Theory for the power threshold of the L-H transition in tokamaks
Abstract
Flux-driven two-fluid simulations in a diverted tokamak exhibit a confinement transition when a critical heating threshold is exceeded, as in experimental observations of the L-H transition. The simulations show that electromagnetic drift-wave turbulence spontaneously generates a sheared E× B flow responsible for transport suppression in the edge. The toroidal-field asymmetry of the transition, here reproduced in simulations for the first time, arises from time-reversal symmetry breaking by finite collisionality, as demonstrated by a quasilinear calculation of the turbulent momentum flux. Scaling laws are analytically derived for the L-H power threshold in the high- and low-density branches, for the density minimum, and for the minimum power, all matching or surpassing the accuracy of existing empirical scalings.
Versions
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BibTeX
@misc{lucca2026theory,
title = {{Theory for the power threshold of the L-H transition in tokamaks}},
author = {Brenno De Lucca and Paolo Ricci and Benoit Labit and Davide Mancini and Louis Stenger and Zeno Tecchiolli},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2605.00624},
eprint = {2605.00624},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2605.00624},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Theory for the power threshold of the L-H transition in tokamaks
AU - Brenno De Lucca
AU - Paolo Ricci
AU - Benoit Labit
AU - Davide Mancini
AU - Louis Stenger
AU - Zeno Tecchiolli
PY - 2026
DA - 2026/10/26
PB - arXiv
DO - 10.48550/arxiv.2605.00624
UR - https://arxiv.org/abs/2605.00624
AB - Flux-driven two-fluid simulations in a diverted tokamak exhibit a confinement transition when a critical heating threshold is exceeded, as in experimental observations of the L-H transition. The simulations show that electromagnetic drift-wave turbulence spontaneously generates a sheared E× B flow responsible for transport suppression in the edge. The toroidal-field asymmetry of the transition, here reproduced in simulations for the first time, arises from time-reversal symmetry breaking by finite collisionality, as demonstrated by a quasilinear calculation of the turbulent momentum flux. Scaling laws are analytically derived for the L-H power threshold in the high- and low-density branches, for the density minimum, and for the minimum power, all matching or surpassing the accuracy of existing empirical scalings.
ER -