3 research outputs found

    The AdS/CFT/Unparticle Correspondence

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    We examine the correspondence between the anti-de Sitter (AdS) description of conformal field theories (CFTs) and the unparticle description of CFTs. We show how unparticle actions are equivalent to holographic boundary actions for fields in AdS, and how massive unparticles provide a new type of infrared cutoff that can be simply implemented in AdS by a soft breaking of conformal symmetry. We also show that processes involving scalar unparticles with dimensions d_s<2 or fermion unparticles with dimensions d_f<5/2 are insensitive to ultraviolet cutoff effects. Finally we show that gauge interactions for unparticles can be described by bulk gauge interactions in AdS and that they correspond to minimal gauging of the non-local effective action, and we compute the fermion unparticle production cross-section.Comment: 26 pages, 1 figur

    Constraints on Astro-unparticle Physics from SN 1987A

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    SN 1987A observations have been used to place constraints on the interactions between standard model particles and unparticles. In this study we calculate the energy loss from the supernovae core through scalar, pseudo scalar, vector, pseudo vector unparticle emission from nuclear bremsstrahlung for degenerate nuclear matter interacting through one pion exchange. In order to examine the constraints on dU=1d_{\cal U}=1 we considered the emission of scalar, pseudo scalar, vector, pseudo vector and tensor through the pair annihilation process e+e−→Uγe^+e^-\to {\cal U} \gamma . In addition we have re-examined other pair annihilation processes. The most stringent bounds on the dimensionless coupling constants for dU=1d_{\cal U} =1 and ΛU=mZ\Lambda_{\cal U}= m_Z are obtained from nuclear bremsstrahlung process for the pseudo scalar and pseudo-vector couplings ∣λ0,1P∣≤4×10−11\bigl|\lambda^{\cal P}_{0,1}\bigr|\leq 4\times 10^{-11} and for tensor interaction, the best limit on dimensionless coupling is obtained from e+e−→Uγe^+ e^-\to {\cal U} \gamma and we get ∣λT∣≤6×10−6\bigl|\lambda^{\cal T}\bigr| \leq 6\times 10^{-6}.Comment: 12 pages, 2 postscript figure
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