{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:PMRSSGJ7CVCBJ6CNGGE6LBHEJD","short_pith_number":"pith:PMRSSGJ7","canonical_record":{"source":{"id":"2605.15101","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2026-05-14T17:19:49Z","cross_cats_sorted":[],"title_canon_sha256":"7e276375955cb24a2a2d06fb702f3e09117b206c671a2971547c92b36434974c","abstract_canon_sha256":"b4bb1e426ddad4815538b5d86f4617da8ee3fa16aa543c7ca6c39930f322acea"},"schema_version":"1.0"},"canonical_sha256":"7b2329193f154414f84d3189e584e448cfc794e2771df63e9dfac0e7bd8463ca","source":{"kind":"arxiv","id":"2605.15101","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.15101","created_at":"2026-05-17T21:18:33Z"},{"alias_kind":"arxiv_version","alias_value":"2605.15101v1","created_at":"2026-05-17T21:18:33Z"},{"alias_kind":"pith_short_12","alias_value":"PMRSSGJ7CVCB","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"PMRSSGJ7CVCBJ6CN","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"PMRSSGJ7","created_at":"2026-05-18T12:33:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:PMRSSGJ7CVCBJ6CNGGE6LBHEJD","target":"record","payload":{"canonical_record":{"source":{"id":"2605.15101","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2026-05-14T17:19:49Z","cross_cats_sorted":[],"title_canon_sha256":"7e276375955cb24a2a2d06fb702f3e09117b206c671a2971547c92b36434974c","abstract_canon_sha256":"b4bb1e426ddad4815538b5d86f4617da8ee3fa16aa543c7ca6c39930f322acea"},"schema_version":"1.0"},"canonical_sha256":"7b2329193f154414f84d3189e584e448cfc794e2771df63e9dfac0e7bd8463ca","receipt":{"kind":"pith_receipt","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.2","canonical_sha256":"7b2329193f154414f84d3189e584e448cfc794e2771df63e9dfac0e7bd8463ca","last_reissued_at":"2026-05-17T21:57:19.147697Z","signature_status":"unsigned_v0","first_computed_at":"2026-05-17T21:40:25.816978Z"},"source_kind":"arxiv","source_id":"2605.15101","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":"2026-05-17T21:18:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"edEnfKnx6yaDMt9Cr+bmx18mLKVZQfwec1ro09Odl+4Vgcm1qCkx6LRgRkt79NjwUUFLLB+Ej85M5W+5TxRsCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T15:24:45.948071Z"},"content_sha256":"3f4b2ecb8868f0710f856e60d1ac24ef8b79f663589998d950ea9f98cefc7f8e","schema_version":"1.0","event_id":"sha256:3f4b2ecb8868f0710f856e60d1ac24ef8b79f663589998d950ea9f98cefc7f8e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:PMRSSGJ7CVCBJ6CNGGE6LBHEJD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The Emergence of Photonic Crystalline Order and Time-Series Dynamics in NaCl Droplet Deposition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"Diffusion anisotropy governs the maximal size of crystalline structures in evaporating NaCl droplets on germanium.","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Benedykt R. Jany, Grzegorz Cios, Grzegorz S. \\.Zmija","submitted_at":"2026-05-14T17:19:49Z","abstract_excerpt":"Crystallization during droplet evaporation gives rise to complex, self-organized structures, yet the mechanisms underlying the emergence of ordered functional phases remain poorly understood. In this study, we present a comprehensive, multi-scale investigation into the crystallization dynamics of NaCl during droplet evaporation on a germanium (001) substrate, relevant for its IR applications. Through systematic microscopic characterization, we identify the formation of diverse microstructures, including 1D photonic crystal nanostructures formed within hybrid crystal-glass photonic system. To e"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"diffusion anisotropy, rather than growth kinetics, primarily governs the maximal attainable structure size. Quantitative thin film interference analysis demonstrates the presence of discrete thickness layers in the film.