relaxing to three dimensions relaxing to three dimensions lisa randall harvard university

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Relaxing to Three Relaxing to Three Dimensions Dimensions Lisa Randall Lisa Randall Harvard University Harvard University

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Page 1: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Relaxing to Three Relaxing to Three DimensionsDimensions

Lisa Randall Lisa Randall

Harvard UniversityHarvard University

Page 2: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

IntroductionIntroduction

• Very basic question about the world is Very basic question about the world is why we seem to experience three why we seem to experience three spatial dimensionsspatial dimensions

• Are three dimensions special?Are three dimensions special?• We’ll address this question in a higher-We’ll address this question in a higher-

dimensional universedimensional universe• Show that not only is it possible to Show that not only is it possible to

mimic three dimensions, might even mimic three dimensions, might even be likely!be likely!

Page 3: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

ContextContext

• Lots of attention of late paid to the Lots of attention of late paid to the landscape idealandscape idea

• In some scenarios (string theory, In some scenarios (string theory, inflation) there are many possible inflation) there are many possible vacuavacua

• We live in one of themWe live in one of them

• That part of the story is very likely That part of the story is very likely truetrue

Page 4: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

ButBut

• However, often combined with However, often combined with anthropic principle anthropic principle

• Before making predictions based on Before making predictions based on known vacuaknown vacua

• Want to determine as many Want to determine as many possibilities as we can possibilities as we can

• Perhaps qualitatively new phenomena Perhaps qualitatively new phenomena in vacua we haven’t yet discoveredin vacua we haven’t yet discovered

Page 5: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

So farSo far

• The vacua most string theorists The vacua most string theorists study are based on curled-up study are based on curled-up dimensions dimensions

• Essentially all such work assumes six Essentially all such work assumes six dimensions compactifieddimensions compactified

• Even more restrictive: almost all Even more restrictive: almost all assume Calabi-Yau compactificationassume Calabi-Yau compactification

Page 6: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Alternative selection principles Alternative selection principles possiblepossible

• Localization—where gravity is concentrated in a Localization—where gravity is concentrated in a finite region even though extra dimensions are finite region even though extra dimensions are infinite-- can perhaps help exploit new selection infinite-- can perhaps help exploit new selection principles for finding where we liveprinciples for finding where we live

• After all, initial evolution would be quite different After all, initial evolution would be quite different • Want to ask –quite generally--could there be a Want to ask –quite generally--could there be a

dynamical explanation for more observable dynamical explanation for more observable aspects of the universe?aspects of the universe?

• And does localized gravity help us understand And does localized gravity help us understand such phenomena?such phenomena?

Page 7: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

The Relaxation PrincipleThe Relaxation Principle

• Proposal: The Relaxation PrincipleProposal: The Relaxation Principle• The universe naturally evolves into the The universe naturally evolves into the

favored vacuum: the one with maximum favored vacuum: the one with maximum filling fractionfilling fraction

• Cosmological evolution determines which of Cosmological evolution determines which of many possible vacua are favoredmany possible vacua are favored

• Shinji Mukohyama and I applied this ideaShinji Mukohyama and I applied this idea(with partial success) to the cosmological (with partial success) to the cosmological

constant problemconstant problem

Page 8: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Localized gravity and the Localized gravity and the relaxation principlerelaxation principle

• Localized gravity gives a new scenario in Localized gravity gives a new scenario in which to apply the relaxation principle which to apply the relaxation principle

• Potentially address difficult questions such Potentially address difficult questions such asas– Why are there three dimensions of space that Why are there three dimensions of space that

we experience?we experience?– Why do forces act in three spatial dimensions?Why do forces act in three spatial dimensions?– Why should three dimensions be special at Why should three dimensions be special at

all??all??

Page 9: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

OutlineOutline

• Review Localized GravityReview Localized Gravity• Review old ideas for explaining 3 Review old ideas for explaining 3

dimensions of spacedimensions of space• New ideasNew ideas• Potential relevance of localized Potential relevance of localized

gravity to explaining relevance of gravity to explaining relevance of there spatial dimensions there spatial dimensions

• ConcludeConclude

Page 10: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Catalyst for Recent Catalyst for Recent Developments about extra Developments about extra dimensions: Branesdimensions: Branes

• Branes are membrane-Branes are membrane-like objects in higher-like objects in higher-dimensional spacedimensional space

• Differentiate space on Differentiate space on and orthogonal to and orthogonal to branebrane

• Can confine particles Can confine particles and forces on their and forces on their surfacesurface

Page 11: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

BraneworldBraneworldParticles can be confined to Particles can be confined to branesbranesEverything but gravity on a braneEverything but gravity on a brane

