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Title: Hadron Spectroscopy and Dynamics from Light-Front Holography and Superconformal Algebra

Journal Article · · Few-Body Systems
 [1]
  1. Stanford Univ., Stanford, CA (United States). SLAC National Accelerator Lab

QCD is not supersymmetrical in the traditional sense – the QCD Lagrangian is based on quark and gluonic fields, not squarks nor gluinos. However, its hadronic eigensolutions conform to a representation of superconformal algebra, reflecting the underlying conformal symmetry of chiral QCD and its Pauli matrix representation. The eigensolutions of superconformal algebra provide a unified Regge spectroscopy of meson, baryon, and tetraquarks of the same parity and twist as equal-mass members of the same 4-plet representation with a universal Regge slope. The pion $$q\bar{q}$$ eigenstate has zero mass for mq = 0. The superconformal relations also can be extended to heavy-light quark mesons and baryons. The combined approach of light-front holography and superconformal algebra also provides insight into the origin of the QCD mass scale and color confinement. A key observation is the remarkable dAFF principle which shows how a mass scale can appear in the Hamiltonian and the equations of motion while retaining the conformal symmetry of the action. When one applies the dAFF procedure to chiral QCD, a mass scale κ appears which determines universal Regge slopes, hadron masses in the absence of the Higgs coupling, and the mass parameter underlying the Gaussian functional form of the nonperturbative QCD running coupling: αs(Q2) ∝ exp-Q2/4κ2, in agreement with the effective charge determined from measurements of the Bjorken sum rule. The mass scale κ underlying hadron masses can be connected to the parameter Λ$$\overline{MS}$$ in the QCD running coupling by matching its predicted nonperturbative form to the perturbative QCD regime. The result is an effective coupling αs(Q2) defined at all momenta. In conclusion, one also obtains empirically viable predictions for spacelike and timelike hadronic form factors, structure functions, distribution amplitudes, and transverse momentum distributions.

Research Organization:
SLAC National Accelerator Lab., Menlo Park, CA (United States)
Sponsoring Organization:
USDOE Office of Science (SC)
Grant/Contract Number:
AC02-76SF00515
OSTI ID:
1443973
Report Number(s):
SLAC-PUB-17201; TRN: US1900950
Journal Information:
Few-Body Systems, Vol. 59, Issue 5; Conference: NSTAR 2017, The 11th International Workshop on the Physics of Excited Nucleons, Univ. of South Carolina, Columbia, SC (United States), 20-23 Aug 2017; ISSN 0177-7963
Publisher:
SpringerCopyright Statement
Country of Publication:
United States
Language:
English
Citation Metrics:
Cited by: 1 work
Citation information provided by
Web of Science

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padding-left: 0; line-height:1.8em;"> <li class="authors">Lorcé, C.; Pasquini, B.; Vanderhaeghen, M.</li> <li class="mb-0-5 source"> <span class="mr-1">Journal of High Energy Physics, Vol. 2011, Issue 5</span> <span class="text-muted"><a href="https://doi.org/10.1007/JHEP05(2011)041" class="text-muted" target="_blank" rel="noopener noreferrer">https://doi.org/10.1007/JHEP05(2011)041<span class="fa fa-external-link" aria-hidden="true"></span></a></span> </li> </ul> </td> <td class="small text-muted biblio-refs-td-secondary"> <span class="biblio-refs-type-badge ml-1 type" data-type="journal">journal</span> </td> <td class="small text-muted biblio-refs-td-secondary biblio-refs-td-secondary-date"><span class="date" data-date="2011-05-01">May 2011</span></td> </tr></tbody></table> </div> </div> </section> <hr class="mt-2 mb-2"/> <section id="section-images" data-list="list_img" class="tab-content-sec osti-curated biblio-section