More varieties of 4-d gauge theories: product representations

A bstract Recently, we used methods of arithmetic geometry to study the anomaly-free irreducible representations of an arbitrary gauge Lie algebra. Here we generalize to the case of products of irreducible representations, where it is again possible to give a complete description. A key result is that the projective variety corresponding to m -fold product representations of the Lie algebra $$ {\mathfrak{su}}_n $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>su</mml:mi> <mml:mi>n</mml:mi> </mml:msub> </mml:math> is a rational variety for every m and n . We study the simplest case of $$ {\mathfrak{su}}_3 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>su</mml:mi> <mml:mn>3</mml:mn> </mml:msub> </mml:math> (corresponding to the strong interaction) in detail. We also describe the implications of a number-theoretic conjecture of Manin (and related theorems) for the number of chiral representations of bounded size B (measured roughly by the Dynkin labels) compared to non-chiral ones, giving a precise meaning to the sense in which the former (which are those most relevant for phenomenology) are rare compared to the latter. As examples, we show that, for both irreducible representations of $$ {\mathfrak{su}}_5 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>su</mml:mi> <mml:mn>5</mml:mn> </mml:msub> </mml:math> and once-reducible product representations of $$ {\mathfrak{su}}_3 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>su</mml:mi> <mml:mn>3</mml:mn> </mml:msub> </mml:math> that are non-anomalous, the number of chiral representations is asymptotically between B (log B ) 5 and $$ {B}^{\frac{4}{3}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mi>B</mml:mi> <mml:mfrac> <mml:mn>4</mml:mn> <mml:mn>3</mml:mn> </mml:mfrac> </mml:msup> </mml:math> , while the number of non-chiral representations is asymptotically B 2 . Despite this rarity of chiral, anomaly-free, product representations, we show that there are examples relevant for phenomenology, including one that gives an asymptotically-free gauge theory with Lie algebra $$ {\mathfrak{su}}_7 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>su</mml:mi> <mml:mn>7</mml:mn> </mml:msub> </mml:math> .

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Publication Details

Journal
Journal of High Energy Physics
Published
2025-08-18
DOI
https://doi.org/10.1007/jhep08(2025)133
Citations
2
Primary Topic
Black Holes and Theoretical Physics
Type
article
Field-Weighted Citation Impact
3.74

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article

More varieties of 4-d gauge theories: product representations

Ben Gripaios, Khoi Le Nguyen Nguyen
2 citations
Journal of High Energy Physics
Black Holes and Theoretical Physics
3.74
article

More varieties of 4-d gauge theories: product representations

Ben Gripaios, Khoi Le Nguyen Nguyen
article en
2 citations

Abstract

A bstract Recently, we used methods of arithmetic geometry to study the anomaly-free irreducible representations of an arbitrary gauge Lie algebra. Here we generalize to the case of products of irreducible representations, where it is again possible to give a complete description. A key result is that the projective variety corresponding to m -fold product representations of the Lie algebra $$ {\mathfrak{su}}_n $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>su</mml:mi> <mml:mi>n</mml:mi> </mml:msub> </mml:math> is a rational variety for every m and n . We study the simplest case of $$ {\mathfrak{su}}_3 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>su</mml:mi> <mml:mn>3</mml:mn> </mml:msub> </mml:math> (corresponding to the strong interaction) in detail. We also describe the implications of a number-theoretic conjecture of Manin (and related theorems) for the number of chiral representations of bounded size B (measured roughly by the Dynkin labels) compared to non-chiral ones, giving a precise meaning to the sense in which the former (which are those most relevant for phenomenology) are rare compared to the latter. As examples, we show that, for both irreducible representations of $$ {\mathfrak{su}}_5 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>su</mml:mi> <mml:mn>5</mml:mn> </mml:msub> </mml:math> and once-reducible product representations of $$ {\mathfrak{su}}_3 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>su</mml:mi> <mml:mn>3</mml:mn> </mml:msub> </mml:math> that are non-anomalous, the number of chiral representations is asymptotically between B (log B ) 5 and $$ {B}^{\frac{4}{3}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mi>B</mml:mi> <mml:mfrac> <mml:mn>4</mml:mn> <mml:mn>3</mml:mn> </mml:mfrac> </mml:msup> </mml:math> , while the number of non-chiral representations is asymptotically B 2 . Despite this rarity of chiral, anomaly-free, product representations, we show that there are examples relevant for phenomenology, including one that gives an asymptotically-free gauge theory with Lie algebra $$ {\mathfrak{su}}_7 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>su</mml:mi> <mml:mn>7</mml:mn> </mml:msub> </mml:math> .

Journal of High Energy PhysicsVol. 2025(8)
University of Cambridge (GB)
Science and Technology Facilities Council, Japan Society for the Promotion of Science
Openalex Percentile: Top 7%
Black Holes and Theoretical Physics
3.74
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