On the trivalent junction of three non-tachyonic heterotic string theories

A bstract Recently, Altavista, Anastasi, Angius and Uranga discussed a method to construct junctions and bouquets of different perturbative string theories. Following this analysis, we here argue that three non-tachyonic ten-dimensional heterotic string theories can be joined together at a nine-dimensional junction. This is done by creating a two-dimensional non-conformal 𝒩 = (0 , 1) supersymmetric quantum field theory with three asymptotic ends, each equipped with one of the worldsheet theories of the supersymmetric E 8 × E 8 theory, the supersymmetric SO(32) theory, and the non-supersymmetric SO(16) × SO(16) theory, respectively. It is actually a special case of a more general construction involving an arbitrary ℤ 2 -symmetric theory T , its ℤ 2 -orbifold T/ ℤ 2 , and the modified ℤ 2 -orbifold ( T × q ) / ℤ 2 , where q is a certain ℤ 2 -symmetric spin invertible theory.

Authors

Institutions

Publication Details

Journal
Journal of High Energy Physics
Published
2026-06-18
DOI
https://doi.org/10.1007/jhep06(2026)194
Primary Topic
Black Holes and Theoretical Physics
Type
article
Field-Weighted Citation Impact
0.00
Controls
|||
ALL TIME
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
article

On the trivalent junction of three non-tachyonic heterotic string theories

Yuji Tachikawa
Journal of High Energy Physics
Black Holes and Theoretical Physics
article

On the trivalent junction of three non-tachyonic heterotic string theories

Yuji Tachikawa
article en

Abstract

A bstract Recently, Altavista, Anastasi, Angius and Uranga discussed a method to construct junctions and bouquets of different perturbative string theories. Following this analysis, we here argue that three non-tachyonic ten-dimensional heterotic string theories can be joined together at a nine-dimensional junction. This is done by creating a two-dimensional non-conformal 𝒩 = (0 , 1) supersymmetric quantum field theory with three asymptotic ends, each equipped with one of the worldsheet theories of the supersymmetric E 8 × E 8 theory, the supersymmetric SO(32) theory, and the non-supersymmetric SO(16) × SO(16) theory, respectively. It is actually a special case of a more general construction involving an arbitrary ℤ 2 -symmetric theory T , its ℤ 2 -orbifold T/ ℤ 2 , and the modified ℤ 2 -orbifold ( T × q ) / ℤ 2 , where q is a certain ℤ 2 -symmetric spin invertible theory.

Journal of High Energy PhysicsVol. 2026(6)
The University of Tokyo (JP)
Openalex Percentile: Top 6%
Black Holes and Theoretical Physics
AI Navigator

Ask Laika to Summarize, Analyze, and Connect papers live on the map.

Summarize Papers & Methodologies

Extract key findings, datasets, and comparative methods across publications.

Benchmark Rankings & Visual Analytics

Rank top research institutions, authors, funders, topics, and journals by Field-Weighted Citation Impact (FWCI) and paper volume with instant charts.

Connect Distant Disciplines

Bridge topological clusters on the map to find hidden collaborative intersections.