section-scroll" style="scroll-margin-top:110px;"> <div class="biblio-section-navbar active row"> <div class="col"> <h2 class="abstract biblio-section-title mt-0 mb-0-5" style="cursor:pointer;"><span class="fa indicator"></span> Figures / Tables (16) <span class="text-muted list-table-filternum"></span></h2> </div> <div class="col-md-12 col-lg-auto"> <form class="pure-form reference-filter d-print-none"> <div class="small biblio-section-navbar-tool"> <label for="list-table-search-figures" class="sr-only">Search figures / tables: </label> <input type="text" class="list-table-search mt-0 mb-0-5 ml-1" id="list-table-search-figures" placeholder="Search figures / tables ..."> </div> <div class="small biblio-section-navbar-tool"> <select class="list-table-sort mt-0 mb-0-5"> <option value="date">Sort by Date</option> <option value="title">Sort by Title</option> </select> </div> <div class="small biblio-section-navbar-tool"> <button type="reset" class="pure-button list-table-reset mt-0 mb-0-5">↺</button> </div> </form> </div> </div> <div class="row"> <div class="col-sm-12"> <table id="list-table-images" class="truncate-rows list-table list-table-images table-to-tiles" data-rows="1" style="width:100%;"><tbody class="list"> <tr class="biblio-image-tile "><td class="col-sm-3"> <a id="img-1443973-img85078" data-pos="first" href="#modal-image" data-modal-toggle="true" class="biblio-image-tile-a ga-click-event apporder order title desc" data-imgid="1443973-img85078" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1443973-img85078" data-apporder="p. 2" data-order="1" data-imgid="1443973-img85078" data-imgsrc="/biblio/1443973/image/001/160/0011607/3/0085078.png" data-title="Figure 1" data-desc="Comparison of the $$ρ$$ mesonic and $$Δ$$ baryonic Regge trajectories by Klempt and Metsch [1]." data-ostiid="1443973"> <div class="biblio-image-tile-inner"> <small class="name">Figure 1<small class="pull-right text-muted" style="margin-right: .5em;top: 3px;position: relative;">(p. 2)</small><span class="d-none type">figure</span></small> <img class="img-responsive mt-0-5" alt="Figure 1" src="/biblio/1443973/image/001/160/0011607/3/t0085078.png"/> </div> </a> </td></tr> <tr class="biblio-image-tile "><td class="col-sm-3"> <a id="img-1443973-img85082" data-pos="" href="#modal-image" data-modal-toggle="true" class="biblio-image-tile-a ga-click-event apporder order title desc" data-imgid="1443973-img85082" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1443973-img85082" data-apporder="p. 3" data-order="2" data-imgid="1443973-img85082" data-imgsrc="/biblio/1443973/image/001/160/0011607/3/0085082.png" data-title="Figure 2" data-desc="Comparison of the slopes of the Regge trajectories in angular momentum: $$M$$<sup>2</sup> $$∝$$ $$L$$ and in the radial quantum number $$n$$: $$M$$<sup>2</sup> $$∝$$ $$n$$." data-ostiid="1443973"> <div class="biblio-image-tile-inner"> <small class="name">Figure 2<small class="pull-right text-muted" style="margin-right: .5em;top: 3px;position: relative;">(p. 3)</small><span class="d-none type">figure</span></small> <img class="img-responsive mt-0-5" alt="Figure 2" src="/biblio/1443973/image/001/160/0011607/3/t0085082.png"/> </div> </a> </td></tr> <tr class="biblio-image-tile "><td class="col-sm-3"> <a id="img-1443973-img85089" data-pos="" href="#modal-image" data-modal-toggle="true" class="biblio-image-tile-a ga-click-event apporder order title desc" data-imgid="1443973-img85089" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1443973-img85089" data-apporder="p. 5" data-order="3" data-imgid="1443973-img85089" data-imgsrc="/biblio/1443973/image/001/160/0011607/3/0085089.png" data-title="Figure 3" data-desc="Comparison of the $$ρ$$/$$ω$$ meson Regge trajectory with the $$J$$ = 3/2 $$Δ$$ baryon trajectory. Superconformal algebra predicts the mass degeneracy of the meson