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BT 134.415 716.845 Td /F2 24.0 Tf [(Gauge Field Topology: From Lattice )] TJ ET
BT 99.027 688.333 Td /F2 24.0 Tf [(Simulations and Solvable Models workshop )] TJ ET
BT 252.387 659.821 Td /F2 24.0 Tf [(Talk Schedule)] TJ ET
BT 282.666 620.758 Td /F2 18.0 Tf [(Events for:)] TJ ET
BT 158.898 599.331 Td /F2 18.0 Tf [(Monday, August 17th - Friday, August 21st)] TJ ET
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BT 260.650 563.059 Td /F2 14.0 Tf [(Monday, August 17th)] TJ ET
BT 36.266 545.182 Td /F1 12.0 Tf [(9:00am)] TJ ET
BT 83.497 544.577 Td /F2 12.0 Tf [(Edward Shuryak - SCGP 102)] TJ ET
BT 36.266 524.926 Td /F1 12.0 Tf [(10:00am)] TJ ET
BT 83.497 524.321 Td /F2 12.0 Tf [(Mithat Unsal - SCGP 102)] TJ ET
BT 83.497 494.950 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 494.950 Td /F1 12.0 Tf [(Confinement in compactified SUSY setting )] TJ ET
BT 83.497 466.265 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 466.265 Td /F1 12.0 Tf [(Using the twisted partition function on R3×S1, we argue that the deconfinement phase )] TJ ET
BT 83.497 452.009 Td /F1 12.0 Tf [(transition in pure Yang-Mills theory for all simple gauge groups is continuously connected to a )] TJ ET
BT 83.497 437.753 Td /F1 12.0 Tf [(quantum phase transition that can be studied in a controlled way. We explicitly consider two classes )] TJ ET
BT 83.497 423.497 Td /F1 12.0 Tf [(of theories, gauge theories with a center symmetry, such as SU\(Nc\) gauge theory for arbitrary Nc, )] TJ ET
BT 83.497 409.241 Td /F1 12.0 Tf [(and theories without a center symmetry, such as G2 gauge theory. The mechanism governing the )] TJ ET
BT 83.497 394.985 Td /F1 12.0 Tf [(phase transition is universal and valid for all simple groups. The perturbative one-loop potential as )] TJ ET
BT 83.497 380.729 Td /F1 12.0 Tf [(well as monopole-instantons generate attraction among the eigenvalues of the Wilson line. This is )] TJ ET
BT 83.497 366.473 Td /F1 12.0 Tf [(counter-acted by neutral bions — topological excitations which generate eigenvalue repulsion for )] TJ ET
BT 83.497 352.217 Td /F1 12.0 Tf [(all simple groups. The transition is driven by the competition between these three effects. We study )] TJ ET
BT 83.497 337.961 Td /F1 12.0 Tf [(the transition in more detail for the gauge groups SU\(Nc\), Nc>2, and G2. In the case of G2, there is )] TJ ET
BT 83.497 323.705 Td /F1 12.0 Tf [(no change of symmetry, but the expectation value of the Wilson line exhibits a discontinuity. We )] TJ ET
BT 83.497 309.449 Td /F1 12.0 Tf [(also examine the effect of the ?-angle on the phase transition and critical temperature Tc\(?\). The )] TJ ET
BT 83.497 295.193 Td /F1 12.0 Tf [(critical temperature is a multi-branched function, which has a minimum at ?=? as a result of )] TJ ET
BT 83.497 280.822 Td /F1 12.0 Tf [(topological intereference.)] TJ ET
BT 36.266 237.742 Td /F1 12.0 Tf [(11:00am)] TJ ET
BT 83.497 237.137 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 217.486 Td /F1 12.0 Tf [(11:20am)] TJ ET
BT 83.497 216.881 Td /F2 12.0 Tf [(Ismail Zahed - SCGP 102)] TJ ET
BT 83.497 187.510 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 187.510 Td /F1 12.0 Tf [(Dense instanton-dyon plasma )] TJ ET
BT 36.266 144.430 Td /F1 12.0 Tf [(12:05pm)] TJ ET
BT 83.497 143.825 Td /F2 12.0 Tf [(Yizhuang Liu - SCGP 102)] TJ ET
BT 83.497 114.454 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 114.454 Td /F1 12.0 Tf [(Fermions in a dense instanton-dyon plasma )] TJ ET
BT 36.266 71.374 Td /F1 12.0 Tf [(12:40pm)] TJ ET
BT 83.497 70.769 Td /F2 12.0 Tf [(Lunch - SCGP Cafe)] TJ ET
BT 36.266 51.118 Td /F1 12.0 Tf [(2:00pm)] TJ ET
BT 83.497 50.513 Td /F2 12.0 Tf [(Rasmus Larsen - SCGP 102)] TJ ET
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BT 83.497 732.214 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 732.214 Td /F1 12.0 Tf [(Classical interactions and numerical studies of the instanton-dyon ensemble )] TJ ET
BT 83.497 703.529 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 703.529 Td /F1 12.0 Tf [("Instanton-dyons, also known as instanton-monopoles or instanton-quarks, are )] TJ ET
BT 83.497 689.273 Td /F1 12.0 Tf [(topological constituents of the instantons at nonzero temperature and holonomy. Classical )] TJ ET
BT 83.497 675.017 Td /F1 12.0 Tf [(interactions of the dyons have been found and included in numerical simulations of the ensemble of )] TJ ET