Page 12: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Branes that Distort Space:Branes that Distort Space:New Way to Hide Dimensions New Way to Hide Dimensions

• If we’re confined to branes, only If we’re confined to branes, only problematic aspect of dimensions is gravityproblematic aspect of dimensions is gravity

• However, energetic branes in an energetic However, energetic branes in an energetic bulk can distort spacebulk can distort space

• So much so that an infinite extra dimension So much so that an infinite extra dimension is possibleis possible

• Gravitational field (and graviton) get Gravitational field (and graviton) get localized near a brane—localized near a brane—RS2RS2

Page 13: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Scenario for Warped Scenario for Warped GeometryGeometry

Page 14: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Find Localized gravity Find Localized gravity

• Lower-dimensional gravity survives in this Lower-dimensional gravity survives in this warped spacewarped space

• dsds22=dr=dr22+e+e-kr-kr(dx(dx dx dx • Warped metric: overall scale factorWarped metric: overall scale factor• Here it exponentially decreasesHere it exponentially decreases• Consequence is that the zero mode in a KK Consequence is that the zero mode in a KK

reduction, ereduction, e-kr-kr, is normalizable, is normalizable• Find you get a four-dimensional gravitonFind you get a four-dimensional graviton• Even though space is fundamentally five-Even though space is fundamentally five-

dimensionaldimensional

Page 15: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Graviton in this geometryGraviton in this geometry

Page 16: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Gravitational Field Near Gravitational Field Near BraneBrane

Page 17: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Even More Dramatic: Even More Dramatic: Locality of Four DimensionsLocality of Four Dimensions

• Why should you need to know about Why should you need to know about space far from the brane?space far from the brane?

• w/ Karch, an example based on AdS w/ Karch, an example based on AdS branebrane

• Warp factor turns aroundWarp factor turns around

• We find four-dimensional gravity We find four-dimensional gravity (mediated by massive graviton) near (mediated by massive graviton) near the brane!the brane!

Page 18: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

AdS5/AdS4AdS5/AdS4

Again, graviton gets localized near brane

No gravity localization

Unless another brane

Page 19: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Locally localized gravityLocally localized gravity

• Dimensionality depends on locationDimensionality depends on location

• See different dimensions in different See different dimensions in different placesplaces

• Determined by gravity bound state in Determined by gravity bound state in that regionthat region

4D gravity4D gravity

5D gravity

5D gravity

4D gravity

4D gravity

5D gravity

5D gravity

Page 20: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Four dimensions might be a Four dimensions might be a local phenomenon local phenomenon

• Why should you need Why should you need to know about space to know about space far from the brane?far from the brane?

• four-dimensional four-dimensional gravity (mediated by gravity (mediated by massive graviton) near massive graviton) near the branethe brane

• But higher-dimensional But higher-dimensional elsewhereelsewhere

• Copernican revolution Copernican revolution continues!continues!

Page 21: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

• So it’s conceivable that space looks So it’s conceivable that space looks three-dimensional even though the three-dimensional even though the world is truly higher-dimensionalworld is truly higher-dimensional

• But is there a reason to single out But is there a reason to single out three dimensions?three dimensions?

• We know three dimensions is We know three dimensions is possible but is it likely?possible but is it likely?

Page 22: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Existing Ideas to explain three Existing Ideas to explain three spatial dimensions (in string spatial dimensions (in string theory)?theory)?• Most popular: Brandenberger-Vafa proposalMost popular: Brandenberger-Vafa proposal

• They assume compactified dimensionsThey assume compactified dimensions

• (As does everyone else who tries to ask this (As does everyone else who tries to ask this question)question)

• Their idea is that only a few dimensions Their idea is that only a few dimensions grow large—grow large—

• Those for which there isn’t an opposing Those for which there isn’t an opposing force due to wrapped stringsforce due to wrapped strings

Page 23: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Brandenberger-VafaBrandenberger-Vafa

• In general, there will be wrapped stringsIn general, there will be wrapped strings

• UNLESS the strings can meet and annihilateUNLESS the strings can meet and annihilate

• However, strings won’t meet if there are more However, strings won’t meet if there are more than four-dimensions in spacetime (2+2=4)than four-dimensions in spacetime (2+2=4)

• But if there are four or fewer dimensions, the But if there are four or fewer dimensions, the dimensions will grow larger dimensions will grow larger

• Conclude: 4 (or fewer) dimensions will be Conclude: 4 (or fewer) dimensions will be largelarge

Page 24: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Nice ideaNice idea

• But…But…• Depends on initial conditionsDepends on initial conditions• Depends on poorly understood dynamics—Depends on poorly understood dynamics—

everything is happening at the Planck everything is happening at the Planck scalescale

