Sothesethreepossibilitiesareallbeingactivelypursued, a zawayofunderstandingtheobservationthattheuniverseisacceleratingtodayand I'vebeeninvolvedin a kindofallthreeofthemtryingtocomeupwithmodelswhichtryandmimicthese.
Weknowthattherearethatgalaxyis a kindofclusteredtogetheroninfilamentsonthosefilamentskindofsurroundvoid, sovoicewherethereislowerdensitythanontheaverage.
Butthethoughtisthatasyougettobiggerandbiggerscalesintheuniverse, thatthatthedistributionofthosevoicebecomes a bitmoreuniformsAnditherethattheireffectdropsoff, givingyouthisnethomogeneity.
Andifit's inhomogeneous, thenandwehappentobelivingin a voidin a regionthat's gottalowerdensitythanonaveragethanwewouldactuallyperceivetheuniversetobeexpandingat a differentratefromoutsideon, itcouldbethatthat's whatwe'reseeinghere, thattheeffectofthisaccelerationis, andthat's whatanaccelerationis.
You'reseeing a differentratehere, comparedtohereontheeffectsoftheexplosionisjustthat.
Soit's kindofbeingit's underunderthreat a CZ a model, butithasn't beenruledoutyet, butit's certainlyveryfinetunedififunderthetheoryof I knowtherearealwayspossiblewascauseifitisthecliche, darkenergyisthis, likesomekindofparticleorfieldthatcanbemeasuredisthatisthatthingisthethingwithmassornomasshas a coreenergythatcanbemeasuredinjewels.
Maura's thislikeit's darkandyoujustfeellike I shall I getmycupofgetmycuptoshowyouthehowmuchenergythereis.
Okay, ifyoujusthangon, I'llgogetit.
What a shamehastakenit.
I think I'm justtakingittouniversity.
Andshehad a darkenergycut, butthatisitforthiscuphere.
It's aboutthissizethiscuphasinitabout, I think, is a yacktoGrahamofOh, 10 totheminus 24 jewelsofenergyofdarkenergy.
Andnowweusuallythinkofpressuresof a positivequantity.
Youthinkofparticlesbangingagainstthesurfaceof a container, creating a pressurepushingout.
Andthat's that's a positivequantityofradiationhasintheintheearlyuniverse.
Relativisticredparticleshave a radiationpressure, whichis 1/3 oftheenergydensityhaddarkmatterparticlesandtheparticlesthatyouand I ammadeupofftherecalleddustparticleswritten.
Soyouthinkofputtingsomedoubtmatterorsomebarriersthatweremadeofin a in A in a tinon, they'llhardlyhitthesideofthetentbecausethey'removingsetsotheydon't create a pressure.
Youneedsomethingthatcanthatcanproduce, have a positiveenergydensitybuthavethisnegativepressurethat's actingintheoppositedirectiontowhatyoumightimagine.
Andthereisn't anystandardstuff.
Doesthatthestuffthatyouand I aremadeof, theparticlesthatyouknowitjustdoesnotdothat.
Youneedsomethingmore a bitmoreexoticonthetookthatthetwofavoritewhere's ofdoingitarebasicallytousewhattheparticlecosmologistlovestouse, whichis a scaleoffieldon a scaleoffieldhasboth.
A It's a it's anobjectthat's got a valueeverywhereonDhe.
What's itspotentialassociatedwithitnow, ifitturnsoutthatpotentialdominatesoverthekinetic, sothekineticenergyofthefieldisSasalettingaround a smallcomparedtoitspotentialenergy, thenitwillhave a negativepressure, anditcancause a kindof a repulsiveeffectintermsofcausingactingagainstgravityondhe.
Andsothat's what a quintessencescenariowilldoforyou.
Youworkin a regimewherethepotentialdominanceoverthekineticenergyanditwillgivemethisnegativepressure.
It's what a cosmologicalconstantdoes, infact, in a cosmologicalconstant.
It's a uniquecasewheretheenergydensityisexactlyminusthepressure.
Thedatasuggeststhattheuniverseisperfectlyconsistentwiththecosmologicalconstantsothattheaccelerationoftheuniversehasbeandrivenbysomethingthatlookslike a cosmologicalconstant.
Inactualfact.
Justrecently, there's a setofdeathhavebeencomingout.
Sothat's lowerthan a cosmologicalconstantwouldgive.
That's a weirdscenarioonit.
It's probablynotgonnalastthat I imaginethedatawillpusheverythingbackuptowardsthecosmologicalconstant.