BT 83.497 660.761 Td /F1 12.0 Tf [(interacting dyons for SU\(2\) pure gauge theory. The focus of the talk is the back reaction on the )] TJ ET
BT 83.497 646.505 Td /F1 12.0 Tf [(holonomy and the issue of confinement, but I will also devote time to explain the structure of the )] TJ ET
BT 83.497 632.249 Td /F1 12.0 Tf [(dyons and their classical interactions. The free energy has been calculated as a function of the )] TJ ET
BT 83.497 617.993 Td /F1 12.0 Tf [(holonomy and the dyon densities, using standard Metropolis Monte Carlo and integration over )] TJ ET
BT 83.497 603.737 Td /F1 12.0 Tf [(parameter methods. It is observed that as the temperature decreases and the dyon density grows, the )] TJ ET
BT 83.497 589.481 Td /F1 12.0 Tf [(minimum of the free energy indeed moves from small holonomy to the value corresponding to )] TJ ET
BT 83.497 575.110 Td /F1 12.0 Tf [(confinement.")] TJ ET
BT 36.266 532.030 Td /F1 12.0 Tf [(2:40pm)] TJ ET
BT 83.497 531.425 Td /F2 12.0 Tf [(Tin Sulejmanpasic - SCGP 102)] TJ ET
BT 83.497 502.054 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 502.054 Td /F1 12.0 Tf [(Instanton interactions in \(SUSY\) quantum mechanics )] TJ ET
BT 36.266 458.974 Td /F1 12.0 Tf [(3:20pm)] TJ ET
BT 83.497 458.369 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 438.718 Td /F1 12.0 Tf [(3:40pm)] TJ ET
BT 83.497 438.113 Td /F2 12.0 Tf [(Dmitri Kharzeev - SCGP 102)] TJ ET
BT 83.497 408.742 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 408.742 Td /F1 12.0 Tf [(Overview of the chiral magnetic effect )] TJ ET
BT 36.266 365.662 Td /F1 12.0 Tf [(4:30pm)] TJ ET
BT 83.497 365.057 Td /F2 12.0 Tf [(Huan Huang - SCGP 102)] TJ ET
BT 83.497 335.801 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 335.801 Td /F1 12.0 Tf [(Experimental Searches for Chirality and Magnetic Field Effects in Heavy Ion Collisions at )] TJ ET
BT 83.497 321.430 Td /F1 12.0 Tf [(RHIC)] TJ ET
BT 36.266 278.350 Td /F1 12.0 Tf [(5:00pm)] TJ ET
BT 83.497 277.745 Td /F2 12.0 Tf [(Michael Ogilvie - SCGP 102)] TJ ET
BT 83.497 248.374 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 248.374 Td /F1 12.0 Tf [(A holistic approach to instantons on R^3 x S^1 )] TJ ET
BT 83.497 219.689 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 219.689 Td /F1 12.0 Tf [(Abelianizing deformations provide important tools for understanding the phase structure )] TJ ET
BT 83.497 205.433 Td /F1 12.0 Tf [(and topological excitations in both continuum and lattice field theories. Such deformations typically )] TJ ET
BT 83.497 191.177 Td /F1 12.0 Tf [(produce a rich phase structure, and allow additional analytic control over nonperturbative effects. In )] TJ ET
BT 83.497 176.921 Td /F1 12.0 Tf [(lattice models, Abelianizing deformations typically lead to the emergence of the constituents of )] TJ ET
BT 83.497 162.665 Td /F1 12.0 Tf [(instantons as primary objects. They can also provide a stabilizing mechanism for classically )] TJ ET
BT 83.497 148.409 Td /F1 12.0 Tf [(conformal theories, removing problems in the naive instanton expansion. Finally, Abelianizing )] TJ ET
BT 83.497 134.153 Td /F1 12.0 Tf [(deformations play a crucial role in phenomenological models of QCD at nonzero temperature and )] TJ ET
BT 83.497 119.782 Td /F1 12.0 Tf [(density, thus providing a bridge between theory and phenomenology.)] TJ ET
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BT 260.258 73.447 Td /F2 14.0 Tf [(Tuesday, August 18th)] TJ ET
BT 36.266 55.570 Td /F1 12.0 Tf [(9:00am)] TJ ET
BT 83.497 54.965 Td /F2 12.0 Tf [(Ernst-Michael Ilgenfritz - SCGP 102)] TJ ET
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BT 83.497 732.329 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 732.329 Td /F1 12.0 Tf [(Signatures of dyons or KvBLL calorons from lattice gluodynamics at nonzero temperature )] TJ ET
BT 83.497 718.073 Td /F1 12.0 Tf [(Abstract 1: We will present an overview of attempts and results of a Berlin-ITEP \(Moscow\) )] TJ ET
BT 83.497 703.817 Td /F1 12.0 Tf [(collaboration to establish evidence for Kraan-van Baal/Lee-Lu calorons and fordyon structures in )] TJ ET
BT 83.497 689.561 Td /F1 12.0 Tf [(lattice gauge field ensembles, whichhas begun more than 10 years ago. Some attempts are )] TJ ET
BT 83.497 675.190 Td /F1 12.0 Tf [(alsodescribed to perform simulations of confinement within corresponding models. )] TJ ET
BT 36.266 632.110 Td /F1 12.0 Tf [(9:50am)] TJ ET
BT 83.497 631.505 Td /F2 12.0 Tf [(Michael Muller-Preussker - SCGP 102)] TJ ET
