{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:VNQDVC3FO27ECSQV7QUI7BFUI5","short_pith_number":"pith:VNQDVC3F","canonical_record":{"source":{"id":"1711.00914","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-11-02T20:15:24Z","cross_cats_sorted":[],"title_canon_sha256":"3a7e9917bc1a373d3a49e42d408603d92ae845c744a9e25017af2168c10e688e","abstract_canon_sha256":"15af052ffc1dda09fcded5ec36523965c9df4e29804c07cfc5b9e1911e90dcb6"},"schema_version":"1.0"},"canonical_sha256":"ab603a8b6576be414a15fc288f84b4477908c7fd0a84ca8b0836481f0b8bde7d","source":{"kind":"arxiv","id":"1711.00914","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.00914","created_at":"2026-05-17T23:59:10Z"},{"alias_kind":"arxiv_version","alias_value":"1711.00914v3","created_at":"2026-05-17T23:59:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.00914","created_at":"2026-05-17T23:59:10Z"},{"alias_kind":"pith_short_12","alias_value":"VNQDVC3FO27E","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_16","alias_value":"VNQDVC3FO27ECSQV","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_8","alias_value":"VNQDVC3F","created_at":"2026-05-18T12:31:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:VNQDVC3FO27ECSQV7QUI7BFUI5","target":"record","payload":{"canonical_record":{"source":{"id":"1711.00914","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-11-02T20:15:24Z","cross_cats_sorted":[],"title_canon_sha256":"3a7e9917bc1a373d3a49e42d408603d92ae845c744a9e25017af2168c10e688e","abstract_canon_sha256":"15af052ffc1dda09fcded5ec36523965c9df4e29804c07cfc5b9e1911e90dcb6"},"schema_version":"1.0"},"canonical_sha256":"ab603a8b6576be414a15fc288f84b4477908c7fd0a84ca8b0836481f0b8bde7d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:59:10.103914Z","signature_b64":"QUpz2NhNzKTSUx6Cde7CjU9n1UeW9ZrqkaiK74JcoEZN+ismuUtR8WHDlmrkL1yN0ZZw6pKc4hV1fEpq2KlSCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ab603a8b6576be414a15fc288f84b4477908c7fd0a84ca8b0836481f0b8bde7d","last_reissued_at":"2026-05-17T23:59:10.103215Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:59:10.103215Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1711.00914","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":"2026-05-17T23:59:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wFY1+jcNO1/N1FY7UAwBT11kIOTfKLDGeX51ryrmKTqG4c0syKmpYMQQtoeaL6PrXeGvda31nFMpE+XvlUXRAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-30T12:31:33.408175Z"},"content_sha256":"34775ce8c6d796791b54c603f0cc0146a07f8f0394a25b815212f311353b296c","schema_version":"1.0","event_id":"sha256:34775ce8c6d796791b54c603f0cc0146a07f8f0394a25b815212f311353b296c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:VNQDVC3FO27ECSQV7QUI7BFUI5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Spinor frame formalism for amplitudes and constrained superamplitudes of 10D SYM and 11D supergravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Igor Bandos","submitted_at":"2017-11-02T20:15:24Z","abstract_excerpt":"We show that 10D spinor helicity formalism can be understood as spinor moving frame approach to supersymmetric particles extended to the description of amplitudes. This allows us to develop the spinor helicity formalism for 11D supergravity and a new constrained superfield formalism for 10D SYM and 11D SUGRA amplitudes. We show how the constrained on-shell superfields, one-particle counterparts of the superamplitudes, can be obtained by quantization of massless superparticle mechanics.\n  We make some stages towards the calculation of amplitudes of 10D SYM and 11D SUGRA in this framework. In pa"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.00914","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":"2026-05-17T23:59:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"p01TXLlvutrGnFeDQ8/UIynUv+9WLTpSWoRb8HUCWSR04xUqcs/Lfk/62nMkdlawaq9xtVPgRbYhAim5aHxZAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-30T12:31:33.408526Z"},"content_sha256":"c15d10a6822adc686bac54089865148eb62671c515273f7d61bc80ad958f1567","schema_version":"1.0","event_id":"sha256:c15d10a6822adc686bac54089865148eb62671c515273f7d61bc80ad958f1567"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VNQDVC3FO27ECSQV7QUI7BFUI5/bundle.json","state_url":"https://pith.science