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Dark Energy and Dark matter in A Superfluid Universe Kerson Huang Physics Department, MIT, Cambridge, USA Institute of Advanced Studies NTU Singapore Institute of Advanced Studies, NTU, Singapore 1 Dr. Johann Faust (Heidelberg 1509) 2 From Goethe’s Faust, Quoted by Boltzmann on Maxwell’ss equations Quoted by Boltzmann on Maxwell equations War es ein Gott der diese Zeichen schrieb, Die mit geheimnisvoll verborg’nen Trieb Die Kräfte der Natur um mich enthüllen Und mir das Herz mit stiller Freud erfüllen? Goethe Was it a god who wrote these signs, That have calmed yearnings of my soul That have calmed yearnings of my soul, And opened to me a secret of Nature? 3 Physics in the 20th century General relativity • Expanding universe • Dark energy Quantum theory • Superfluidity: Quantum phase coherence • Dynamical vacuum: Quantum field theory 4 Expanding universe • The more distant the galaxy, the faster it moves away from us. • Extrapolated backwards to “big bang” l db k d “b b ” a(t) Hubble’s law: Velocity proportional to distance Hubble’s parameter: H 1 da 1 a dt 15 10 9 yrs Accelerated expansion: Dark energy Edwin Hubble 5 Superconductivity superfluidity Superconductivity, superfluidity • Quantum phase coherence over macroscopic distances macroscopic distances • Phenomenological description: order parameter = complex scalar field p p x Fx e ix v s ∇x ∇ H Kamerlingh Onnes (1908) H. Kamerlingh (1908) 6 Dynamical vacuum ‐‐‐ QFT • Lamb shift in hydrogen: E(2S) – E(2P) E(2S) E(2P) = 1060 mhz 1060 mhz = 10 10‐6 eV • Electron anomalous moment: (g‐2)/2 = 10‐3 • Vacuum complex scalar field: Higgs field in standard model Others in grand unified theories A vacuum complex scalar field makes the universe a superfluid A vacuum complex scalar field makes the universe a superfluid. We investigate • Emergence of vacuum scalar field in big bang E f l fi ld i bi b • Observable effects 7 Scalar Field Lagrangian density : 1 2 L V 2 • The vacuum field fluctuates about mean value We can treat it as a mean value. We can treat it as a classical field by neglecting flucutuations. Potential : • But quantum effect of renormalization cannot be ignored. V 2 2 4 4 6 6 Equation of motion : 2 V 0 • This makes V dependent on the This makes V dependent on the length scale. • Especially important for big bang, when scale changes rapidly. 8 Renormalization In QFT there exist virtual processes. Spectrum must be cut off at high momentum . is the only scale in the theory. Ignore Cutoff 0 Hide id Effective cutoff (Scale) Renormalization: Renormalization: Adjusting couplings so as to preserve theory, when scale changes. Momentum spectrum 9 Renormalization‐group (RG) trajectory: Trajectory of V ( , ) in function space, space as scale changes. changes Fixed point: system scale invariant, =. UV trajectory: Asymptotic freedom IR trajectory: Triviality 10 The Creation • • • • • At the big bang . At the big bang There was no interaction. Universe was at the Gaussian fixed point (V 0, massless free field). It emerges along some direction, on an RG trajectory. The direction corresponds to a particular form of the potential V. In the space of all possible theories p p Outgoing trajectory ‐‐‐ Asymptotic freedom Ingoing trajectory ‐‐‐ Triviality (free field) The only asymptotically free scalar potential is the Halpern‐Huang potential: • Transcendental function (Kummer function) • Exponential behavior at large fields E ti l b h i tl fi ld • 4D generalization of 2D XY model, or sine‐Gordon theory. 11 Cosmological equations 1 R g R 8 G T ( E in s te in 's e q u a tio n ) 2 2 V 0 ( S c a la r fie ld e q u a tio n ) R o b e rts o n -W a lk e r m e tric ((s p a tia l h o m o g e n e ity) y) G ra v ity s c a le = a (ra d iu s o f u n iv e rs e ) S c a la r fie ld s c a le = (c u to ff m o n e n tu m ) S in c e th e re c a n b e o n ly o n e s c a le in th e u n iv e rs e , = /a Dynamical feedback: Dynamical feedback: Gravity provides cutoff to scalar field, which generates gravitational field. 