{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:4MIEUA5OT24JMJZS7HGAM2WYGY","short_pith_number":"pith:4MIEUA5O","canonical_record":{"source":{"id":"1110.2450","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2011-10-11T17:40:10Z","cross_cats_sorted":["hep-th","math-ph","math.MP"],"title_canon_sha256":"0f5805fd914167474e4141dec85cac1cbe8e4f1ff0b596a91ebf27271518ee7d","abstract_canon_sha256":"eb2c2f15de4a652b3488bfeecb8452e1fcd64aac54daa88348f6fe42b57d13ba"},"schema_version":"1.0"},"canonical_sha256":"e3104a03ae9eb8962732f9cc066ad8361ae3638f0c1e9ff33df0b0bba4263b44","source":{"kind":"arxiv","id":"1110.2450","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1110.2450","created_at":"2026-05-18T02:00:13Z"},{"alias_kind":"arxiv_version","alias_value":"1110.2450v1","created_at":"2026-05-18T02:00:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.2450","created_at":"2026-05-18T02:00:13Z"},{"alias_kind":"pith_short_12","alias_value":"4MIEUA5OT24J","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_16","alias_value":"4MIEUA5OT24JMJZS","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_8","alias_value":"4MIEUA5O","created_at":"2026-05-18T12:26:20Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:4MIEUA5OT24JMJZS7HGAM2WYGY","target":"record","payload":{"canonical_record":{"source":{"id":"1110.2450","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2011-10-11T17:40:10Z","cross_cats_sorted":["hep-th","math-ph","math.MP"],"title_canon_sha256":"0f5805fd914167474e4141dec85cac1cbe8e4f1ff0b596a91ebf27271518ee7d","abstract_canon_sha256":"eb2c2f15de4a652b3488bfeecb8452e1fcd64aac54daa88348f6fe42b57d13ba"},"schema_version":"1.0"},"canonical_sha256":"e3104a03ae9eb8962732f9cc066ad8361ae3638f0c1e9ff33df0b0bba4263b44","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:00:13.607904Z","signature_b64":"epZwLoLMj6CmcCiuWGdZdhrZgVSKK2RKtr/1GEqvuSO4Bu436W4woVEQiohj9Tas0C2gAvA7/m1AoBCSg/+YCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e3104a03ae9eb8962732f9cc066ad8361ae3638f0c1e9ff33df0b0bba4263b44","last_reissued_at":"2026-05-18T02:00:13.607342Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:00:13.607342Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1110.2450","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":"2026-05-18T02:00:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SJvgNncwMD8AI+zaqNonNJ38rVMeJ0PDRnnRADi7lFrgAYhHSMQyvudSJORr5y+2CO5FCxuSi8A2+qNp14bDAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T07:22:06.032933Z"},"content_sha256":"07f4c884ff77a77aee495a8d5b200f1efdca8b2ff07e3124981bbb6ea53c21de","schema_version":"1.0","event_id":"sha256:07f4c884ff77a77aee495a8d5b200f1efdca8b2ff07e3124981bbb6ea53c21de"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:4MIEUA5OT24JMJZS7HGAM2WYGY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Non-singular screw dislocations as the Coulomb gas with smoothed out coupling and the renormalization of the shear modulus","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","math-ph","math.MP"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"C. Malyshev","submitted_at":"2011-10-11T17:40:10Z","abstract_excerpt":"A field theory is developed for a thermodynamical description of array of parallel non-singular screw dislocations in elastic cylinder. The partition function of the system is considered in the functional integral form. Self-energy of the dislocation cores is chosen in the form suggested by the gauge-translational model of non-singular screw dislocation. It is shown that the system of the dislocations is equivalent to the two-dimensional Coulomb gas. The coupling potential is prevented from a short-distance divergency since the core energies are taken into account. Two-point correlation