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Paper Citation Record · LEDGER

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling

As of 15 August 2026, this Paper Citation Record lists 100 of 167 outbound references and 0 inbound Pith citation observations for arXiv:1908.05113.

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pith.paper-citation-record.v1
1908.05113 v1

Coverage vector

measured 100 of 167 reference resolution

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Source: paper_references, paper_reference_links, observed 2026-08-14T13:31:47.424891Z

measured 100 of 100 standing notices

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Source: scholarly_work_events, retraction_status_cache, observed 2026-08-14T06:32:32.682623+00:00

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measured 0 of 1 external citation measurements

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Reference resolution

100 of 167 outbound references displayed

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External citation measurements

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Outbound references

Observation fab59f99-90bf-49e0-917a-a0ed13e76ac6 · outbound

This paper cites Reggeization of the Vector Meson and the Vacuu m Singularity in Nonabelian Gauge Theories,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Reggeization of the Vector Meson and the Vacuu m Singularity in Nonabelian Gauge Theories,

Reference 1

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Observation a02d7bf4-8525-4792-a941-1d2f927c61d5 · outbound

This paper cites On the Pomeranch uk Singularity in Asymptotically Free Theories,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling On the Pomeranch uk Singularity in Asymptotically Free Theories,

Reference 2

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Observation eae2c165-f861-45ae-b271-075ade3e5bd0 · outbound

This paper cites Multi - Reggeon Pr ocesses in the Yang-Mills Theory,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Multi - Reggeon Pr ocesses in the Yang-Mills Theory,

Reference 3

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Observation 19f5db54-20b8-45ab-bb6f-27e29ed6d3f1 · outbound

This paper cites The Pomeranchuk Singularity in Nonabelian Gauge Theories,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The Pomeranchuk Singularity in Nonabelian Gauge Theories,

Reference 4

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Observation eb306a15-82bd-49d2-a605-70ba040c7237 · outbound

This paper cites The Pomeranchuk Singularity in Q uantum Chromodynamics,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The Pomeranchuk Singularity in Q uantum Chromodynamics,

Reference 5

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Observation eb1b3f59-60ed-4826-b272-d5194fcbe85c · outbound

This paper cites Calculation of meson meson inter action cross- section in quantum chromodynamics. (in russian),.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Calculation of meson meson inter action cross- section in quantum chromodynamics. (in russian),

Reference 6

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Observation d3126d9c-fb1e-42aa-9e0e-f3357ae2a49a · outbound

This paper cites e+ e- pair annihilation and deep inela stic e p scattering in perturbation theory,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling e+ e- pair annihilation and deep inela stic e p scattering in perturbation theory,

Reference 7

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Observation ebaf4c33-87af-4a74-94c5-acdae0c7d180 · outbound

This paper cites Deep inelastic e p scattering in per turbation theory,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Deep inelastic e p scattering in per turbation theory,

Reference 8

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Observation 05e641e7-51b8-40d0-a921-b839a2c48134 · outbound

This paper cites The parton model and perturbation theory,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The parton model and perturbation theory,

Reference 9

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Observation 06f5221c-e026-40e9-9ced-a3eb3cb9f23e · outbound

This paper cites Asymptotic Freedom in Parton Langua ge,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Asymptotic Freedom in Parton Langua ge,

Reference 10

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Observation 0a077fc6-5ebd-472c-932e-4ee52586c683 · outbound

This paper cites Calculation of the Structure Functions for Deep Inelastic Scatter- ing and e+ e- Annihilation by Perturbation Theory in Quantum Chromod ynamics.,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Calculation of the Structure Functions for Deep Inelastic Scatter- ing and e+ e- Annihilation by Perturbation Theory in Quantum Chromod ynamics.,

Reference 11

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Observation d223cdb5-a554-4ac7-a5fc-71a28bd80943 · outbound

This paper cites Supersymmetric Yan g-Mills Theories,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Supersymmetric Yan g-Mills Theories,

Reference 12

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Observation 0310118d-58af-4e8d-87e4-b10fe803da60 · outbound

This paper cites Supersymmetry, Superg ravity Theories and the Dual Spinor Model,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Supersymmetry, Superg ravity Theories and the Dual Spinor Model,

Reference 13

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Observation ea919887-e878-40c0-a2de-1d018ce09ef5 · outbound

This paper cites DGLAP and BFKL equations in th e N = 4 supersymmetric gauge theory,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling DGLAP and BFKL equations in th e N = 4 supersymmetric gauge theory,

Reference 14

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Observation 5ced216e-9d90-40bb-a391-a53f4fb05ad8 · outbound

This paper cites Supersym- metry and anomalous dimensionalities of quasi - parton operators in quantum chromodynamics,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Supersym- metry and anomalous dimensionalities of quasi - parton operators in quantum chromodynamics,

Reference 15

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Observation 8b48e3b9-d470-4388-bd3e-f01ccc02b34d · outbound

