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Scheme invariants in phi⁴ theory in four dimensions

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arxiv 1806.08598 v3 pith:EUDQ3G3L submitted 2018-06-22 hep-th

Scheme invariants in phi⁴ theory in four dimensions

classification hep-th
keywords invariantsfourdimensionsloopsschemetheoryanalysiscase
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We provide an analysis of the structure of renormalisation scheme invariants for the case of $\phi^4$ theory, relevant in four dimensions. We give a complete discussion of the invariants up to four loops and include some partial results at five loops, showing that there are considerably more invariants than one might naively have expected. We also show that one-vertex reducible contributions may consistently be omitted in a well-defined class of schemes which of course includes MSbar.

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Cited by 4 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Gradient RG Flow in Scalar-Fermion QFTs

    hep-th 2025-11 conditional novelty 7.0

    RG flow in scalar-fermion theories is gradient through four loops only when the 'beta shift' is included, via over a thousand scheme-independent constraints that hold wherever current data allow a check.

  2. $\phi^6$ at $6$ (and some $8$) loops in $3d$

    hep-th 2026-05 accept novelty 6.0

    Six-loop beta-function graphs for general ϕ⁶ theory in 3d are recalculated (differing from Hager, agreeing with recent work), with large-N eight-loop results, O(ε³) exponents, and gradient-flow linear relations.

  3. $\phi^6$ at $6$ (and some $8$) loops in $3d$

    hep-th 2026-05 unverdicted novelty 5.0

    Recalculation of individual six-loop graph contributions to the beta function in 3d phi^6 theory with arbitrary potential, plus large-N eight-loop terms and O(epsilon^3) critical exponents at the O(N) fixed point.

  4. $\phi^6$ at $6$ (and some $8$) loops in $3d$

    hep-th 2026-05 unverdicted novelty 5.0

    Recalculation of individual six-loop graph contributions to the β-function in 3d φ⁶ theory with arbitrary potential, plus large-N eight-loop diagrams and O(ε³) critical exponents at the O(N) fixed point.