Presentation on theme: "Yu Nakayama (Kavli IPMU, Caltech)"— Presentation transcript:
1 Understanding phase transitions and critical phenomena from conformal bootstrap Yu Nakayama (Kavli IPMU, Caltech)in collaboration with Tomoki Ohtsuki (Kavli IPMU)
2 Critical point of H2O phase diagram At T= 647K, P = 22MPa, we have a critical pointSecond order phase transitionCritical behavior is universal
3 Universal critical behavior 1 Various thermodynamic quantities show scaling lawThe origin of the critical behavior is scale invariance at the critical point as a result of renormalization group flowAt second order phase transition, critical behavior appears in thermodynamic quantities
4 Universal critical behavior 2 Various thermodynamic quantities scale asThe origin of the critical behavior is scale invariance at the critical point (fixed point of RG flow)One of the greatest challenges to human intellect is to understand the origin of universality, and determine critical exponentsThe same critical behavior is seen in 3D Ising model
5 Scaling hypothesisAssume free energy shows the scaling behaviorThen, scaling relations can be derivedThe scaling hypothesis and universality may be understood from the renormalization group (Wilson)But the scaling hypothesis itself does not explain the value of andAt the critical point, the thermodynamic free energy satisfies the scaling law
6 From scale to conformal hypothesis At the critical point, the system is not only scale invariant, but is invariant under the enhanced symmetry known as conformal symmetryThe universality of the critical behavior is governed by the conformal symmetry as a result of local renormalization groupThe critical exponent may be understood from the hidden conformal symmetry (~ solution of 3d Ising)There exists hidden enhanced symmetry called conformal invariance
7 Scale vs Conformal invariance Scale transformationConformal transformation
8 Conformal transformation Scale transformation:Conformal transformation:It is not immediately obvious if global scale invariance means conformal invariance (see my review paper arXiv: )
9 Conformal hypothesis in 3D Ising model Consistency of 4-point functions in conformal invariant system gives a bound on scaling dimensions of operators (El-Showk et al)Explains critical exponents (3d Ising model solved)!Assuming the conformal invariance, critical exponents can be determined from conformal bootstrap
10 O(n) x O(m) symmetric CFTs and critical phenomena
11 O(n)xO(m) Landau-Ginzburg model Field transforms vector x vector rep under O(n) x O(m) global symmetryu preserves O(nm) symmetry, but v breaks itAlways exists O(nm) symmetric Heisenberg fixed point with v = 0d= 3 model appears in effective theories of frustrated spins or chiral transition in QCDAlthough we won’t need Hamiltonian (Lagrangian), we start with the concrete model…
12 Frustrated spins in non-collinear order Effective theory = O(n) x O(m) LG model:n = components of spin, m = non-collinear dim1st order phase transition or 2nd order phase transition? Huge debate in experimentsTheoretical controversy as well. Monte Carlo, epsilon expansions, large N expansions, exact RG all disagree which values of n and m, the fixed points exist ( 2nd order phase transition)…Anti-ferro spins in frustrated lattice (Kawamura)n=2, m=2n=3, m=3chiralanti-chiral
13 Chiral phase transition in QCD A long standing debate if the QCD chiral phase transition with Nf=2 massless flavors is 1st order or 2nd orderLattice simulations are again controversialEffective theory description is SU(2) x SU(2) x U(1) (= O(4) x O(2)) LG model in d=3RG computation is also controversial…SUSY does not help (with many respects…)What is the order of chiral phase transition in QCD (Pisarsky-Wilczek)
14 Schematic RG picture (Un)stable one is called (anti-)chiral fixed For sufficiently large n with fixed m, they both existNobody has agreed what happens for smaller nMultiple fixed points cannot appear in SUSY theories…
15 Why controversial?Large n (with fixed m) expansion or epsilon expansion are asymptoticResults depend on how you resum the diverging 5- loop or 6-loop series (need artisan technique. OK for Ising but…)Exact (or functional) RG directly in d=3 needs “truncation”, which is not a controlled approximationNo SUSY, no large n, no holography. We are talking about real problems.
16 The questions to be answered To fix the conformal window for O(n) x O(m) symmetric Landau-Ginzburg models in d=3(Non-)Existence of non-Heisenberg fixed point determine the order of phase transitionsCompute critical exponents to compare with experiments (or simulations)Our conformal bootstrap approach is non-perturbative without assuming any Hamiltonian (c.f. “Hamiltonian is dead”)
18 Schematic conformal bootstrap equations Consider 4pt functionsOPE expansionsI: SS, ST, TS, TT, AS, SA, AA … (S: Singlet, T: Traceless symmetric, A: Anti-symmetric)Crossing relationsAssume spectra (e.g , )to see if you can solve the crossing relations (non-trivial due to unitarity ) convex optimization problem(but 100 times more complicated than Ising model)
19 Results Begin with O(3) x O(m) with m=15 Can we see Heisenberg/chiral/anti-chiral fixed point?Each plots need 1~2 weeks computation on our cluster computersHypothesis: non-trivial behavior of the bound indicates conformal fixed point
20 Heisenberg fixed point in SS sector Constraint is same as O(45) (symmetry enhancement) “Kink” is Heisenberg fixed pointConsistent but cannot see chiral/anti-chiral
21 Anti-chiral fixed point in TA spin 1 op We can read spectra at the “kink”Dimension of SS operatorSeems to agree with large n prediction of anti-chiral fixed point
22 Anti-chiral fixed point in ST spin 0 op We can read spectral at the “kink(?)”Dimension of SS operatorAgrees with anti-chiral fixed point?
23 Chiral fixed point in TS spin 0 op We can read spectral at the “kink”Dimension of SS operatorSeems to agree with large n prediction of chiral fixed point
24 Finding conformal window n*(m=3) Change n (with m=3) to see if the kink disappears (suggesting no anti-chiral fixed point!)n = 6~7 seems the edge of the conformal window?
25 Finding conformal window n*(m=3) Differentiated plotKink disappears for n<6~7!
26 Quick summary for O(n) x O(3) A single conformal bootstrap equation can detect all Heisenberg/chiral/anti-chiral fixed points in different sectorsLarge n (with fixed m) analysis agrees with usWe predict that n= 6~7 is the edge of the conformal window for anti-chiral fixed point in m=3 (e.g. large n expansion n= 7.3, epsilon expansion n = 9.5)First example of determining conformal window from (numerical) conformal bootstrap
27 Toward O(n) x O(2) under controversies Situation is much controversialn > n*~5,6, chiral and anti-chiral exitn =2,3,4, some say there are (non-perturbative) chiral fixed point (cannot seen in 1/n expansions)Can we see it?Found conformal window in spin 1 sectorWe have preliminary results on controversial regime, but my collaborator refuses to show them here…
28 Summary and discussions Conformal hypothesis is very powerfulO(n) x O(m) bootstrap is excitingApplications to real physics (frustrated spin, QCD…)Determination of conformal window is now possible!Theoretical backup needed? Still empirical science.If you have any models to be studied with conformal bootstrap, let us know