2021
DOI: 10.1016/j.ppnp.2021.103908
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Parton distributions and lattice-QCD calculations: Toward 3D structure

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Cited by 119 publications
(54 citation statements)
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References 434 publications
(538 reference statements)
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“…In fact, our operator has the structure λβργ G µα (z)G ργ (0), where G(z) and G(0) is the same field. As we will see in section 2.5, this imposes two relations (2.28), (2.33) between some invariant amplitudes M parametrizing M (2) µα;λβ and invariant amplitudes entering into M (1) µα;λβ . One may also incorporate the symmetry properties of M µα;λβ (z, p) with respect to z. Namely, since M µα;λβ (z, p) is odd in z, the invariant amplitudes M sp , M ps , M pzsz , M szpz , M zp , M pz are odd functions of ν, while the remaining ones are even functions of ν.…”
Section: Jhep02(2022)193mentioning
confidence: 96%
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“…In fact, our operator has the structure λβργ G µα (z)G ργ (0), where G(z) and G(0) is the same field. As we will see in section 2.5, this imposes two relations (2.28), (2.33) between some invariant amplitudes M parametrizing M (2) µα;λβ and invariant amplitudes entering into M (1) µα;λβ . One may also incorporate the symmetry properties of M µα;λβ (z, p) with respect to z. Namely, since M µα;λβ (z, p) is odd in z, the invariant amplitudes M sp , M ps , M pzsz , M szpz , M zp , M pz are odd functions of ν, while the remaining ones are even functions of ν.…”
Section: Jhep02(2022)193mentioning
confidence: 96%
“…To extract polarized gluon distributions of a nucleon, we consider matrix elements of bilocal operators G µα (z) G λβ (0) composed of two gluon fields, with the dual field defined by G λβ = 1 2 λβργ G ργ . The matrix elements are specified by…”
Section: Definitionsmentioning
confidence: 99%
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“…In [115][116][117] one can find reviews of all the aforementioned lattice approaches to the extraction of light cone PDFs.…”
Section: Introductionmentioning
confidence: 99%
“…Less than a decade ago, a breakthrough was made by large-momentum effective theory (LaMET) [3][4][5], which starts from a Euclidean "quasi-PDF" (qPDF) in a boosted hadron and calculates the PDF through a largemomentum expansion and perturbative matching of the qPDF in the Bjorken-x (the longitudinal momentum fraction) space. Over the past years, LaMET has led to much progress in the calculations of PDFs and other parton physics [5,6], which reinvigorated the field as other proposals are also being studied and implemented [7][8][9][10][11][12][13]. After considerable development, especially in lattice renormalization [14][15][16][17][18][19] and perturbative matching at next-to-next-to-leading order (NNLO) [20,21], the LaMET approach is entering the stage where the systematic errors [22] are both controllable and improvable.…”
mentioning
confidence: 99%