BT 83.497 602.249 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 602.249 Td /F1 12.0 Tf [(Determining the topological susceptibility in lattice QCD at nonzero temperature Abstract 2: )] TJ ET
BT 83.497 587.993 Td /F1 12.0 Tf [(We would like to present an overview of recent determinations of the topological suceptibility in )] TJ ET
BT 83.497 573.737 Td /F1 12.0 Tf [(lattice QCD using \(and comparing\) various smoothing methods, in particular the gradient flow. )] TJ ET
BT 83.497 559.481 Td /F1 12.0 Tf [(How the latter works will be first demonstrated in the simple one-dimensional quantum mechanical )] TJ ET
BT 83.497 545.225 Td /F1 12.0 Tf [(case of an \(un\)harmonic oscillator. Finally we will focus on the topological susceptibility in full )] TJ ET
BT 83.497 530.854 Td /F1 12.0 Tf [(QCD with flavor number N_f=2 and the more realistic case 2+1+1 at non-zero temperature. )] TJ ET
BT 36.266 487.774 Td /F1 12.0 Tf [(10:40am)] TJ ET
BT 83.497 487.169 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 467.518 Td /F1 12.0 Tf [(11:00am)] TJ ET
BT 83.497 466.913 Td /F2 12.0 Tf [(Leonid Glozman - SCGP 102)] TJ ET
BT 83.497 437.542 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 437.542 Td /F1 12.0 Tf [(Hadrons with and without zero-mode-zone )] TJ ET
BT 36.266 394.462 Td /F1 12.0 Tf [(11:50am)] TJ ET
BT 83.497 393.857 Td /F2 12.0 Tf [(Ivan Horvath - SCGP 102)] TJ ET
BT 83.497 364.486 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 364.486 Td /F1 12.0 Tf [(Studies of fermionic zero-mode-zone states )] TJ ET
BT 83.497 335.801 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 335.801 Td /F1 12.0 Tf [(I discuss elements of a long-term effort to characterize QCD vacuum \(and its thermal )] TJ ET
BT 83.497 321.545 Td /F1 12.0 Tf [(states\) in a model-independent manner using lattice QCD. Local behavior of topological density )] TJ ET
BT 83.497 307.289 Td /F1 12.0 Tf [(and properties of \(overlap\) Dirac eigenmodes are given a particular attention. Regarding the latter, )] TJ ET
BT 83.497 293.033 Td /F1 12.0 Tf [(construction of non-Pearson correlations describing chiral polarization of modes will be covered in )] TJ ET
BT 83.497 278.777 Td /F1 12.0 Tf [(some detail, including the proposed equivalence between chiral symmetry breaking and )] TJ ET
BT 83.497 264.521 Td /F1 12.0 Tf [(condensation of local chirality defined accordingly. In the last part of the talk, recent developments )] TJ ET
BT 83.497 250.265 Td /F1 12.0 Tf [(suggesting connections between the properties of Dirac modes and confinement are discussed, )] TJ ET
BT 83.497 236.009 Td /F1 12.0 Tf [(emphasizing the existence of deconfined phase with broken valence chiral symmetry in thermal )] TJ ET
BT 83.497 221.638 Td /F1 12.0 Tf [(QCD, and in systems with many light fundamental flavors.)] TJ ET
BT 36.266 178.558 Td /F1 12.0 Tf [(12:40pm)] TJ ET
BT 83.497 177.953 Td /F2 12.0 Tf [(Lunch - SCGP Cafe)] TJ ET
BT 36.266 158.302 Td /F1 12.0 Tf [(2:00pm)] TJ ET
BT 83.497 157.697 Td /F2 12.0 Tf [(Sayatan Sharma - SCGP 102)] TJ ET
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BT 83.497 732.214 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 732.214 Td /F1 12.0 Tf [(The axial U\(1\) anomaly and topological structures in finite temperature QCD )] TJ ET
BT 83.497 703.529 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 703.529 Td /F1 12.0 Tf [(The magnitude of axial U\(1\) symmetry breaking is believed to affect nature of Nf = 2 )] TJ ET
BT 83.497 689.273 Td /F1 12.0 Tf [(QCD chiral phase transition. The explicit breaking of chiral symmetry due to realistic light quark )] TJ ET
BT 83.497 675.017 Td /F1 12.0 Tf [(masses is small hence it is important to use fermions which do not break chiral symmetry on the )] TJ ET
BT 83.497 660.761 Td /F1 12.0 Tf [(lattice, to understand the fate of axial U\(1\) near the chiral crossover temperature, Tc. I discuss on )] TJ ET
BT 83.497 646.505 Td /F1 12.0 Tf [(our recent study of the eigenvalue spectrum of QCD with two different lattice fermion )] TJ ET
BT 83.497 632.249 Td /F1 12.0 Tf [(discretizations which retain a remnant of the continuum chiral symmetry, using exact chiral overlap )] TJ ET
BT 83.497 617.993 Td /F1 12.0 Tf [(fermions as probes. From the eigenvalue spectrum of the overlap operator, we do not observe any )] TJ ET
BT 83.497 603.737 Td /F1 12.0 Tf [(hints of the effective restoration of axial U\(1\) near Tc. A pile up of the near-zero eigenmodes is )] TJ ET
BT 83.497 589.481 Td /F1 12.0 Tf [(observed to persist even at 1.5Tc which are primarily responsible for its breaking. These )] TJ ET