and baryon trajectories if one identifies a meson with internal orbital angular momentum $$L$$<sub>$$M$$</sub> with its superpartner baryon with $$L$$<sub>$$M$$</sub> = $$L$$<sub>$$B$$</sub> + 1. See Refs. [2, 3]." data-ostiid="1443973"> <div class="biblio-image-tile-inner"> <small class="name">Figure 3<small class="pull-right text-muted" style="margin-right: .5em;top: 3px;position: relative;">(p. 5)</small><span class="d-none type">figure</span></small> <img class="img-responsive mt-0-5" alt="Figure 3" src="/biblio/1443973/image/001/160/0011607/3/t0085089.png"/> </div> </a> </td></tr> <tr class="biblio-image-tile "><td class="col-sm-3"> <a id="img-1443973-img85079" data-pos="" href="#modal-image" data-modal-toggle="true" class="biblio-image-tile-a ga-click-event apporder order title desc" data-imgid="1443973-img85079" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1443973-img85079" data-apporder="p. 7" data-order="4" data-imgid="1443973-img85079" data-imgsrc="/biblio/1443973/image/001/160/0011607/3/0085079.png" data-title="Figure 4" data-desc="The 4-plet representation of mass-degenerate hadronic states predicted by superconformal algebra. Mesons are $$q\bar{q}$$ bound states, baryons are quark plus anti-diquark bound states and tetraquarks are diquark plus antidiquark bound states. The supersymmetric ladder operator $$R^{†}_{λ}$$ connects quarks and anti-diquark clusters of the same color. The baryons have two Fock states with orbital angular momentum $$L$$<sub>$$B$$ </sub>and $$L$$<sub>$$B$$</sub> + 1 with equal weight. The predicted meson baryon and tetraquark masses are identical if one identifies a meson with internal orbital angular momentum $$L$$<sub>$$M$$</sub> with its superpartner baryon or tetraquark with $$L$$<sub>$$B$$</sub> = $$L$$<sub>$$M$$</sub>− 1." data-ostiid="1443973"> <div class="biblio-image-tile-inner"> <small class="name">Figure 4<small class="pull-right text-muted" style="margin-right: .5em;top: 3px;position: relative;">(p. 7)</small><span class="d-none type">figure</span></small> <img class="img-responsive mt-0-5" alt="Figure 4" src="/biblio/1443973/image/001/160/0011607/3/t0085079.png"/> </div> </a> </td></tr> <tr class="biblio-image-tile tr-striped"><td class="col-sm-3"> <a id="img-1443973-img85085" data-pos="" href="#modal-image" data-modal-toggle="true" class="biblio-image-tile-a ga-click-event apporder order title desc" data-imgid="1443973-img85085" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1443973-img85085" data-apporder="p. 8" data-order="5" data-imgid="1443973-img85085" data-imgsrc="/biblio/1443973/image/001/160/0011607/3/0085085.png" data-title="Figure 5" data-desc="The eigenstates of superconformal algebra have a 2 x 2 representation of mass degenerate bosons and fermions: a meson with $$L$$<sub>$$M$$ </sub>= $$L$$<sub>$$B$$ </sub>+ 1, a baryon doublet with $$L$$<sub>$$B$$ </sub>, $$L$$<sub>$$B$$ </sub> + 1 components and a tetraquark with $$L$$<sub>$$T$$</sub> = $$L$$<sub>$$B$$ </sub>. The breakdown of LF kinetic, potential, spin, and quark mass contributions to each hadron is also shown. The virial theorem predicts the equality of the LF kinetic and potential contributions." data-ostiid="1443973"> <div class="biblio-image-tile-inner"> <small class="name">Figure 5<small class="pull-right text-muted" style="margin-right: .5em;top: 3px;position: relative;">(p. 8)</small><span class="d-none type">figure</span></small> <img class="img-responsive mt-0-5" alt="Figure 5" src="/biblio/1443973/image/001/160/0011607/3/t0085085.png"/> </div> </a> </td></tr> <tr class="biblio-image-tile tr-striped"><td class="col-sm-3"> <a id="img-1443973-img85074" data-pos="" href="#modal-image" data-modal-toggle="true" class="biblio-image-tile-a ga-click-event apporder order title desc" data-imgid="1443973-img85074" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1443973-img85074" data-apporder="p. 