This paper cites Evolution Equations for Quasi-Partonic Operators,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Evolution Equations for Quasi-Partonic Operators,

Reference 16

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Observation a5736c32-8b37-4b65-8eb8-9d38fa7ebc98 · outbound

This paper cites Perspectives in Hadronic Physics, in Proc. of th e ICTP conf., World Scientific, Singapore,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Perspectives in Hadronic Physics, in Proc. of th e ICTP conf., World Scientific, Singapore,

Reference 17

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Observation 9732fa54-23de-44de-ae6a-dba31e15eb5d · outbound

This paper cites Next-to-leading corrections to the BFKL equa tion and the effec- tive action for high energy processes in QCD,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Next-to-leading corrections to the BFKL equa tion and the effec- tive action for high energy processes in QCD,

Reference 18

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Observation 7f14849b-0dbd-45db-8680-ccacc327cfc1 · outbound

This paper cites Integra bility of three particle evolution equations in QCD,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Integra bility of three particle evolution equations in QCD,

Reference 19

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Observation 87c34793-ea1b-4ccd-8e0f-b7c856e499a3 · outbound

This paper cites Fine structure of spectrum of twist-three operators in QCD.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Fine structure of spectrum of twist-three operators in QCD

Reference 20

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Observation baf34567-de18-41bc-8597-5cac91e11e2f · outbound

This paper cites New Integrable Structures in Large-N QCD.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling New Integrable Structures in Large-N QCD

Reference 21

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Observation eea3ab1d-ed63-4d49-9279-026495f024b5 · outbound

This paper cites One-Loop QCD Spin Chain and its Spectrum.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling One-Loop QCD Spin Chain and its Spectrum

Reference 22

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Observation e9384210-753b-4f0f-ba79-9a2b76e4dbb8 · outbound

This paper cites The Dilatation Operator of Conformal N=4 Super Yang-Mills Theory.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The Dilatation Operator of Conformal N=4 Super Yang-Mills Theory

Reference 25

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Observation 1454da51-2ad0-4ff8-992c-10ee55782e93 · outbound

This paper cites High-Energy Behavior in a Nonabelian Gauge Theory (II),.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling High-Energy Behavior in a Nonabelian Gauge Theory (II),

Reference 26

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Observation 5ff695cf-caca-4fe3-92cb-1d730978708b · outbound

This paper cites Three Gluon Integral Equa tion and Odd c Singlet Regge Singularities in QCD,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Three Gluon Integral Equa tion and Odd c Singlet Regge Singularities in QCD,

Reference 27

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Observation d43dcebf-f357-4458-ac42-606d33f0602e · outbound

This paper cites High Energy Asymptotics of Multi--Colour QCD and Exactly Solvable Lattice Models.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling High Energy Asymptotics of Multi--Colour QCD and Exactly Solvable Lattice Models

Reference 28

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Observation 031ede97-7c44-4c66-9f86-5e0fc5d927db · outbound

This paper cites BFKL pomeron in the next-to-leading approximation.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling BFKL pomeron in the next-to-leading approximation

Reference 29

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Observation bab6dcb0-e7d6-4145-b638-ad9735b279d8 · outbound

This paper cites Energy Scale(s) and Next-to-leading BFKL Equation.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Energy Scale(s) and Next-to-leading BFKL Equation

Reference 30

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Observation f2e5ab3f-c2cd-42ff-aac4-799c91d19fe7 · outbound

This paper cites The dipole form of the BFKL kernel in supersymmetric Yang--Mills theories.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The dipole form of the BFKL kernel in supersymmetric Yang--Mills theories

Reference 31

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Observation 36ca5928-b68d-42f2-8d26-b0ee59091ec4 · outbound

This paper cites NLO corrections to the BFKL equation in QCD and in supersymmetric gauge theories.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling NLO corrections to the BFKL equation in QCD and in supersymmetric gauge theories

Reference 32

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Observation 3f204f52-cbad-4d85-8b53-1e51a50d7193 · outbound

This paper cites Supersymmetric Dimensional Regularization via Dimens ional Reduc- tion,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Supersymmetric Dimensional Regularization via Dimens ional Reduc- tion,

Reference 33

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Observation c55df376-8c11-4137-8670-ce2d57016d6a · outbound

This paper cites QCD Nonlead ing Corrections to Weak Decays as an Application of Regularization by Dimensional Red uction,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling QCD Nonlead ing Corrections to Weak Decays as an Application of Regularization by Dimensional Red uction,

Reference 34

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Observation fd1c92a9-c693-4bec-ab4b-1709bb550887 · outbound

This paper cites Use of Four- dimensional Spin Methods in the Calculation of Radiative QCD Corrections,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Use of Four- dimensional Spin Methods in the Calculation of Radiative QCD Corrections,

