{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:G54XO3NWG3UDDYJ25FWRYAH7H7","short_pith_number":"pith:G54XO3NW","canonical_record":{"source":{"id":"1510.07914","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-10-27T14:12:32Z","cross_cats_sorted":[],"title_canon_sha256":"783a2cca92c293480af9d43f69e245b926086babc192629392304ff701a83d87","abstract_canon_sha256":"9de851a16c889846005c3acaa74c73129b52abbb47cf6c4ae392ae7bc471fab6"},"schema_version":"1.0"},"canonical_sha256":"3779776db636e831e13ae96d1c00ff3fdef12738cd09d40c18ccda1418467e16","source":{"kind":"arxiv","id":"1510.07914","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1510.07914","created_at":"2026-05-18T01:08:20Z"},{"alias_kind":"arxiv_version","alias_value":"1510.07914v3","created_at":"2026-05-18T01:08:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.07914","created_at":"2026-05-18T01:08:20Z"},{"alias_kind":"pith_short_12","alias_value":"G54XO3NWG3UD","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_16","alias_value":"G54XO3NWG3UDDYJ2","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_8","alias_value":"G54XO3NW","created_at":"2026-05-18T12:29:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:G54XO3NWG3UDDYJ25FWRYAH7H7","target":"record","payload":{"canonical_record":{"source":{"id":"1510.07914","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-10-27T14:12:32Z","cross_cats_sorted":[],"title_canon_sha256":"783a2cca92c293480af9d43f69e245b926086babc192629392304ff701a83d87","abstract_canon_sha256":"9de851a16c889846005c3acaa74c73129b52abbb47cf6c4ae392ae7bc471fab6"},"schema_version":"1.0"},"canonical_sha256":"3779776db636e831e13ae96d1c00ff3fdef12738cd09d40c18ccda1418467e16","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:08:20.753182Z","signature_b64":"5NHOQmKLBtjb1s9+FagWh41v3n72tZHMVvf+plRQr3xuHwkLFzPQLrblic3yDLHoTouEC6o0DqOOBQ1DFkmTBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3779776db636e831e13ae96d1c00ff3fdef12738cd09d40c18ccda1418467e16","last_reissued_at":"2026-05-18T01:08:20.752494Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:08:20.752494Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1510.07914","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:08:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ac/mjfbovVHQu8AFxh/D8Fby+vb+vVPPBN+5jQpOJeUQKG5a8Gf0UXl+rYdw9K0HvHfDh3SJpZmOX/dprZwXCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T21:47:47.338297Z"},"content_sha256":"286173bc15fa92b40aa0bfde5206bcbfe211b8e1a34dedb4e92df235133ab555","schema_version":"1.0","event_id":"sha256:286173bc15fa92b40aa0bfde5206bcbfe211b8e1a34dedb4e92df235133ab555"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:G54XO3NWG3UDDYJ25FWRYAH7H7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Simulations of the angular dependence of the dipole-dipole interaction among Rydberg atoms","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Jacob L. Bigelow, Jacob T. Paul, Matan Peleg, Michael W. Noel, Thomas J. Carroll, Veronica L. Sanford","submitted_at":"2015-10-27T14:12:32Z","abstract_excerpt":"The dipole-dipole interaction between two Rydberg atoms depends on the relative orientation of the atoms and on the change in the magnetic quantum number. We simulate the effect of this anisotropy on the energy transport in an amorphous many atom system subject to a homogeneous applied electric field. We consider two experimentally feasible geometries and find that the effects should be measurable in current generation imaging experiments. In both geometries atoms of $p$ character are localized to a small region of space which is immersed in a larger region that is filled with atoms of $s$ cha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.07914","kind":"arxiv","version":3},"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":"2026-05-18T01:08:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UNSLUkk78QBqqjdHLCyR+m3FqHo7WFnp0pi9zdMFAXoEluSSbnSfTbTx/3CH9IfpM8IeoUpziuFuTJa2gddBCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T21:47:47.339041Z"},"content_sha256":"9ab2aebdee661d99b8cd4499d8f5fd84e49fac13111a15c23ffe680584526817","schema_version":"1.0","event_id":"sha256:9ab2aebdee661d99b8cd4499d8f5fd84e49fac13111a15c23ffe680584526817"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/G54XO3NWG3UDDYJ25FWRYAH7H7/bundle.json","state_url":"https://pith.science/pith/G