0107126v3[1] dilaton spacetimes with a liouville potential(christos charmousis)

0107126v3[1] dilaton spacetimes with a liouville potential(christos charmousis)

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1、UFIFT-HEP-01-10DilatonspacetimeswithaLiouvillepotentialChristosCharmousis∗†InstituteforFundamentalTheoryDepartmentofPhysics,UniversityofFloridaGainesvilleFL32611-8440,USA(February1,2008)AbstractWefindandstudysolutionstotheEinsteinequationsinDdimensionscou-pledtoascalarfieldsource

2、withaLiouvillepotentialundertheassumptionofD−2planarsymmetry.Thegeneralstaticortime-dependentsolutionsarefoundyieldingthreeclassesofSO(D−2)symmetricspacetimes.InD=4homogeneousandisotropicsubsetsofthesesolutionsyieldplanarscalarfieldcosmologies.InD=5theyrepresentthegeneralstatico

3、rtime-dependentbackgroundsforadilatonicwall-typebraneUniverseofplanarcosmologicalsymmetry.HereweapplythesesolutionsasSO(8)symmetricbackgroundstonon-supersymmetric10dimensionalstringtheories,theopenUSp(32)typeIstringandtheheteroticstringSO(16)×SO(16).WeobtainthegeneralSO(9)solut

4、ionsasaparticularcase.Allstaticsolutionsarefoundtobesin-gularwiththesingularitysometimeshiddenbyahorizon.Thesolutionsarenotasymptoticallyflatorofconstantcurvature.Thesingularbehaviorisnolongertrueoncewepermitspaceandtimedependenceofthespacetimemet-ricmuchlikethickdomainwallorglo

5、balvortexspacetimes.WeanalyzethearXiv:hep-th/0107126v35Nov2001generaltimeandspacedependentsolutionsgivingimplicitlyaclassoftimeandspacedependentsolutionsanddescribethebreakdownofanextensiontoBirkhoff’stheoreminthepresenceofscalarmatter.Wearguethatthesolutionsdescribedconstitutet

6、hegeneralsolutiontothefieldconfigurationunderD−2planarsymmetry.I.INTRODUCTIONThedimensionalnatureofthemanifoldweliveinhasbeenanintriguingquestionformathematiciansandphysicistsalikeinthepastcentury.Minkowskimadethefirstcrucialstep[1]inthisdirectionintroducingtimeaspartofa4dimension

7、alspace-timemanifold.Of∗E-mailaddress:charmousis@phys.ufl.edu†Actualaddress:LPT,Universit´edeParisSud,Bˆat.210,91405OrsayCEDEX,France1coursetime,ateverydaylowvelocities,isnotperceivedasacoordinate,however,ataccel-eratorvelocitiesclosetothespeedoflight,timeandlengthcanvary,thepre

8、factorc2actingasadimensional‘warp-like’factorinEinstei

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