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Quantum Hamiltonian Reduction of the Schwinger Model

High Energy Physics - Theory · Submitted 29 Jun 1994

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim However, we find that the discrepancy is resolved by redefinitions of fermion currents and that the results are again consistent with those of the classical reduction.

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arXiv IDhep-th/9406195 (version 1)
Pith IDM3CODZFK, Pith's permanent record of this paper and its review
CitationKazunori Itakura, Koichi Ohta. "Quantum Hamiltonian Reduction of the Schwinger Model." arXiv:hep-th/9406195 (1994). https://pith.science/paper/M3CODZFK
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What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.60 · human participants 0.01 · controlled comparison 0.22 · randomized assignment 0.01 · states quantitative result 0.04 · compares with prior results 0.95 · mentions code or data availability 0.02.

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arXiv listing abstract v1. Results and the main claim are underlined; .

We reexamine a unitary-transformation method of extracting a physical Hamiltonian from a gauge field theory after quantizing all degrees of freedom including redundant variables. We show that this {\it quantum Hamiltonian reduction} method suffers from crucial modifications arising from regularization of composite operators. We assess the effects of regularization in the simplest gauge field theory, the Schwinger model. Without regularization, the quantum reduction yields the identical Hamiltonian with the classically reduced one. On the other hand, with regularization incorporated, the resulting Hamiltonian of the quantum reduction disagrees with that of the classical reduction. However, we find that the discrepancy is resolved by redefinitions of fermion currents and that the results are again consistent with those of the classical reduction.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 We reexamine a unitary-transformation method of extracting a physical Hamiltonian from a gauge field theory after quantizing all degrees of freedom including redundant variables. background 0.49 0.46 0.04 asserted 0.71
s1 We show that this {\it quantum Hamiltonian reduction} method suffers from crucial modifications arising from regularization of composite operators. result 0.83 0.74 0.37 asserted 1.00
s2 We assess the effects of regularization in the simplest gauge field theory, the Schwinger model. contribution 0.56 0.83 0.04 asserted 0.82
s3 Without regularization, the quantum reduction yields the identical Hamiltonian with the classically reduced one. result 1.00 0.73 0.08 asserted 1.00
s4 On the other hand, with regularization incorporated, the resulting Hamiltonian of the quantum reduction disagrees with that of the classical reduction. result 1.00 0.85 0.13 asserted 1.00
s5 However, we find that the discrepancy is resolved by redefinitions of fermion currents and that the results are again consistent with those of the classical reduction. result 0.98 0.95 0.75 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 1.00.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

We reexamine a unitary-transformation method of extracting a physical Hamiltonian from a gauge field theory after quantizing all degrees of freedom including redundant variables. We show that this {\it quantum Hamiltonian reduction} method suffers from crucial modifications arising from regularization of composite operators. We assess the effects of regularization in the simplest gauge field theory, the Schwinger model. Without regularization, the quantum reduction yields the identical Hamiltonian with the classically reduced one. On the other hand, with regularization incorporated, the resulting Hamiltonian of the quantum reduction disagrees with that of the classical reduction. However, we find that the discrepancy is resolved by redefinitions of fermion currents and that the results are again consistent with those of the classical reduction.

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