40
USTC, March 18 Cosmology, Imaginary Black Holes, Extra Dimensions 1 Cosmology, Imaginary Black Holes and Extra Dimensions John Wang @USTC-ICTS on March 18 2005

Dimensions Extra and - icts.ustc.edu.cn

  • Upload
    others

  • View
    3

  • Download
    0

Embed Size (px)

Citation preview

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions1

'

&

$

%

Cosmology,ImaginaryBlackHoles

andExtraDimensions

JohnWang@USTC-ICTSonMarch182005

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions2

'

&

$

%

Outline

·QuickSummaryofResults

·StandardModel,Cosmology:ComparingTheoryversusExperiments

·ExtraDimensions,ImaginaryBlackHolesandStringFormation

Mostrelevantreferences

·C-MChen,P-MHo,I.NeupaneandJ.E.Wang,JHEP,

hep-th/0304177

·G.C.JonesandJ.E.Wang,PRDhep-th/0409070

·K.Hashimoto,P-MHoandJ.E.Wang,Phys.Rev.Lett.,

hep-th/0211090

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions3

'

&

$

%

zoom in

our

universe

our

universe

USTC

PhysicsExtra

Dims

time T

iT

EE

Recentprojectsinclude-1)extradimensionscandrivecosmic

acceleration2)Imaginaryblackholesareconsistentandrelatedtode

Sitterspace3)cosmicstringnucleationcanbesmoothlydescribed

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions4

'

&

$

%

Inthe1980’sand1990’sthegrowingaccumulationoflaboratorydata

supportedthenowstandardmodelofgaugeinteractions

SU(3)×SU(2)×U(1)plusgravity.Allobservableandtestable

phenomenonseemedtofit.

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions5

'

&

$

%

ConceivablytheSMwouldcontinuetobeexplainallphysicsuptoat

least1013

GeVwherethegaugecouplingsappeartounify.Suchnew

highenergyphysicsrelatedtograndunifiedtheories,superstringsor

somethingelsemightneverbeseen.

log E (GeV)

20

40

20 1015 5

α

α

α α1

1

1

1

1

2

3−

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions6

'

&

$

%

However...

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions7

'

&

$

%

Inspiteofthesesuccesses,thereappearstobegrowingevidencefora

potentialREVOLUTIONinphysics!

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions8

'

&

$

%

Thisnewmysteriousphysicshasbeennameddarkmatterand

darkenergy.

Wecanexplainearthboundphysicsinacceleratorsandlaboratories,

butunderstandingcosmologicalphenomenaappearstorequirea

changeinourbasicsconceptsofphysics!

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions9

'

&

$

%

Recentobservationshowasurprisingaccelerationtoouruniverseon

thelargestscales.Notonlyisouruniverseexpandingbutitis

undergoingacceleratedexpansion!Darkenergyisthetermusedto

describetheapparentcosmologicalacceleration.Cosmologistsobserve

thatthestarsinouruniversearenotonlymovingawayfromusbut

doingsoateverincreasingspeeds!

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions10

'

&

$

%

Gravityisanattractiveforceandsoourexpectationisthattheremust

beanenergysourcetoaccelerateobjectsawayfromeachotherinour

universe.

Howthendoweexplainthisdarkenergy?

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions11

'

&

$

%

StandardCosmology

Toattempttoanswerthisquestionletmebemoreconcreteand

discussthestatusofcosmologyandtheunderlyingobservational

assumptions.

Overlargescalescoveringmanygalaxies,itappearsthatouruniverse

isapproximatelyuniform.Thedensityofstars(andplanets)isroughly

thesameeverywhere.

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions12

'

&

$

%

Asanapproximationletustakeourmodeloftheuniversetobe

exactlyuniform.Thisiswhatiscalleda

F(riedman)R(oberston)W(alker)universespecifiedinEinstein’s

languagebyametric

ds2

=−dt2

+1×

[

dr2

+r2(dθ

2+sin

2θdφ

2)]

(1)

ds2FRW=−dt

2+a

2(t)

[

dr2

1−kr2+r2(dθ

2+sin

2θdφ

2)]

(2)

S=

d4xR(3)

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions13

'

&

$

%

Astimepasses,theuniverseexpandsandhastwopossiblefates.Itcan

eitherexpandateverslowerratesorcollapseinabigcrunch.

big bang

big crunch

big bang

universe expands forever

FRWisnotourpresentuniverse!

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions14

'

&

$

%

Einsteingravityalsoallowsfortheadditionofwhatiscalleda

cosmologicalconstantΛ.

S=

d4x(R+Λ)(4)

Thistermcanbeaddedwithoutspoilingthetheoreticalconsistencyof

theequations.Physicallythistermcanariseduetothevacuumenergy

ofvariousfields,iezeropointenergy.

Apositivecosmologicalconstantcausesspacetimetoexpand,

counteractingtheusualgravitybetweenmasses.