functi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.2450","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":"2026-05-18T02:00:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"++LoYVOdz63ANuj43zYqEeCiPyALwHGrqgqNyox3rIKqHOYp2WFHieebVi2tHulI5+rhGfQ56W6OU7C+5HUzBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T07:22:06.033275Z"},"content_sha256":"26e1e3d6c16c0c43a46d0a3c1b8df01099f3b043595a4cb85469e03422475bba","schema_version":"1.0","event_id":"sha256:26e1e3d6c16c0c43a46d0a3c1b8df01099f3b043595a4cb85469e03422475bba"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4MIEUA5OT24JMJZS7HGAM2WYGY/bundle.json","state_url":"https://pith.science/pith/4MIEUA5OT24JMJZS7HGAM2WYGY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4MIEUA5OT24JMJZS7HGAM2WYGY/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":"2026-06-25T07:22:06Z","links":{"resolver":"https://pith.science/pith/4MIEUA5OT24JMJZS7HGAM2WYGY","bundle":"https://pith.science/pith/4MIEUA5OT24JMJZS7HGAM2WYGY/bundle.json","state":"https://pith.science/pith/4MIEUA5OT24JMJZS7HGAM2WYGY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4MIEUA5OT24JMJZS7HGAM2WYGY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:4MIEUA5OT24JMJZS7HGAM2WYGY","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":"eb2c2f15de4a652b3488bfeecb8452e1fcd64aac54daa88348f6fe42b57d13ba","cross_cats_sorted":["hep-th","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2011-10-11T17:40:10Z","title_canon_sha256":"0f5805fd914167474e4141dec85cac1cbe8e4f1ff0b596a91ebf27271518ee7d"},"schema_version":"1.0","source":{"id":"1110.2450","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1110.2450","created_at":"2026-05-18T02:00:13Z"},{"alias_kind":"arxiv_version","alias_value":"1110.2450v1","created_at":"2026-05-18T02:00:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.2450","created_at":"2026-05-18T02:00:13Z"},{"alias_kind":"pith_short_12","alias_value":"4MIEUA5OT24J","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_16","alias_value":"4MIEUA5OT24JMJZS","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_8","alias_value":"4MIEUA5O","created_at":"2026-05-18T12:26:20Z"}],"graph_snapshots":[{"event_id":"sha256:26e1e3d6c16c0c43a46d0a3c1b8df01099f3b043595a4cb85469e03422475bba","target":"graph","created_at":"2026-05-18T02:00:13Z","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":"A field theory is developed for a thermodynamical description of array of parallel non-singular screw dislocations in elastic cylinder. The partition function of the system is considered in the functional integral form. Self-energy of the dislocation cores is chosen in the form suggested by the gauge-translational model of non-singular screw dislocation. It is shown that the system of the dislocations is equivalent to the two-dimensional Coulomb gas. The coupling potential is prevented from a short-distance divergency since the core energies are taken into account. Two-point correlation functi","authors_text":"C. Malyshev","cross_cats":["hep-th","math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2011-10-11T17:40:10Z","title":"Non-singular screw dislocations as the Coulomb gas with smoothed out coupling and the renormalization of the shear modulus"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.2450","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":"sha256:07f4c884ff77a77aee495a8d5b200f1efdca8b2ff07e3124981bbb6ea53c21de","target":"record","created_at":"2026-05-18T02:00:13Z","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":"eb2c2f15de4a652b3488bfeecb8452e1fcd64aac54daa88348f6fe42b57d13ba","cross_cats_sorted":["hep-th","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2011-10-11T17:40:10Z","title_canon_sha256":"0f5805fd914167474e4141dec85cac1cbe8e4f1ff0b596a91ebf27271518ee7d"},"schema_version":"1.0","source":{"id":"1110.2450","kind":"arxiv","version":1}},"canonical_sha256":"e3104a03ae9eb8962732f9cc066ad8361ae3638f0c1e9ff33df0b0bba4263b44","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e3104a03ae9eb8962732f9cc066ad8361ae3638f0c1e9ff33df0b0bba4263b44","first_computed_at":"2026-05-18T02:00:13.607342Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:00:13.607342Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"epZwLoLMj6CmcCiuWGdZdhrZgVSKK2RKtr/1GEqvuSO4Bu436W4woVEQiohj9Tas0C2gAvA7/m1AoBCSg/+YCA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:00:13.607904Z","signed_message":"canonical_sha256_bytes"},"source_id":"1110.2450","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:07f4c884ff77a77aee495a8d5b200f1efdca8b2ff07e3124981bbb6ea53c21de","sha256:26e1e3d6c16c0c43a46d0a3c1b8df01099f3b043595a4cb85469e03422475bba"],"state_sha256":"3cc49a6d1e2a00b6168a98a50d738ccc90636dc97b5f62eeaaa3b84643438fe4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tSjtsa5TcqhMsJaXjuPaprqpyNfQroEx3Tgi96CcrfealJm4GY0UTW5nKVJI3DqgkpNfHqx8bGmXPwkZ4IIlCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-25T07:22:06.035196Z","bundle_sha256":"c92251ef7d07ad541331be9d0345db37d918c23bca10208cec6bb559a2f3f92c"}}