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Novel QCD Phenomena
High Energy Physics - Phenomenology · Submitted 18 Jul 2007
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Initial- and final-state interactions from gluon-exchange, normally neglected in the parton model, have a profound effect in QCD hard-scattering reactions, leading to leading-twist single-spin asymmetries, diffractive deep inelastic scattering, diffractive hard hadronic reactions, the breakdown of the Lam Tung relation in Drell-Yan reactions, and nuclear shadowing and non-universal antishadowing--leading-twist physics not incorporated in the light-front wavefunctions of the target computed in isolation.
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The abstract, sentence by sentence
I discuss a number of novel topics in QCD, including the use of the AdS/CFT correspondence between Anti-de Sitter space and conformal gauge theories to obtain an analytically tractable approximation to QCD in the regime where the QCD coupling is large and constant. In particular, there is an exact correspondence between the fifth-dimension coordinate z of AdS space and a specific impact variable zeta which measures the separation of the quark constituents within the hadron in ordinary space-time. This connection allows one to compute the analytic form of the frame-independent light-front wavefunctions of mesons and baryons, the fundamental entities which encode hadron properties and allow the computation of exclusive scattering amplitudes. I also discuss a number of novel phenomenological features of QCD. Initial- and final-state interactions from gluon-exchange, normally neglected in the parton model, have a profound effect in QCD hard-scattering reactions, leading to leading-twist single-spin asymmetries, diffractive deep inelastic scattering, diffractive hard hadronic reactions, the breakdown of the Lam Tung relation in Drell-Yan reactions, and nuclear shadowing and non-universal antishadowing--leading-twist physics not incorporated in the light-front wavefunctions of the target computed in isolation. I also discuss tests of hidden color in nuclear wavefunctions, the use of diffraction to materialize the Fock states of a hadronic projectile and test QCD color transparency, and anomalous heavy quark effects. The presence of direct higher-twist processes where a proton is produced in the hard subprocess can explain the large proton-to-pion ratio seen in high-centrality heavy-ion collisions.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | I discuss a number of novel topics in QCD, including the use of the AdS/CFT correspondence between Anti-de Sitter space and conformal gauge theories to obtain an analytically tractable approximation to QCD in the regime where the QCD coupling is large and constant. | contribution 0.95 | 0.53 | 0.14 | asserted 0.93 |
| s1 | In particular, there is an exact correspondence between the fifth-dimension coordinate z of AdS space and a specific impact variable zeta which measures the separation of the quark constituents within the hadron in ordinary space-time. | method 0.35 | 0.38 | 0.13 | asserted 1.00 |
| s2 | This connection allows one to compute the analytic form of the frame-independent light-front wavefunctions of mesons and baryons, the fundamental entities which encode hadron properties and allow the computation of exclusive scattering amplitudes. | result 0.42 | 0.61 | 0.18 | asserted 0.86 |
| s3 | I also discuss a number of novel phenomenological features of QCD. | contribution 0.98 | 0.61 | 0.03 | asserted 0.51 |
| s4 | Initial- and final-state interactions from gluon-exchange, normally neglected in the parton model, have a profound effect in QCD hard-scattering reactions, leading to leading-twist single-spin asymmetries, diffractive deep inelastic scattering, diffractive hard hadronic reactions, the breakdown of the Lam Tung relation in Drell-Yan reactions, and nuclear shadowing and non-universal antishadowing--leading-twist physics not incorporated in the light-front wavefunctions of the target computed in isolation. | contribution 0.54 | 0.20 | 0.17 | asserted 1.00 |
| s5 | I also discuss tests of hidden color in nuclear wavefunctions, the use of diffraction to materialize the Fock states of a hadronic projectile and test QCD color transparency, and anomalous heavy quark effects. | contribution 1.00 | 0.33 | 0.06 | unclear 0.66 |
| s6 | The presence of direct higher-twist processes where a proton is produced in the hard subprocess can explain the large proton-to-pion ratio seen in high-centrality heavy-ion collisions. | interpretation 0.49 | 0.36 | 0.17 | hedged possibility 0.56 |
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The paper
Original abstract
I discuss a number of novel topics in QCD, including the use of the AdS/CFT correspondence between Anti-de Sitter space and conformal gauge theories to obtain an analytically tractable approximation to QCD in the regime where the QCD coupling is large and constant. In particular, there is an exact correspondence between the fifth-dimension coordinate z of AdS space and a specific impact variable zeta which measures the separation of the quark constituents within the hadron in ordinary space-time. This connection allows one to compute the analytic form of the frame-independent light-front wavefunctions of mesons and baryons, the fundamental entities which encode hadron properties and allow the computation of exclusive scattering amplitudes. I also discuss a number of novel phenomenological features of QCD. Initial- and final-state interactions from gluon-exchange, normally neglected in the parton model, have a profound effect in QCD hard-scattering reactions, leading to leading-twist single-spin asymmetries, diffractive deep inelastic scattering, diffractive hard hadronic reactions, the breakdown of the Lam Tung relation in Drell-Yan reactions, and nuclear shadowing and non-universal antishadowing--leading-twist physics not incorporated in the light-front wavefunctions of the target computed in isolation. I also discuss tests of hidden color in nuclear wavefunctions, the use of diffraction to materialize the Fock states of a hadronic projectile and test QCD color transparency, and anomalous heavy quark effects. The presence of direct higher-twist processes where a proton is produced in the hard subprocess can explain the large proton-to-pion ratio seen in high-centrality heavy-ion collisions.