BT 83.497 575.225 Td /F1 12.0 Tf [(eigenmodes are localized unlike those in the bulk, with a mobility edge similar to a Mott-Anderson )] TJ ET
BT 83.497 560.969 Td /F1 12.0 Tf [(like system. The origin of such near-zero mode spectrum can be traced back to the dilute instanton )] TJ ET
BT 83.497 546.598 Td /F1 12.0 Tf [(gas ensemble already setting in at 1.5 Tc.)] TJ ET
BT 36.266 503.518 Td /F1 12.0 Tf [(2:45pm)] TJ ET
BT 83.497 502.913 Td /F2 12.0 Tf [(Maria Lombardo - SCGP 102)] TJ ET
BT 83.497 473.657 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 473.657 Td /F1 12.0 Tf [(Scale separation, walking dynamics and approach to criticality in QCD with varying number )] TJ ET
BT 83.497 459.286 Td /F1 12.0 Tf [(of flavors. )] TJ ET
BT 83.497 430.601 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 430.601 Td /F1 12.0 Tf [(QCD with Nf fundamental fermions has a rich phase structure which has been explored )] TJ ET
BT 83.497 416.345 Td /F1 12.0 Tf [(with analytic and numerical studies. In the massless case and at zero temperature an essential )] TJ ET
BT 83.497 402.089 Td /F1 12.0 Tf [(singularity is expected to separate the QCD-like phase from the conformal phase, and this should be )] TJ ET
BT 83.497 387.833 Td /F1 12.0 Tf [(reflected by Miransky scaling of infrared observables. In turn, the conformal phase can be seen as )] TJ ET
BT 83.497 373.577 Td /F1 12.0 Tf [(the zero temperature limit of a \(strongly\)interactive quark gluon plasma when the number of flavors )] TJ ET
BT 83.497 359.321 Td /F1 12.0 Tf [(approach its critical value. In lattice simulations a nonzero quark mass is usually included, and )] TJ ET
BT 83.497 345.065 Td /F1 12.0 Tf [(conformality is explicitely broken, with two main consequences: a\) The would-be conformal phase )] TJ ET
BT 83.497 330.809 Td /F1 12.0 Tf [(is continuously connected with the QCD-like phase and features of the conformal phase such as the )] TJ ET
BT 83.497 316.553 Td /F1 12.0 Tf [(anomalous dimension are still observable below the critical number of flavors; b\)The critical )] TJ ET
BT 83.497 302.297 Td /F1 12.0 Tf [(singularity disappears however ratios of homogeneous observables still carry an imprinting of the )] TJ ET
BT 83.497 288.041 Td /F1 12.0 Tf [(critical dynamics. The talk is a brief overview of these phenomena, elucidated by the behaviour of )] TJ ET
BT 83.497 273.785 Td /F1 12.0 Tf [(the \(pseudo\)critical temperature, mass spectrum, string tension and Wilson flow in the )] TJ ET
BT 83.497 259.414 Td /F1 12.0 Tf [(preconformal region.)] TJ ET
BT 36.266 216.334 Td /F1 12.0 Tf [(3:30pm)] TJ ET
BT 83.497 215.729 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 196.078 Td /F1 12.0 Tf [(4:00pm)] TJ ET
BT 83.497 195.473 Td /F2 12.0 Tf [(Kenji Fukushima - SCGP 102)] TJ ET
BT 83.497 166.102 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 166.102 Td /F1 12.0 Tf [(QCD under curvature and magnetic effects )] TJ ET
BT 36.266 123.022 Td /F1 12.0 Tf [(5:15pm)] TJ ET
BT 83.497 122.417 Td /F2 12.0 Tf [(Vasily Sazonov - SCGP 102)] TJ ET
BT 83.497 93.046 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 93.046 Td /F1 12.0 Tf [(Convergent Series)] TJ ET
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BT 250.927 46.711 Td /F2 14.0 Tf [(Wednesday, August 19th)] TJ ET
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BT 36.266 744.934 Td /F1 12.0 Tf [(9:00am)] TJ ET
BT 83.497 744.329 Td /F2 12.0 Tf [(Misha Shifman - SCGP 102)] TJ ET
BT 83.497 714.958 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 714.958 Td /F1 12.0 Tf [(Topological defects in Yang-Mills with non-abelian moduli and their implications. )] TJ ET
BT 83.497 686.273 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 686.273 Td /F1 12.0 Tf [("I discuss developments of the last decade in Yang-Mills theories \(including those at )] TJ ET
BT 83.497 672.017 Td /F1 12.0 Tf [(strong coupling\) with or without supersymmetry. I focus on the progress in understanding non-)] TJ ET
BT 83.497 657.761 Td /F1 12.0 Tf [(Abelian dynamics, 2D-4D correspondence and various applications. In the supersymmetric case )] TJ ET
BT 83.497 643.390 Td /F1 12.0 Tf [(remarkable exact results ensue.")] TJ ET
BT 36.266 600.310 Td /F1 12.0 Tf [(10:00am)] TJ ET
BT 83.497 599.705 Td /F2 12.0 Tf [(Gerald Dunne - SCGP 102)] TJ ET
BT 83.497 570.334 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 570.334 Td /F1 12.0 Tf [(Overview of the resurgence program )] TJ ET
BT 36.266 527.254 Td /F1 12.0 Tf [(11:00am)] TJ ET