12 Planck units: Planck length Planck time Planck energy 4G 5. 73 10 −35 m c3 4G 1. 91 10 −43 s c5 c 5 3. 44 10 18 GeV 5.5 108 Joule 4G We shall put 13 Initial‐value problem For illlustration, first use real scalar field. , a Ha k a V H 2 2 a 3 a V 3 H X H2 k = curvature parameter = 0, +1,‐1 k 2 1 2 V 0 a 32 Trace anomaly Constraint equation Constraint equation X 0 is a constraint on initial values. Equations guarantee X 0. 14 ? The big bang Time Model starts here O(10‐43 s) • Initial condition: Vacuum field already present. • Universe could be created in hot “normal phase”, then make phase transition to “superfluid phase”. Numerical solutions Time‐averaged asymptotic behavior : H tp a exp t 1 p Gives dark energy without “fine‐tuning” problem 16 Comparison of power‐law prediction on galactic redshift with observations ‐‐> earlier epoch d L = luminosity distance Different exponents p only affects vertical displacement, such as A and B. Horizontal line corresponds to Hubble’s law. Deviation indicates accelerated expansion (dark energy) Deviation indicates accelerated expansion (dark energy). Indication of a crossover transition between two different phase B ‐> A. 17 Cosmic inflation 1. Matter creation How to create enough matter for subsequent nucleogenesis before universe gets too large before universe gets too large. 2. Decoupling of matter scale and Planck scale Matter interactions proceed at nuclear scale of 1 GeV. p But equations have built‐in Planck scale of 1018 GeV. How do these scales decouple in the equations? Model with complete spatial homogeneity fail to answer these questions. Generalization: Complex scalar field, homogeneous modulus, spatially varying phase. New physics: Superfluidity in particular quantum vorticity New physics: Superfluidity, in particular quantum vorticity. 18 Complex scalar field Vortex line Fei v (Superfluid velocity) F 2 v 2 = Energy density of superflow C ds v C ds 2 n 2 rv 2 n v n r Like magnetic field from line current Vortex has cutoff radius of order a(t). Vortex line has energy per unit length. 19 • Replace vortex core by tube. • Scalar field remains uniform outside. • Can still use RW metric, • but space is multiply‐connected. The “worm‐hole” cosmos The vortex‐tube system represent emergent degrees of freedom. 20 Nanowires Vortex tubes in superfluid helium made visible by adsorption of metallic powder on surface metallic powder on surface (University of Fribourg expt.) (a) Copper (b) gold Under electron microscope 21 Vortex dynamics Elementary structure is vortex ring v 1 4R ln Self‐induced vortex motion R R0 The smaller the radius of curvature R, the faster it moves normal to R. 22 Vortex reconnection Feynman’s conjecture Signature: two cusps spring away from each other at very away from each other at very high speed (due to small radii), creating two jets of energy. Observed vortex reconnection in liquid helium‐‐ a millisecond event. D. Lathrop, Physics Today, 3 June, 2010. 23 Magnetic reconnections in sun’s corona Responsible for solar flares. 24 Change of topology due to reconnections Microscopic rings eventually decay. Quantum turbulence: Steady‐state “vortex tangle” Quantum turbulence: Steady state “vortex tangle” when there is steady supply of large vortex rings. K.W. Schwarz, Phys. Rev. Lett. ,49,283 (1982). , y , , ( ) 25 Simulation of quantum turbulence Creation of vortex tangle in presence of “counterflow” (friction). K W Schwarz Phys Rev B 38, 2398 (1988). K.W. Schwarz, Phys. Rev. B 38 2398 (1988) Number of reconnections: Number of reconnections: 0 3 18 18 844 844 1128 14781 Fractal dimension = 1.6 