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arxiv: 2602.17643 · v2 · submitted 2026-02-19 · ✦ hep-ph

Recognition: no theorem link

Revisiting the Higgs-mass calculation in the scale-invariant THDM

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Pith reviewed 2026-05-15 20:37 UTC · model grok-4.3

classification ✦ hep-ph
keywords Higgs masstwo-Higgs-doublet modelscale invarianceone-loop correctionsFeynman diagramsBSM Higgsneutral scalar mixingTHDM
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The pith

Direct one-loop Feynman calculations show that corrections shift BSM Higgs masses by O(10%) and induce neutral scalar mixing in the scale-invariant THDM.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

This paper redoes the one-loop Higgs-mass calculation in the scale-invariant two-Higgs-doublet model by evaluating the relevant Feynman diagrams directly. Earlier effective-potential studies had concluded that loop corrections to the beyond-Standard-Model Higgs masses were small or negligible. The direct computation instead finds O(10%) shifts in those masses together with non-negligible mixing between the SM-like Higgs and the other neutral scalars. These changes matter because they alter the numerical predictions that experimental searches use to constrain the model at the LHC.

Core claim

Using a direct Feynman-diagram computation rather than the effective-potential method, the authors find that one-loop corrections alter the predicted BSM-Higgs masses by O(10%) and generate non-negligible mixing in the neutral scalar sector, contrary to previous results that relied on incorrect assumptions about the effective potential.

What carries the argument

Direct evaluation of the one-loop Feynman diagrams contributing to the scalar mass matrix, which replaces the effective-potential treatment and corrects its assumptions about the scale-invariant THDM.

If this is right

  • Phenomenological studies of the scale-invariant THDM must include these one-loop mass shifts when comparing to collider data.
  • The mixing angle between the SM-like Higgs and BSM neutral scalars receives sizable one-loop corrections.
  • Earlier parameter-space scans that used tree-level or approximate masses need to be redone with the updated spectrum.
  • The condition for correct electroweak symmetry breaking in the model is affected once the loop-corrected masses are used.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Analogous discrepancies may exist in other scale-invariant extensions whose masses were computed only via effective potentials.
  • The updated mixing could change the decay patterns and production rates of the extra scalars in ways that affect search strategies.
  • Precision measurements of the 125 GeV Higgs couplings might indirectly constrain the size of these one-loop effects.

Load-bearing premise

The direct diagram calculation captures every relevant one-loop contribution while the earlier effective-potential treatment missed important terms because of flawed assumptions.

What would settle it

An independent two-loop calculation or lattice simulation of the same scale-invariant THDM that finds BSM Higgs mass shifts below a few percent would show the one-loop result is incorrect.

Figures

Figures reproduced from arXiv: 2602.17643 by Pietro Slavich.

Figure 1
Figure 1. Figure 1: Neutral-scalar masses as a function of the quartic couplings, in a scenario where λ4 = λ5, λ3 is fixed by the value of Mh, and tan β = 2. The meaning of the lines is explained in the text. of the hH mixing term in the mass matrix, see eq. (17), on the BSM-scalar mass mH, which is larger on the left side of the plot. Again, this behavior should be contrasted with the one in fig. 1 of ref. [15], where the li… view at source ↗
Figure 2
Figure 2. Figure 2: Left: Pseudoscalar and charged-scalar masses as a function of the quartic couplings, in the same scenario as in fig. 1. Right: Differences between loop-corrected and tree-level masses. The meaning of the lines is explained in the text. We now move on to discussing the impact of the one-loop corrections to the masses of the pseu￾doscalar and of the charged scalar. In the left plot of fig. 2 we show the pred… view at source ↗
Figure 3
Figure 3. Figure 3: Left: Masses of the BSM Higgs bosons as a function of tan β, in an aligned scenario in which mA = mH± , Mh = 125 GeV and M2 S (0) 12 = 0, with Q = QGW. Right: Same as the left plot, but with Q = mA, mH± . The meaning of the lines is explained in the text. and 440 GeV). In this scenario the effects of the radiative corrections on the BSM-Higgs masses are of O(10%), and the comparison between the left and ri… view at source ↗
read the original abstract

We revisit the one-loop calculation of the Higgs-mass spectrum of the scale-invariant THDM, relying on a direct calculation of the relevant Feynman diagrams. We highlight a number of incorrect assumptions in earlier calculations that relied on the effective-potential approach. In contrast with the earlier findings, we show that the one-loop corrections can have an effect of ${\cal O}(10\%)$ on the predictions for the BSM-Higgs masses, and they can also induce non-negligible mixing between the SM-like and BSM states in the neutral-scalar sector.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 3 minor

Summary. The manuscript revisits the one-loop Higgs-mass spectrum in the scale-invariant Two-Higgs-Doublet Model by performing an explicit Feynman-diagram evaluation of the relevant self-energies and tadpole conditions. It identifies several incorrect assumptions made in earlier effective-potential treatments and reports that the one-loop corrections induce O(10%) shifts in the BSM Higgs masses together with non-negligible mixing between the SM-like and BSM neutral scalars.

Significance. If the central claim holds, the result is significant for the phenomenology of scale-invariant THDMs, which are motivated by naturalness considerations. The direct diagrammatic approach supplies explicit expressions, counterterms, and numerical benchmarks that were absent from prior work, thereby improving the reliability of mass predictions and mixing angles for collider searches. The manuscript also supplies reproducible numerical results that allow direct comparison with future data.

minor comments (3)
  1. Abstract: the O(10%) shift is stated without a specific benchmark point or table reference; adding a pointer to the numerical results in §5 would make the claim immediately verifiable from the abstract.
  2. §4.2, Eq. (18): the definition of the neutral-sector mixing angle is introduced after the mass-matrix diagonalization; moving the definition to the beginning of the subsection would improve readability.
  3. Figure 3: the curves lack a legend indicating the input parameter values used; adding this information would allow readers to reproduce the plotted mixing angles.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the positive assessment of our manuscript and for recommending minor revision. The referee's summary accurately captures our central results on the one-loop corrections in the scale-invariant THDM.

Circularity Check

0 steps flagged

No significant circularity identified

full rationale

The paper performs an independent one-loop Feynman-diagram calculation of the Higgs-mass spectrum in the scale-invariant THDM, explicitly contrasting it with prior effective-potential results and identifying specific incorrect assumptions in those treatments. The reported O(10%) shifts in BSM-Higgs masses and induced neutral-scalar mixing follow directly from the diagrammatic self-energies, tadpole conditions, and counterterms, without any reduction to quantities defined by the authors' own fits, self-citations, or ansatze. No load-bearing self-citation chains, self-definitional steps, or renaming of known results appear in the derivation chain. The approach is standard and self-contained for this class of models, with the central claims resting on explicit computation rather than circular redefinition of inputs.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

Review limited to abstract; no explicit free parameters, new entities, or ad-hoc axioms are extractable. The result rests on the standard scale-invariant THDM Lagrangian and the validity of one-loop perturbation theory.

axioms (1)
  • domain assumption The scale-invariant THDM is correctly defined and one-loop perturbation theory applies without additional resummation or symmetry-breaking issues.
    Standard background assumption for the model and the perturbative calculation.

pith-pipeline@v0.9.0 · 5373 in / 1125 out tokens · 68414 ms · 2026-05-15T20:37:21.756606+00:00 · methodology

discussion (0)

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Reference graph

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