BT 83.497 526.649 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 506.998 Td /F1 12.0 Tf [(11:20am)] TJ ET
BT 83.497 506.393 Td /F2 12.0 Tf [(Ariel Zhitnitsky - SCGP 102)] TJ ET
BT 83.497 477.022 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 477.022 Td /F1 12.0 Tf [(Vacuum energy, contact term and all that in gauge systems with nontrivial holonomy )] TJ ET
BT 83.497 448.337 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 448.337 Td /F1 12.0 Tf [( I present few highly nontrivial features of the gauge theories when the configurations )] TJ ET
BT 83.497 434.081 Td /F1 12.0 Tf [(with nontrivial holonomy play the crucial role in dynamics. First example is the computation of the )] TJ ET
BT 83.497 419.825 Td /F1 12.0 Tf [(contact term in a weakly coupled gauge theory, the so-called "deformed QCD". I argue that the )] TJ ET
BT 83.497 405.569 Td /F1 12.0 Tf [(configurations with nontrivial holonomy saturate the contact term which was conjectured for )] TJ ET
BT 83.497 391.313 Td /F1 12.0 Tf [(strongly coupled QCD long ago by Witten and Veneziano. Second example is computations of the )] TJ ET
BT 83.497 377.057 Td /F1 12.0 Tf [(contact term in nontrivial curved hyperbolic background. I argue that correction to the energy is )] TJ ET
BT 83.497 362.801 Td /F1 12.0 Tf [(linear in inverse size of the system L^{-1}. The correction is expressed in terms of gauge invariant )] TJ ET
BT 83.497 348.545 Td /F1 12.0 Tf [(holonomy, but can not be formulated in terms of local operators. It might be the key element in )] TJ ET
BT 83.497 334.289 Td /F1 12.0 Tf [(understanding of the observed cosmological dark energy, which is interpreted in this framework as )] TJ ET
BT 83.497 319.918 Td /F1 12.0 Tf [(the modification of the QCD vacuum energy in topologically nontrivial background. )] TJ ET
BT 36.266 276.838 Td /F1 12.0 Tf [(12:05pm)] TJ ET
BT 83.497 276.233 Td /F2 12.0 Tf [(Yachao Qian - SCGP 102)] TJ ET
BT 83.497 246.862 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 246.862 Td /F1 12.0 Tf [(Spin Asymmetries and P-odd Effects through QCD Instantons)] TJ ET
BT 36.266 203.782 Td /F1 12.0 Tf [(12:50pm)] TJ ET
BT 83.497 203.177 Td /F2 12.0 Tf [(Juven Wang \(IAS Princeton\) - SCGP 102)] TJ ET
BT 83.497 173.806 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 173.806 Td /F1 12.0 Tf [(Quantum Statistics, Spacetime Topology and Lattice Chiral Fermions of Condensed Matter )] TJ ET
BT 36.266 130.726 Td /F1 12.0 Tf [(1:35pm)] TJ ET
BT 83.497 130.121 Td /F2 12.0 Tf [(Lunch - SCGP Cafe)] TJ ET
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BT 256.366 107.215 Td /F2 14.0 Tf [(Thursday, August 20th)] TJ ET
BT 36.266 89.338 Td /F1 12.0 Tf [(9:00am)] TJ ET
BT 83.497 88.733 Td /F2 12.0 Tf [(Jeff Greensite - SCGP 102)] TJ ET
endstream
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BT 83.497 732.214 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 732.214 Td /F1 12.0 Tf [( Confinement via center vortices )] TJ ET
BT 83.497 703.529 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 703.529 Td /F1 12.0 Tf [( I review the motivation and numerical evidence for the center vortex confinement )] TJ ET
BT 83.497 689.158 Td /F1 12.0 Tf [(mechanism.)] TJ ET
BT 36.266 646.078 Td /F1 12.0 Tf [(10:00am)] TJ ET
BT 83.497 645.473 Td /F2 12.0 Tf [(Kej-Ichi Kondo - SCGP 102)] TJ ET
BT 83.497 616.102 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 616.102 Td /F1 12.0 Tf [(Monopoles and confinement )] TJ ET
BT 83.497 587.417 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 587.417 Td /F1 12.0 Tf [(We give a review on the recent developments on quark confinement from the viewpoint )] TJ ET
BT 83.497 573.161 Td /F1 12.0 Tf [(of dual superconductivity based on [Physics Report Vol.579, pp.1--226 \(2015\)]. First, we give the )] TJ ET
BT 83.497 558.905 Td /F1 12.0 Tf [(SU\(N\) extension of the Diakonov-Petrov version of the non-Abelian Stokes theorem for the Wilson )] TJ ET
BT 83.497 544.649 Td /F1 12.0 Tf [(loop operator to give a gauge-invariant definition for the magnetic monopole in the SU\(N\) Yang-)] TJ ET
BT 83.497 530.393 Td /F1 12.0 Tf [(Mills theory without the scalar field. Second, we give a new framework for reformulating the )] TJ ET
BT 83.497 516.137 Td /F1 12.0 Tf [(SU\(N\) Yang-Mills theory using new field variables. This includes the preceding works on field )] TJ ET
BT 83.497 501.881 Td /F1 12.0 Tf [(decompositions given by Cho, Duan and Ge, Faddeev and Niemi, as a special case called the )] TJ ET
