{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:26UNR7AQYULBIPGDK46UWUNPMB","short_pith_number":"pith:26UNR7AQ","canonical_record":{"source":{"id":"1709.07977","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-09-23T00:29:35Z","cross_cats_sorted":[],"title_canon_sha256":"8e355383dd514330970a1c4600cde22a04ffbaeca7eb9f4a90124906c981b455","abstract_canon_sha256":"256fc8fd354ac60f6385ff606c56401ab15cddd7d12867bef89d6842a04c39a3"},"schema_version":"1.0"},"canonical_sha256":"d7a8d8fc10c516143cc3573d4b51af60564282595afbec55cc2bb649f38b4064","source":{"kind":"arxiv","id":"1709.07977","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.07977","created_at":"2026-05-17T23:57:44Z"},{"alias_kind":"arxiv_version","alias_value":"1709.07977v1","created_at":"2026-05-17T23:57:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.07977","created_at":"2026-05-17T23:57:44Z"},{"alias_kind":"pith_short_12","alias_value":"26UNR7AQYULB","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"26UNR7AQYULBIPGD","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"26UNR7AQ","created_at":"2026-05-18T12:30:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:26UNR7AQYULBIPGDK46UWUNPMB","target":"record","payload":{"canonical_record":{"source":{"id":"1709.07977","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-09-23T00:29:35Z","cross_cats_sorted":[],"title_canon_sha256":"8e355383dd514330970a1c4600cde22a04ffbaeca7eb9f4a90124906c981b455","abstract_canon_sha256":"256fc8fd354ac60f6385ff606c56401ab15cddd7d12867bef89d6842a04c39a3"},"schema_version":"1.0"},"canonical_sha256":"d7a8d8fc10c516143cc3573d4b51af60564282595afbec55cc2bb649f38b4064","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:57:44.423110Z","signature_b64":"PVcRwSgMxFBTIien32l3qV43Xv32I3jOA2xt2RG8wGVNX1JrBQuo9oLrBdeQAtaP4MlI0OP/REsZiMNMlAOgAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d7a8d8fc10c516143cc3573d4b51af60564282595afbec55cc2bb649f38b4064","last_reissued_at":"2026-05-17T23:57:44.422648Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:57:44.422648Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1709.07977","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":"2026-05-17T23:57:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"k6FQGZdc6Ytk2g9uZyW5swefYTd966p2ytQPzTaX7uC/RPWNEqcaRUkpgBe8je/S/RwnbVpjfXwm5ZVTpVa0Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T07:44:13.796007Z"},"content_sha256":"0b4ec7cf7bb5e7a251082f64cb53a0a18d1eb620bd977e4cb8f23bad3688d522","schema_version":"1.0","event_id":"sha256:0b4ec7cf7bb5e7a251082f64cb53a0a18d1eb620bd977e4cb8f23bad3688d522"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:26UNR7AQYULBIPGDK46UWUNPMB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Exploring matter wave scattering by means of the phase diagram","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Jeng Yi Lee, Ray-Kuang Lee","submitted_at":"2017-09-23T00:29:35Z","abstract_excerpt":"For matter wave scattering from passive quantum obstacles, we propose a phase diagram in terms of phase and modulus of scattering coefficients to explore all possible directional scattering patterns. In the phase diagram, we can not only have the physical bounds on scattering coefficients for all channels, but also indicate the competitions among absorption, extinction, and scattering cross sessions. With help of this phase diagram, we discuss different scenarios to steer scattering probability distribution, through the interference between $s$- and $p$-channels. In particular, we reveal the r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.07977","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":"2026-05-17T23:57:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"p9X9gFB/9HAGx27Xy5J1KXHFdCu5lTJ3XueUNHnj6v2Fjg8UG8kEV91DVwtf9eJvbuChM4aofjy7jwPLy/96Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T07:44:13.796665Z"},"content_sha256":"5eb36a940182add403c4e4bac608c26bb36dd7e88e71c55ee9896f32040e9e2f","schema_version":"1.0","event_id":"sha256:5eb36a940182add403c4e4bac608c26bb36dd7e88e71c55ee9896f32040e9e2f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/26UNR7AQYULBIPGDK46UWUNPMB/bundle.json","state_url":"https://pith.science/