Butatthemomentthere's a slightpressuretoeinthedata, suggestingitmightbelessthanminusone.
Thatmeansthattheuniverseisactuallynotjustgoingtoisgoingtoendupwith a bigrip.
Itiscalled a phantomscenario, andintheendtherewillbe a futuresingularitywhereitwilljusttearapartbecauseit's expandingsorapidlythatfirstofalltheGalaxiesbegintomoveapartrapidlyon.
Youcouldalsothinkofitispushingthemapartaswell, though, but I I think I think I wouldno, actually, I think I thinkofitispushingtheGalaxiesapartbecausetobepullingitapart, youneedsomethingoutsideofittobedoingthat.
So, forexample, thecosmicmicrowavebackgroundisreallyprobingtheuniverse, asitwas 300,000 yearsaftertheBigBangistellingyouwhattheuniverselookedlikeasthosephotonsdecoupledfromonthematter.
Butontheotherhand, if I lookat, say, thedistributionofGalaxiesareofclustersofGalaxies, that's tellingmeabouttheuniversemuchlateron a few 1,000,000,000 yearslater.
If I lookattheabundanceoftheprimordialelementsintheuniverse, that's tellingmeabouttheuniversemuchearlierin a fewminutesaftertheBigBangsothattherearethesedifferentepochs I canprobe.
I canlook, forexample, ofthedistributionofthesupernovaindistantGalaxies.
Thatisgivingme a snapshotofhowtheuniverseisexpandingatdifferentmomentsonbyeachofthesethatthedistributionoftheGalaxies, thedistributionofthehotandcoldspotsinthemicrowavebackground, therelativedistancebetweenthisdistantsupernovas.
Theyalldependuponhowtheuniverseisexpanding, thatthatmeanstheyalldependuponthesourceofdarkenergythatyou'vegot, Whetherit's a sourcethat's constantovertimeorwhetherit's thesource, it's varyingovertime.
Itwon't bethatthemicrowavebackgroundwillpinitdownformeortheclustersofGalaxieswillpinit, and I willneedallthree, and I'llhavetobeabletobringthemtogetherandandfindwhichoftheifanyofthemodelsbestfitsthecombinedtotalthatthat'llbethewaythatwe'lltryanddoit.
Butif I turnedthatifthatiftheuniversealwaysaccelerated, thenwewouldhaveneverformstructuresright, theatomsintheuniversewouldneverhavehad a chancetopulltogetheronthegravitationalattractionbecausetheaccelerationwouldhavepushed, pulledthemapart, pushedthemaparttooquicklyforgravitytopullthemback.
Soweknowtheuniversecan't havealwaysaccelerated.
Sothatmeansthere's a kneepop.
There's a timeintheintheuniversewhereitwentfrom a periodofnotacceleratingtoeaccelerating.
Now, ifwecangetenoughinformationaboutthatperiod, thenwhatwewillbeabletodohopefullyisstartdiscriminatingbetweenthevariousmodelsthattryandexplaindarkenergylikethecosmologicalconstant, like a contestant's modellike a modifiedgravitymodel.
Actuallyit's has a negativepressureassociatedwithit, anditactslike a effectivecosmological.
Constantdrivestheacceleration, sowe'vegot a difference, right?
We'vegotifif I have a verylightdensityofmatter, itit's a verylowdensityofmatter.
Thefieldisverylightif I have a highdensityofmatter.
Thefieldisverymassiveanditreactstothedensity.
Sowhat?
Thisexperimentthatisthatwe'reproposingwith a colleagueofminethat's a NaziinClareBurrageandthenwithEdHeinzatImperialiswe'regoingtohaveIfitworksout, we'regonnahave a comment, make a condensates.
A BoseEinsteincondensateinthelab, in a in a chamber.
Butmostpeople, I think, believethatthisisprobably a transientfeatureandthatwhatwe'regoingtoseeisthatthere'llbesomedecayofifit's a field, a scaleoffieldresponsible, likequintessencethatwilldecayjustlikethedecayandinflation, whichthenallowstheuniversetoreheatthattherewillbesomedecaywillmovebackintosomethinglike a matteror a radiationdominateduniverseagain.
Zerodegrees.
Youwalkallthewayaroundandyoucomebackto 360 degreeswith a straightstringThat's notquiteright.
Stringsortofcutsout a bitofspace, sowhenyouwalkaroundit, itmakesyoursparesconical.