Triple

T22842409
Position Surface form Disambiguated ID Type / Status
Subject Dirac quantization condition E566115 entity
Predicate usedIn P98 FINISHED
Object ’t Hooft–Polyakov monopole analysis NE NERFINISHED

How this triple was built (2 steps)

Every LLM step that produced this triple, in pipeline order — named-entity classification, the disambiguation choices (the exact options shown, with the pick highlighted), and the generated description. The batch + timestamp of each is in the Provenance table below.

NER Named-entity recognition gpt-5-mini
Instruction
Given a phrase, classify it is english named entity (e.g., persons, organizations, works of art) in Latin script, or not (e.g., literals, dates, URLs, verbose phrases). For disambiguation, the statement where the phrase occurs as object is also given. Please return a JSON object with `phrase` (string, the phrase being analyzed) and `is_ne` (boolean, indicating whether the phrase is a Named Entity).
Input
Phrase: ’t Hooft–Polyakov monopole analysis | Statement: [Dirac quantization condition, usedIn, ’t Hooft–Polyakov monopole analysis]
NED1 Entity disambiguation (via context triple) gpt-5-mini-2025-08-07
Target entity: ’t Hooft–Polyakov monopole analysis
Context triple: [Dirac quantization condition, usedIn, ’t Hooft–Polyakov monopole analysis]
  • A. ’t Hooft–Polyakov monopoles chosen
    ’t Hooft–Polyakov monopoles are theoretical, finite-energy magnetic monopole solutions arising in certain non-abelian gauge theories with spontaneous symmetry breaking.
  • B. Dirac magnetic monopoles
    Dirac magnetic monopoles are hypothetical elementary particles proposed by Paul Dirac that carry isolated magnetic charge, whose existence would explain the quantization of electric charge and profoundly impact fundamental physics.
  • C. Yang monopole
    The Yang monopole is a theoretical higher-dimensional generalization of the magnetic monopole introduced by physicist C. N. Yang in the context of non-Abelian gauge theories and fiber bundles.
  • D. ’t Hooft–Veltman gauge
    The ’t Hooft–Veltman gauge is a renormalizable gauge-fixing scheme in quantum field theory, particularly used in non-Abelian gauge theories to simplify calculations and maintain consistency of the theory.
  • E. Georgi–Glashow model
    The Georgi–Glashow model is a grand unified theory in particle physics that unifies the strong, weak, and electromagnetic interactions within an SU(5) gauge symmetry framework.
  • F. None of above.
  • G. Unsure - the case is ambiguous/there is not enough information to decide.

Provenance (2 batches)

The batch behind each pipeline step, in order, with when it ran. Timestamps are batch-level — stages were processed in waves, so the object chain (NER → NED1 → NEDg → NED2) reads in order, but predicate / elicitation batches can sit in a different wave.

Step Stage Batch ID Status When
creating Elicitation batch_69e245869e188190a196584f36e682da completed April 17, 2026, 2:36 p.m.
NER Named-entity recognition batch_69f17e855abc8190b9cf8cc515090a7f completed April 29, 2026, 3:44 a.m.
Created at: April 17, 2026, 3:35 p.m.