Reference 35

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Observation 3a95e2e7-96d2-4364-ade0-a705281628f3 · outbound

This paper cites DGLAP and BFKL evolution equations in the N=4 supersymmetric gauge theory.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling DGLAP and BFKL evolution equations in the N=4 supersymmetric gauge theory

Reference 36

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Observation a654f34c-f136-4d30-9e26-698cfda9e2e9 · outbound

This paper cites BFKL Spectrum of N=4 SYM: non-Zero Conformal Spin.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling BFKL Spectrum of N=4 SYM: non-Zero Conformal Spin

Reference 37

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source=pdf_text observed=2026-08-14T13:31:47.207868Z digest=sha256:e70b2f72100288bff6578810d9f5b6bd7b853e32cce1eadf2d4a6be8e795bf10

Observation a86a3835-f685-4632-9980-d39be59226a4 · outbound

This paper cites Harmonic sums, Mellin transforms and Integrals.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Harmonic sums, Mellin transforms and Integrals

Reference 38

Resolution
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no resolver link, observed 2026-08-14T13:31:47.211505Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.211505Z digest=sha256:b682b9cfe900054b7fd7829ca29aba6e372e72bd783a08acb3c81132a508099a

Observation 195d8215-8e07-46bc-8806-983682fcb4af · outbound

This paper cites The Large N Limit of Superconformal Field Theories and Supergravity.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The Large N Limit of Superconformal Field Theories and Supergravity

Reference 39

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.214862Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.214862Z digest=sha256:1f255980fc67389924debaf6c5cb834f82372dfb1bca7e17898bc8e13507b4d7

Observation 2321cb2d-5b03-425d-90c1-09f39c58d59e · outbound

This paper cites Gauge theo ry correlators from noncritical string theory,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Gauge theo ry correlators from noncritical string theory,

Reference 40

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.218274Z

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source=pdf_text observed=2026-08-14T13:31:47.218274Z digest=sha256:c051422c750255c4eda13853c2c39673b3fadce6fa5bdb340c70d66ab3d7664d

Observation 14cafe37-17f0-4047-9844-8e2b96175d05 · outbound

This paper cites Anti De Sitter Space And Holography.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Anti De Sitter Space And Holography

Reference 41

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.221451Z

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source=pdf_text observed=2026-08-14T13:31:47.221451Z digest=sha256:4f2ebd8f0dc27fee7200d6930ed23d5c0c74a0493ea21b05c9ff9b6ffa66cd66

Observation e3af1569-2e45-4bb4-a0a3-61c69ca97a54 · outbound

This paper cites Deep Inelastic Scattering and Gauge/String Duality.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Deep Inelastic Scattering and Gauge/String Duality

Reference 42

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.225603Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.225603Z digest=sha256:f65db5d2cf62fcdeacb6a32d24ee94e0664559fcdb51882420d39ac32ffb60e5

Observation 078ba1af-3b1b-49d7-b84b-fe81efe51dea · outbound

This paper cites Effective action for the Regge processes in gravity.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Effective action for the Regge processes in gravity

Reference 43

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.229070Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.229070Z digest=sha256:b75fa6a7809ded132c1701ebc432be5ee7b1afb7fe4ee526cb59539ebd665edd

Observation 8b99cb25-2686-439c-89da-0188ee0ddd7a · outbound

This paper cites A semi-classical limit of the gauge/string correspondence.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling A semi-classical limit of the gauge/string correspondence

Reference 44

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.231853Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.231853Z digest=sha256:1c85d365752b10f05333731c4f7c4ec51f7debc1ef5207b2cdbea25fc652b714

Observation 219a15f6-be1c-4eb0-a15e-1a5fbfc5dc5d · outbound

This paper cites Semiclassical quantization of rotating superstring in AdS_5 x S^5.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Semiclassical quantization of rotating superstring in AdS_5 x S^5

Reference 45

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.234596Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.234596Z digest=sha256:083b83168a1b85737999b3e144c4d6597ea7e5bc39c394d8fdcba40e47284086

Observation 124c6d59-cc43-40f7-a5d1-378838922455 · outbound

This paper cites Two-loop world-sheet corrections in AdS_5 x S^5 superstring.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Two-loop world-sheet corrections in AdS_5 x S^5 superstring

Reference 46

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.237298Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.237298Z digest=sha256:a304aabb83172c7707d29a92b96cd1cce326a892c4499239dbda770e92b52be2

Observation 4c84d0b4-cc52-455d-9b97-d9e9b35ae3fc · outbound

This paper cites Hard Scattering and Gauge/String Duality.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Hard Scattering and Gauge/String Duality

Reference 47

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.240441Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.240441Z digest=sha256:85d34694a6ec62d28967f8bcc56b9b523cb01c9c69bb7c51bc291ff7f2b20c88

