1 | For simplicity we take ![]() |
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2 | This suppression only occurs if at least one angular momentum on the five sphere becomes large. If this is not the case,
e.g. for a spinning string purely on the ![]() ![]() |
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3 | This metric arises from a parameterization of the five sphere ![]() ![]() ![]() ![]() ![]() ![]() ![]() |
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4 | The case ![]() |
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5 | Our conventions are (![]() ![]() |
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6 | For a nice and detailed review on this topic see [73![]() |
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7 | ![]() |
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8 | Our convention is ![]() |
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9 | We are actually using a slightly modified definition of these functions (compared to the one presented in [109]) which was considered in [58]. | |
10 | The full conjecture for all the higher charge densities ![]() |
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http://www.livingreviews.org/lrr-2005-9 |
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