11" data-order="6" data-imgid="1443973-img85074" data-imgsrc="/biblio/1443973/image/001/160/0011607/3/0085074.png" data-title="Figure 6" data-desc="The LF Schrödinger equations for baryons and mesons for zero quark mass derived from the Pauli 2 x 2 4-plet matrix representation of superconformal algebra. The $$ψ$$<sup>±</sup> are the baryon quark-diquark LFWFs where the quark spin $$S^{z}_{q}$$ = ± 1/2 is parallel or antiparallel to the baryon spin $$J$$<sup>$$z$$</sup> = ± 1/2. The predicted meson and baryon masses are identical if one identifies a meson with internal orbital angular momentum $$L$$<sub>$$M$$ </sub>with its superpartner baryon with $$L$$<sub>$$B$$</sub> = $$L$$<sub>$$M$$</sub> − 1. See Refs. [2, 3, 4]." data-ostiid="1443973"> <div class="biblio-image-tile-inner"> <small class="name">Figure 6<small class="pull-right text-muted" style="margin-right: .5em;top: 3px;position: relative;">(p. 11)</small><span class="d-none type">figure</span></small> <img class="img-responsive mt-0-5" alt="Figure 6" src="/biblio/1443973/image/001/160/0011607/3/t0085074.png"/> </div> </a> </td></tr> <tr class="biblio-image-tile tr-striped"><td class="col-sm-3"> <a id="img-1443973-img85087" data-pos="" href="#modal-image" data-modal-toggle="true" class="biblio-image-tile-a ga-click-event apporder order title desc" data-imgid="1443973-img85087" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1443973-img85087" data-apporder="p. 12" data-order="7" data-imgid="1443973-img85087" data-imgsrc="/biblio/1443973/image/001/160/0011607/3/0085087.png" data-title="Figure 7" data-desc="Classification and quantum numbers of mesons, baryons, and tetraquarks composed of light quarks related by superconformal algebra." data-ostiid="1443973"> <div class="biblio-image-tile-inner"> <small class="name">Figure 7<small class="pull-right text-muted" style="margin-right: .5em;top: 3px;position: relative;">(p. 12)</small><span class="d-none type">figure</span></small> <img class="img-responsive mt-0-5" alt="Figure 7" src="/biblio/1443973/image/001/160/0011607/3/t0085087.png"/> </div> </a> </td></tr> <tr class="biblio-image-tile tr-striped"><td class="col-sm-3"> <a id="img-1443973-img85084" data-pos="" href="#modal-image" data-modal-toggle="true" class="biblio-image-tile-a ga-click-event apporder order title desc" data-imgid="1443973-img85084" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1443973-img85084" data-apporder="p. 13" data-order="8" data-imgid="1443973-img85084" data-imgsrc="/biblio/1443973/image/001/160/0011607/3/0085084.png" data-title="Figure 8" data-desc="Comparison of the meson and baryon Regge trajectories for hadrons with a single charm quark. See Refs. [2, 3]." data-ostiid="1443973"> <div class="biblio-image-tile-inner"> <small class="name">Figure 8<small class="pull-right text-muted" style="margin-right: .5em;top: 3px;position: relative;">(p. 13)</small><span class="d-none type">figure</span></small> <img class="img-responsive mt-0-5" alt="Figure 8" src="/biblio/1443973/image/001/160/0011607/3/t0085084.png"/> </div> </a> </td></tr> <tr class="biblio-image-tile "><td class="col-sm-3"> <a id="img-1443973-img85081" data-pos="" href="#modal-image" data-modal-toggle="true" class="biblio-image-tile-a ga-click-event apporder order title desc" data-imgid="1443973-img85081" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1443973-img85081" data-apporder="p. 14" data-order="9" data-imgid="1443973-img85081" data-imgsrc="/biblio/1443973/image/001/160/0011607/3/0085081.png" data-title="Figure 9" data-desc="The convergence of theoretical methods for generating a model of hadron spectroscopy and dynamics with color confinement and meson-baryon supersymmetric relations. ." data-ostiid="1443973"> <div class="biblio-image-tile-inner"> <small