Observation 5e7d1a78-69f2-46da-bda5-8e1780b5172b · outbound

This paper cites Three-loop universal anomalous dimension of the Wilson operators in N=4 SUSY Yang-Mills model.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Three-loop universal anomalous dimension of the Wilson operators in N=4 SUSY Yang-Mills model

Reference 48

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.243853Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.243853Z digest=sha256:65fffb5f96656c95583ac4fa8ef0750f12d3614262f9773cbaa9d532b5749b14

Observation 42cfdbb3-baf4-4d67-b2ca-f4959b169c40 · outbound

This paper cites The Pomeron and Gauge/String Duality.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The Pomeron and Gauge/String Duality

Reference 49

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.247598Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.247598Z digest=sha256:d995c3f215a9eb6a368c7eeb9ec95bc860ca0bdb1ceb2e9d37f5491b46702e4b

Observation 9f0a4bca-d454-484f-aef4-a489618bb3e1 · outbound

This paper cites Pomeron in the N=4 supersymmetric gauge model at strong couplings.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Pomeron in the N=4 supersymmetric gauge model at strong couplings

Reference 50

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.251720Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.251720Z digest=sha256:3d935bec7dfb1a26ced36ba07cc2708ac03ca3e979e93ecb7c66ebd9f404c4b4

Observation 295d3a9b-ce6d-446e-856b-553ff607cfb3 · outbound

This paper cites A resummation of large sub-leading corrections at small x.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling A resummation of large sub-leading corrections at small x

Reference 51

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.255292Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.255292Z digest=sha256:2804191b9476907ae958c38d7515f9d3057435ebb8b8bb40f2e8bf24db608765

Observation 583ee129-09fd-459a-9f3e-fcfe42086591 · outbound

This paper cites An introduction to leading and next-to-leading BFKL.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling An introduction to leading and next-to-leading BFKL

Reference 52

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.258399Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.258399Z digest=sha256:010adeb9fcd56f7ea33198eb1ad17030710ff7d5f2addf5dbdcb6d1706f611b2

Observation fab52773-9dbf-4374-95b5-0d1914180d44 · outbound

This paper cites Quantum folded string and integrability: from finite size effects to Konishi dimension.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Quantum folded string and integrability: from finite size effects to Konishi dimension

Reference 53

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.261639Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.261639Z digest=sha256:62a6a5d26b005de41c49bbb8ca15b0220272ed07b3d963ef916f1c5ce545d31c

Observation b5eaae3c-5a25-4120-b65c-94f0f82066b1 · outbound

This paper cites Semiclassical string computation of strong-coupling corrections to dimensions of operators in Konishi multiplet.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Semiclassical string computation of strong-coupling corrections to dimensions of operators in Konishi multiplet

Reference 54

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.264900Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.264900Z digest=sha256:9da05c146875947f42c91a67708df3f516400fd00dbb9df60feca6c72c1128c4

Observation 0386f645-7b91-42cd-bfdb-6986d672ab33 · outbound

This paper cites An exact slope for AdS/CFT.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling An exact slope for AdS/CFT

Reference 55

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.268021Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.268021Z digest=sha256:16c8cc96e79c0aa11364ffd2d1b3332bf67a7e014ca22cea2b22f6c723ca27b4

Observation 32e452d8-c5dd-4521-95d5-45093dd69d46 · outbound

This paper cites Scaling dimensions at small spin in N=4 SYM theory.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Scaling dimensions at small spin in N=4 SYM theory

Reference 56

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.271354Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.271354Z digest=sha256:bbf5ef58570b4ef7f4a09bb539724b966bb26869d6c0de3324c8299ed7e9a5fc

Observation dbb11433-8f99-4462-86e6-5474a1b9b544 · outbound

This paper cites Deeper Look into Short Strings.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Deeper Look into Short Strings

Reference 57

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.274662Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.274662Z digest=sha256:255b598e1028f1b2289532081b7bb8565421aa0a9f4828863402023735b0447a

Observation 1aa3b13c-4446-4cf3-8b24-410887bf9a0d · outbound

This paper cites Conformal Regge theory.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Conformal Regge theory

Reference 58

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.277712Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.277712Z digest=sha256:1d59ce73d19630c39b4aa914827f5215b1a221a83aa7a3c00051594be5d79ef0

Observation 89321c05-5905-44f2-844c-8976a9c594c6 · outbound

This paper cites Quantum Spectral Curve at Work: From Small Spin to Strong Coupling in N=4 SYM.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Quantum Spectral Curve at Work: From Small Spin to Strong Coupling in N=4 SYM

Reference 59

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.280773Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.280773Z digest=sha256:b389997a869581581344221dbae90dbe93ec6a0e4727c627bcf308dc2b96dafc

Observation 893e58bb-ff8c-4014-97f0-e02f661b6b03 · outbound

This paper cites Review of AdS/CFT Integrability: An Overview.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Review of AdS/CFT Integrability: An Overview