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions15

'

&

$

%

Ahomogeneousuniversewithapositivecosmologicalconstantis

calleddeSitterspace

ds2

=−dt2

+cosh2t[

dθ2

+sin2θdφ

2+cos

2θdψ

2]

(5)

Time

Recentaccelerationobservationscombinedwiththeapparent

uniformityofouruniverseshowouruniverseisapproximatelydeSitter.

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions16

'

&

$

%

Theproblemisthatouruniverse’scurrentwouldbecosmological

constantisabout(10−3eV)

4whichisaverysmall.Howdoweexplain

suchasmallnumberwhenourscalesinphysicsaretypicallymuch

larger?Thisisthesocalledcosmologicalconstantproblem.

Onesuggestionisthattheaccelerationisnotcausedbyacosmological

constantbutbysomethingwhichonlyactssimilarlytoit.Our

accelerationmightbemoreeasilyexplainedinthismanner.

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions17

'

&

$

%

Letusattackthesenewopenproblemsfromcosmology!

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions18

'

&

$

%

Therehavebeenmanyproposalstoexplainwhatdarkenergymight

be.Almostalloftheseproposalsareessentiallyguessesinthatthey

introducenewphysicalinteractions(=fields).

·inflatons,phantommatter,tachyonmatter,ghosts

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions19

'

&

$

%

Canweestablishwhatdarkenergyanddarkmatterarewithless

guessing?

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions20

'

&

$

%

Oneapproachistotrytostartwiththestringtheorywhichbeganasa

theoryforstronginteractionsandevolvedtoatheoryencompassing

gaugeinteractions,gravityandquantummechanics!

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions21

'

&

$

%

ExtraDimensions:

Asacandidatetheoryofouruniverse,canstringtheoryprovideus

withasensiblesourceofdarkenergy?

Toanswerthisquestionitisimportanttoknowwhatisdifferentor

newaboutstringtheory.Onerelevantfactaboutstringtheoryisthat

itrequires10dimensionsforspaceandtime!

Howdowedealwiththefactthatouruniversehasfourapparent

dimensions?

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions22

'

&

$

%

Oneideaistodividethetendimensionsofstringtheoryintolargefour

dimensionsandsixsmalldimensions.

zoom in

our

universe

our

universe

USTC

PhysicsExtra

Dims

Despitetheirsmallsize,sincestringtheoryhasextradimensions,my

collaboratorsandIcheckedtoseeiftheyarerelevanttocosmology.

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions23

'

&

$

%

Wefoundthatevensmalldimensionscanaccelerateourlarge

dimensions!ThisissurprisingsinceweearliersaidthatwithoutΛ

thereisnoacceleration.

Speciallychosentimedependentextradimensionsprovideenergyas

seenbythelargefourdimensions.

USTC

Physics

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions24

'

&

$

%

WeexaminedthespacetimesolutionofEinsteingravity

R1,3

×H6(6)

ds2

=α2(t)

[

−a6(t)dt

2+a

2(t)dx

23

]

+α−2/3

(t)[

dψ2+sinh

2ψdΩ

25

]

(7)

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions25

'

&

$

%

Dimensionallyreducethistofourdimensionstofindthespacetimeas

seenbythefourdimensionalobservers,us!

S=

d4x[R−(∂φ)

2−15e

3φ/8]∼

d4x[R−Λ(=15e

3φ/8)](8)

Thisisgravityandascalartheorywhichproducesaccelerationwhen

∂φ∼0.Toafourdimensionalobserver,extradimensionsactlikea

scalarfield.

Infactasopposedtomorephenomenologicalmodels,theinflatonhere

isnotarbitrarybutdeterminedbygravity!

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions26

'

&

$

%

ImaginaryBlackHoles:

Blackholesarecrazy,interestingandhavebeenextremelyusefulin

betterunderstandingquantumgravity!Theyarefascinatingandtoday

Ihavethepleasuretodiscussaninterestingtwistontheusualstory

andwilldescribetheirapplicationinanewsetting.

ThepointIwishtogetacrossisthatthereisanaturalconceptof

imaginaryblackholeswhichisconsistent,hasusefulapplicationsand

afterthistalkIhopeyouwillagreethattheyarenotsostrange!

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions27

'

&

$

%

BeforegoingintodetailsIwanttosummarizemymainpoint.

Imaginaryblackholesareblackholesplacedatimaginarycoordinate

valuesforexampleimaginarytime.Theyproducetimedependent

spacetimeswithinterestingproperties.

time T

iT

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions28

'

&

$

%

Ablackholeisthespacetimecreatedbyapoint-likesourcewithmass.

Farawayfromthissourcethenwearemovearoundaswewantbutif

wepasstheblackholehorizonthenwearedoomed!

ThesimplestSchwarzschildblackholesolutionis

ds2BH=−(1−

2M

r)dt

2+

dr2

1−2Mr

+r2(dθ

2+sin

2θdφ

2)(9)

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions29

'

&

$

%

Howeverletusstripawayallthesecomplexitiesofblackholeslike

theirnon-linearity,horizonstructure.Thisisacomplexityofthe

Einsteinaction.Wewanttojustdealwiththeessenceofablackhole

whichisitsmassivepoint-likeobjectsourcewhichwecanmove

aroundinspace.

x

y

z

mass

source

t=time

r=space

Notewehavespacetimenotspaceandthesourceexistsforalltime.