BT 83.497 487.625 Td /F1 12.0 Tf [(maximal option in our reformulations. An advantage of the reformulations is that the original Yang-)] TJ ET
BT 83.497 473.369 Td /F1 12.0 Tf [(Mills gauge field variables can be changed into the new field variables such that one of them called )] TJ ET
BT 83.497 459.113 Td /F1 12.0 Tf [(the restricted field gives the dominant contribution to quark confinement in the gauge-independent )] TJ ET
BT 83.497 444.857 Td /F1 12.0 Tf [(way. Then, our reformulations can be combined with the non-Abelian Stokes theorem. In the so-)] TJ ET
BT 83.497 430.601 Td /F1 12.0 Tf [(called minimal option, especially, the restricted field is non-Abelian and involves the non-Abelian )] TJ ET
BT 83.497 416.345 Td /F1 12.0 Tf [(magnetic monopole with the stability group U\(N-1\). This suggests the non-Abelian dual )] TJ ET
BT 83.497 402.089 Td /F1 12.0 Tf [(superconductivity picture for quark confinement. This should be compared with the maximal )] TJ ET
BT 83.497 387.833 Td /F1 12.0 Tf [(option: the restricted field is Abelian and involves only the Abelian magnetic monopoles with the )] TJ ET
BT 83.497 373.577 Td /F1 12.0 Tf [(stability group U\(1\)$^{N-1}$, just like the Abelian projection. Third, we give the lattice version of )] TJ ET
BT 83.497 359.321 Td /F1 12.0 Tf [(the reformulations of the SU\(N\) Yang-Mills theory and present the results of the numerical )] TJ ET
BT 83.497 345.065 Td /F1 12.0 Tf [(simulations of the SU\(3\) Yang-Mills theory on a lattice. The numerical simulations include the )] TJ ET
BT 83.497 330.809 Td /F1 12.0 Tf [(derivation of the linear potential for static interquark potential, i.e., non-vanishing string tension, in )] TJ ET
BT 83.497 316.553 Td /F1 12.0 Tf [(which the restricted field dominance and magnetic monopole dominance are established, )] TJ ET
BT 83.497 302.297 Td /F1 12.0 Tf [(confirmation of the dual Meissner effect by measuring the chromoelectric flux tube between quark-)] TJ ET
BT 83.497 287.926 Td /F1 12.0 Tf [(antiquark pair, the induced magnetic-monopole current, and the type of dual superconductivity, etc.)] TJ ET
BT 36.266 244.846 Td /F1 12.0 Tf [(11:00am)] TJ ET
BT 83.497 244.241 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 224.590 Td /F1 12.0 Tf [(11:20am)] TJ ET
BT 83.497 223.985 Td /F2 12.0 Tf [(Chris Korthals-Altes - SCGP 102)] TJ ET
BT 83.497 194.614 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 194.614 Td /F1 12.0 Tf [(The magnetic component of the QCD plasma. )] TJ ET
BT 83.497 165.929 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 165.929 Td /F1 12.0 Tf [(I review the necessity of a magnetic component in the QCD plasma, as seen by lattice )] TJ ET
BT 83.497 151.558 Td /F1 12.0 Tf [(simulations of spatial Wilsonloops.)] TJ ET
BT 36.266 108.478 Td /F1 12.0 Tf [(12:00pm)] TJ ET
BT 83.497 107.873 Td /F2 12.0 Tf [(Peter Petreczky - SCGP 102)] TJ ET
BT 83.497 78.502 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 78.502 Td /F1 12.0 Tf [(The Polyakov loop from the lattice )] TJ ET
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BT 36.266 744.934 Td /F1 12.0 Tf [(12:40pm)] TJ ET
BT 83.497 744.329 Td /F2 12.0 Tf [(Lunch: - SCGP Cafe)] TJ ET
BT 36.266 724.678 Td /F1 12.0 Tf [(3:30pm)] TJ ET
BT 83.497 724.073 Td /F2 12.0 Tf [(Coffee Break - SCGP 102)] TJ ET
BT 36.266 704.422 Td /F1 12.0 Tf [(4:00pm)] TJ ET
BT 83.497 703.817 Td /F2 12.0 Tf [(Jinfeng Liao - SCGP 102)] TJ ET
BT 83.497 674.446 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 674.446 Td /F1 12.0 Tf [(Electric flux tube and thermal monopoles in the deconfined phase )] TJ ET
BT 83.497 645.761 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 645.761 Td /F1 12.0 Tf [(The QCD vacuum structure and the mechanism for confinement provides a persistent )] TJ ET
BT 83.497 631.505 Td /F1 12.0 Tf [(challenge to our understanding of nonperturbative gauge dynamics. One compelling idea is to )] TJ ET
BT 83.497 617.249 Td /F1 12.0 Tf [(consider the vacuum as a monopole condensate and the confinement/deconfinement transition as )] TJ ET
BT 83.497 602.993 Td /F1 12.0 Tf [(the Bose condensation of monopoles. In recent years a new route to explore this idea has been )] TJ ET
BT 83.497 588.737 Td /F1 12.0 Tf [(proposed, namely to understand confinement from above i.e. in the deconfined phase, by studying )] TJ ET
BT 83.497 574.481 Td /F1 12.0 Tf [(the thermal monopole ensemble in the vicinity of Tc. The so-called ``magnetic scenario'' suggests )] TJ ET