D. Kivotides, C.F. Barenghi, and D.C. Samuels. Phys. Rev. Lett. 87, 155301 (2001). Cosmology with quantum turbulence a (t ) Radius of universe F (t ) Modulus of scalar field ((t ) Vortex tube densityy (t ) Matter density • Scalar field has uniform modulus F. • Phase dynamics manifested via vortex tangle l. Ph d i if t d i t t l l • Matter created in vortex tangle (physically, via reconnections). Equations for the time derivatives: Equations for the time derivatives: a (t ) from Einstein's equation with RW metric. Source of ggravity: y Ttot = TF T T F (t ) from field equation. (t ) from Vinen's equations in liquid helium. (t ) determined by energy-momentum conservation Ttot; = 0. 27 Vinen’s equation in liquid helium vortex tube density (length per unit spatial volume) A 2 B3/2 Growth Decay In expanding universe this generalizes to 3H A 2 B3/2 • Proposed phenomenologically Proposed phenomenologically by Vinen by Vinen (1957). (1957) • Derived from vortex dynamics by Schwarz (1988). • Verified by many experiments. Put Ev =a 3 0 (Total vortex energy) Em =a 3 ((Total matter energy) gy) 28 4G c 1 Cosmological equations: Generalized: Old: dH k − 2 dF 2 a ∂V − 1 E E m v 3 ∂a a 3 dt dt a2 0 Ev d 2 F −3H dF 3H − F − 1 ∂V 2 3 2 ∂F dt dt a k a V H 2 2 a 3 a V 3H Constraint: dE v k 21 H 2 V 0 a 32 2 d dE m d Essentially constant 3/2 −E 2v E v • Rapid change • Av. over t • of order 1018 0 dF 2 s 1 dt E v Constraint: H2 k a2 − 2 3 Ḟ 2 V 1 0 a 3 Ev 1 a3 Em 0 Decouples into two sets because s1 t Planck time scale Nuclear time scale Nuclear energy scale Planck energy scale 18 10 −18 29 Decoupling: • From the point of view of the cosmic expansion, the From the point of view of the cosmic expansion the vortex‐matter system is essentially static. • From the viewpoint vortex‐matter system, cosmic expansion is extremely fast, but its average effect is to give an "abnormally" large rate of matter production. Inflation scenario: Inflation scenario: • Vortex tangle (quantum turbulence) grows and eventually decays. • All the matter needed for galaxy formation was created in the tangle. • Inflation era = lifetime of quantum turbulence. After decay of quantum turbulence, the standard hot big After decay of quantum turbulence the standard hot big bang theory takes over, but the universe remains a superfluid. 30 Era of quantum turbulence Cosmic inflation: • Radius increases by factor 10 27 • in 10 ‐30 seconds. • Matter created = 10 22 sun masses • Eventually form galaxies outside of vortex cores. • Large‐scale uniformity 31 10‐26 s Big Bi bang 105 yrs Time Quantum turbulence CMB formed Inflation Validity of this model Standard hot big bang theory Plus effects of superfluidity 32 Legacies in the post‐inflation universe Remnant vortex tubes with empty cores grow into cosmic voids in galactic distribution. The large‐scale structure of the Universe from the CfA2 galaxy survey. 34 Reconnection of huge vortex tubes in the later universe will be rare but spectacular. Gamma ray burst • A few events per galaxy per million yrs • Lasting ms to minutes • Energy output in 1 s = Sun’s output in entire life (billions of years) (billions of years). Jet of matter 27 light years long 35 Dark matter Halo in “bullet cluster” H l i “b ll t l t ” from gravitational lensing (blue) Galaxyy Dark matter halo 36 “Hair” on black hole Artist’s conception: g j p Rotating object in superfluid induce vortex filaments. Observed: “Non‐thermal filaments" near center of Milky Way. 37 Research team at IAS, NTU Michael Good H Hwee‐Boon Low B L Roh‐Suan Tung Chi Xiong KH References: K. Huang, H.‐B. Low, and R.‐S. Tung, 1. “Scalar field cosmology I: asymptotic freedom and the initial‐value problem”, arXiv:1106.5282 (2011). arXiv:1106.5282 (2011). 2. “Scalar field cosmology II: superfluidity and quantum turbulence”, arXiv:1106.5283 (2011). 38