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"That the newly introduced NaCl equivalent height metric provides an unbiased, condition-independent classifier of crystalline morphology without hidden dependence on substrate interactions or imaging resolution.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"NaCl droplet evaporation on germanium produces 1D photonic crystal nanostructures whose maximum size is set by diffusion anisotropy, enabled by a new equivalent-height metric and time-series height analysis.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"Diffusion anisotropy governs the maximal size of crystalline structures in evaporating NaCl droplets on germanium.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"08e3a132484768c66564c5bbf35ae8ce927f39afd69a2621104a2349214b80d1"},"source":{"id":"2605.15101","kind":"arxiv","version":1},"verdict":{"id":"b938cd26-f6f0-477e-975a-c98b33bcfa6c","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-15T03:14:21.385403Z","strongest_claim":"diffusion anisotropy, rather than growth kinetics, primarily governs the maximal attainable structure size. Quantitative thin film interference analysis demonstrates the presence of discrete thickness layers in the film.","one_line_summary":"NaCl droplet evaporation on germanium produces 1D photonic crystal nanostructures whose maximum size is set by diffusion anisotropy, enabled by a new equivalent-height metric and time-series height analysis.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"That the newly introduced NaCl equivalent height metric provides an unbiased, condition-independent classifier of crystalline morphology without hidden dependence on substrate interactions or imaging resolution.","pith_extraction_headline":"Diffusion anisotropy governs the maximal size of crystalline structures in evaporating NaCl droplets on germanium."},"references":{"count":3,"sample":[{"doi":"10.1016/j.physrep.2003.09.001","year":2003,"title":"29 Zandvliet, H. J. W. (2003). The Ge(001) surface. Physics Reports, 388, 1–40. https://doi.org/10.1016/j.physrep.2003.09.001 30 Lee, D. and Lee, S. (2025). Color simulation of multilayered thin films","work_id":"b1ee9587-fa04-4077-8a48-1c889ce809d4","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"10.3390/app15094814","year":2012,"title":"Fiji: an open-source platform for biological-image analysis","work_id":"582ffa6e-ce21-4cf9-a4b0-34b6f6af5648","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"10.1016/0304-4076(86)90063-1","year":null,"title":"https://doi.org/10.1016/0304-4076(86)90063-1 Supporting Information The Emergence of Photonic Crystalline Order and Time-Series Dynamics in NaCl Droplet Deposition Grzegorz S. Żmija1, Grzegorz Cios2, ","work_id":"d1f1a331-83b7-4904-b836-e96f9c1e53b8","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":3,"snapshot_sha256":"ac99fb2fb6e5c7bb59f699ff7db4b1cc17201551a9215ee79946831d8ee056ca","internal_anchors":0},"formal_canon":{"evidence_count":2,"snapshot_sha256":"d07cd2bdd1de35a24fa7dc7c636a7e0d1cd634a78cb74f13a963439ac66f9edf"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":"b938cd26-f6f0-477e-975a-c98b33bcfa6c"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T21:57:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2/oJ9z7+/8/yF9a/JmiJedQcMMIGpAEg7olFMbeGprFx0IYZYKPub0Fb2udHTzgZW7Hy9OgKObby1By8OolVDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T15:24:45.949281Z"},"content_sha256":"c1275251d6adf219f8f2db31188370c45f5c7fec826caf1492fb6cf4ffa037e1","schema_version":"1.0","event_id":"sha256:c1275251d6adf219f8f2db31188370c45f5c7fec826caf1492fb6cf4ffa037e1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PMRSSGJ7CVCBJ6CNGGE6LBHEJD/bundle.json","