Giant magnons and non-maximal giant gravitons

A. Ciavarella

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Giant magnons and non-maximal giant gravitons

A. Ciavarella

High Energy Physics - Theory · Submitted 5 Nov 2010

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

The authors' main claim Relating the two boundary parameters in a special way we describe the scattering of giant magnons with non-maximal $Y=0$ giant gravitons and calculate the leading contribution to the associated magnon scattering phase.

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We produce the open strings on $\mathbb{R}\times S^{2}$ that correspond to the solutions of integrable boundary sine-Gordon theory by making use of the $N$-magnon solutions provided in \cite{KPV} together with explicit moduli. Relating the two boundary parameters in a special way we describe the scattering of giant magnons with non-maximal $Y=0$ giant gravitons and calculate the leading contribution to the associated magnon scattering phase.

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#	sentence	role	the authors' own work	states the main conclusion	strength
s0	We produce the open strings on $\mathbb{R}\times S^{2}$ that correspond to the solutions of integrable boundary sine-Gordon theory by making use of the $N$-magnon solutions provided in \cite{KPV} together with explicit moduli.	contribution 0.60	0.92	0.16	asserted 1.00
s1	Relating the two boundary parameters in a special way we describe the scattering of giant magnons with non-maximal $Y=0$ giant gravitons and calculate the leading contribution to the associated magnon scattering phase.	contribution 0.65	0.94	0.50	asserted 1.00

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The paper

Original abstract

We produce the open strings on $\mathbb{R}\times S^{2}$ that correspond to the solutions of integrable boundary sine-Gordon theory by making use of the $N$-magnon solutions provided in \cite{KPV} together with explicit moduli. Relating the two boundary parameters in a special way we describe the scattering of giant magnons with non-maximal $Y=0$ giant gravitons and calculate the leading contribution to the associated magnon scattering phase.

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1 arXiv paper cite this in 2 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

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We produce the open strings on $ℝ×S^2$ that correspond to the solutions of integrable boundary sine-Gordon theory by making use of the $N$-magnon solutions provided in [ref] together with explicit moduli.

Exact solutions for N-magnon scattering · Introduction · 0.80

Uses data or values from 1 paper

The leading contribution to the magnon boundary scattering phase as calculated in [ref] is δ_B^Max Z=0=-4gcosp/2ln{cosp/2(1-sinp/2/1+sinp/2)}.

Reflecting magnons · Scattering with maximal $Z=0$ and $Y=0$ giant gravitons · 0.85

Cites as background 7 papers

We follow Hofman and Maldacena's convention [ref] of taking the large angular momentum possessed by the strings and branes to be in the ${X_5,X_6}$ direction and hence referring to the physically distinct orientations of the branes as either $Y=0$ or $Z=0$.

Reflecting magnons · Scattering giant magnons off giant gravitons and semi-classical phase shifts · 0.80
Sine-Gordon theory for a single scalar field $φ(x,t)∈ℝ$ may be defined on the half-line [ref] while preserving its integrability, i.e. conserving an infinite number of constants of motion and $N$-soliton solutions.

The boundary sine-Gordon theory: classical and semi-classical analysis · Boundary sine-Gordon theory · 0.89
Giant gravitons [ref] are stable but finite energy D-branes on the $AdS_5×S^5$ background that may act as end points for the open strings that emerge as their excitations [ref] .

Open Strings from N=4 Super Yang-Mills · Introduction · 0.98

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