pith/26UNR7AQYULBIPGDK46UWUNPMB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/26UNR7AQYULBIPGDK46UWUNPMB/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":"2026-06-05T07:44:13Z","links":{"resolver":"https://pith.science/pith/26UNR7AQYULBIPGDK46UWUNPMB","bundle":"https://pith.science/pith/26UNR7AQYULBIPGDK46UWUNPMB/bundle.json","state":"https://pith.science/pith/26UNR7AQYULBIPGDK46UWUNPMB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/26UNR7AQYULBIPGDK46UWUNPMB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:26UNR7AQYULBIPGDK46UWUNPMB","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":"256fc8fd354ac60f6385ff606c56401ab15cddd7d12867bef89d6842a04c39a3","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-09-23T00:29:35Z","title_canon_sha256":"8e355383dd514330970a1c4600cde22a04ffbaeca7eb9f4a90124906c981b455"},"schema_version":"1.0","source":{"id":"1709.07977","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.07977","created_at":"2026-05-17T23:57:44Z"},{"alias_kind":"arxiv_version","alias_value":"1709.07977v1","created_at":"2026-05-17T23:57:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.07977","created_at":"2026-05-17T23:57:44Z"},{"alias_kind":"pith_short_12","alias_value":"26UNR7AQYULB","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"26UNR7AQYULBIPGD","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"26UNR7AQ","created_at":"2026-05-18T12:30:55Z"}],"graph_snapshots":[{"event_id":"sha256:5eb36a940182add403c4e4bac608c26bb36dd7e88e71c55ee9896f32040e9e2f","target":"graph","created_at":"2026-05-17T23:57:44Z","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":"For matter wave scattering from passive quantum obstacles, we propose a phase diagram in terms of phase and modulus of scattering coefficients to explore all possible directional scattering patterns. In the phase diagram, we can not only have the physical bounds on scattering coefficients for all channels, but also indicate the competitions among absorption, extinction, and scattering cross sessions. With help of this phase diagram, we discuss different scenarios to steer scattering probability distribution, through the interference between $s$- and $p$-channels. In particular, we reveal the r","authors_text":"Jeng Yi Lee, Ray-Kuang Lee","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-09-23T00:29:35Z","title":"Exploring matter wave scattering by means of the phase diagram"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.07977","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":"sha256:0b4ec7cf7bb5e7a251082f64cb53a0a18d1eb620bd977e4cb8f23bad3688d522","target":"record","created_at":"2026-05-17T23:57:44Z","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":"256fc8fd354ac60f6385ff606c56401ab15cddd7d12867bef89d6842a04c39a3","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-09-23T00:29:35Z","title_canon_sha256":"8e355383dd514330970a1c4600cde22a04ffbaeca7eb9f4a90124906c981b455"},"schema_version":"1.0","source":{"id":"1709.07977","kind":"arxiv","version":1}},"canonical_sha256":"d7a8d8fc10c516143cc3573d4b51af60564282595afbec55cc2bb649f38b4064","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d7a8d8fc10c516143cc3573d4b51af60564282595afbec55cc2bb649f38b4064","first_computed_at":"2026-05-17T23:57:44.422648Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:57:44.422648Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PVcRwSgMxFBTIien32l3qV43Xv32I3jOA2xt2RG8wGVNX1JrBQuo9oLrBdeQAtaP4MlI0OP/REsZiMNMlAOgAQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:57:44.423110Z","signed_message":"canonical_sha256_bytes"},"source_id":"1709.07977","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0b4ec7cf7bb5e7a251082f64cb53a0a18d1eb620bd977e4cb8f23bad3688d522","sha256:5eb36a940182add403c4e4bac608c26bb36dd7e88e71c55ee9896f32040e9e2f"],"state_sha256":"8893280d05a112823075681cf7709feef4e560878a80b4804cce303f44671cc1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Gu5ukN6NdeDuJCWuZGVUIzmA0INpSHwv2s9Avb44TV52U+ZBdIFsRJIWFNTRbNujkgDdNlHliQswA4UstT3tCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T07:44:13.800648Z","bundle_sha256":"e38b68790458c2809d021c2d71103a30c0be5bc6a6ee17a19f2121ff6e9fe9ae"}}