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Featured researches published by Makiko Nio.


Physical Review Letters | 2012

Tenth-Order QED Contribution to the Electron g-2 and an Improved Value of the Fine Structure Constant

Tatsumi Aoyama; Masashi Hayakawa; Toichiro Kinoshita; Makiko Nio

This letter presents the complete QED contribution to the electron g-2 up to the tenth order. With the help of the automatic code generator, we evaluate all 12,672 diagrams of the tenth-order diagrams and obtain 9.16 (58)(α/π)(5). We also improve the eighth-order contribution obtaining -1.9097 (20)(α/π)(4), which includes the mass-dependent contributions. These results lead to a(e)(theory)=1,159,652,181.78(77)×10(-12). The improved value of the fine-structure constant α(-1)=137.035999173 (35) [0.25 ppb] is also derived from the theory and measurement of a(e).


Physical Review Letters | 2012

Complete tenth-order QED contribution to the muon g-2.

Tatsumi Aoyama; Masashi Hayakawa; Toichiro Kinoshita; Makiko Nio

We report the result of our calculation of the complete tenth-order QED terms of the muon g-2. Our result is a(μ)((10))=753.29 (1.04) in units of (α/π)(5), which is about 4.5 s.d. larger than the leading-logarithmic estimate 663(20). We also improve the precision of the eighth-order QED term of a(μ), obtaining a(μ)((8))=130.8794 (63) in units of (α/π)(4). The new QED contribution is a(μ)(QED)=116,584,718,951 (80)×10(-14), which does not resolve the existing discrepancy between the standard-model prediction and measurement of a(μ).


Physical Review D | 2006

The Tenth-order QED contribution to the lepton g-2: Evaluation of dominant alpha**5 terms of muon g-2

Toichiro Kinoshita; Makiko Nio

The QED contribution to the anomalous magnetic moments of electron and muon are known very precisely up to the order {alpha}{sup 4}. However, the knowledge of the {alpha}{sup 5} term will also be required when the precision of measurement improves further. This paper reports the first systematic attempt to evaluate the {alpha}{sup 5} term. Feynman diagrams contributing to this term can be classified into six gauge-invariant sets which can be subdivided further into 32 gauge-invariant subsets. Thus far we have numerically evaluated all integrals of 17 gauge-invariant subsets which contain light-by-light-scattering subdiagrams and/or vacuum-polarization subdiagrams. They cover most of leading terms of muon g-2 and lead to a preliminary result 663 (20) ({alpha}/{pi}){sup 5}, which is 8.5 times more precise than the old estimate.


Physical Review D | 2006

Improved {alpha}{sup 4} term of the electron anomalous magnetic moment

Toichiro Kinoshita; Makiko Nio

We report a new value of electron


Physical Review Letters | 2007

Revised value of the eighth-order contribution to the electron g -2

Tatsumi Aoyama; Masashi Hayakawa; Toichiro Kinoshita; Makiko Nio

g\ensuremath{-}2


Physical Review D | 2004

Improved alpha**4 term of the muon anomalous magnetic moment

Toichiro Kinoshita; Makiko Nio

, or


Physical Review D | 2008

Revised value of the eighth-order QED contribution to the anomalous magnetic moment of the electron

Tatsumi Aoyama; Makiko Nio; Masashi Hayakawa; Toichiro Kinoshita

{a}_{e}


Physical Review D | 2015

Tenth-Order Electron Anomalous Magnetic Moment --- Contribution of Diagrams without Closed Lepton Loops

Tatsumi Aoyama; Masashi Hayakawa; Toichiro Kinoshita; Makiko Nio

, from 891 Feynman diagrams of order


Physical Review D | 1996

Radiative corrections to the muonium hyperfine structure. 1. The alpha**2 (Z-alpha) correction

Toichiro Kinoshita; Makiko Nio

{\ensuremath{\alpha}}^{4}


Physical Review D | 2008

Eighth-Order Vacuum-Polarization Function Formed by Two Light-by-Light-Scattering Diagrams and its Contribution to the Tenth-Order Electron g-2

Tatsumi Aoyama; Masashi Hayakawa; Toichiro Kinoshita; Makiko Nio; N. Watanabe

. The FORTRAN codes of 373 diagrams containing closed electron loops have been verified by at least two independent formulations. For the remaining 518 diagrams, which have no closed lepton loop, verification by a second formulation is not yet attempted because of the enormous amount of additional work required. However, these integrals have structures that allow extensive cross-checking as well as detailed comparison with lower-order diagrams through the renormalization procedure. No algebraic error has been uncovered for them. The numerical evaluation of the entire

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