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What this paper does with the arXiv papers it cites
Papers whose main result relates to this one's
States the same result 1 paper
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Initial- and final-state rescattering, neglected in the parton model, can have a profound effect in QCD hard-scattering reactions, producing single-spin asymmetries, diffractive deep inelastic scattering, diffractive hard hadronic reactions, the breakdown of the Lam-Tung relation in Drell-Yan reactions, nuclear shadowing, and non-universal nuclear antishadowing--novel leading-twist physics not incorporated in the light-front wavefunctions of the target computed in isolation.
What it cites · 86 sentences without a confident label
Uses the method or tool of 2 papers
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Equivalently, one can use the scheme-independent BLM procedure [ref] to eliminate the appearance of the $β$-function in the perturbative series.
Commensurate Scale Relations in Quantum Chromodynamics · Setting the Renormalization Scale in Perturbative QCD · 0.85
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Equivalently, one can use the scheme-independent BLM procedure [ref] to eliminate the appearance of the $β$-function in the perturbative series.
Fixing the renormalisation scheme in NNLO perturbative QCD using conformal limit arguments · Setting the Renormalization Scale in Perturbative QCD · 0.85
Uses data or values from 3 papers
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A remarkable feature of deep inelastic lepton-proton scattering at HERA is that approximately 10% events are diffractive [ref] : the target proton remains intact, and there is a large rapidity gap between the proton and the other hadrons in the final state.
Inclusive Measurement of Diffractive Deep-inelastic ep Scattering · Diffractive Deep Inelastic Scattering · 0.80
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A remarkable feature of deep inelastic lepton-proton scattering at HERA is that approximately 10% events are diffractive [ref] : the target proton remains intact, and there is a large rapidity gap between the proton and the other hadrons in the final state.
Measurement of the Diffractive Cross Section in Deep Inelastic Scattering using ZEUS 1994 Data · Diffractive Deep Inelastic Scattering · 0.80
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Recently the Hall A collaboration at Jefferson Laboratory [ref] has reported a significant exception to the general empirical success of dimensional counting in fixed CM angle Compton scattering $dσdt(γp →γp) ∼F(θ_CM)s^8$ instead of the predicted $1s^6$ scaling.
Compton Scattering Cross Section on the Proton at High Momentum Transfer · AdS/QCD as a First Approximant to Nonperturbative QCD · 0.81
Cites as support 20 papers
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The resulting diffractive contributions leave the target intact and do not resolve its quark structure; thus there are contributions to the DIS structure functions which cannot be interpreted as parton probabilities [ref] ; the leading-twist contribution to DIS from rescattering of a quark in the target is a coherent effect which is not included in the light-front wave functions computed in isolation.
Structure Functions are not Parton Probabilities · Diffractive Deep Inelastic Scattering · 0.99
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In fact, final-state interactions from gluon exchange between the outgoing quarks and the target spectator system lead to single-spin asymmetries in semi-inclusive deep inelastic lepton-proton scattering which are not power-law suppressed at large photon virtuality $Q^2$ at fixed $x_bj$ [ref] .
Final-State Interactions and Single-Spin Asymmetries in Semi-Inclusive Deep Inelastic Scattering · Single-Spin Asymmetries from Final-State Interactions · 1.00
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Such a gauge link is process dependent [ref] , so the resulting augmented LFWFs are not universal [ref] .
Final state interactions and gauge invariant parton distributions · Diffractive Deep Inelastic Scattering · 0.98
Cites as background 6 papers
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One of the most interesting new developments in hadron physics has been the application of the AdS/CFT correspondence [ref] to nonperturbative QCD problems [ref] .
QCD and a Holographic Model of Hadrons · AdS/QCD as a First Approximant to Nonperturbative QCD · 0.96
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One of the most interesting new developments in hadron physics has been the application of the AdS/CFT correspondence [ref] to nonperturbative QCD problems [ref] .
Linear Confinement and AdS/QCD · AdS/QCD as a First Approximant to Nonperturbative QCD · 0.96
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One of the most interesting new developments in hadron physics has been the application of the AdS/CFT correspondence [ref] to nonperturbative QCD problems [ref] .
Hadronic Spectrum of a Holographic Dual of QCD · AdS/QCD as a First Approximant to Nonperturbative QCD · 0.96
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