BT 83.497 560.225 Td /F1 12.0 Tf [(that an ensemble of abundant and light thermal monopoles emerges above Tc and reaches )] TJ ET
BT 83.497 545.969 Td /F1 12.0 Tf [(condensation condition at Tc thus leading to confinement transition. In this talk we focus on how )] TJ ET
BT 83.497 531.713 Td /F1 12.0 Tf [(such a scenario sheds light on two interesting phenomena: \(1\) the survival of extended electric flux )] TJ ET
BT 83.497 517.457 Td /F1 12.0 Tf [(tube into the deconfined phase as indicated by the static Q-bar-Q potentials; \(2\) the dependence of )] TJ ET
BT 83.497 503.201 Td /F1 12.0 Tf [(the confinement transition parameters on the fermion contents, which provides a unique test of the )] TJ ET
BT 83.497 488.945 Td /F1 12.0 Tf [(the mechanism of confinement as monopole condensation. Lastly we briefly comment upon how )] TJ ET
BT 83.497 474.689 Td /F1 12.0 Tf [(these monopoles behave as a color-opaque low-viscosity matter and help understand a few key )] TJ ET
BT 83.497 460.433 Td /F1 12.0 Tf [(properties of the quark-gluon plasma observed in heavy ion collision experiments. [References: )] TJ ET
BT 83.497 446.177 Td /F1 12.0 Tf [(Jinfeng Liao & Edward Shuryak, PRL109\(2012\)152001; PRD82\(2010\)094007; )] TJ ET
BT 83.497 431.806 Td /F1 12.0 Tf [(PRL101\(2008\)162302; PRC75\(2007\)054907.])] TJ ET
BT 36.266 388.726 Td /F1 12.0 Tf [(4:40pm)] TJ ET
BT 83.497 388.121 Td /F2 12.0 Tf [(Claudia Ratti - SCGP 102)] TJ ET
BT 83.497 358.750 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 358.750 Td /F1 12.0 Tf [(Thermal monopoles and kinetics of sQGP )] TJ ET
BT 36.266 315.670 Td /F1 12.0 Tf [(5:20pm)] TJ ET
BT 83.497 315.065 Td /F2 12.0 Tf [(Shu Lin - SCGP 102)] TJ ET
BT 83.497 285.694 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 285.694 Td /F1 12.0 Tf [(The Polyakov loop potential and semi-QGP )] TJ ET
BT 83.497 257.009 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 257.009 Td /F1 12.0 Tf [(I will discuss lattice results on gauge theory thermodynamics and Polyakov loop. In )] TJ ET
BT 83.497 242.753 Td /F1 12.0 Tf [(temperature window 1.2~2Tc, the interaction measure features a T^2 scaling law and smooth rising )] TJ ET
BT 83.497 228.497 Td /F1 12.0 Tf [(of Polyakov loop. This is the regime of semi-QGP with the scaling law and behavior of Polyakov )] TJ ET
BT 83.497 214.241 Td /F1 12.0 Tf [(loop due to non-perturbative effect. I will discuss model of semi-QGP and the non-perturbative )] TJ ET
BT 83.497 199.870 Td /F1 12.0 Tf [(effect on gluons and quarks. I will also discuss its phenomenological implications.)] TJ ET
BT 36.266 156.790 Td /F1 12.0 Tf [(6:00pm)] TJ ET
BT 83.497 156.185 Td /F2 12.0 Tf [(Jiechen Xu - SCGP 102)] TJ ET
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BT 83.497 732.214 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 732.214 Td /F1 12.0 Tf [(The sQGP as semi-quark-gluon & monopole plasma \(sQGMP\) )] TJ ET
BT 83.497 703.529 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 703.529 Td /F1 12.0 Tf [(In relativistic heavy-ion collisions at RHIC and LHC, it has been a long-standing puzzle )] TJ ET
BT 83.497 689.273 Td /F1 12.0 Tf [(for all pQCD based jet energy loss models to simultaneously explain data on the high $p_T$ )] TJ ET
BT 83.497 675.017 Td /F1 12.0 Tf [(nuclear modification factor and azimuthal asymmetry of light hadrons/open heavy flavors. In this )] TJ ET
BT 83.497 660.761 Td /F1 12.0 Tf [(talk, I will present a new jet quenching framework, CUJET3.0, where three novel features of )] TJ ET
BT 83.497 646.505 Td /F1 12.0 Tf [(nonperturbative physics origin are integrated in the pQCD opacity expansion theory: \(1\) the )] TJ ET
BT 83.497 632.249 Td /F1 12.0 Tf [(Polyakov loop suppression of color-electric scatterings \(a.k.a. "semi-QGP" of Pisarski et al.\) and )] TJ ET
BT 83.497 617.993 Td /F1 12.0 Tf [(\(2\) the enhancement of jet scattering due to emergent chromomagnetic monopoles near $T_c$ )] TJ ET
BT 83.497 603.737 Td /F1 12.0 Tf [(\(a.k.a. "magnetic scenario" of Liao and Shuryak\) and \(3\) thermodynamic properties constrained by )] TJ ET
BT 83.497 589.481 Td /F1 12.0 Tf [(lattice QCD data. CUJET3.0 reduces to the pQCD limit at high temperatures $T > 400$ MeV; but )] TJ ET
BT 83.497 575.225 Td /F1 12.0 Tf [(thanks to the presence of the semi-quark-gluon monopole plasma \(sQGMP\) near the QCD )] TJ ET
BT 83.497 560.969 Td /F1 12.0 Tf [(deconfinement transition temperature, it greatly enhances the jet quenching parameter $\\hat{q}$ in )] TJ ET