class="name">Figure 9<small class="pull-right text-muted" style="margin-right: .5em;top: 3px;position: relative;">(p. 14)</small><span class="d-none type">figure</span></small> <img class="img-responsive mt-0-5" alt="Figure 9" src="/biblio/1443973/image/001/160/0011607/3/t0085081.png"/> </div> </a> </td></tr> <tr class="biblio-image-tile "><td class="col-sm-3"> <a id="img-1443973-img85086" data-pos="" href="#modal-image" data-modal-toggle="true" class="biblio-image-tile-a ga-click-event apporder order title desc" data-imgid="1443973-img85086" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1443973-img85086" data-apporder="p. 17" data-order="10" data-imgid="1443973-img85086" data-imgsrc="/biblio/1443973/image/001/160/0011607/3/0085086.png" data-title="Figure 10" data-desc="The meson LFWF connects the intermediate $$q\bar{q}$$ state, which is off of the $$P$$<sup>− </sup>energy shell and thus off-the-invariant mass shell $$\mathcal{M}$$<sup>2</sup> > $$m^{2}_{H}$$T to the physical meson state with $$\mathcal{M}$$<sup>2</sup> = $$m^{2}_{H}$$. The $$q$$ and $$\bar{q}$$ can be regarded as effective dressed fields ." data-ostiid="1443973"> <div class="biblio-image-tile-inner"> <small class="name">Figure 10<small class="pull-right text-muted" style="margin-right: .5em;top: 3px;position: relative;">(p. 17)</small><span class="d-none type">figure</span></small> <img class="img-responsive mt-0-5" alt="Figure 10" src="/biblio/1443973/image/001/160/0011607/3/t0085086.png"/> </div> </a> </td></tr> <tr class="biblio-image-tile "><td class="col-sm-3"> <a id="img-1443973-img85077" data-pos="" href="#modal-image" data-modal-toggle="true" class="biblio-image-tile-a ga-click-event apporder order title desc" data-imgid="1443973-img85077" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1443973-img85077" data-apporder="p. 21" data-order="11" data-imgid="1443973-img85077" data-imgsrc="/biblio/1443973/image/001/160/0011607/3/0085077.png" data-title="Figure 11" data-desc="The holographic dictionary which maps the fifth dimension variable $$z$$ of the five-dimensional AdS<sub>5</sub> space to the LF radial variable $$ζ$$ where $$ζ$$ <sup>2</sup> = $$b^{2}_{⊥}$$(1−$$x$$). The same physics transformation maps the AdS<sub>5</sub> and (3 + 1) LF expressions for electromagnetic and gravitational form factors to each other. From ref. [33]" data-ostiid="1443973"> <div class="biblio-image-tile-inner"> <small class="name">Figure 11<small class="pull-right text-muted" style="margin-right: .5em;top: 3px;position: relative;">(p. 21)</small><span class="d-none type">figure</span></small> <img class="img-responsive mt-0-5" alt="Figure 11" src="/biblio/1443973/image/001/160/0011607/3/t0085077.png"/> </div> </a> </td></tr> <tr class="biblio-image-tile "><td class="col-sm-3"> <a id="img-1443973-img85083" data-pos="" href="#modal-image" data-modal-toggle="true" class="biblio-image-tile-a ga-click-event apporder order title desc" data-imgid="1443973-img85083" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1443973-img85083" data-apporder="p. 23" data-order="12" data-imgid="1443973-img85083" data-imgsrc="/biblio/1443973/image/001/160/0011607/3/0085083.png" data-title="Figure 12" data-desc="Prediction from AdS/QCD and Light-Front Holography for meson LFWFs $$ψ$$<sub>$$M$$</sub>($$x$$, $$\vec{k}$$<sub>⊥</sub>) and the pion distribution amplitude." data-ostiid="1443973"> <div class="biblio-image-tile-inner"> <small class="name">Figure 12<small class="pull-right text-muted" style="margin-right: .5em;top: 3px;position: relative;">(p. 23)</small><span class="d-none type">figure</span></small> <img class="img-responsive mt-0-5" alt="Figure 12" src="/biblio/1443973/image/001/160/0011607/3/t0085083.png"/> </div> </a> </td></tr> <tr class="biblio-image-tile tr-striped"><td class="col-sm-3"> <a