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Bosonic Fractionalisation Transitions
High Energy Physics - Theory · Submitted 15 Aug 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Using a minimal bottom-up model we exhibit phase transitions between the two cases, under the influence of a relevant operator in the dual field theory.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
At finite density, charge in holographic systems can be sourced either by explicit matter sources in the bulk or by bulk horizons. In this paper we find bosonic solutions of both types, breaking a global U(1) symmetry in the former case and leaving it unbroken in the latter. Using a minimal bottom-up model we exhibit phase transitions between the two cases, under the influence of a relevant operator in the dual field theory. We also embed solutions and transitions of this type in M-theory, where, holding the theory at constant chemical potential, the cohesive phase is connected to a neutral phase of Schr\"odinger type via a z=2 QCP.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | At finite density, charge in holographic systems can be sourced either by explicit matter sources in the bulk or by bulk horizons. | background 1.00 | 0.05 | 0.03 | asserted 0.84 |
| s1 | In this paper we find bosonic solutions of both types, breaking a global U(1) symmetry in the former case and leaving it unbroken in the latter. | result 0.85 | 0.96 | 0.31 | asserted 1.00 |
| s2 | Using a minimal bottom-up model we exhibit phase transitions between the two cases, under the influence of a relevant operator in the dual field theory. | contribution 0.50 | 0.96 | 0.31 | asserted 1.00 |
| s3 | We also embed solutions and transitions of this type in M-theory, where, holding the theory at constant chemical potential, the cohesive phase is connected to a neutral phase of Schr\"odinger type via a z=2 QCP. | result 0.77 | 0.90 | 0.23 | asserted 1.00 |
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The paper
Original abstract
At finite density, charge in holographic systems can be sourced either by explicit matter sources in the bulk or by bulk horizons. In this paper we find bosonic solutions of both types, breaking a global U(1) symmetry in the former case and leaving it unbroken in the latter. Using a minimal bottom-up model we exhibit phase transitions between the two cases, under the influence of a relevant operator in the dual field theory. We also embed solutions and transitions of this type in M-theory, where, holding the theory at constant chemical potential, the cohesive phase is connected to a neutral phase of Schr\"odinger type via a z=2 QCP.
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References
How the literature uses it
7 arXiv papers cite this in 16 sentences
Papers citing it · 9 sentences without a confident label
Builds on it 1 paper
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In Appendix [ref], we extend this analysis to include groundstates which feature hyperscaling violation [ref] as well as cases with novel superfluid actions.[An analytic top-down solution featuring hyperscaling violation in the normal state can be found in [ref] .] $$
Non-vanishing normal density in cold holographic superfluids · Introduction and results · 0.94
Compares with it 1 paper
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Another related work [ref] considers also a competition between fractionalization and superconductivity, but with a bulk system consisting of a charged scalar and a neutral one (a dilaton).
Dressing the Electron Star in a Holographic Superconductor · Introduction · 0.93
Cites it as background 4 papers
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The phase transition corresponding to the onset of fractionalization was studied in [ref] .
Polarized solutions and Fermi surfaces in holographic Bose-Fermi systems · Introduction · 0.85
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We refer the reader to e.g. [ref] for various properties of these geometries, and attempts to classify the corresponding phases.
Spatially Modulated Instabilities of Geometries with Hyperscaling Violation · Introduction · 1.00
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Our results shed new light on the relation between charge densities in the boundary theory and in the bulk, various aspects of which have been explored in previous literature [ref] .
Non-vanishing normal density in cold holographic superfluids · Introduction and results · 1.00
What it cites · 51 sentences without a confident label
Builds on 1 paper
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In this work we explore bosonic analogues of the fractionalisation transition of [ref] , corresponding to transitions from phases with broken U(1) symmetry to phases with intact U(1) symmetry and all charge associated with a horizon.
Fractionalization of holographic Fermi surfaces · Introduction · 0.98
Uses the method or tool of 2 papers
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Using techniques of [ref] one can show that this is the negative of the pressure ω(μ,T)=-P .
A gravity derivation of the Tisza-Landau Model in AdS/CFT · Thermodynamic Relations · 0.99
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Using techniques of [ref] one can show that this is the negative of the pressure ω(μ,T)=-P .
A theory of first order dissipative superfluid dynamics · Thermodynamic Relations · 0.99
Compares with 2 papers
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Both these results can be compared to the case of fermionic fractionalisation transitions [ref] , where the roles are reversed.
Fractionalization of holographic Fermi surfaces · The Fractionalisation Transition · 1.00
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A similar structure was seen in the zero-temperature superconducting solutions of [ref] .
Zero Temperature Limit of Holographic Superconductors · Cohesive IR Solution · 1.00
Cites as support 1 paper
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This point of view has recently been bolstered by the identification of the corresponding $2k_F$ singularities associated with the `hidden' fermionic degrees of freedom by Faulkner and Iqbal [ref] .
Friedel oscillations and horizon charge in 1D holographic liquids · Introduction · 0.98
Cites as background 21 papers
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Lately such questions have attracted a great deal of interest leading to general statements along the lines of a holographic Luttinger relation and its bosonic analogue [ref] .
Fermi surfaces and gauge-gravity duality · Introduction · 0.96
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Lately such questions have attracted a great deal of interest leading to general statements along the lines of a holographic Luttinger relation and its bosonic analogue [ref] .
Fractionalization of holographic Fermi surfaces · Introduction · 0.96
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Lately such questions have attracted a great deal of interest leading to general statements along the lines of a holographic Luttinger relation and its bosonic analogue [ref] .
Luttinger's theorem, superfluid vortices, and holography · Introduction · 0.96
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