Reference 60

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.283479Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.283479Z digest=sha256:8dd635d64a3de352447d09ce2ca0f114b1af78c9f7b67445d967e7b8c8308c26

Observation 6d985db9-57bc-463a-b002-e32b8e5ed64d · outbound

This paper cites High energy QCD as a completely integrable model.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling High energy QCD as a completely integrable model

Reference 61

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.286215Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.286215Z digest=sha256:49d452d60299dc3570e6fc5ea935c441a240da99ec724e48d527f547687b6426

Observation 73c435d0-8320-47a0-bee1-080e0623ce5a · outbound

This paper cites The Bethe-Ansatz for N=4 Super Yang-Mills.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The Bethe-Ansatz for N=4 Super Yang-Mills

Reference 62

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.289567Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.289567Z digest=sha256:2ef354f559621088659d764fec1c2617113366168e889bf7cea59d18f3eb8837

Observation 67cec521-5882-4ab5-968e-f2debf491bd7 · outbound

This paper cites The N=4 SYM Integrable Super Spin Chain.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The N=4 SYM Integrable Super Spin Chain

Reference 63

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.292464Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.292464Z digest=sha256:572fb35d7034d5f383c327a69fd49e9314552923c143413c1026c9e289272abb

Observation 8c45a37f-b2a5-4fb7-a9d5-4683593fe344 · outbound

This paper cites The Factorized S-Matrix of CFT/AdS.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The Factorized S-Matrix of CFT/AdS

Reference 64

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.295989Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.295989Z digest=sha256:8a2dd21fe6bb69c245166c5df01abdf77271e428080765eaa14f0f82f3841148

Observation 04aecafa-0ae1-4a92-8684-ad6b4eea3d3d · outbound

This paper cites Bethe Ansatz for Quantum Strings.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Bethe Ansatz for Quantum Strings

Reference 65

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.299193Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.299193Z digest=sha256:58541694f6f1d7505c49ee3c0951fa39876e86d2cbe64086650e8c3238d14935

Observation fc775250-ce50-4251-9693-9ef8aea4f013 · outbound

This paper cites The su(2|2) Dynamic S-Matrix.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The su(2|2) Dynamic S-Matrix

Reference 66

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.302337Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.302337Z digest=sha256:14aeb2321589f4fd11e1da8f2436cf3ce84bcf8b8d0b861704bf01b4f7621ff8

Observation b59b4500-e785-4b36-81ea-076bbe2010b4 · outbound

This paper cites The Analytic Bethe Ansatz for a Chain with Centrally Extended su(2|2) Symmetry.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The Analytic Bethe Ansatz for a Chain with Centrally Extended su(2|2) Symmetry

Reference 67

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.305697Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.305697Z digest=sha256:b694a79938a4869c1ef1a5ba096f8536d6682812f269653359c5138b2d68fa31

Observation 3460df63-e1ba-4b20-abc4-deb128391540 · outbound

This paper cites The AdS_5xS^5 superstring worldsheet S-matrix and crossing symmetry.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The AdS_5xS^5 superstring worldsheet S-matrix and crossing symmetry

Reference 69

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.312796Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.312796Z digest=sha256:2b87593c6fb406cb74e1a71051a49408ffe2a3fe67825bf5008a75758133770f

Observation acd6e753-ddef-4f1a-a563-f2f305703681 · outbound

This paper cites On AdS_5 x S^5 String S-matrix.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling On AdS_5 x S^5 String S-matrix

Reference 70

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.315881Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.315881Z digest=sha256:c7c7bbcbfdd5d67bb5441f0b78b9d3d83fd2117d758d4f390e9adbf6d7df0be1

Observation 11976a5a-c8d9-456b-a06d-d7350d89c768 · outbound

This paper cites The Zamolodchikov-Faddeev Algebra for AdS_5 x S^5 Superstring.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The Zamolodchikov-Faddeev Algebra for AdS_5 x S^5 Superstring

Reference 71

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.319217Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.319217Z digest=sha256:d24424bbaeca253fb0916729220a5168692434fed9929bc5ee5b91300ef6a35f

Observation fba29897-8722-4fb9-b436-57982fee5652 · outbound

This paper cites Long-Range PSU(2,2|4) Bethe Ansaetze for Gauge Theory and Strings.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Long-Range PSU(2,2|4) Bethe Ansaetze for Gauge Theory and Strings

Reference 72

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.322511Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.322511Z digest=sha256:31f8fe0631716ac0ed2f368e3f556f1bf356080dab701a84588c002eb55287ec

Observation d2adbff5-7e3c-412e-8df7-ce92f251f145 · outbound

This paper cites Integrability for the Full Spectrum of Planar AdS/CFT.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Integrability for the Full Spectrum of Planar AdS/CFT

Reference 73

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.325798Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.325798Z digest=sha256:52bf385c536363bbcb305736898e4383a7c472f3e511174776194d690596c95b

