{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:2WQN3ZMSI3J736JZB242PNHINF","short_pith_number":"pith:2WQN3ZMS","canonical_record":{"source":{"id":"1402.0019","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-01-31T22:07:53Z","cross_cats_sorted":[],"title_canon_sha256":"72f3c23932795e98f10c85e4180d8bdebf9b64bddd75b3a75a91f7281fbb6235","abstract_canon_sha256":"c4d62e07e4e73184c03ba5daf0f9228208a5b8f6246f689434de16ae51cabaf4"},"schema_version":"1.0"},"canonical_sha256":"d5a0dde59246d3fdf9390eb9a7b4e86957f8ba3fce3cf4728aa69de1a4031a9c","source":{"kind":"arxiv","id":"1402.0019","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.0019","created_at":"2026-05-18T02:57:26Z"},{"alias_kind":"arxiv_version","alias_value":"1402.0019v1","created_at":"2026-05-18T02:57:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.0019","created_at":"2026-05-18T02:57:26Z"},{"alias_kind":"pith_short_12","alias_value":"2WQN3ZMSI3J7","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"2WQN3ZMSI3J736JZ","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"2WQN3ZMS","created_at":"2026-05-18T12:28:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:2WQN3ZMSI3J736JZB242PNHINF","target":"record","payload":{"canonical_record":{"source":{"id":"1402.0019","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-01-31T22:07:53Z","cross_cats_sorted":[],"title_canon_sha256":"72f3c23932795e98f10c85e4180d8bdebf9b64bddd75b3a75a91f7281fbb6235","abstract_canon_sha256":"c4d62e07e4e73184c03ba5daf0f9228208a5b8f6246f689434de16ae51cabaf4"},"schema_version":"1.0"},"canonical_sha256":"d5a0dde59246d3fdf9390eb9a7b4e86957f8ba3fce3cf4728aa69de1a4031a9c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:57:26.062779Z","signature_b64":"u3fDP0qhiT+ub+ltwq4TTFxGvV5th/p0isbEOXuctI4BFgjZuZD0Y8PfAUgp7A6EukEd1FeUmYfYoAx+fpoCAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d5a0dde59246d3fdf9390eb9a7b4e86957f8ba3fce3cf4728aa69de1a4031a9c","last_reissued_at":"2026-05-18T02:57:26.062087Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:57:26.062087Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1402.0019","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":"2026-05-18T02:57:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TD+BxBYiOCNy7ib5hjX1aFUdxx1xYBPYzgLszvyuCpKtsRrCCzMQQAfsBhWkkeQLLVs8IVUgClSBY88TgZXNAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-18T15:37:56.714665Z"},"content_sha256":"2dfa48300926e6e3c430d30790d9715c014e6c6939c7fccbe1925e39b270939a","schema_version":"1.0","event_id":"sha256:2dfa48300926e6e3c430d30790d9715c014e6c6939c7fccbe1925e39b270939a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:2WQN3ZMSI3J736JZB242PNHINF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"BPS solitons in a Dirac-Born-Infeld action","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"C. dos Santos, D. Rubiera-Garcia","submitted_at":"2014-01-31T22:07:53Z","abstract_excerpt":"We present several classes of solitons in ($1+1$)-dimensional models where the standard canonical kinetic term is replaced by a Dirac-Born-Infeld (DBI) one. These are static solutions with finite energy and different properties, namely, they can have compact support, or be kink or lump-like, according to the type of potential chosen, which depend on the DBI parameter $\\beta$. Through a combination of numerical and analytical arguments, by which the equation of motion is seen as that corresponding to \\emph{another} canonical model with a new $\\beta$-dependent potential and a $\\beta$-deformed en"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.0019","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":"2026-05-18T02:57:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"v4WYvIeK0caUAIg8i0bB6mkr70hQh6BD8CSMBZYurLD3ao0s+uLU7vMxSPllfda1VX7airmCDEjsbJRdP7OeBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-18T15:37:56.715022Z"},"content_sha256":"9518d87bd7ba5c2b1afa6245c231833b1f009d6d0edbc8401801d5d3bbdf1164","schema_version":"1.0","event_id":"sha256:9518d87bd7ba5c2b1afa6245c231833b1f009d6d0edbc8401801d5d3bbdf1164"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2WQN3ZMSI3J736JZB242PNHINF/bundle.json","state_url":"https://pith.science/pith/2WQN3ZMSI3J736JZB242PNHINF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2WQN3ZMSI3J736JZB242PNHINF/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":"2026-05-18T15:37:56Z","links":{"resolver":"https://pith.science/pith/2WQN3ZMSI3J736JZB242PNHINF","bundle":"https://pith.science/pith/2WQN3ZMSI3J736JZB242PNHINF/bundle.json","state":"https://pith.science/pith/2WQN3ZMSI3J736JZB242PNHINF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2WQN3ZMSI3J736JZB242PNHINF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:2WQN3ZMSI3J736JZB242PNHINF","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":"c4d62e07e4e73184c03ba5daf0f9228208a5b8f6246f689434de16ae51cabaf4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-01-31T22:07:53Z","title_canon_sha256":"72f3c23932795e98f10c85e4180d8bdebf9b64bddd75b3a75a91f7281fbb6235"},"schema_version":"1.0","source":{"id":"1402.0019","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.0019","created_at":"2026-05-18T02:57:26Z"},{"alias_kind":"arxiv_version","alias_value":"1402.0019v1","created_at":"2026-05-18T02:57:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.0019","created_at":"2026-05-18T02:57:26Z"},{"alias_kind":"pith_short_12","alias_value":"2WQN3ZMSI3J7","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"2WQN3ZMSI3J736JZ","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"2WQN3ZMS","created_at":"2026-05-18T12:28:11Z"}],"graph_snapshots":[{"event_id":"sha256:9518d87bd7ba5c2b1afa6245c231833b1f009d6d0edbc8401801d5d3bbdf1164","target":"graph","created_at":"2026-05-18T02:57:26Z","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 several classes of solitons in ($1+1$)-dimensional models where the standard canonical kinetic term is replaced by a Dirac-Born-Infeld (DBI) one. These are static solutions with finite energy and different properties, namely, they can have compact support, or be kink or lump-like, according to the type of potential chosen, which depend on the DBI parameter $\\beta$. Through a combination of numerical and analytical arguments, by which the equation of motion is seen as that corresponding to \\emph{another} canonical model with a new $\\beta$-dependent potential and a $\\beta$-deformed en","authors_text":"C. dos Santos, D. Rubiera-Garcia","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-01-31T22:07:53Z","title":"BPS solitons in a Dirac-Born-Infeld action"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.0019","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":"sha256:2dfa48300926e6e3c430d30790d9715c014e6c6939c7fccbe1925e39b270939a","target":"record","created_at":"2026-05-18T02:57:26Z","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":"c4d62e07e4e73184c03ba5daf0f9228208a5b8f6246f689434de16ae51cabaf4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-01-31T22:07:53Z","title_canon_sha256":"72f3c23932795e98f10c85e4180d8bdebf9b64bddd75b3a75a91f7281fbb6235"},"schema_version":"1.0","source":{"id":"1402.0019","kind":"arxiv","version":1}},"canonical_sha256":"d5a0dde59246d3fdf9390eb9a7b4e86957f8ba3fce3cf4728aa69de1a4031a9c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d5a0dde59246d3fdf9390eb9a7b4e86957f8ba3fce3cf4728aa69de1a4031a9c","first_computed_at":"2026-05-18T02:57:26.062087Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:57:26.062087Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"u3fDP0qhiT+ub+ltwq4TTFxGvV5th/p0isbEOXuctI4BFgjZuZD0Y8PfAUgp7A6EukEd1FeUmYfYoAx+fpoCAw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:57:26.062779Z","signed_message":"canonical_sha256_bytes"},"source_id":"1402.0019","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2dfa48300926e6e3c430d30790d9715c014e6c6939c7fccbe1925e39b270939a","sha256:9518d87bd7ba5c2b1afa6245c231833b1f009d6d0edbc8401801d5d3bbdf1164"],"state_sha256":"7893b491634037446d197cf81608fd26a58f701d9a568ed780c8110608263a15"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VreYVnmJqtVmOyKILnkrVxT7pnEDZDwMoK4txHDnO7fcuSCnG1HeYS8ln8furG5nWdzhXv1B8NOtYzYcMdJJDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-18T15:37:56.717016Z","bundle_sha256":"698e1e02da9064576bb4e26e0675b52058e7a1b06d5428d3b818bdb59e6d7438"}}