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Holography in the Penrose limit of AdS space
High Energy Physics - Theory · Submitted 30 May 2002
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Even though there is no holographic principle, we construct a ``holographic screen'' on which information on the corresponding CFT is encoded.
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The abstract, sentence by sentence
We discuss the Penrose limit of pure AdS space, which is flat Minkowski space. Even though there is no holographic principle, we construct a ``holographic screen'' on which information on the corresponding CFT is encoded. The screen is obtained as a gauge-fixing condition upon restricting the Hilbert space to the states that are annihilated by the generator of scale transformations. This constraint leads to Dirac brackets which turn the Poincare algebra into the algebra of the conformal group on the ``holographic screen.''
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We discuss the Penrose limit of pure AdS space, which is flat Minkowski space. | background 0.93 | 0.24 | 0.07 | asserted 1.00 |
| s1 | Even though there is no holographic principle, we construct a ``holographic screen'' on which information on the corresponding CFT is encoded. | contribution 0.98 | 0.92 | 0.53 | asserted 1.00 |
| s2 | The screen is obtained as a gauge-fixing condition upon restricting the Hilbert space to the states that are annihilated by the generator of scale transformations. | method 0.94 | 0.84 | 0.13 | asserted 1.00 |
| s3 | This constraint leads to Dirac brackets which turn the Poincare algebra into the algebra of the conformal group on the ``holographic screen.'' | result 0.95 | 0.84 | 0.29 | asserted 1.00 |
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Original abstract
We discuss the Penrose limit of pure AdS space, which is flat Minkowski space. Even though there is no holographic principle, we construct a ``holographic screen'' on which information on the corresponding CFT is encoded. The screen is obtained as a gauge-fixing condition upon restricting the Hilbert space to the states that are annihilated by the generator of scale transformations. This constraint leads to Dirac brackets which turn the Poincare algebra into the algebra of the conformal group on the ``holographic screen.''
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