{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:4FCWK7G3BRHY7RSTUTDEDO653J","short_pith_number":"pith:4FCWK7G3","canonical_record":{"source":{"id":"1512.04238","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2015-12-14T09:54:41Z","cross_cats_sorted":[],"title_canon_sha256":"ce712ad2dbee66cdd4fcf05514b1217c855f0400745f49db861ab97c23ebf2b6","abstract_canon_sha256":"6ac883a3f0c9ddcf5782834360dd692be789f74a50aa4be8da07046ffe599a86"},"schema_version":"1.0"},"canonical_sha256":"e145657cdb0c4f8fc653a4c641bbddda6354dab94afd220fd15c061f149e0b53","source":{"kind":"arxiv","id":"1512.04238","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1512.04238","created_at":"2026-05-18T01:17:59Z"},{"alias_kind":"arxiv_version","alias_value":"1512.04238v1","created_at":"2026-05-18T01:17:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.04238","created_at":"2026-05-18T01:17:59Z"},{"alias_kind":"pith_short_12","alias_value":"4FCWK7G3BRHY","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_16","alias_value":"4FCWK7G3BRHY7RST","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_8","alias_value":"4FCWK7G3","created_at":"2026-05-18T12:29:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:4FCWK7G3BRHY7RSTUTDEDO653J","target":"record","payload":{"canonical_record":{"source":{"id":"1512.04238","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2015-12-14T09:54:41Z","cross_cats_sorted":[],"title_canon_sha256":"ce712ad2dbee66cdd4fcf05514b1217c855f0400745f49db861ab97c23ebf2b6","abstract_canon_sha256":"6ac883a3f0c9ddcf5782834360dd692be789f74a50aa4be8da07046ffe599a86"},"schema_version":"1.0"},"canonical_sha256":"e145657cdb0c4f8fc653a4c641bbddda6354dab94afd220fd15c061f149e0b53","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:17:59.416855Z","signature_b64":"4yJ+N4QHrJOgMIth4nu1mMYxrDXdzwU3elveLFZ/XzmjF/KCqJEffXqZ5+Uv15GpNMChjNLV9j4/bb0v7cVDBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e145657cdb0c4f8fc653a4c641bbddda6354dab94afd220fd15c061f149e0b53","last_reissued_at":"2026-05-18T01:17:59.416040Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:17:59.416040Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1512.04238","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":"2026-05-18T01:17:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GI3YjrzNS++jc0xQ2gdl5p3i7VfXL+e2O0V3fY0txs+RLArPkKTnl3a91FQcAGj82wHAaUqzpJYu9yRhBFaVBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T17:50:06.916982Z"},"content_sha256":"c6610a67e916948c659dd6cf516b2a504e559149d24f7d925c01f7738b58a5fa","schema_version":"1.0","event_id":"sha256:c6610a67e916948c659dd6cf516b2a504e559149d24f7d925c01f7738b58a5fa"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:4FCWK7G3BRHY7RSTUTDEDO653J","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Finite-temperature effects on interacting bosonic 1D systems in disordered lattices","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.dis-nn","authors_text":"Avinash Kumar, Chiara D'Errico, Eleonora Lucioni, Giovanni Modugno, Guillaume Roux, Lorenzo Gori, Luca Tanzi, Massimo Inguscio, Thierry Giamarchi, Thomas Barthel","submitted_at":"2015-12-14T09:54:41Z","abstract_excerpt":"We analyze the finite-temperature effects on the phase diagram describing the insulating properties of interacting 1D bosons in a quasi-periodic lattice. We examine thermal effects by comparing experimental results to exact diagonalization for small-sized systems and to density-matrix renormalization group (DMRG) computations. At weak interactions, we find short thermal correlation lengths, indicating a substantial impact of temperature on the system coherence. Conversely, at strong interactions, the obtained thermal correlation lengths are significantly larger than the localization