• Depends on moduli stabilization (what Depends on moduli stabilization (what ultimately determines size and shape) and ultimately determines size and shape) and assumes simple toroidal compatificationassumes simple toroidal compatification

• Neglects nonstring objects in Neglects nonstring objects in “string”theory—branes“string”theory—branes

Page 25: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Four dimensions in context of Four dimensions in context of branes and localized gravitybranes and localized gravityw/Andeasw/Andeas KarchKarch

• Make opposite assumptions from BVMake opposite assumptions from BV• Assume the number of large dimensions of Assume the number of large dimensions of

space is fixed (by string theory?)space is fixed (by string theory?)• Ask instead which branes (that is which Ask instead which branes (that is which

dimensionalities of branes) survivedimensionalities of branes) survive• If 3-branes survive, possible candidates for If 3-branes survive, possible candidates for

a four-dimensional universea four-dimensional universe• If 3-branes have the biggest filling fraction, If 3-branes have the biggest filling fraction,

they are the most likely candidatethey are the most likely candidate

Page 26: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

BasicsBasics

• Consider a ten-dimensional universeConsider a ten-dimensional universe• And let it evolve according to conventional And let it evolve according to conventional

FRW evolutionFRW evolution• Assume universe starts with an equal number Assume universe starts with an equal number

of branes and antibranes (generic initial of branes and antibranes (generic initial conditions; branes at random orientations)conditions; branes at random orientations)

• Of all dimensions Of all dimensions • Let the energy of the branes determine the Let the energy of the branes determine the

equation of state that enters the FRW equation of state that enters the FRW evolutionevolution

Page 27: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

What happens?What happens?

• During the universe’s evolution, some During the universe’s evolution, some branes will dilute more than othersbranes will dilute more than others

• After some time, we’ll be left with a After some time, we’ll be left with a universe in which certain types of universe in which certain types of branes will be much more numerousbranes will be much more numerous

• Those are likely to be the ones on Those are likely to be the ones on which we livewhich we live

Page 28: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

10 d FRW evolution10 d FRW evolution

ds2=-dt2+a2(t) d k2

Page 29: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Evolution in n-dimensions with Evolution in n-dimensions with p=wp=w

With energy conservation

kk

k

kk

H2=-k/a2+16GN/(n(n-1))

Page 30: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

More evolutionMore evolution

• Assume the equation of state is dominated by a Assume the equation of state is dominated by a single component (single w)single component (single w)

• Even if not initially true, will be the stable Even if not initially true, will be the stable attractor of the evolutionattractor of the evolution

• SolveSolve

~a-n(1+w)->t~an/2(w+1)

Page 31: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Equation of state for branesEquation of state for branes

• We are interested in a brane-dominated We are interested in a brane-dominated universeuniverse

• (We’ll see that’s what happens if we mix (We’ll see that’s what happens if we mix branes and dust and radiation in any case)branes and dust and radiation in any case)

• Let’s consider the argument for strings Let’s consider the argument for strings and generalize and generalize

• String has String has =-p like a cc, but only one =-p like a cc, but only one component of p is nonzerocomponent of p is nonzero

• So with strings in random directions in So with strings in random directions in n=3, p=-n=3, p=-/3/3

Page 32: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Brane equation of stateBrane equation of state

• Using exactly the same logicUsing exactly the same logic

• For a d-brane with a d+1-For a d-brane with a d+1-dimensional world volumedimensional world volume

• In n spatial dimensionsIn n spatial dimensions

• w=-d/nw=-d/n

• From this, we concludeFrom this, we conclude

• a~ta~t(n-d)/2(n-d)/2

Page 33: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

How do branes evolve in this How do branes evolve in this expanding universe?expanding universe?

• If branes are non-interacting, we know If branes are non-interacting, we know how they scale how they scale

• Even without knowing the FRW evolution Even without knowing the FRW evolution preciselyprecisely

• The volume of the branes goes like aThe volume of the branes goes like add

• Whereas the volume of space goes like aWhereas the volume of space goes like ann

• So the density of d-branes (here d is So the density of d-branes (here d is merely dimension)merely dimension)

• aad-nd-n

Page 34: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

• Clearly if this were all that were going on, Clearly if this were all that were going on, the largest branes would dominate the the largest branes would dominate the energy density after enough time has energy density after enough time has elapsedelapsed

• But this is not the caseBut this is not the case

• In a 10-dimensional universe, 9-branes and In a 10-dimensional universe, 9-branes and anti-9-branes overlap everywhere anti-9-branes overlap everywhere

• So they will instantaneously annihilateSo they will instantaneously annihilate

• And cannot dominate the energy densityAnd cannot dominate the energy density

Page 35: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

8-branes8-branes

• 8-branes are tricky8-branes are tricky• They always overlap over most coordinates and They always overlap over most coordinates and

possibly annihilatepossibly annihilate• Also in flat metric, 8-branes cannot be very far Also in flat metric, 8-branes cannot be very far

apart with space becoming singularapart with space becoming singular• Finally, if we have IIB and a complex tachyon, we Finally, if we have IIB and a complex tachyon, we

don’t expect 8-branes to formdon’t expect 8-branes to form• Upshot: 8-branes potentially a problem, but many Upshot: 8-branes potentially a problem, but many

reasons to think they aren’t therereasons to think they aren’t there• (As with domain walls in four-dimensional (As with domain walls in four-dimensional

universe)universe)

Page 36: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Other branesOther branes

• Here’s where things become interestingHere’s where things become interesting

• And we see that 3-branes are specialAnd we see that 3-branes are special

• Higher-dimensional branes must always Higher-dimensional branes must always intersectintersect

• Their world volumes are such thatTheir world volumes are such that

• 2(d+1)≥10 (=n+1 for what we are 2(d+1)≥10 (=n+1 for what we are interested in)interested in)

• So for us, rather than 2+2=4, use 4+4<10!So for us, rather than 2+2=4, use 4+4<10!

Page 37: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

ConsequencesConsequences

• The density of branes with more than 3+1 The density of branes with more than 3+1 dimensions is less than you would thinkdimensions is less than you would think

• We use the same (now standard) argument We use the same (now standard) argument that is used for strings to establish their that is used for strings to establish their dilution ratedilution rate

• Strings that intersect spawn loops Strings that intersect spawn loops

• Those loops radiate energy away through Those loops radiate energy away through gravitational wavesgravitational waves

• We’ll assume similar dynamics for branesWe’ll assume similar dynamics for branes

Page 38: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Intersecting brane densityIntersecting brane density

• Assume decay processes happen at the Assume decay processes happen at the maximum efficiency allowed by causalitymaximum efficiency allowed by causality

• The network at all times looks the same The network at all times looks the same when viewed on the scale “t”, the horizon when viewed on the scale “t”, the horizon sizesize

• Scaling solutionScaling solution• Length of string is some number times tLength of string is some number times t• Volume of d-brane some number times tVolume of d-brane some number times tdd

Page 39: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Cont’dCont’d

• Horizon volume is tHorizon volume is tnn so so

True for any branes that can find each other and interact and trigger decay that’s limited only by causality

id~td-n

Page 40: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Who Wins?Who Wins?

• Suppose 3-branes dominateSuppose 3-branes dominate• w=-1/3 w=-1/3 t~an/2(w+1)

• a~ta~t1/3; 1/3; 7-branes: t7-branes: t-(9-7)-(9-7) ; 3-branes: a ; 3-branes: a-(9-3)-(9-3)

• 7-branes and 3-branes dominate7-branes and 3-branes dominate• Density for both decreases as tDensity for both decreases as t22

• All other branes dilute more quicklyAll other branes dilute more quickly• (Possible concern about 8-branes(Possible concern about 8-branes• But no worse than domain walls for But no worse than domain walls for

cosmic-string dominated scenarios)cosmic-string dominated scenarios)

Page 41: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Where are we?Where are we?

• The only stable evolution has 3-branes and The only stable evolution has 3-branes and 7-branes dominating7-branes dominating

• No other set of branes can consistently No other set of branes can consistently dominate the energy densitydominate the energy density

• Remarkable resultRemarkable result

• 3-branes and 7-branes appear in particle 3-branes and 7-branes appear in particle physics and cosmologyphysics and cosmology

• Used only generic assumptions and Used only generic assumptions and evolutionevolution

Page 42: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

• 3-branes winning might seem best but3-branes winning might seem best but

• 3-branes and 7-branes are both 3-branes and 7-branes are both needed to have viable gauge theory needed to have viable gauge theory with matterwith matter

• Furthermore, 3-branes and 7-branes Furthermore, 3-branes and 7-branes can generate an inflationary scenariocan generate an inflationary scenario

Page 43: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Localized Gravity in Ten Localized Gravity in Ten Dimensions Dimensions w/ Liam Fitzpatrickw/ Liam Fitzpatrick

• System of 3 intersecting 7-branesSystem of 3 intersecting 7-branes• (0,1,2,3,4,5,6,7,8,9)(0,1,2,3,4,5,6,7,8,9)• (x,x,x,x,x,x,x,x,-,-)(x,x,x,x,x,x,x,x,-,-)• (x,x,x,x,x,x,-,-,x,x,)(x,x,x,x,x,x,-,-,x,x,)• (x,x,x,x,-,-,x,x,x,x)(x,x,x,x,-,-,x,x,x,x)• Generically the 3 branes intersect over a four-Generically the 3 branes intersect over a four-

dimensional world volumedimensional world volume• Find gravity gets localized on the intersectionFind gravity gets localized on the intersection• New geometries and cosmological scenariosNew geometries and cosmological scenarios

Page 44: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Why is there gravity?Why is there gravity?