Observation d5a798a3-543e-47e0-81a6-afb8300a0204 · outbound

This paper cites Thermodynamic Bethe Ansatz for planar AdS/CFT: a proposal.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Thermodynamic Bethe Ansatz for planar AdS/CFT: a proposal

Reference 74

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.329277Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.329277Z digest=sha256:9a04441d4c50d968c5c6f2349a04c2b0f41da343f75f0d0f0f9d9cba7c3ee7e4

Observation 8ccdcdf1-51eb-4016-949b-a55669a43c9f · outbound

This paper cites Integrability for the Full Spectrum of Planar AdS/CFT II.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Integrability for the Full Spectrum of Planar AdS/CFT II

Reference 75

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.332145Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.332145Z digest=sha256:35cd5d97f68458e3a43d98f8b046b6178d5f9c78d3f6cdf15e73a974813387e4

Observation d31c4bc9-47b1-4462-87d3-6d185895cc5d · outbound

This paper cites Thermodynamic Bethe Ansatz for the AdS_5 x S^5 Mirror Model.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Thermodynamic Bethe Ansatz for the AdS_5 x S^5 Mirror Model

Reference 76

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.335051Z

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source=pdf_text observed=2026-08-14T13:31:47.335051Z digest=sha256:e9826844b03d909a8e348fa53a05a54d862875964ba7b07643bf7dbd676a886b

Observation 57f64f3e-e7ba-4644-8084-17230962828d · outbound

This paper cites Extended Y-system for the $AdS_5/CFT_4$ correspondence.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Extended Y-system for the $AdS_5/CFT_4$ correspondence

Reference 77

Resolution
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no resolver link, observed 2026-08-14T13:31:47.337793Z

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source=pdf_text observed=2026-08-14T13:31:47.337793Z digest=sha256:95d5275335a124439743ec45cdf68d24adb842ebd48765c6476ae09dd3fb3fb5

Observation 3e8395de-a819-4067-9e68-d33c5f8c489f · outbound

This paper cites $AdS_5\times S^5$ mirror TBA equations from Y-system and discontinuity relations.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling $AdS_5\times S^5$ mirror TBA equations from Y-system and discontinuity relations

Reference 78

Resolution
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no resolver link, observed 2026-08-14T13:31:47.340856Z

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Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.340856Z digest=sha256:23f82052e3455745e75052a6e76fe12e2d2b40c78fdacb009b05edf1a976c602

Observation 06e439f0-96fd-4aae-9ee7-6f6d415ece90 · outbound

This paper cites Wronskian Solution for AdS/CFT Y-system.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Wronskian Solution for AdS/CFT Y-system

Reference 79

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no resolver link, observed 2026-08-14T13:31:47.344779Z

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source=pdf_text observed=2026-08-14T13:31:47.344779Z digest=sha256:5350e37ca0b4e2538eca8c81dc7c770bece55c732eb03191c2fcddd71f61d2c7

Observation 4fe280b4-a94a-46f8-bbe7-0bb8b27a00ac · outbound

This paper cites Solving the AdS/CFT Y-system.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Solving the AdS/CFT Y-system

Reference 80

Resolution
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no resolver link, observed 2026-08-14T13:31:47.348000Z

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source=pdf_text observed=2026-08-14T13:31:47.348000Z digest=sha256:5608fb43ed813116be8a6f35be165841f6c8469572436ef5ff11cee8ff698622

Observation 4ae74ea3-4f90-42f0-838b-b371d56af32b · outbound

This paper cites Quantum spectral curve for AdS_5/CFT_4.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Quantum spectral curve for AdS_5/CFT_4

Reference 81

Resolution
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no resolver link, observed 2026-08-14T13:31:47.351147Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.351147Z digest=sha256:e2316bb2ab1e800f682d4ec958efc0a7d0031d1c5ff8663afe9f6ed38bb17967

Observation f29be5d7-96da-4189-94ae-cfde37508527 · outbound

This paper cites Quantum spectral curve for arbitrary state/operator in AdS$_5$/CFT$_4$.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Quantum spectral curve for arbitrary state/operator in AdS$_5$/CFT$_4$

Reference 82

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.354457Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.354457Z digest=sha256:7f615a51e2a37ee2c5b05b2614ed960a78ee2221fcce0bbde96cd56345c758d1

Observation e4a906ee-4d68-4a4a-bdb8-f122f8a1bca0 · outbound

This paper cites T-system on T-hook: Grassmannian Solution and Twisted Quantum Spectral Curve.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling T-system on T-hook: Grassmannian Solution and Twisted Quantum Spectral Curve

Reference 83

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.357974Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.357974Z digest=sha256:42d42eb8c7db86b9ef626e26dcd043271b55cf1d57911d1f33d213fcd994c4ed

Observation bad369b1-1805-4467-989e-86a7eacd46db · outbound

This paper cites The full spectrum of AdS5/CFT4 I: Representation theory and one-loop Q-system.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The full spectrum of AdS5/CFT4 I: Representation theory and one-loop Q-system

