{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:SNUXS7KAK5EBN65EGPO6W33J6X","short_pith_number":"pith:SNUXS7KA","canonical_record":{"source":{"id":"1604.00238","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2016-04-01T13:41:43Z","cross_cats_sorted":[],"title_canon_sha256":"024ad50007cd91cef5bf6880d3504fa95f07204025205b42846ee703259a6f78","abstract_canon_sha256":"d56b5bac753021f9ef415c8f0cdd66cdd57725360626e88b7b5c3dc80563e024"},"schema_version":"1.0"},"canonical_sha256":"9369797d40574816fba433ddeb6f69f5c053a841505185a71ed8e7796f3289df","source":{"kind":"arxiv","id":"1604.00238","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.00238","created_at":"2026-05-18T01:17:16Z"},{"alias_kind":"arxiv_version","alias_value":"1604.00238v1","created_at":"2026-05-18T01:17:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.00238","created_at":"2026-05-18T01:17:16Z"},{"alias_kind":"pith_short_12","alias_value":"SNUXS7KAK5EB","created_at":"2026-05-18T12:30:44Z"},{"alias_kind":"pith_short_16","alias_value":"SNUXS7KAK5EBN65E","created_at":"2026-05-18T12:30:44Z"},{"alias_kind":"pith_short_8","alias_value":"SNUXS7KA","created_at":"2026-05-18T12:30:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:SNUXS7KAK5EBN65EGPO6W33J6X","target":"record","payload":{"canonical_record":{"source":{"id":"1604.00238","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2016-04-01T13:41:43Z","cross_cats_sorted":[],"title_canon_sha256":"024ad50007cd91cef5bf6880d3504fa95f07204025205b42846ee703259a6f78","abstract_canon_sha256":"d56b5bac753021f9ef415c8f0cdd66cdd57725360626e88b7b5c3dc80563e024"},"schema_version":"1.0"},"canonical_sha256":"9369797d40574816fba433ddeb6f69f5c053a841505185a71ed8e7796f3289df","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:17:16.719445Z","signature_b64":"5NKVWdyPIAlk6tf6963Y7YtN0V1fymGInRjL2VCvlmfzB5fdObFccMn16cwD+RZAJodo1132fXfkdXs1y9BtAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9369797d40574816fba433ddeb6f69f5c053a841505185a71ed8e7796f3289df","last_reissued_at":"2026-05-18T01:17:16.718669Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:17:16.718669Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1604.00238","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":"2026-05-18T01:17:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Zx/Qip6JIecbQ2YaT5mkqSDehJFJmvvMUsgjeihl52jYIeMU2/ymrlYorot1O8eubI/Lk65CrHc8v1k78PEsDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T07:40:27.709650Z"},"content_sha256":"13fde7c57a28f32ec71aa863fb0a6dd554f6612659e2c5eb4b808abdff915519","schema_version":"1.0","event_id":"sha256:13fde7c57a28f32ec71aa863fb0a6dd554f6612659e2c5eb4b808abdff915519"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:SNUXS7KAK5EBN65EGPO6W33J6X","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Influence of the energy-band structure on ultracold reactive processes in lattices","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"Andrea Simoni, Hugo Terrier, Jean-Michel Launay","submitted_at":"2016-04-01T13:41:43Z","abstract_excerpt":"We study theoretically ultracold collisions in quasi one-dimensional optical traps for bosonic and fermionic reactive molecules in the presence of a periodic potential along the trap axis. Elastic, reactive, and umklapp processes due to non-conservation of the center of mass motion are investigated for parameters of relevant experimental interest. The model naturally keeps into account the effect of excited energy bands and is particularly suited for being adapted to rigorous close-coupled calculations. Our formalism shows that a correct derivation of the parameters in tight-binding effective "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.00238","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":"2026-05-18T01:17:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XJ4X1xFBVehV/J6PQad/SBlgUeDkjdZ/SKJjqZC9+lH8WhNWY/eCkegIZkLlKfOprN9Q/RAmZYEALxtIbgLfAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T07:40:27.710113Z"},"content_sha256":"22026916d085c8048273b4e573b37a8d59ccc64f4acb8d152849102e31c71e22","schema_version":"1.0","event_id":"sha256:22026916d085c8048273b4e573b37a8d59ccc64f4acb8d152849102e31c71e22"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SNUXS7KAK5EBN65EGPO6W33J6X/bundle.json","state_url":"https://pith.science