state_url":"https://pith.science/pith/PMRSSGJ7CVCBJ6CNGGE6LBHEJD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PMRSSGJ7CVCBJ6CNGGE6LBHEJD/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":"2026-05-31T15:24:45Z","links":{"resolver":"https://pith.science/pith/PMRSSGJ7CVCBJ6CNGGE6LBHEJD","bundle":"https://pith.science/pith/PMRSSGJ7CVCBJ6CNGGE6LBHEJD/bundle.json","state":"https://pith.science/pith/PMRSSGJ7CVCBJ6CNGGE6LBHEJD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PMRSSGJ7CVCBJ6CNGGE6LBHEJD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:PMRSSGJ7CVCBJ6CNGGE6LBHEJD","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":"b4bb1e426ddad4815538b5d86f4617da8ee3fa16aa543c7ca6c39930f322acea","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2026-05-14T17:19:49Z","title_canon_sha256":"7e276375955cb24a2a2d06fb702f3e09117b206c671a2971547c92b36434974c"},"schema_version":"1.0","source":{"id":"2605.15101","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.15101","created_at":"2026-05-17T21:18:33Z"},{"alias_kind":"arxiv_version","alias_value":"2605.15101v1","created_at":"2026-05-17T21:18:33Z"},{"alias_kind":"pith_short_12","alias_value":"PMRSSGJ7CVCB","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"PMRSSGJ7CVCBJ6CN","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"PMRSSGJ7","created_at":"2026-05-18T12:33:37Z"}],"graph_snapshots":[{"event_id":"sha256:c1275251d6adf219f8f2db31188370c45f5c7fec826caf1492fb6cf4ffa037e1","target":"graph","created_at":"2026-05-17T21:57:19Z","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":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"diffusion anisotropy, rather than growth kinetics, primarily governs the maximal attainable structure size. Quantitative thin film interference analysis demonstrates the presence of discrete thickness layers in the film."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"That the newly introduced NaCl equivalent height metric provides an unbiased, condition-independent classifier of crystalline morphology without hidden dependence on substrate interactions or imaging resolution."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"NaCl droplet evaporation on germanium produces 1D photonic crystal nanostructures whose maximum size is set by diffusion anisotropy, enabled by a new equivalent-height metric and time-series height analysis."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Diffusion anisotropy governs the maximal size of crystalline structures in evaporating NaCl droplets on germanium."}],"snapshot_sha256":"08e3a132484768c66564c5bbf35ae8ce927f39afd69a2621104a2349214b80d1"},"formal_canon":{"evidence_count":2,"snapshot_sha256":"d07cd2bdd1de35a24fa7dc7c636a7e0d1cd634a78cb74f13a963439ac66f9edf"},"paper":{"abstract_excerpt":"Crystallization during droplet evaporation gives rise to complex, self-organized structures, yet the mechanisms underlying the emergence of ordered functional phases remain poorly understood. In this study, we present a comprehensive, multi-scale investigation into the crystallization dynamics of NaCl during droplet evaporation on a germanium (001) substrate, relevant for its IR applications. Through systematic microscopic characterization, we identify the formation of diverse microstructures, including 1D photonic crystal nanostructures formed within hybrid crystal-glass photonic system. To e","authors_text":"Benedykt R. Jany, Grzegorz Cios, Grzegorz S. \\.Zmija","cross_cats":[],"headline":"Diffusion anisotropy governs the maximal size of crystalline structures in evaporating NaCl droplets on germanium.","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2026-05-14T17:19:49Z","title":"The Emergence of Photonic Crystalline Order and Time-Series Dynamics in NaCl Droplet