Maria Paola Lombardo GGI Firenze March 2014
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1 Dense matter from lattice QCD (?) Maria Paola Lombardo GGI Firenze March 2014
2 The phases of strong interactions Andronic et al 2010 Tojo et al 2011
3 ..and the experimental programs First proposal: Cabibbo and Parisi, 1975 LHC RHIC NICA /FAIR / RHIC II US NSAC Long RangePlan (adapted)
4 (Dense) matter on the lattice QCD, and the lattice Few body physics, nuclear potential and the nuclear equation of state EoS and condensates from first principles in QCDlike models I: fermionic models EoS and condensates from first principles in QCD-like models II: two color QCD Overview of methods and results in QCD The critical point of QCD
5 Fundamental theory of strong interactions QCD, AND THE LATTICE
6
7 QCD
8 ..on the lattice
9 Designing a simulation Choice of the discretization Input parameters
10 Dimensional transmutation 1/T a L..and check of the continuumlimit
11
12 Option 1:
13 Option 2
14
15 FEW BODY RESULTS
16 Wuppertal- Budapest 2013
17
18
19 H dibaryon
20
21 Nuclear force from Lattice QCD Phenomenological NN forces have fitting parameters. For hyperon nucleon and nucleon nucleon a factor 3 more However in QCD all interactions are controlled only by the scale parameter and the physical quark masses NN potentials are determined from the equal time Nambu-Bethe-Salpeter wave function
22 Wave function, Schroedinger equation and potential
23
24
25 Fits to phenomenological form
26 Overview of the results
27 Three nucleon forces
28 The short distance repulsion among baryons Aoki, Balog, Weisz 2013 The wave function at short distance Diverges at r = 0 if n1 > 0 Vanishes at r = 0 if n1 < 0 Implies for the short distance potential Attractive if n1 > 0 Repulsive if n1 < 0 In some cases a mismatch was observed between the sign of the potential and these estimates, indicating that the asymptotic behaviour has not been reached yet on the lattice
29 September 2013
30 EoS from lattice nuclear forces Input : NN potentials from zero strangeness sector in flavor SU(3) QCD
31 Ground state energies
32 Ground state energies
33 Mass-radius relation
34
35 I. Dense Matter from First Principles QCD-like models and the strong coupling expansion : condensates, equation of state, search for exotic phases II. QCD, and its critical point
36 Observables and EoS
37 GN 2+1, NJL 3+1 FERMIONIC MODELS
38 2+1 Gross-Neveu model Phase diagram in ordinary conditions
39 GN model on the continuum and on the lattice
40 Mean field solution vs lattice results Set S=0 and obtain the critical line Note for T=0 m independence till mc = S0
41 The Phase Diagram of 2+1 GN model : mean field and exact Hands, Kocic, Kogut 1993
42 Condensate and EOS in NJL 3+1 Hands and Walters 2003
43 Diquark condensation
44 From QCD to four fermion models Lattice QCD action with staggered fermions
45 From QCD to four fermion models Cfr Lectures by Massimo Mannarelli Gauge part disappears in the infinite coupling limit
46 From QCD to four fermion models Gauge part disappears in the infinite coupling limit Meson operators
47 Sketch of the calculations (T,m=0) 1) Bosonization Z 2) Mean field Z
48 Results from the strong coupling expansion for finite T and m
49
50 TWO COLOR QCD
51 QCD with two colors Pauli Gursey Symmetry: quarks and antiquarks transform according to equivalent reps.
52 Spectrum and condensates Quark propagator SU(2) matrix Mesons and Baryons are degenerate at T,m=0 The degeneracy is lifted at T,m 0 Hands, Kogut, MpL, Morrison 1999
53 Rotation of condensates
54
55
56 Phases of two color QCD? Hands, Skullerud, Kim 2013
57 QCD
58 The sign problem Complex for real m Possibilities for a real determinant: Four fermion models Imaginary m Wilson fermions Two color, isospin density
59 Features of the phase of the determinant MpL, Splittorff, Verbaarschot 2010
60
61
62
63
64
65 All methods work at high T
66 SEARCHING FOR THE QCD CRITICAL POINT
67
68 Back to the complex m plane
69 The radius of convergence (?)
70 Has the critical point of QCD being found?? Nt=4 Nt = 6 Nt=8
71 Lower bound on the radius of convergence And freezout point Data from RBC Collaboration Courtesy E. Laermann and C. Schmidt. C. Ratti and MpL QM09 Freezout point
72 Use imaginary m to validate radius of convergence Falcone, Meyer, Laermann, MpL I m a g i n a r y Check radius of convergence here! c e m i c a l p o t e n t a l Candidate Critical point Observed radius Of convergence T ay l o r e x p a n s i o n
73 Alternative estimate of the radius of convergence Laermann, MpL, Meyer 2013
74 Falcone, Laermann, Meyer, MpL A proposal for a better control on the QCD critical point
75 LHC RHIC NICA /FAIR / RHIC II US NSAC Long RangePlan (adapted)
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