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85037243660
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Although singular solutions in the two conformal frames are not necessarily equivalent owing to the possibility of a singularity residing in the conformal rescaling (scalar field), solutions will map onto each other provided that they have a regular horizon and are asymptotically flat, which we assume here
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Although singular solutions in the two conformal frames are not necessarily equivalent owing to the possibility of a singularity residing in the conformal rescaling (scalar field), solutions will map onto each other provided that they have a regular horizon and are asymptotically flat, which we assume here.
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55
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85037213321
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Similar phenomena can be seen in the cosmic string. There exist string solution and the Melvin solution under some value of (Formula presented). As (Formula presented) gets larger, both solution approaches each other. When it reaches critical value for which the deficit angle becomes (Formula presented), there exists only cylindrical solution
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Similar phenomena can be seen in the cosmic string. There exist string solution and the Melvin solution under some value of (Formula presented). As (Formula presented) gets larger, both solution approaches each other. When it reaches critical value for which the deficit angle becomes (Formula presented), there exists only cylindrical solution 32.
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57
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85037185413
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For the very large value of (Formula presented), it is discussed in Ref
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For the very large value of (Formula presented), it is discussed in Ref. 34 that there appears a second minimum for (Formula presented) inside a first minimum near the (Formula presented) As (Formula presented) increase, the outer minimum moves upward, while the inner minimum downward.
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60
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0032327454
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O. Dando, gr-qc/9904058.
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Dando, O.1
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69
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85037179097
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The precise diagram is given in Ref
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The precise diagram is given in Ref. 11.
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74
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85037196947
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It was shown that gravitational mass in the Einstein frame satisfy the first law of black hole thermodynamics
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It was shown that gravitational mass in the Einstein frame satisfy the first law of black hole thermodynamics 44.
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