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Renormalization, Decoupling and the Hierarchy Problem

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arxiv 2408.06406 v3 pith:MKUQBZKQ submitted 2024-08-12 hep-ph hep-th

Renormalization, Decoupling and the Hierarchy Problem

classification hep-ph hep-th
keywords massdecouplingloopscalarcorrectionsexternalheavyhierarchy
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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The hierarchy problem is associated with renormalization and decoupling. We can account for the smallness of the scalar mass against loop corrections and its insensitivity to ultraviolet physics through the decoupling of heavy fields. It is essential to correctly identify the observable physical mass as the renormalized one that depends on the external momentum, as opposed to the constant mass. We reconsider the properties of the renormalized loop corrections, which are finite, independent of regularization and admit a well-defined perturbation. By explicit calculation, we show that any loop corrections to the scalar mass-squared are suppressed as $(p^2-m^2)^2/M^2$, where $p,m$ and $M$ are the external momentum, the scalar pole mass and the heavy field mass in the loop, respectively. This is in accordance with the Appelquist-Carazzone decoupling theorem, which we have explicitized and completed for the case of the scalar mass.

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Cited by 3 Pith papers

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  1. Gauge-Invariant Off-Shell Mass

    hep-th 2026-07 conditional novelty 6.5

    A segment-local Ward–Takahashi cancellation makes the fermion self-energy equal to its Feynman-gauge value off shell, yielding a gauge-invariant, on-shell-renormalized mass function m(q).

  2. The Gauge-Invariant Mass Function

    hep-th 2026-04 unverdicted novelty 6.0

    Renormalization defines a gauge-invariant mass function at every virtuality in gauge theories.

  3. Natural Higgs Mass from Power-Law Running

    hep-ph 2026-03 conditional novelty 5.0

    Power-law running of the renormalized scalar mass function maps an order-one GUT boundary condition to the electroweak Higgs mass via the SM's small top-dominated anomalous dimension, without protective symmetries.