ABJM Baryon Stability and Myers effect

Konstadinos Sfetsos; Konstadinos Siampos; Marco Picos; Yolanda Lozano

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ABJM Baryon Stability and Myers effect

Yolanda Lozano, Marco Picos, Konstadinos Sfetsos, Konstadinos Siampos

High Energy Physics - Theory · Submitted 4 May 2011

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim We show that these configurations are solutions to the classical equations of motion and are stable beyond a critical value of l.

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We consider magnetically charged baryon vertex like configurations in AdS^4 X CP^3 with a reduced number of quarks l. We show that these configurations are solutions to the classical equations of motion and are stable beyond a critical value of l. Given that the magnetic flux dissolves D0-brane charge it is possible to give a microscopical description in terms of D0-branes expanding into fuzzy CP^n spaces by Myers dielectric effect. Using this description we are able to explore the region of finite 't Hooft coupling.

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#	sentence	role	the authors' own work	states the main conclusion	strength
s0	We consider magnetically charged baryon vertex like configurations in AdS^4 X CP^3 with a reduced number of quarks l.	contribution 0.88	0.59	0.04	asserted 0.60
s1	We show that these configurations are solutions to the classical equations of motion and are stable beyond a critical value of l.	result 0.99	0.94	0.68	asserted 1.00
s2	Given that the magnetic flux dissolves D0-brane charge it is possible to give a microscopical description in terms of D0-branes expanding into fuzzy CP^n spaces by Myers dielectric effect.	method 0.66	0.48	0.13	hedged possibility 0.96
s3	Using this description we are able to explore the region of finite 't Hooft coupling.	contribution 0.55	0.90	0.08	asserted 0.95

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Original abstract

We consider magnetically charged baryon vertex like configurations in AdS^4 X CP^3 with a reduced number of quarks l. We show that these configurations are solutions to the classical equations of motion and are stable beyond a critical value of l. Given that the magnetic flux dissolves D0-brane charge it is possible to give a microscopical description in terms of D0-branes expanding into fuzzy CP^n spaces by Myers dielectric effect. Using this description we are able to explore the region of finite 't Hooft coupling.

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7 arXiv papers cite this in 14 sentences

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Uses its method or tool 1 paper

We then have that [equation] The determinant of $Q$ can be computed as explained for instance in [ref] , with the result [equation] As explained in [ref] this expression is valid in the limit $R>>1$, $m>>1$, with $R^3/m$ finite.

Dielectric 5-Branes and Giant Gravitons in ABJM · Expanded graviton configurations · 0.93

Cites it as background 4 papers

For more details see [ref] .

From Schurs to Giants in ABJ(M) · Schurs and giants in $AdS_4/CFT_3$ · 0.96
In the context of Myers dielectric effect it was first studied in [ref] and then in [ref] .

Dielectric 5-Branes and Giant Gravitons in ABJM · Expanded graviton configurations · 0.97
Its maximal version was discussed in [ref] , see also [ref] , but the general solution was first constructed in [ref] .

Giant Gravitons on AdS_4 x CP^3 and their Holographic Three-point Functions · Introduction · 0.90

What it cites · 62 sentences without a confident label

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In this section we show that generalizing the microscopical Chern-Simons action in [ref] to include higher curvature terms [ref] we can predict the existence of a dielectric higher curvature coupling in the action for multiple D0-branes that exactly cancels the $k/8$ contribution to the D6-brane tadpole that we obtained above.

I-Brane Inflow and Anomalous Couplings on D-Branes · Dielectric higher-curvature terms · 0.99
In this section we show that generalizing the microscopical Chern-Simons action in [ref] to include higher curvature terms [ref] we can predict the existence of a dielectric higher curvature coupling in the action for multiple D0-branes that exactly cancels the $k/8$ contribution to the D6-brane tadpole that we obtained above.

Anomalies, Branes, and Currents · Dielectric higher-curvature terms · 0.99
In this section we show that generalizing the microscopical Chern-Simons action in [ref] to include higher curvature terms [ref] we can predict the existence of a dielectric higher curvature coupling in the action for multiple D0-branes that exactly cancels the $k/8$ contribution to the D6-brane tadpole that we obtained above.

Curvature terms in D-brane actions and their M-theory origin · Dielectric higher-curvature terms · 0.99

Compares with 8 papers

Note as well that ([ref]) reduces to the expression found in [ref] when $l=q$.

Charged particle-like branes in ABJM · Varying the number of fundamental strings · 0.86
In all these cases the constituents contribute with an energy $l T_F1∫_0^∞dρ$ and the binding energy is given by: [equation] This expression has again the same form than the corresponding expressions in [ref] [In this case we have added the on-shell energy of the D$p$-brane.].

Wilson loops in large N field theories · Varying the number of fundamental strings · 0.90
In all these cases the constituents contribute with an energy $l T_F1∫_0^∞dρ$ and the binding energy is given by: [equation] This expression has again the same form than the corresponding expressions in [ref] [In this case we have added the on-shell energy of the D$p$-brane.].

The baryon vertex with magnetic flux · Varying the number of fundamental strings · 0.90

Cites as background 8 papers

The organization of the paper is as follows: We start in section 2 by summarizing some of the properties of the magnetized baryon vertex like configurations constructed in [ref] .

Charged particle-like branes in ABJM · Introduction · 0.85
The $AdS_4/CFT_3$ duality relates the Type IIA superstring on $AdS_4×CP^3$ to an $N=6$ quiver Chern-Simons-matter theory with gauge group $U(N)_k ×U(N)_-k$ known as the ABJM model [ref] .

N=6 superconformal Chern-Simons-matter theories, M2-branes and their gravity duals · Introduction · 1.00
It is well known that the macroscopical and microscopical descriptions have complementary ranges of validity [ref] .

Dielectric-Branes · The microscopical description · 0.93

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