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Duality, Phases, Spinors and Monopoles in SO(N) and Spin(N) Gauge Theories
High Energy Physics - Theory · Submitted 11 Sep 1997
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim It follows that electric sources in the spinor representation, needed as test charges to determine the phase of an SO(N) gauge theory, can be introduced as Z_2-valued magnetic sources in the dual nonabelian gauge theory.
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The abstract, sentence by sentence
Four-dimensional N=1 supersymmetric Spin(N) gauge theories with matter in the vector and spinor representations are considered. Dual descriptions are known for some of these theories. It is noted that when masses are given to all fields in the spinor representation, the dual gauge group G breaks to a group H such that \pi_2(G/H)=Z_2. The quantum numbers of the associated Z_2 monopole and those of the massive spinors are shown to agree, suggesting that the monopole is the image of the massive spinors under duality. It follows that electric sources in the spinor representation, needed as test charges to determine the phase of an SO(N) gauge theory, can be introduced as Z_2-valued magnetic sources in the dual nonabelian gauge theory. This fact is used to study the phases of SO(N) gauge theories with matter in the vector representation.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Four-dimensional N=1 supersymmetric Spin(N) gauge theories with matter in the vector and spinor representations are considered. | background 0.79 | 0.37 | 0.03 | asserted 0.77 |
| s1 | Dual descriptions are known for some of these theories. | background 0.99 | 0.05 | 0.02 | asserted 0.99 |
| s2 | It is noted that when masses are given to all fields in the spinor representation, the dual gauge group G breaks to a group H such that \pi_2(G/H)=Z_2. | result 0.87 | 0.27 | 0.10 | asserted 0.99 |
| s3 | The quantum numbers of the associated Z_2 monopole and those of the massive spinors are shown to agree, suggesting that the monopole is the image of the massive spinors under duality. | interpretation 0.59 | 0.82 | 0.32 | hedged possibility 0.87 |
| s4 | It follows that electric sources in the spinor representation, needed as test charges to determine the phase of an SO(N) gauge theory, can be introduced as Z_2-valued magnetic sources in the dual nonabelian gauge theory. | interpretation 0.64 | 0.71 | 0.33 | asserted 0.99 |
| s5 | This fact is used to study the phases of SO(N) gauge theories with matter in the vector representation. | contribution 0.82 | 0.79 | 0.26 | asserted 0.99 |
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The paper
Original abstract
Four-dimensional N=1 supersymmetric Spin(N) gauge theories with matter in the vector and spinor representations are considered. Dual descriptions are known for some of these theories. It is noted that when masses are given to all fields in the spinor representation, the dual gauge group G breaks to a group H such that \pi_2(G/H)=Z_2. The quantum numbers of the associated Z_2 monopole and those of the massive spinors are shown to agree, suggesting that the monopole is the image of the massive spinors under duality. It follows that electric sources in the spinor representation, needed as test charges to determine the phase of an SO(N) gauge theory, can be introduced as Z_2-valued magnetic sources in the dual nonabelian gauge theory. This fact is used to study the phases of SO(N) gauge theories with matter in the vector representation.
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References
How the literature uses it
7 arXiv papers cite this in 11 sentences
Papers citing it · 6 sentences without a confident label
Builds on it 1 paper
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This was then extended to $(8)$ in [ref] , to $(10)$ in [ref] , to $(11)$ in [ref] , and to $(12)$ in [ref] . $(N)$ gauge theories with multiple chiral fields in the spinor representation was considered in [ref] .
Lectures on 4d N=1 dynamics and related topics · Other dualities · 0.91
Cites it as support 1 paper
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This interpretation is reiterated (albeit without explicitly naming a gerbe structure) in [ref] [section 2], [ref] in terms of screening effects, and further examples of the same general form are given in [ref] .
Sums over topological sectors and quantization of Fayet-Iliopoulos parameters · Field theory · 0.96
Cites it as background 3 papers
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Following a crucial set of observations in [ref] that spinors in the original theory are mapped to magnetic monopoles in the dual theory, the Intriligator-Seiberg duality of 1 $$ theories was refined in [ref] , to account for the global form of the gauge group and the discrete theta angle.
Matching higher symmetries across Intriligator-Seiberg duality · Introduction and summary · 0.83
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Let us next consider some examples of gerbe structures appearing in the field theories discussed in [ref] .
Sums over topological sectors and quantization of Fayet-Iliopoulos parameters · Field theory · 0.81
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Such theories have also been discussed implicitly in a number of other places in the physics literature (see for example [ref] ).
Rigidly Supersymmetric Gauge Theories on Curved Superspace · Sigma models on stacks and restrictions on nonperturbative sectors · 0.91
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