Reference 84

Resolution
verified exact
local_arxiv, observed 2026-08-14T13:31:48.635674Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.

source=pdf_text observed=2026-08-14T13:31:47.361416Z digest=sha256:80e68f9264ed89853dad94b0eb0701af39898117aea7e36aecbe2347a1f7e375

Observation 7f99ab36-5fb3-4ba0-bf5f-f76aadf4e3a9 · outbound

This paper cites The full spectrum of AdS$_5$/CFT$_4$ II: Weak coupling expansion via the quantum spectral curve.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The full spectrum of AdS$_5$/CFT$_4$ II: Weak coupling expansion via the quantum spectral curve

Reference 85

Resolution
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no resolver link, observed 2026-08-14T13:31:47.364700Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.364700Z digest=sha256:c4db1bbb3f96e6a8032091e1f93d915fb4749eb718ae8e298bead58202449304

Observation f0df3ee0-200f-4d84-b3fb-77b53838fa21 · outbound

This paper cites Quantum Spectral Curve and the Numerical Solution of the Spectral Problem in AdS5/CFT4.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Quantum Spectral Curve and the Numerical Solution of the Spectral Problem in AdS5/CFT4

Reference 86

Resolution
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no resolver link, observed 2026-08-14T13:31:47.367944Z

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source=pdf_text observed=2026-08-14T13:31:47.367944Z digest=sha256:2f502eae31ec9d29fbf354903101c8767b93ca7b70922069209dc5b3f4fd354f

Observation bc1178b2-32a5-45cc-8c99-d247dbf413ba · outbound

This paper cites Strong coupling results from the numerical solution of the quantum spectral curve.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Strong coupling results from the numerical solution of the quantum spectral curve

Reference 87

Resolution
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no resolver link, observed 2026-08-14T13:31:47.372138Z

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source=pdf_text observed=2026-08-14T13:31:47.372138Z digest=sha256:8ad0a836a155c2e10630bd9da1445be97ca75148b728c54e1d66f91f1f57c98c

Observation c5156c80-be5a-48e4-a123-69273da79ac5 · outbound

This paper cites Quantum spectral curve as a tool for a perturbative quantum field theory.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Quantum spectral curve as a tool for a perturbative quantum field theory

Reference 88

Resolution
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no resolver link, observed 2026-08-14T13:31:47.375354Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.375354Z digest=sha256:1d1c34c18b9ab635d680c10c2594495e2b18b1c1ea6b97498df5f904e728745e

Observation cf20a7d1-d516-40da-803f-eeb1e42b1713 · outbound

This paper cites QCD Pomeron from AdS/CFT Quantum Spectral Curve.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling QCD Pomeron from AdS/CFT Quantum Spectral Curve

Reference 89

Resolution
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no resolver link, observed 2026-08-14T13:31:47.378057Z

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source=pdf_text observed=2026-08-14T13:31:47.378057Z digest=sha256:642d022b735414973c46c1dddfdd81c527ffde1d8cf36a268cccd609c856354c

Observation a722d510-7d8d-4e3f-9dd2-73630cb3f6cd · outbound

This paper cites NNLO BFKL Pomeron eigenvalue in N=4 SYM.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling NNLO BFKL Pomeron eigenvalue in N=4 SYM

Reference 90

Resolution
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no resolver link, observed 2026-08-14T13:31:47.381542Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.381542Z digest=sha256:2434a4a487280cc4832cd24db23a4a90b0409a1c929ab4bb4818d43b1130e4a6

Observation 84826002-92b8-4451-9395-53cc9deeba8c · outbound

This paper cites The Bare Pomeron in Quantum Chromodynamics,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The Bare Pomeron in Quantum Chromodynamics,

Reference 91

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.384672Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.384672Z digest=sha256:4d8c030ddf5535600e8f3f7d8b3f4c7e9e86532e2e11aad64df9ffe8c5c4d653

Observation e9159613-df62-469f-bd77-ffdd7ebfc7f4 · outbound

This paper cites BFKL pomeron in the next-to-next-to-leading approximation in the planar N=4 SYM theory.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling BFKL pomeron in the next-to-next-to-leading approximation in the planar N=4 SYM theory

Reference 92

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.387733Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.387733Z digest=sha256:5d2a1af81435352c4e8292e4fe98af286fa23b8f465caa864e931977719d9e69

Observation e9a88586-b78f-4169-b352-969db1155406 · outbound

This paper cites High-energy evolution to three loops.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling High-energy evolution to three loops

Reference 93

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.391413Z

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source=pdf_text observed=2026-08-14T13:31:47.391413Z digest=sha256:bbdfb7185ae813514b5052d776df0c03fb4594fb1cf724d5d3ab00d17aacfab9

