2004
DOI: 10.1016/j.nuclphysb.2004.04.022
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Zero-norm states and high-energy symmetries of string theory

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Cited by 52 publications
(192 citation statements)
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“…On the contrary, for the high energy scatterings of the compactified closed string considered in this paper, one gets more kinematic variables, namely ( m R , 1 2 nR), to cover both GR and MR, so that one can see this interesting transition. Through the observation of this transition, one further confirms that the infinite linear relations obtained in [4,5,6,7,8,9,10,11] are responsible for the UV softer string scattering amplitudes than the field theory scatterings.…”
Section: Discussionsupporting
confidence: 52%
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“…On the contrary, for the high energy scatterings of the compactified closed string considered in this paper, one gets more kinematic variables, namely ( m R , 1 2 nR), to cover both GR and MR, so that one can see this interesting transition. Through the observation of this transition, one further confirms that the infinite linear relations obtained in [4,5,6,7,8,9,10,11] are responsible for the UV softer string scattering amplitudes than the field theory scatterings.…”
Section: Discussionsupporting
confidence: 52%
“…This is physically consistent as one expects a m R , 1 2 nR dependent Regge-pole and zero structures in the high energy string scattering amplitudes. In conclusion, in the GR, Presumably, the infinite linear relations obtained above can be reproduced by using the method of high energy ZNS, or high energy Ward identities, adopted in the previous works [4,5,6,7,8,9,10,11]. The existence of Soliton ZNS at arbitrary mass levels was constructed in [22].…”
Section: B the Infinite Linear Relations In The Grmentioning
confidence: 81%
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“…Recently high-energy, fixed-angle behavior of string scattering amplitudes [1,2,3] was intensively reinvestigated [4,5,6,7,8,9,10]. The motivation was to uncover the long-sought hidden stringy space-time symmetry.…”
Section: Introductionmentioning
confidence: 99%
“…However, a simple calculation shows that T 4 LLL = T 4 LT T = T 4 (LL) = 0.So the real leading order amplitudes correspond to E 3 , which appear in eqs. (10), (12) and (14). A simple calculation shows that…”
mentioning
confidence: 99%