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How the Fine-Structure Changes from \({\simeq } 1/137\) to \({\simeq }1/128\) at High Energies

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Abstract

At present available high-energies such as at an energy corresponding to the mass of the neutral \(Z^0\) vector boson, the fine-structure coupling attains a value \({\simeq } 1/128\) at \(Q^2 = (M_{Z})^2=(91.188)^2\,\text {GeV}^2\) starting form the well known constant value of \({\simeq } 1/137\) at low \(Q^2\simeq 0\), with the latter corresponding to a measurement of the fine-structure constant at large distances, say from an electron, in laboratory experiments.

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Notes

  1. 1.

    See, e.g., Patrignani et al. [8], and update (2017).

  2. 2.

    Patrignani et al. [8], and (2017) update.

  3. 3.

    See, e.g, Symanzik [9], for pioneering early work which has led to much of the subsequent work on the asymptotic analysis of Feynman integrals. See also Weinberg [10]. For a proof of the decoupling theorem and its generalizations, see, Manoukian [1, 2, 4, 5]. See also Manoukian [3].

  4. 4.

    See also Manoukian [6].

  5. 5.

    For the related experiment, see Mele [7].

References

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Manoukian, E.B. (2020). How the Fine-Structure Changes from \({\simeq } 1/137\) to \({\simeq }1/128\) at High Energies . In: 100 Years of Fundamental Theoretical Physics in the Palm of Your Hand. Springer, Cham. https://doi.org/10.1007/978-3-030-51081-7_28

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