2506","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-05-11T13:55:06Z","cross_cats_sorted":[],"title_canon_sha256":"7167421c342cd2bf790770a1e15778929deca5c1b77b758c8912811c91d38f62","abstract_canon_sha256":"58f1aaec018c34e0ec71d282bb17b6bd0b51be4dc2fe91b1ab246bdbe931daac"},"schema_version":"1.0"},"canonical_sha256":"2919e4941fa4a0c25c26ec84913364bb8c190b321627c65c5d0ba5206442d9ef","source":{"kind":"arxiv","id":"1305.2506","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1305.2506","created_at":"2026-05-18T03:16:18Z"},{"alias_kind":"arxiv_version","alias_value":"1305.2506v3","created_at":"2026-05-18T03:16:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.2506","created_at":"2026-05-18T03:16:18Z"},{"alias_kind":"pith_short_12","alias_value":"FEM6JFA7USQM","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_16","alias_value":"FEM6JFA7USQMEXBG","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_8","alias_value":"FEM6JFA7","created_at":"2026-05-18T12:27:45Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:FEM6JFA7USQMEXBG5SCJCM3EXO","target":"record","payload":{"canonical_record":{"source":{"id":"1305.2506","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-05-11T13:55:06Z","cross_cats_sorted":[],"title_canon_sha256":"7167421c342cd2bf790770a1e15778929deca5c1b77b758c8912811c91d38f62","abstract_canon_sha256":"58f1aaec018c34e0ec71d282bb17b6bd0b51be4dc2fe91b1ab246bdbe931daac"},"schema_version":"1.0"},"canonical_sha256":"2919e4941fa4a0c25c26ec84913364bb8c190b321627c65c5d0ba5206442d9ef","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:16:18.788113Z","signature_b64":"fxYQVe5Nhdqnujb+ANsnB9yXXd2tpm7ZQIeydHGUlUjgoTVEPOQfUcKkEioOv/lCVOMJug1xoCsKGmGL5GxtDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2919e4941fa4a0c25c26ec84913364bb8c190b321627c65c5d0ba5206442d9ef","last_reissued_at":"2026-05-18T03:16:18.787419Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:16:18.787419Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1305.2506","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":"2026-05-18T03:16:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RhinvMaO3HeEvY1sOFKqrvZMWILEfLWcsMWDx7hrE/XtUoPGR+ylv0tn9BNiX+UL/BtzxdCpQOHUAV6qVZ0UAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T16:34:09.657353Z"},"content_sha256":"42e5a3f53988f8d1362f8efee0d3c88cc68bf88e27126c20a23720fb317f4eb7","schema_version":"1.0","event_id":"sha256:42e5a3f53988f8d1362f8efee0d3c88cc68bf88e27126c20a23720fb317f4eb7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:FEM6JFA7USQMEXBG5SCJCM3EXO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Linear responses of D0-branes via gauge/gravity correspondence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Yasuhiro Sekino, Yoshinori Matsuo, Yuya Sasai","submitted_at":"2013-05-11T13:55:06Z","abstract_excerpt":"We study linear responses of D0-branes in the low frequency region by using gauge/gravity correspondence. The dynamics of the D0-branes is described by Matrix theory with finite temperature, which is dual to a near extremal D0-brane black hole solution. We analyze the tensor mode and vector modes of a stress tensor and a Ramond-Ramond 1-form current of Matrix theory. Then, we show that if a cutoff surface is close to a horizon of the D0-brane black hole, the linear responses take forms similar to the hydrodynamic stress tensor and current on S^8. By taking a Rindler limit, those linear respons"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.2506","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":"2026-05-18T03:16:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/xB2pOIlxp4oCPO+sZ0FQsMBqKt7KvwsRtfehMtfo1D5cfQ90luKHirKuexAhowMcsV5MG6GQDRUtM3hg1oHDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T16:34:09.657706Z"},"content_sha256":"dcd9f97a36e9bfe3970f1699915b272d6006589bff69e6b9016f429ae2d93ad7","schema_version":"1.0","event_id":"sha256:dcd9f97a36e9bfe3970f1699915b272d6006589bff69e6b9016f429ae2d93ad7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FEM6JFA7USQMEXBG5SCJCM3EXO/bundle.json","state_url":"https://pith.science/pith/FEM6JFA7USQMEXBG5SCJCM3EXO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