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Selected: E

E11 and Supersymmetry

Physics – High Energy Physics – High Energy Physics - Theory
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E11 as E10 representation at low levels

Physics – High Energy Physics – High Energy Physics - Theory
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E11, generalised space-time and IIA string theory

Physics – High Energy Physics – High Energy Physics - Theory
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E11, generalised space-time and IIA string theory; the R-R sector

Physics – High Energy Physics – High Energy Physics - Theory
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E2 and C2 amplitudes for electroproduction of $Δ$

Physics – High Energy Physics – High Energy Physics - Phenomenology
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E2 and M1 strengths in heavy deformed nuclei

Physics – Nuclear Physics – Nuclear Theory
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E2 component in subcoulomb breakup of ^{8}B

Physics – Nuclear Physics – Nuclear Theory
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E2 Instanton Effects and Higgs Physics In Intersecting Brane Models

Physics – High Energy Physics – High Energy Physics - Theory
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E2 properties of nuclei far from stability and the proton-halo problem of 8B

Physics – Nuclear Physics – Nuclear Theory
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E2 Strength in the Radiative Charmed Baryon Decay

Physics – High Energy Physics – High Energy Physics - Phenomenology
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E2 transitions in Ti XII. Relativistic calculations

Physics
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E2/M1 Mixing Ratio of $Δ\to Nγ$ and Hyperon Resonance Radiative Decay

Physics – High Energy Physics – High Energy Physics - Phenomenology
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E2/M1 ratio from the Mainz $p(\vec γ, p)π^0$ data

Physics – Nuclear Physics – Nuclear Theory
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E2/M1 ratio from the Mainz $p(\vecγ, p)π^0$

Physics – Nuclear Physics – Nuclear Theory
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E3-brane instantons and baryonic operators for D3-branes on toric singularities

Physics – High Energy Physics – High Energy Physics - Theory
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E3200PH

Physics
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E4015WH

Physics
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E4015WH2

Physics
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E4179TOU

Physics
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E4197

Physics
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