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The electroweak chiral parameters for a heavy Higgs in the Standard Model
High Energy Physics - Phenomenology · Submitted 8 Aug 1994
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The values of the chiral parameters representing the non-decoupling effects of the heavy Higgs are presented.
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We study the electroweak interactions within the standard electroweak theory in the case where the Higgs particle is heavy, namely, $M_H \leq 1\;TeV$. By integrating out the Higgs boson to one loop we find the complete effective lagrangian, called electroweak chiral lagrangian, that is $SU(2)_L\times U(1)_Y$ invariant and contains the whole set of operators up to dimension four. The values of the chiral parameters representing the non-decoupling effects of the heavy Higgs are presented. Some examples have been chosen to show the applicability of this effective lagrangian approach to compute phenomenologically relevant quantities that either are being meassured at present or will be meassured in future experiments.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study the electroweak interactions within the standard electroweak theory in the case where the Higgs particle is heavy, namely, $M_H \leq 1\;TeV$. | contribution 0.62 | 0.66 | 0.05 | asserted 0.97 |
| s1 | By integrating out the Higgs boson to one loop we find the complete effective lagrangian, called electroweak chiral lagrangian, that is $SU(2)_L\times U(1)_Y$ invariant and contains the whole set of operators up to dimension four. | method 0.52 | 0.96 | 0.34 | asserted 1.00 |
| s2 | The values of the chiral parameters representing the non-decoupling effects of the heavy Higgs are presented. | result 0.98 | 0.91 | 0.58 | asserted 1.00 |
| s3 | Some examples have been chosen to show the applicability of this effective lagrangian approach to compute phenomenologically relevant quantities that either are being meassured at present or will be meassured in future experiments. | contribution 0.70 | 0.86 | 0.09 | asserted 1.00 |
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Original abstract
We study the electroweak interactions within the standard electroweak theory in the case where the Higgs particle is heavy, namely, $M_H \leq 1\;TeV$. By integrating out the Higgs boson to one loop we find the complete effective lagrangian, called electroweak chiral lagrangian, that is $SU(2)_L\times U(1)_Y$ invariant and contains the whole set of operators up to dimension four. The values of the chiral parameters representing the non-decoupling effects of the heavy Higgs are presented. Some examples have been chosen to show the applicability of this effective lagrangian approach to compute phenomenologically relevant quantities that either are being meassured at present or will be meassured in future experiments.
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States the same result 1 paper
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An appropriate set of matching conditions connecting the Green's functions of the two theories allows us to derive, systematically, the values of the chiral Lagrangian coefficients corresponding to the large Higgs mass limit of the standard model.
The Electroweak Chiral Lagrangian for the Standard Model with a Heavy Higgs · 0.90
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