• We want to show that we have We want to show that we have localized gravity at that intersectionlocalized gravity at that intersection

• To do so, we combine (and To do so, we combine (and generalize) two ideasgeneralize) two ideas

• Gherghetta, Shaposhnikov-Gherghetta, Shaposhnikov-codimension-2 localizaiotncodimension-2 localizaiotn

• Arkani-Hamed, Dimopoulos, Kaloper-Arkani-Hamed, Dimopoulos, Kaloper-intersecting codimension-1 branesintersecting codimension-1 branes

Page 45: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Gherghetta-Shaposhnikov set-Gherghetta-Shaposhnikov set-upup

• They assume a They assume a string-like defect in string-like defect in AdS6AdS6

Page 46: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Transverse DimensionsTransverse Dimensions

Page 47: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Intersecting codimension-1 Intersecting codimension-1 branesbranes

• Idea is that if we can get localization Idea is that if we can get localization from a single codimension-1 branefrom a single codimension-1 brane

• Generating gravity on one lower Generating gravity on one lower dimensional volumedimensional volume

• We should be able to get (d+1)-We should be able to get (d+1)-dimensional gravity if we have n-dimensional gravity if we have n-(d+1) branes(d+1) branes

Page 48: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Einstein’s EquationsEinstein’s Equations

Page 49: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Our SetupOur Setup

• We combine these two ideasWe combine these two ideas• Matching is a little tricker because we have two Matching is a little tricker because we have two

nontrivial metric componentsnontrivial metric components• And two nontrivial tensionsAnd two nontrivial tensions• Key is to treat the additional curled-up dimension Key is to treat the additional curled-up dimension

as an additional flat dimensionas an additional flat dimension• Take into account the fact that the metric Take into account the fact that the metric

components change at the branecomponents change at the brane• Also show you can use Stoke’s Theorem to get an Also show you can use Stoke’s Theorem to get an

exact resultexact result• Also account for inner contribution from string-Also account for inner contribution from string-

like singularitylike singularity

Page 50: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

ExpectExpect

AdS outside (suitable warping) and AdS outside (suitable warping) and therefore a normalizable zero modetherefore a normalizable zero mode

Conditions on various tension Conditions on various tension componentscomponents

More complicated because not just More complicated because not just delta-function singularitiesdelta-function singularities

Nonetheless, gravity localized at the Nonetheless, gravity localized at the intersectionintersection

ThTh

Page 51: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

ResultResult

Get 3-d gravity Get 3-d gravity

• 3 branes, 7 branes,3 branes, 7 branes,

• And these 3+1-d intersectionsAnd these 3+1-d intersections

• Get gauge forces and gravity tooGet gauge forces and gravity too

Page 52: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

Either scenarioEither scenario

• Reason to have coincident 3-branes Reason to have coincident 3-branes and 7-branesand 7-branes

• Even better—slightly mismatched Even better—slightly mismatched generates hierarchy!generates hierarchy!

• Cosmology interesting: linking Cosmology interesting: linking different horizon-sized regionsdifferent horizon-sized regions

• Brane inflation possible—3-brane Brane inflation possible—3-brane annihilationsannihilations

Page 53: Relaxing to Three Dimensions Relaxing to Three Dimensions Lisa Randall Harvard University

ConclusionsConclusions

• New way of thinking about cosmologyNew way of thinking about cosmology• Many new and interesting questionsMany new and interesting questions• Two aspects of our discussionTwo aspects of our discussion• First fairly robust and remarkable First fairly robust and remarkable • We put in very little but 3-branes and 7-branes We put in very little but 3-branes and 7-branes

specialspecial• Show up all over the place in string-theory Show up all over the place in string-theory • 3+1-dimensions really is special3+1-dimensions really is special• Second part: new cosmologies with localized gravitySecond part: new cosmologies with localized gravity• Ripe for further explorationRipe for further exploration• Dynamical relaxation principle very satisfying-Dynamical relaxation principle very satisfying-

merits further studymerits further study