FEM6JFA7USQMEXBG5SCJCM3EXO/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":"2026-06-03T16:34:09Z","links":{"resolver":"https://pith.science/pith/FEM6JFA7USQMEXBG5SCJCM3EXO","bundle":"https://pith.science/pith/FEM6JFA7USQMEXBG5SCJCM3EXO/bundle.json","state":"https://pith.science/pith/FEM6JFA7USQMEXBG5SCJCM3EXO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FEM6JFA7USQMEXBG5SCJCM3EXO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:FEM6JFA7USQMEXBG5SCJCM3EXO","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":"58f1aaec018c34e0ec71d282bb17b6bd0b51be4dc2fe91b1ab246bdbe931daac","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-05-11T13:55:06Z","title_canon_sha256":"7167421c342cd2bf790770a1e15778929deca5c1b77b758c8912811c91d38f62"},"schema_version":"1.0","source":{"id":"1305.2506","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1305.2506","created_at":"2026-05-18T03:16:18Z"},{"alias_kind":"arxiv_version","alias_value":"1305.2506v3","created_at":"2026-05-18T03:16:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.2506","created_at":"2026-05-18T03:16:18Z"},{"alias_kind":"pith_short_12","alias_value":"FEM6JFA7USQM","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_16","alias_value":"FEM6JFA7USQMEXBG","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_8","alias_value":"FEM6JFA7","created_at":"2026-05-18T12:27:45Z"}],"graph_snapshots":[{"event_id":"sha256:dcd9f97a36e9bfe3970f1699915b272d6006589bff69e6b9016f429ae2d93ad7","target":"graph","created_at":"2026-05-18T03:16:18Z","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 study linear responses of D0-branes in the low frequency region by using gauge/gravity correspondence. The dynamics of the D0-branes is described by Matrix theory with finite temperature, which is dual to a near extremal D0-brane black hole solution. We analyze the tensor mode and vector modes of a stress tensor and a Ramond-Ramond 1-form current of Matrix theory. Then, we show that if a cutoff surface is close to a horizon of the D0-brane black hole, the linear responses take forms similar to the hydrodynamic stress tensor and current on S^8. By taking a Rindler limit, those linear respons","authors_text":"Yasuhiro Sekino, Yoshinori Matsuo, Yuya Sasai","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-05-11T13:55:06Z","title":"Linear responses of D0-branes via gauge/gravity correspondence"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.2506","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":"sha256:42e5a3f53988f8d1362f8efee0d3c88cc68bf88e27126c20a23720fb317f4eb7","target":"record","created_at":"2026-05-18T03:16:18Z","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":"58f1aaec018c34e0ec71d282bb17b6bd0b51be4dc2fe91b1ab246bdbe931daac","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-05-11T13:55:06Z","title_canon_sha256":"7167421c342cd2bf790770a1e15778929deca5c1b77b758c8912811c91d38f62"},"schema_version":"1.0","source":{"id":"1305.2506","kind":"arxiv","version":3}},"canonical_sha256":"2919e4941fa4a0c25c26ec84913364bb8c190b321627c65c5d0ba5206442d9ef","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2919e4941fa4a0c25c26ec84913364bb8c190b321627c65c5d0ba5206442d9ef","first_computed_at":"2026-05-18T03:16:18.787419Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:16:18.787419Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"fxYQVe5Nhdqnujb+ANsnB9yXXd2tpm7ZQIeydHGUlUjgoTVEPOQfUcKkEioOv/lCVOMJug1xoCsKGmGL5GxtDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:16:18.788113Z","signed_message":"canonical_sha256_bytes"},"source_id":"1305.2506","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:42e5a3f53988f8d1362f8efee0d3c88cc68bf88e27126c20a23720fb317f4eb7","sha256:dcd9f97a36e9bfe3970f1699915b272d6006589bff69e6b9016f429ae2d93ad7"],"state_sha256":"d1091d6112d6a32809e6e0fdd271e32bc92c15daa89db2776d7ba8a441805992"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4cWobOZHej6YOSWarOUrlDhGIDaoZt1hRlXlyKU6e65331IdMfoZ5LFVnuDnmdilXyJxJwYQQ7NRr3sL6iOUDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T16:34:09.659766Z","bundle_sha256":"3ddd50c210e952d7016054ff868c97ac56376f050ca6443449da4be901a69d82"}}