id="img-1443973-img85088" data-pos="" href="#modal-image" data-modal-toggle="true" class="biblio-image-tile-a ga-click-event apporder order title desc" data-imgid="1443973-img85088" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1443973-img85088" data-apporder="p. 24" data-order="13" data-imgid="1443973-img85088" data-imgsrc="/biblio/1443973/image/001/160/0011607/3/0085088.png" data-title="Figure 13" data-desc="Comparison of the AdS/QCD prediction $$M$$<sup>2</sup>($$n$$, $$L$$, $$S$$) = 4$$κ$$<sup>2</sup>($$n$$ + $$L$$ + $$S$$/2) for the orbital $$L$$ and radial $$n$$ excitations of the meson spectrum with experiment. The pion is predicted to be massless for zero quark mass. The $$u$$, $$d$$, $$s$$ quark masses can be taken into account by perturbing in $$\langle$$ $$m^{2}_{q}$$/x $$\rangle$$. The fitted value of $$κ$$ = 0.59 GeV for pseudoscalar mesons, and $$κ$$ = 0.54 GeV for vector mesons." data-ostiid="1443973"> <div class="biblio-image-tile-inner"> <small class="name">Figure 13<small class="pull-right text-muted" style="margin-right: .5em;top: 3px;position: relative;">(p. 24)</small><span class="d-none type">figure</span></small> <img class="img-responsive mt-0-5" alt="Figure 13" src="/biblio/1443973/image/001/160/0011607/3/t0085088.png"/> </div> </a> </td></tr> <tr class="biblio-image-tile tr-striped"><td class="col-sm-3"> <a id="img-1443973-img85075" data-pos="" href="#modal-image" data-modal-toggle="true" class="biblio-image-tile-a ga-click-event apporder order title desc" data-imgid="1443973-img85075" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1443973-img85075" data-apporder="p. 25" data-order="14" data-imgid="1443973-img85075" data-imgsrc="/biblio/1443973/image/001/160/0011607/3/0085075.png" data-title="Figure 14" data-desc="Predictions for baryon elastic and transition spacelike form factors using AdS/QCD and superconformal algebra." data-ostiid="1443973"> <div class="biblio-image-tile-inner"> <small class="name">Figure 14<small class="pull-right text-muted" style="margin-right: .5em;top: 3px;position: relative;">(p. 25)</small><span class="d-none type">figure</span></small> <img class="img-responsive mt-0-5" alt="Figure 14" src="/biblio/1443973/image/001/160/0011607/3/t0085075.png"/> </div> </a> </td></tr> <tr class="biblio-image-tile tr-striped"><td class="col-sm-3"> <a id="img-1443973-img85076" data-pos="" href="#modal-image" data-modal-toggle="true" class="biblio-image-tile-a ga-click-event apporder order title desc" data-imgid="1443973-img85076" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1443973-img85076" data-apporder="p. 26" data-order="15" data-imgid="1443973-img85076" data-imgsrc="/biblio/1443973/image/001/160/0011607/3/0085076.png" data-title="Figure 15" data-desc="Predictions for baryon elastic and transition spacelike form factors using AdS/QCD and superconformal algebra. The fit allows for five-quark |$$uudq\bar{q}$$ > Fock state in the proton." data-ostiid="1443973"> <div class="biblio-image-tile-inner"> <small class="name">Figure 15<small class="pull-right text-muted" style="margin-right: .5em;top: 3px;position: relative;">(p. 26)</small><span class="d-none type">figure</span></small> <img class="img-responsive mt-0-5" alt="Figure 15" src="/biblio/1443973/image/001/160/0011607/3/t0085076.png"/> </div> </a> </td></tr> <tr class="biblio-image-tile tr-striped"><td class="col-sm-3"> <a id="img-1443973-img85080" data-pos="last" href="#modal-image" data-modal-toggle="true" class="biblio-image-tile-a ga-click-event apporder order title desc" data-imgid="1443973-img85080" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1443973-img85080" data-apporder="p. 29" data-order="16" data-imgid="1443973-img85080" data-imgsrc="/biblio/1443973/image/001/160/0011607/3/0085080.png" data-title="Figure 16" data-desc="Doubly Virtual Compton scattering