Deposition"},"references":{"count":3,"internal_anchors":0,"resolved_work":3,"sample":[{"cited_arxiv_id":"","doi":"10.1016/j.physrep.2003.09.001","is_internal_anchor":false,"ref_index":1,"title":"29 Zandvliet, H. J. W. (2003). The Ge(001) surface. Physics Reports, 388, 1–40. https://doi.org/10.1016/j.physrep.2003.09.001 30 Lee, D. and Lee, S. (2025). Color simulation of multilayered thin films","work_id":"b1ee9587-fa04-4077-8a48-1c889ce809d4","year":2003},{"cited_arxiv_id":"","doi":"10.3390/app15094814","is_internal_anchor":false,"ref_index":2,"title":"Fiji: an open-source platform for biological-image analysis","work_id":"582ffa6e-ce21-4cf9-a4b0-34b6f6af5648","year":2012},{"cited_arxiv_id":"","doi":"10.1016/0304-4076(86)90063-1","is_internal_anchor":false,"ref_index":3,"title":"https://doi.org/10.1016/0304-4076(86)90063-1 Supporting Information The Emergence of Photonic Crystalline Order and Time-Series Dynamics in NaCl Droplet Deposition Grzegorz S. Żmija1, Grzegorz Cios2, ","work_id":"d1f1a331-83b7-4904-b836-e96f9c1e53b8","year":null}],"snapshot_sha256":"ac99fb2fb6e5c7bb59f699ff7db4b1cc17201551a9215ee79946831d8ee056ca"},"source":{"id":"2605.15101","kind":"arxiv","version":1},"verdict":{"created_at":"2026-05-15T03:14:21.385403Z","id":"b938cd26-f6f0-477e-975a-c98b33bcfa6c","model_set":{"reader":"grok-4.3"},"one_line_summary":"NaCl droplet evaporation on germanium produces 1D photonic crystal nanostructures whose maximum size is set by diffusion anisotropy, enabled by a new equivalent-height metric and time-series height analysis.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Diffusion anisotropy governs the maximal size of crystalline structures in evaporating NaCl droplets on germanium.","strongest_claim":"diffusion anisotropy, rather than growth kinetics, primarily governs the maximal attainable structure size. Quantitative thin film interference analysis demonstrates the presence of discrete thickness layers in the film.","weakest_assumption":"That the newly introduced NaCl equivalent height metric provides an unbiased, condition-independent classifier of crystalline morphology without hidden dependence on substrate interactions or imaging resolution."}},"verdict_id":"b938cd26-f6f0-477e-975a-c98b33bcfa6c"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:3f4b2ecb8868f0710f856e60d1ac24ef8b79f663589998d950ea9f98cefc7f8e","target":"record","created_at":"2026-05-17T21:18:33Z","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":"b4bb1e426ddad4815538b5d86f4617da8ee3fa16aa543c7ca6c39930f322acea","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2026-05-14T17:19:49Z","title_canon_sha256":"7e276375955cb24a2a2d06fb702f3e09117b206c671a2971547c92b36434974c"},"schema_version":"1.0","source":{"id":"2605.15101","kind":"arxiv","version":1}},"canonical_sha256":"7b2329193f154414f84d3189e584e448cfc794e2771df63e9dfac0e7bd8463ca","receipt":{"builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7b2329193f154414f84d3189e584e448cfc794e2771df63e9dfac0e7bd8463ca","first_computed_at":"2026-05-17T21:40:25.816978Z","kind":"pith_receipt","last_reissued_at":"2026-05-17T21:57:19.147697Z","receipt_version":"0.2","signature_status":"unsigned_v0"},"source_id":"2605.15101","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3f4b2ecb8868f0710f856e60d1ac24ef8b79f663589998d950ea9f98cefc7f8e","sha256:c1275251d6adf219f8f2db31188370c45f5c7fec826caf1492fb6cf4ffa037e1"],"state_sha256":"a9c0985ca977a32ce861e5acdbbe187b9ceb52e7ab9266289a7ce20564cbc4c0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gERfoVRGnOlwFK58UV56VAzmot20AsrkeAXz2JC1nTEPJBBq70zqgsZiDMl+PtFxvKi/FPAiSLrWaEsMgwrgAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T15:24:45.954288Z","bundle_sha256":"d66d62a572f9a8ad414387c0221e2a0f8ed251df917ced4d2f003a867b0b14d3"}}