Observation 58130597-220b-4b32-936d-aa72e90d8eff · outbound

This paper cites The Three loop sp litting functions in QCD: The Nonsinglet case,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The Three loop sp litting functions in QCD: The Nonsinglet case,

Reference 94

Resolution
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no resolver link, observed 2026-08-14T13:31:47.394413Z

Source-reported events for the cited work

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source=pdf_text observed=2026-08-14T13:31:47.394413Z digest=sha256:c4af900b8e3adc9e4de7ef661d18eb552b621d587ba7b91f1f85fb39cdc99623

Observation 0da06cfa-13a5-40c6-b213-f3b1f199e781 · outbound

This paper cites The Three-Loop Splitting Functions in QCD: The Singlet Case.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling The Three-Loop Splitting Functions in QCD: The Singlet Case

Reference 95

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.397346Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.397346Z digest=sha256:bd7f50a2c61b69ad42419ea6e42da2db8b9300b0771bfb33787387757accb4b6

Observation 1f2eeffb-f230-4e43-9143-d7016a8db841 · outbound

This paper cites Anomalous dimensions of Wilson operators in N=4 SYM theory.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Anomalous dimensions of Wilson operators in N=4 SYM theory

Reference 96

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.400906Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.400906Z digest=sha256:db5b05945f0baa430ade5d0b6fe83a5d8e5f41f376bc883cd53d41e42ce49c24

Observation 3313db76-c0e8-4f06-983b-bf56660c201a · outbound

This paper cites Dressing and Wrapping.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Dressing and Wrapping

Reference 97

Resolution
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no resolver link, observed 2026-08-14T13:31:47.404080Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.404080Z digest=sha256:a643224ef19dd8603cae0dfec1eb459ee39e404972051d586fbf894cedd6cedd

Observation d1857821-48ef-4fc0-8134-1f58bbae09b9 · outbound

This paper cites Four loop twist two, BFKL, wrapping and strings.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Four loop twist two, BFKL, wrapping and strings

Reference 98

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.407280Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.407280Z digest=sha256:842895c098faa26b68d5239e9f101c121a019f722a933995700c2b99c1aa9605

Observation 2d3c82af-7d71-490f-80c2-53b81854b33e · outbound

This paper cites Five-Loop Anomalous Dimension of Twist-Two Operators.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Five-Loop Anomalous Dimension of Twist-Two Operators

Reference 99

Resolution
verified exact
local_arxiv, observed 2026-08-14T13:31:48.470884Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.

source=pdf_text observed=2026-08-14T13:31:47.411087Z digest=sha256:b565160be4ec25a60c0339866835d2dea33feb101f8f800e86e935109bab0d0b

Observation 6d924a79-c769-4d43-af9f-3437514b9a3c · outbound

This paper cites Analytic three-loop Solutions for N=4 SYM Twist Operators.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Analytic three-loop Solutions for N=4 SYM Twist Operators

Reference 100

Resolution
verified exact
local_arxiv, observed 2026-08-14T13:31:48.457720Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.

source=pdf_text observed=2026-08-14T13:31:47.414629Z digest=sha256:c1b977ea612ffcce7d97b828f48a73fab432458b1830733c943491cc9ce7b905

Observation 82be9f32-54ec-469d-b357-4826de082fcb · outbound

This paper cites Analytic solution of the multiloop Baxter equation.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Analytic solution of the multiloop Baxter equation

Reference 101

Resolution
verified exact
local_arxiv, observed 2026-08-14T13:31:48.444757Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.

source=pdf_text observed=2026-08-14T13:31:47.417946Z digest=sha256:52bd5ac0a990971842ecf0a09f25e96933a569a3c21d5fc72b0c69736002d6aa

Observation ff60b5b3-03e4-4b4a-b77b-349ffb9291fd · outbound

This paper cites Analytic two-loop results for selfenergy- and vertex-type diagrams with one non-zero mass.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Analytic two-loop results for selfenergy- and vertex-type diagrams with one non-zero mass

Reference 102

Resolution
unresolved
no resolver link, observed 2026-08-14T13:31:47.421385Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-14T13:31:47.421385Z digest=sha256:2acb3b17b4291e0a2cf8346c490488ad651ef4506d6915134b1c851f2a66fe69

Observation 4da04854-8b6f-42c3-a197-50e035a8beed · outbound

This paper cites Two-Loop Formfact ors in Theories with Mass Gap and Z-Boson Production,.

DGLAP and BFKL equations in $\mathcal{N}=4$ SYM: from weak to strong coupling Two-Loop Formfact ors in Theories with Mass Gap and Z-Boson Production,

Reference 103

Resolution
verified exact
raw_fallback, observed 2026-08-14T13:31:48.421231Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.

source=pdf_text observed=2026-08-14T13:31:47.424891Z digest=sha256:618df3964ce48c473a684b446c5f0ad138b82c86014d8164fd8f06537dd0b3b6

Pith citing papers

No inbound Pith citation observations are available.