54XO3NWG3UDDYJ25FWRYAH7H7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/G54XO3NWG3UDDYJ25FWRYAH7H7/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":"2026-05-28T21:47:47Z","links":{"resolver":"https://pith.science/pith/G54XO3NWG3UDDYJ25FWRYAH7H7","bundle":"https://pith.science/pith/G54XO3NWG3UDDYJ25FWRYAH7H7/bundle.json","state":"https://pith.science/pith/G54XO3NWG3UDDYJ25FWRYAH7H7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/G54XO3NWG3UDDYJ25FWRYAH7H7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:G54XO3NWG3UDDYJ25FWRYAH7H7","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":"9de851a16c889846005c3acaa74c73129b52abbb47cf6c4ae392ae7bc471fab6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-10-27T14:12:32Z","title_canon_sha256":"783a2cca92c293480af9d43f69e245b926086babc192629392304ff701a83d87"},"schema_version":"1.0","source":{"id":"1510.07914","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1510.07914","created_at":"2026-05-18T01:08:20Z"},{"alias_kind":"arxiv_version","alias_value":"1510.07914v3","created_at":"2026-05-18T01:08:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.07914","created_at":"2026-05-18T01:08:20Z"},{"alias_kind":"pith_short_12","alias_value":"G54XO3NWG3UD","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_16","alias_value":"G54XO3NWG3UDDYJ2","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_8","alias_value":"G54XO3NW","created_at":"2026-05-18T12:29:22Z"}],"graph_snapshots":[{"event_id":"sha256:9ab2aebdee661d99b8cd4499d8f5fd84e49fac13111a15c23ffe680584526817","target":"graph","created_at":"2026-05-18T01:08:20Z","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":"The dipole-dipole interaction between two Rydberg atoms depends on the relative orientation of the atoms and on the change in the magnetic quantum number. We simulate the effect of this anisotropy on the energy transport in an amorphous many atom system subject to a homogeneous applied electric field. We consider two experimentally feasible geometries and find that the effects should be measurable in current generation imaging experiments. In both geometries atoms of $p$ character are localized to a small region of space which is immersed in a larger region that is filled with atoms of $s$ cha","authors_text":"Jacob L. Bigelow, Jacob T. Paul, Matan Peleg, Michael W. Noel, Thomas J. Carroll, Veronica L. Sanford","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-10-27T14:12:32Z","title":"Simulations of the angular dependence of the dipole-dipole interaction among Rydberg atoms"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.07914","kind":"arxiv","version":3},"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":"sha256:286173bc15fa92b40aa0bfde5206bcbfe211b8e1a34dedb4e92df235133ab555","target":"record","created_at":"2026-05-18T01:08:20Z","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":"9de851a16c889846005c3acaa74c73129b52abbb47cf6c4ae392ae7bc471fab6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-10-27T14:12:32Z","title_canon_sha256":"783a2cca92c293480af9d43f69e245b926086babc192629392304ff701a83d87"},"schema_version":"1.0","source":{"id":"1510.07914","kind":"arxiv","version":3}},"canonical_sha256":"3779776db636e831e13ae96d1c00ff3fdef12738cd09d40c18ccda1418467e16","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3779776db636e831e13ae96d1c00ff3fdef12738cd09d40c18ccda1418467e16","first_computed_at":"2026-05-18T01:08:20.752494Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:08:20.752494Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"5NHOQmKLBtjb1s9+FagWh41v3n72tZHMVvf+plRQr3xuHwkLFzPQLrblic3yDLHoTouEC6o0DqOOBQ1DFkmTBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:08:20.753182Z","signed_message":"canonical_sha256_bytes"},"source_id":"1510.07914","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:286173bc15fa92b40aa0bfde5206bcbfe211b8e1a34dedb4e92df235133ab555","sha256:9ab2aebdee661d99b8cd4499d8f5fd84e49fac13111a15c23ffe680584526817"],"state_sha256":"761adc91c942a72f11afefb07dd825d9d0fb926aa6c7df029d60d7e55f9478c6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"N/tFCAkqQukXs3rym6X79e29L5wGujq3FjsvjPL56AwcHytWCWETNAkxTLTedFL40UMqn+gpWQ7APzveWi0aAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T21:47:47.342753Z","bundle_sha256":"d2902064e3e8672d0f797b9fb735f22684d00d239820c8160c3c3d20c0a1f7e3"}}