/pith/SNUXS7KAK5EBN65EGPO6W33J6X/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SNUXS7KAK5EBN65EGPO6W33J6X/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":"2026-06-25T07:40:27Z","links":{"resolver":"https://pith.science/pith/SNUXS7KAK5EBN65EGPO6W33J6X","bundle":"https://pith.science/pith/SNUXS7KAK5EBN65EGPO6W33J6X/bundle.json","state":"https://pith.science/pith/SNUXS7KAK5EBN65EGPO6W33J6X/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SNUXS7KAK5EBN65EGPO6W33J6X/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:SNUXS7KAK5EBN65EGPO6W33J6X","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":"d56b5bac753021f9ef415c8f0cdd66cdd57725360626e88b7b5c3dc80563e024","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2016-04-01T13:41:43Z","title_canon_sha256":"024ad50007cd91cef5bf6880d3504fa95f07204025205b42846ee703259a6f78"},"schema_version":"1.0","source":{"id":"1604.00238","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.00238","created_at":"2026-05-18T01:17:16Z"},{"alias_kind":"arxiv_version","alias_value":"1604.00238v1","created_at":"2026-05-18T01:17:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.00238","created_at":"2026-05-18T01:17:16Z"},{"alias_kind":"pith_short_12","alias_value":"SNUXS7KAK5EB","created_at":"2026-05-18T12:30:44Z"},{"alias_kind":"pith_short_16","alias_value":"SNUXS7KAK5EBN65E","created_at":"2026-05-18T12:30:44Z"},{"alias_kind":"pith_short_8","alias_value":"SNUXS7KA","created_at":"2026-05-18T12:30:44Z"}],"graph_snapshots":[{"event_id":"sha256:22026916d085c8048273b4e573b37a8d59ccc64f4acb8d152849102e31c71e22","target":"graph","created_at":"2026-05-18T01:17:16Z","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 theoretically ultracold collisions in quasi one-dimensional optical traps for bosonic and fermionic reactive molecules in the presence of a periodic potential along the trap axis. Elastic, reactive, and umklapp processes due to non-conservation of the center of mass motion are investigated for parameters of relevant experimental interest. The model naturally keeps into account the effect of excited energy bands and is particularly suited for being adapted to rigorous close-coupled calculations. Our formalism shows that a correct derivation of the parameters in tight-binding effective ","authors_text":"Andrea Simoni, Hugo Terrier, Jean-Michel Launay","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2016-04-01T13:41:43Z","title":"Influence of the energy-band structure on ultracold reactive processes in lattices"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.00238","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":"sha256:13fde7c57a28f32ec71aa863fb0a6dd554f6612659e2c5eb4b808abdff915519","target":"record","created_at":"2026-05-18T01:17:16Z","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":"d56b5bac753021f9ef415c8f0cdd66cdd57725360626e88b7b5c3dc80563e024","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2016-04-01T13:41:43Z","title_canon_sha256":"024ad50007cd91cef5bf6880d3504fa95f07204025205b42846ee703259a6f78"},"schema_version":"1.0","source":{"id":"1604.00238","kind":"arxiv","version":1}},"canonical_sha256":"9369797d40574816fba433ddeb6f69f5c053a841505185a71ed8e7796f3289df","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9369797d40574816fba433ddeb6f69f5c053a841505185a71ed8e7796f3289df","first_computed_at":"2026-05-18T01:17:16.718669Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:17:16.718669Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"5NKVWdyPIAlk6tf6963Y7YtN0V1fymGInRjL2VCvlmfzB5fdObFccMn16cwD+RZAJodo1132fXfkdXs1y9BtAA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:17:16.719445Z","signed_message":"canonical_sha256_bytes"},"source_id":"1604.00238","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:13fde7c57a28f32ec71aa863fb0a6dd554f6612659e2c5eb4b808abdff915519","sha256:22026916d085c8048273b4e573b37a8d59ccc64f4acb8d152849102e31c71e22"],"state_sha256":"99bf96f7719302a106e6f643aa5fa4adf8f35fc3c3643f5bf559d4ed49856942"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lWn7TFxS8Wj5OiQKVfBwWPBwK4mxYK2GnVt5L1o6g6RluaiI3CAvRy05dLhYXCzv56kuLRyhQh3qiOnM3FrMDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-25T07:40:27.712709Z","bundle_sha256":"e9eeb338231d9c22fcb9b9a8e7e2cd28f4a22675790fe18969a786ff6d2826fc"}}