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions30

'

&

$

%

Thefourrealcoordinatesofouruniversearet,x,y,z.Weliveinthe

“real”worldBUTwhataboutmovingsourcesincomplexcoordinates?

real coordinate T

imaginary

coordinate iT

Inotherwordswhilebeforewediscussedmovingtheblackholesource

inrealvalueofspacetime,nowwemovetheblackholesourceinto

complexvaluesofspacetime.Hencetheseareimaginaryblackholes.

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions31

'

&

$

%

Tocreatearealsourceweaddingtwocomplexsources,

z+z∗

=(x+iy)+(x−iy)∈Rforallz∈C.

BHsourceδ(√

x2+y2+z2)

ImagBHsourceδ(√

x2+y2−(t−it0)2)+δ(√

x2+y2−(t+it0)2)

(10)

Taketheblackholesourceand1)rotateitsoitisnowextendedina

spatialdirectionandnottime2)moveitfromtheorigininpairs

it

z

t

it -it0 0

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions32

'

&

$

%

ds2

=(1−2Mt

Σ)2[

(dx4)2

4

(∆+(a2−M2)sinh2θ)3(−

dt2

∆+dθ

2)]

+∆sinh

(1−2MtΣ)2dφ

2

A=2aMtsinh

∆+a2sinh2θdφ

∆=t2−2Mt+a

2,Σ=t

2+a

2cosh

time

space

dS structure

dS structure

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions33

'

&

$

%

ImaginaryblackholessourceafibereddeSitterwithoutrelyingona

cosmologicalconstant!Thisnewresultmayextendfieldtheory/string

theorydualitiestotimedependentsystems.

ds2

=((M2−a

2)cosh

2η+a

2sinh

2η)

2(

σ2(dx

4)2

Σ2+

2+

(M2−a2)3(−dσ2/4σ

2+dη

2))

+(M

2−a

2)Σ

2+cosh

2ηsinh

2ηdφ

2

((M2−a2)cosh2η+a2sinh

2η)2,

A=2aMt

KH+dφ

a2+(M2−a2)coth2η

Σ+=(tKH+)

2+a

2.FiberingofdS2overtheηdirectionforη≥0.

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions34

'

&

$

%

String/defectformation:Pointlikeobjectssuchasblackholes,or

spatiallyextendedobjectslikemassivestrings,canformintheearly

universeduetotheuniverse’ssmallsizeandhencehighenergies.

Insometheories,stringsariseasconfinedfluxtubes.Isthispossible

eveninstringtheorywherethefundamentalobjectsarestrings?YES!

Ifwehavedefects,howdoweseetheirformation?

GenericInitialConditions

T=0Sbraneshaveappeared

late timeremnants

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions35

'

&

$

%

First,astringisaonedimensionalspatialobject.Toformastringwe

needtostartfromsomeotherobjectwhichissimilartoastring.In

otherwordsweneedthecorrectinitialconditions.

Asimplestartingpointforexampleisacylindricaltube.Ifthesizeof

thetubecollapsesthenwewillformastring.

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions36

'

&

$

%

Startingfromstringtheory,wederivedanactiontodescribehowto

interpolatebetweentheinitialconditionsandthefinalstrings/defect.

Wealsofoundanalyticsolutionswhichdescribehowfluxtubesform

intostrings.

S=S0

d3+1

x√

det(δij−∂it∂jt+Fij)(11)

Forexamplethisistheactionforacylinderwith3+1worldvolume

dimensions,locatedatpositionsxiandwithFijfieldstrengthie

electricandmagneticfields.

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions37

'

&

$

%

Searchingforinterestingsolutionswefoundthoserepresentingtime

dependentcollapseoftubesofelectricfluxintothinlines.

EE

r=c

tE=1=criticalvalue(12)

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions38

'

&

$

%

Theformationofsuchobjects,whichtypicallyarecalledtopological

defects,hasbeenstudiedbeforealthoughwithtwodifficulties.

Beforesolutionswereeithernumericalorcollapsedinfinitetimesothe

solutionscouldnotbetrustedatthecollapseddegeneratepoint.This

isthefirsttimeananalyticandnon-singularsolutionhasbeenfound!

Whatisperhapsmostamazingisthatwearedescribingtheformation

ofstringsinastringtheory!

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions39

'

&

$

%

Summary

·Lotsofunexplainedphenomenon

·Extradimensionscanberelatedtocosmicacceleration

·Imaginaryblackholesmakesense!andhavedeSitterusestoo

·Newnon-singulartimedependentsolutionsdescribingstring

formation

USTC,March18Cosmology,ImaginaryBlackHoles,ExtraDimensions40

'

&

$

%

Thanksfortheinvitation!