/pith/VNQDVC3FO27ECSQV7QUI7BFUI5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VNQDVC3FO27ECSQV7QUI7BFUI5/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":"2026-06-30T12:31:33Z","links":{"resolver":"https://pith.science/pith/VNQDVC3FO27ECSQV7QUI7BFUI5","bundle":"https://pith.science/pith/VNQDVC3FO27ECSQV7QUI7BFUI5/bundle.json","state":"https://pith.science/pith/VNQDVC3FO27ECSQV7QUI7BFUI5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VNQDVC3FO27ECSQV7QUI7BFUI5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:VNQDVC3FO27ECSQV7QUI7BFUI5","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":"15af052ffc1dda09fcded5ec36523965c9df4e29804c07cfc5b9e1911e90dcb6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-11-02T20:15:24Z","title_canon_sha256":"3a7e9917bc1a373d3a49e42d408603d92ae845c744a9e25017af2168c10e688e"},"schema_version":"1.0","source":{"id":"1711.00914","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.00914","created_at":"2026-05-17T23:59:10Z"},{"alias_kind":"arxiv_version","alias_value":"1711.00914v3","created_at":"2026-05-17T23:59:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.00914","created_at":"2026-05-17T23:59:10Z"},{"alias_kind":"pith_short_12","alias_value":"VNQDVC3FO27E","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_16","alias_value":"VNQDVC3FO27ECSQV","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_8","alias_value":"VNQDVC3F","created_at":"2026-05-18T12:31:49Z"}],"graph_snapshots":[{"event_id":"sha256:c15d10a6822adc686bac54089865148eb62671c515273f7d61bc80ad958f1567","target":"graph","created_at":"2026-05-17T23:59:10Z","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 show that 10D spinor helicity formalism can be understood as spinor moving frame approach to supersymmetric particles extended to the description of amplitudes. This allows us to develop the spinor helicity formalism for 11D supergravity and a new constrained superfield formalism for 10D SYM and 11D SUGRA amplitudes. We show how the constrained on-shell superfields, one-particle counterparts of the superamplitudes, can be obtained by quantization of massless superparticle mechanics.\n  We make some stages towards the calculation of amplitudes of 10D SYM and 11D SUGRA in this framework. In pa","authors_text":"Igor Bandos","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-11-02T20:15:24Z","title":"Spinor frame formalism for amplitudes and constrained superamplitudes of 10D SYM and 11D supergravity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.00914","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":"sha256:34775ce8c6d796791b54c603f0cc0146a07f8f0394a25b815212f311353b296c","target":"record","created_at":"2026-05-17T23:59:10Z","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":"15af052ffc1dda09fcded5ec36523965c9df4e29804c07cfc5b9e1911e90dcb6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-11-02T20:15:24Z","title_canon_sha256":"3a7e9917bc1a373d3a49e42d408603d92ae845c744a9e25017af2168c10e688e"},"schema_version":"1.0","source":{"id":"1711.00914","kind":"arxiv","version":3}},"canonical_sha256":"ab603a8b6576be414a15fc288f84b4477908c7fd0a84ca8b0836481f0b8bde7d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ab603a8b6576be414a15fc288f84b4477908c7fd0a84ca8b0836481f0b8bde7d","first_computed_at":"2026-05-17T23:59:10.103215Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:59:10.103215Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"QUpz2NhNzKTSUx6Cde7CjU9n1UeW9ZrqkaiK74JcoEZN+ismuUtR8WHDlmrkL1yN0ZZw6pKc4hV1fEpq2KlSCg==","signature_status":"signed_v1","signed_at":"2026-05-17T23:59:10.103914Z","signed_message":"canonical_sha256_bytes"},"source_id":"1711.00914","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:34775ce8c6d796791b54c603f0cc0146a07f8f0394a25b815212f311353b296c","sha256:c15d10a6822adc686bac54089865148eb62671c515273f7d61bc80ad958f1567"],"state_sha256":"aad20161150164dfc571368e853dbb768e2ba2e567bddb6491647e6d18738f9c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/RSFYrL5j6yXmhTtdOjybQGSxrY3q5CovaXTxJ/I0tzzXI9zlJ3UMxQs1VSOBnC1FpDbNb90C8OzlyDfe+MPDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-30T12:31:33.410324Z","bundle_sha256":"b54b6e45f60d14b17b39859af2717ec6cf774a8a1c4aa2323cc63b94f95ca864"}}