2004
DOI: 10.1140/epjc/s2004-01865-6
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Charged tensor matter fields and Lorentz symmetry violation via spontaneous symmetry breaking

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Cited by 19 publications
(13 citation statements)
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“…In this paper, which is part of a program started in a previous work [31], we propose to formulate and analyze the simple dynamics of chargeless vector matter field in a supersymmetric scenario. There are three motivation for this proposal: the lack of this approach in the literature; to get a clue on the possibility of Lorentz symmetry violation in supersymmetric theories; and the role played by the simplest case of high-spin field in field and string theories.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…In this paper, which is part of a program started in a previous work [31], we propose to formulate and analyze the simple dynamics of chargeless vector matter field in a supersymmetric scenario. There are three motivation for this proposal: the lack of this approach in the literature; to get a clue on the possibility of Lorentz symmetry violation in supersymmetric theories; and the role played by the simplest case of high-spin field in field and string theories.…”
Section: Discussionmentioning
confidence: 99%
“…so the complex scalar fields d(x), f (x) and l(x) have no dynamics and arise as auxiliary fields. Thus assuming the action (27) as the sum of the redefined actions (30) and (31) and rearranging 1 the (Dirac) spinor fields Θ and Π it results in an off-shell action S os written in the following form…”
Section: The Chargeless Complex Vector Matter Superfield Modelmentioning
confidence: 99%
“…The overall general behavior is again observed to be qualitatively similar to that found in the case of the flat UED scenario as we see in figure 2. The above analyses for the scalar and vector fields can be immediately extended to the case of bulk fermions which are now described by the action 14) with k Ψ being the fermionic LIV parameter and V a n being the appropriate vielbein. Note that in the presence of LIV, Ψ effectively feels g 55 = 1 + k Ψ .…”
Section: With Sm Fields In the Rs Bulkmentioning
confidence: 99%
“…In such theories it is possible for LIV to manifest itself in many ways, e.g., (i) particles of various spins and flavors may have different dispersion relations correlating their mass, energy and momentum [4][5][6][7] or (ii) the general Poincare algebra itself may be deformed as in Doubly Special Relativity (for a general discussion, see [8][9][10]) such that the Planck mass is left as an invariant quantity. One way of generating LIV is through the vacuum expectation value (vev) of a tensor, usually a 4-vector, which points in a specific direction in a preferred reference frame, i.e., via spontaneous symmetry breaking [11][12][13][14][15][16]. If one imagines that maintaining rotational invariance is more sacrosanct than is boost invariance then the vev may take the time-like form ∼ (v, 0, 0, 0) in such a frame.…”
Section: Introductionmentioning
confidence: 99%
“…Recent theoretical efforts allow for small Lorentz violations, see, e.g., [1][2][3][4][5][6]. For example, Doppler shift experiments such as the Ives-Stillwell experiment are sensitive to Lorentz violating terms in standard model extension [1,2].…”
Section: Introductionmentioning
confidence: 99%