on a proton (or nucleus) can be measured for two <em>spacelike</em> photons $$q^{2}_{1}$$, $$q^{2}_{2}$$ < 0 with minimal, tunable, skewness $$ξ$$ using positronium-proton scattering [$$e$$<sup>+</sup>$$e$$<sup>−</sup>]$$p$$ → $$e$$<sup>+</sup>$$e$$<sup>−</sup>$p′$. One can also measure double deep inelastic scattering and elastic positronium-proton scattering. One can also create a beam of “true muonium” atoms [$$μ$$<sup>−</sup>$$μ$$<sup>−</sup>] using Bethe-Heitler pair production just below threshold." data-ostiid="1443973"> <div class="biblio-image-tile-inner"> <small class="name">Figure 16<small class="pull-right text-muted" style="margin-right: .5em;top: 3px;position: relative;">(p. 29)</small><span class="d-none type">figure</span></small> <img class="img-responsive mt-0-5" alt="Figure 16" src="/biblio/1443973/image/001/160/0011607/3/t0085080.png"/> </div> </a> </td></tr> </tbody></table> </div> </div> </section> <div id="modal-image" class="modal"> <div class="modal-content"> <div class="modal-header"> <span class="close" data-modal-close="true">×</span> <header id="modal-image_label" style="margin:0px;">Image title</header> </div> <div id="modal-image_body" class="modal-body"> </div> </div> </div> <hr class="mt-2 mb-2"/> <section id="section-similar" class="tab-content-sec osti-curated biblio-section section-scroll" style="scroll-margin-top:110px;"> <div class="row"> <div class="col-8" style="padding-right:40px;"> <h2 class="abstract">Similar Records</h2> <div class="" style="line-height:1.6rem;"> <a href="/biblio/1490464" target="_blank">Supersymmetric and Conformal Features of Hadron Physics</a> <div class="small" style="line-height:1.4rem;"> Journal Article <span style="padding-left: 0.75rem;padding-right: 0.75rem;">·</span> Thu Nov 08 00:00:00 EST 2018 <span style="padding-left: 0.75rem;padding-right: 0.75rem;">·</span> Universe <span style="padding-left: 0.75rem;padding-right: 0.75rem;">·</span> <span class="text-muted" style="padding-right:0.5em;">OSTI ID:</span>1443973 </div> <div class="small" style="line-height:1.4rem;"> <span class="author-link"><a href="/search/author:"Brodsky, Stanley"" class="btn btn-link btn-sm"><span class="author" itemprop="author">Brodsky, Stanley</span></a></span> </div> <hr/> <a href="/biblio/1433298" target="_blank">Color Confinement, Hadron Dynamics, and Hadron Spectroscopy from Light-Front Holography and Superconformal Algebra</a> <div class="small" style="line-height:1.4rem;"> Journal Article <span style="padding-left: 0.75rem;padding-right: 0.75rem;">·</span> Mon Jan 01 00:00:00 EST 2018 <span style="padding-left: 0.75rem;padding-right: 0.75rem;">·</span> Advances in High Energy Physics <span style="padding-left: 0.75rem;padding-right: 0.75rem;">·</span> <span class="text-muted" style="padding-right:0.5em;">OSTI ID:</span>1443973 </div> <div class="small" style="line-height:1.4rem;"> <span class="author-link"><a href="/search/author:"Brodsky, Stanley J."" class="btn btn-link btn-sm"><span class="author" itemprop="author">Brodsky, Stanley J.</span></a></span> </div> <hr/> <a href="/biblio/1389548" target="_blank">New Insights into Color Confinement, Hadron Dynamics, Spectroscopy, and Jet Hadronization from Light-Front Holography and Superconformal Algebra</a> <div class="small" style="line-height:1.4rem;"> Journal Article <span style="padding-left: 0.75rem;padding-right: 0.75rem;">·</span> Tue Jul 11 00:00:00 EDT 2017 <span style="padding-left: 0.75rem;padding-right: 0.75rem;">·</span> Russian Physics Journal <span style="padding-left: 0.75rem;padding-right: 0.75rem;">·</span> <span class="text-muted" style="padding-right:0.5em;">OSTI ID:</span>1443973 </div> <div class="small" style="line-height:1.4rem;"> <span class="author-link"><a href="/search/author:"Brodsky, S. 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