Odderon Exchange from Elastic Scattering Differences between 
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 Data at 1.96 TeV and from 
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Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M. R.; Adams, T.; Agnew, J. P.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alves, G. A.; Antchev, G.; Askew, A.; Aspell, P.; Jesus, A. C.S. Assis; Atanassov, I.; Atkins, S.; Augsten, K.; Aushev, V.; Aushev, Y.; Avati, V.; Ávila, C.; Badaud, F.; Baechler, J.; Bagby, L.; Barrera, C. Baldenegro; Baldin, B.; Bandurin, D. V.; Banerjee, S.; Barberis, E.; Baringer, P.; Barreto, J.; Bartlett, J. F.; Bassler, U.; Bazterra, V. E.; Bean, A.; Begalli, M.; Bellantoni, L.; Berardi, V.; Beri, S. B.; Bernardi, G.; Bernhard, R.; Berretti, M.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bhat, P. C.; Bhatia, S.; Bhatnagar, V.; Blazey, G.; Blessing, S.; Bloom, K.; Boehnlein, A.; Boline, D.; Boos, E.; Borchsh, V.; Borissov, G.; Borysova, M.; Bossini, E.; Bottigli, U.; Bozzo, M.; Brandt, A.; Brandt, O.; Brochmann, M.; Brock, R.; Bross, A.; Brown, D.; Bu, X. B.; Buehler, M.; Buescher, V.; Bunichev, Viacheslav; Burdin, S.; Burkhardt, H.; Buszello, C. 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doi:10.1103/physrevlett.127.062003

Cited by 62 publications

(57 citation statements)

References 41 publications

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“…Since gluons interact with each other, they have been hypothesized to form what has been called "glueballs" when not interacting with fermions. The existence of glueballs was initially thought to have been demonstrated in 2015 [34], though empirical evidence of glueballs was first reported in August 2021 [35]. The idea that gluons can form glueballs is incorporated in the Standard Model, but the PST's conceptualization of gluons being derived from a phase change of spacetime itself is new.…”

Section: Massless Gauge Bosonsmentioning

confidence: 99%

Everything is Probabilistic Spacetime: An Integrative Theory

Doren¹

2021

Int J Cosmol Astron Astrophys

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This article describes a new theory formulated to improve our understanding of cosmological phenomena. First, an enumeration is offered of shortcomings of current cosmological theories. Second, the components of the new theory are delineated. Third, the theory's explanations of poorly understood cosmological phenomena are presented. Finally, numerous testable predictions are described that differentiate the theory from existing theories.

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Section: Massless Gauge Bosonsmentioning

confidence: 99%

Everything is Probabilistic Spacetime: An Integrative Theory

Doren¹

2021

Int J Cosmol Astron Astrophys

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“…The sub-eikonal correction we found, once better quantified, may also provide a background for the future spin-dependent odderon searches. These results give an exciting possible new direction for such future experimental studies, particularly in light of the recent announcement by D0 and TOTEM collaborations of odderon detection through the asymmetry between pp and pp collisions [62]. Future experiments such as those to be conducted at the EIC will be able to probe transverse spin asymmetries at small-x and potentially observe both the spin-dependent odderon contribution and the sub-eikonal correction derived in this work.…”

Section: Jhep11(2021)200mentioning

confidence: 60%

“…At leading order in α s , the odderon is given by a three-gluon exchange in the t-channel with the gluons in the symmetric d abc color configuration (d abc = 2 tr t a {t b , t c } with t a the fundamental generators of SU(N c ) and N c the number of colors). The odderon has its own extensive body of research at small-x [50][51][52][53][54][55][56][57][58][59][60][61], as well as an exciting recent announcement of the odderon detection in pp and pp collisions by the D0 and TOTEM collaborations [62] (see also [63][64][65][66][67]). It was shown in [4] that the gluon Sivers function at small x is mainly generated by the spin-dependent odderon, arising from a fundamental-representation Wilson loop in the gauge link of the operator.…”

Section: Jhep11(2021)200mentioning

confidence: 99%

“…Part of the motivation for this is that the effects of the odderon have been historically hard to find in the data. The recent announcement of the odderon discovery [62] was many years in the making and required very careful measurements and extrapolation in energy. It is, therefore, important to understand the background for the odderon contribution (3.24) in order to discover the latter in the future measurements of the Sivers function.…”

Section: Sivers Function At the Sub-eikonal Level: A New Evolutionmentioning

confidence: 99%

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Quark sivers function at small x: spin-dependent odderon and the sub-eikonal evolution

Kovchegov

Santiago

2021

J. High Energ. Phys.

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We apply the formalism developed earlier [1, 2] for studying transverse momentum dependent parton distribution functions (TMDs) at small Bjorken x to construct the small-x asymptotics of the quark Sivers function. First, we explicitly construct the complete fundamental “polarized Wilson line” operator to sub-sub-eikonal order: this object can be used to study a variety of quark TMDs at small x. We then express the quark Sivers function in terms of dipole scattering amplitudes containing various components of the “polarized Wilson line” and show that the dominant (eikonal) term which contributes to the quark Sivers function at small x is the spin-dependent odderon, confirming the re- cent results of Dong, Zheng and Zhou [3]. Our conclusion is also similar to the case of the gluon Sivers function derived by Boer, Echevarria, Mulders and Zhou [4] (see also [5]). We also analyze the sub-eikonal corrections to the quark Sivers function using the constructed “polarized Wilson line” operator. We derive new small-x evolution equations re-summing double-logarithmic powers of αs ln2(1/x) with αs the strong coupling constant. We solve the corresponding novel evolution equations in the large-Nc limit, obtaining a sub-eikonal correction to the spin-dependent odderon contribution. We conclude that the quark Sivers function at small x receives contributions from two terms and is given by$$ {f}_{1T}^{\perp q}\left(x,{k}_T^2\right)={C}_O\left(x,{k}_T^2\right)\frac{1}{x}+{C}_1\left({k}_T^2\right){\left(\frac{1}{x}\right)}^0+\cdots $$ f 1 T ⊥ q x k T 2 = C O x k T 2 1 x + C 1 k T 2 1 x 0 + ⋯ with the function CO(x,$$ {k}_T^2 $$ k T 2 ) varying slowly with x and the ellipsis denoting the subasymptotic and sub-sub-eikonal (order-x) corrections.

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“…[15][16][17][18][19][20][21]. In this model the C = −1 odderon [22] is described as effective vector exchange. Exclusive reactions suitable for studies of the odderon exchange at high energies were discussed in [13,19,20].…”

Section: Introductionmentioning

confidence: 99%