length, an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.04238","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":"2026-05-18T01:17:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HuUZ4GA+yKP1Y5FbDtFCDSFbYR0dwcMK2E0919W8yRzJliXhuoIvf8t4xhR2kntR+4wAV0pVysAucSeaAIwkBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T17:50:06.917357Z"},"content_sha256":"9e745f7a667ab3aae3db633de89bfb6a8dc84754cd88d1b10b217b30efa5f410","schema_version":"1.0","event_id":"sha256:9e745f7a667ab3aae3db633de89bfb6a8dc84754cd88d1b10b217b30efa5f410"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4FCWK7G3BRHY7RSTUTDEDO653J/bundle.json","state_url":"https://pith.science/pith/4FCWK7G3BRHY7RSTUTDEDO653J/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4FCWK7G3BRHY7RSTUTDEDO653J/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":"2026-06-22T17:50:06Z","links":{"resolver":"https://pith.science/pith/4FCWK7G3BRHY7RSTUTDEDO653J","bundle":"https://pith.science/pith/4FCWK7G3BRHY7RSTUTDEDO653J/bundle.json","state":"https://pith.science/pith/4FCWK7G3BRHY7RSTUTDEDO653J/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4FCWK7G3BRHY7RSTUTDEDO653J/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:4FCWK7G3BRHY7RSTUTDEDO653J","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":"6ac883a3f0c9ddcf5782834360dd692be789f74a50aa4be8da07046ffe599a86","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2015-12-14T09:54:41Z","title_canon_sha256":"ce712ad2dbee66cdd4fcf05514b1217c855f0400745f49db861ab97c23ebf2b6"},"schema_version":"1.0","source":{"id":"1512.04238","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1512.04238","created_at":"2026-05-18T01:17:59Z"},{"alias_kind":"arxiv_version","alias_value":"1512.04238v1","created_at":"2026-05-18T01:17:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.04238","created_at":"2026-05-18T01:17:59Z"},{"alias_kind":"pith_short_12","alias_value":"4FCWK7G3BRHY","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_16","alias_value":"4FCWK7G3BRHY7RST","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_8","alias_value":"4FCWK7G3","created_at":"2026-05-18T12:29:05Z"}],"graph_snapshots":[{"event_id":"sha256:9e745f7a667ab3aae3db633de89bfb6a8dc84754cd88d1b10b217b30efa5f410","target":"graph","created_at":"2026-05-18T01:17:59Z","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 analyze the finite-temperature effects on the phase diagram describing the insulating properties of interacting 1D bosons in a quasi-periodic lattice. We examine thermal effects by comparing experimental results to exact diagonalization for small-sized systems and to density-matrix renormalization group (DMRG) computations. At weak interactions, we find short thermal correlation lengths, indicating a substantial impact of temperature on the system coherence. Conversely, at strong interactions, the obtained thermal correlation lengths are significantly larger than the localization length, an","authors_text":"Avinash Kumar, Chiara D'Errico, Eleonora Lucioni, Giovanni Modugno, Guillaume Roux, Lorenzo Gori, Luca Tanzi, Massimo Inguscio, Thierry Giamarchi, Thomas Barthel","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2015-12-14T09:54:41Z","title":"Finite-temperature effects on interacting bosonic 1D systems in disordered lattices"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.04238","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:c6610a67e916948c659dd6cf516b2a504e559149d24f7d925c01f7738b58a5fa","target":"record","created_at":"2026-05-18T01:17:59Z","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":"6ac883a3f0c9ddcf5782834360dd692be789f74a50aa4be8da07046ffe599a86","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2015-12-14T09:54:41Z","title_canon_sha256":"ce712ad2dbee66cdd4fcf05514b1217c855f0400745f49db861ab97c23ebf2b6"},"schema_version":"1.0","source":{"id":"1512.04238","kind":"arxiv","version":1}},"canonical_sha256":"e145657cdb0c4f8fc653a4c641bbddda6354dab94afd220fd15c061f149e0b53","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e145657cdb0c4f8fc653a4c641bbddda6354dab94afd220fd15c061f149e0b53","first_computed_at":"2026-05-18T01:17:59.416040Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:17:59.416040Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4yJ+N4QHrJOgMIth4nu1mMYxrDXdzwU3elveLFZ/XzmjF/KCqJEffXqZ5+Uv15GpNMChjNLV9j4/bb0v7cVDBg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:17:59.416855Z","signed_message":"canonical_sha256_bytes"},"source_id":"1512.04238","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c6610a67e916948c659dd6cf516b2a504e559149d24f7d925c01f7738b58a5fa","sha256:9e745f7a667ab3aae3db633de89bfb6a8dc84754cd88d1b10b217b30efa5f410"],"state_sha256":"ad28290ad222767441083ddd6c9adf2eee23da974ade8497e834a523e2c82690"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"o9PGwjl/hfq+kFisscF3n4mIrvBriJOJ7NwKjLILDu9ULZZFzJPs8EyXrmz64cSW3FtJBNmgrnCUJDC/LublDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-22T17:50:06.919375Z","bundle_sha256":"f51f15e8b689831a451bf47b702026ff2c726df9bf0fd8c11fd4f738a386c7f1"}}