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Quarkonium from the Fifth Dimension
High Energy Physics - Theory · Submitted 5 Dec 2003
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim All of the hadrons are actually of finite size ~ \sqrt{g^2N}/m_Q, regardless of their radial excitation level and of how many valence adjoint particles they contain.
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The abstract, sentence by sentence
Adding fundamental matter of mass m_Q to N=4 Yang Mills theory, we study quarkonium, and "generalized quarkonium" containing light adjoint particles. At large 't Hooft coupling the states of spin<=1 are anomalously light (Kruczenski et al., hep-th/0304032). We examine their form factors, and show these hadrons are unlike any known in QCD. By a traditional yardstick they appear infinite in size (as with strings in flat space) but we show that this is a failure of the yardstick. All of the hadrons are actually of finite size ~ \sqrt{g^2N}/m_Q, regardless of their radial excitation level and of how many valence adjoint particles they contain. Certain form factors for spin-1 quarkonia vanish in the large-g^2N limit; thus these hadrons resemble neither the observed J/Psi quarkonium states nor rho mesons.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Adding fundamental matter of mass m_Q to N=4 Yang Mills theory, we study quarkonium, and "generalized quarkonium" containing light adjoint particles. | contribution 0.96 | 0.73 | 0.04 | asserted 0.70 |
| s1 | At large 't Hooft coupling the states of spin<=1 are anomalously light (Kruczenski et al., hep-th/0304032). | background 0.85 | 0.07 | 0.06 | asserted 1.00 |
| s2 | We examine their form factors, and show these hadrons are unlike any known in QCD. | contribution 0.52 | 0.89 | 0.09 | asserted 1.00 |
| s3 | By a traditional yardstick they appear infinite in size (as with strings in flat space) but we show that this is a failure of the yardstick. | interpretation 0.75 | 0.45 | 0.08 | asserted 0.98 |
| s4 | All of the hadrons are actually of finite size ~ \sqrt{g^2N}/m_Q, regardless of their radial excitation level and of how many valence adjoint particles they contain. | result 0.99 | 0.93 | 0.77 | asserted 1.00 |
| s5 | Certain form factors for spin-1 quarkonia vanish in the large-g^2N limit; thus these hadrons resemble neither the observed J/Psi quarkonium states nor rho mesons. | result 0.75 | 0.89 | 0.13 | asserted 0.99 |
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The paper
Original abstract
Adding fundamental matter of mass m_Q to N=4 Yang Mills theory, we study quarkonium, and "generalized quarkonium" containing light adjoint particles. At large 't Hooft coupling the states of spin<=1 are anomalously light (Kruczenski et al., hep-th/0304032). We examine their form factors, and show these hadrons are unlike any known in QCD. By a traditional yardstick they appear infinite in size (as with strings in flat space) but we show that this is a failure of the yardstick. All of the hadrons are actually of finite size ~ \sqrt{g^2N}/m_Q, regardless of their radial excitation level and of how many valence adjoint particles they contain. Certain form factors for spin-1 quarkonia vanish in the large-g^2N limit; thus these hadrons resemble neither the observed J/Psi quarkonium states nor rho mesons.
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References
How the literature uses it
21 arXiv papers cite this in 31 sentences
Papers citing it · 18 sentences without a confident label
Compares with it 2 papers
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in agreement with results from D3-D7 [ref] and hard and soft wall models [ref] .
Deep Inelastic Scattering in Holographic AdS/QCD Models · DIS in D3-D7 system · 0.92
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This result has been obtained before in [ref] for the D3-D7 model, using different scalar field solutions.
Deep inelastic scattering from gauge string duality in D3-D7 brane model · Elastic form factors · 0.91
Cites it as background 10 papers
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In this Section we review the gravity dual description of strongly coupled $=4$ SYM theory with gauge group $SU(N)$ coupled to $N_f ≪N$ $=2$ hypermultiplets in the fundamental representation of $SU(N)$, introduced in [ref] and studied in [ref] .
A limiting velocity for quarkonium propagation in a strongly coupled plasma via AdS/CFT · D3/D7-brane construction of mesons · 0.92
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For thorough discussions of theories similar to the one we consider, see [ref] .
Alternative large Nc baryons and holography · Field theory preliminaries · 0.99
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In order to introduce fields that are in the fundamental representation, like quarks, one can add $N_f$ D7 brane probes in the space [ref] .
Deep inelastic scattering from gauge string duality in D3-D7 brane model · Introduction · 0.85
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