BT 83.497 546.713 Td /F1 12.0 Tf [(this temperature range. This enhancement renders a perfect description of the observed high $p_T$ )] TJ ET
BT 83.497 532.457 Td /F1 12.0 Tf [(jet suppression factor and elliptic harmonics simultaneously. Extrapolating the data-constrained )] TJ ET
BT 83.497 518.201 Td /F1 12.0 Tf [($\\hat{q}$ down to thermal energy scales, $E \\sim 2$ GeV, a remarkable consistency between the )] TJ ET
BT 83.497 503.945 Td /F1 12.0 Tf [(high energy jet quenching and bulk perfect fluidity with $\\eta/s\\sim T^3/\\hat{q} \\sim 0.1$ near )] TJ ET
BT 83.497 489.574 Td /F1 12.0 Tf [($T_c$ is found for the first time.)] TJ ET
BT 36.266 446.494 Td /F1 12.0 Tf [(6:30pm)] TJ ET
BT 83.497 445.889 Td /F2 12.0 Tf [(Workshop Banquet)] TJ ET
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BT 266.488 422.983 Td /F2 14.0 Tf [(Friday, August 21st)] TJ ET
BT 36.266 405.106 Td /F1 12.0 Tf [(9:00am)] TJ ET
BT 83.497 404.501 Td /F2 12.0 Tf [(Adam Szczepaniak - SCGP 102)] TJ ET
BT 83.497 375.130 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 375.130 Td /F1 12.0 Tf [(Couloumb gauge confinement and emerging phenomenology )] TJ ET
BT 36.266 332.050 Td /F1 12.0 Tf [(10:00am)] TJ ET
BT 83.497 331.445 Td /F2 12.0 Tf [(Alexander Turbiner - SCGP 102)] TJ ET
BT 83.497 302.074 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 302.074 Td /F1 12.0 Tf [(Energy gap in quantum mechanics: double well potential )] TJ ET
BT 83.497 273.389 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 273.389 Td /F1 12.0 Tf [(Exploring the Schr\\"odinger equation the locally accurate wave function of the ground )] TJ ET
BT 83.497 259.133 Td /F1 12.0 Tf [(\(and the first excited\) states will be constructed for 1D double well potential for weak, intermediate )] TJ ET
BT 83.497 244.877 Td /F1 12.0 Tf [(and strong coupling. As for 3D case the example of hydrogen molecular ion will be considered )] TJ ET
BT 83.497 230.506 Td /F1 12.0 Tf [(briefly)] TJ ET
BT 36.266 187.426 Td /F1 12.0 Tf [(11:00am)] TJ ET
BT 83.497 186.821 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 167.170 Td /F1 12.0 Tf [(11:30am)] TJ ET
BT 83.497 166.565 Td /F2 12.0 Tf [(Ismail Zahed - SCGP 102)] TJ ET
BT 83.497 137.194 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 137.194 Td /F1 12.0 Tf [(Holographic Pomeron )] TJ ET
BT 36.266 94.114 Td /F1 12.0 Tf [(12:30pm)] TJ ET
BT 83.497 93.509 Td /F2 12.0 Tf [(Lunch - SCGP Cafe)] TJ ET
BT 36.266 73.858 Td /F1 12.0 Tf [(2:00pm)] TJ ET
BT 83.497 73.253 Td /F2 12.0 Tf [(Ioannis Iatrakis - SCGP 102)] TJ ET
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BT 83.497 732.214 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 732.214 Td /F1 12.0 Tf [(QCD strings and their interactions from the holographic perspective )] TJ ET
BT 36.266 689.134 Td /F1 12.0 Tf [(2:50pm)] TJ ET
BT 83.497 688.529 Td /F2 12.0 Tf [(T. Iritani - SCGP 102)] TJ ET
BT 83.497 659.158 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 659.158 Td /F1 12.0 Tf [(QCD strings on the lattice )] TJ ET
BT 83.497 630.473 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 630.473 Td /F1 12.0 Tf [( In the QCD vacuum, quarks are confined inside hadrons, which can be understood by a )] TJ ET
BT 83.497 616.217 Td /F1 12.0 Tf [(linear rising interquark potential. This linear potential is produced by the string structure of chromo )] TJ ET
BT 83.497 601.961 Td /F1 12.0 Tf [(fields between quarks. We introduce how to observe this phenomenological QCD string in lattice )] TJ ET
BT 83.497 587.705 Td /F1 12.0 Tf [(QCD. Besides the mechanism of quark confinement, QCD string would cause interesting )] TJ ET
BT 83.497 573.449 Td /F1 12.0 Tf [(phenomena. For example, we demonstrate the non-trivial modification of chiral condensate in the )] TJ ET
BT 83.497 559.193 Td /F1 12.0 Tf [(presence of QCD string. We also discuss more precise determination of QCD string features using )] TJ ET
BT 83.497 544.822 Td /F1 12.0 Tf [(gradient flow.)] TJ ET
BT 36.266 501.742 Td /F1 12.0 Tf [(3:30pm)] TJ ET
BT 83.497 501.137 Td /F2 12.0 Tf [(Coffee Break & Workshop Closing - SCGP Cafe)] TJ ET
BT 36.266 481.486 Td /F1 12.0 Tf [(4:00pm)] TJ ET
BT 83.497 480.881 Td /F2 12.0 Tf [(Tigran Kalaydzhyan - SCGP 102)] TJ ET
BT 83.497 451.510 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 451.510 Td /F1 12.0 Tf [(QCD string interactions and implications for high energy collisions )] TJ ET
BT 83.497 422.825 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 422.825 Td /F1 12.0 Tf [(In this talk I would like to introduce an idea of interaction between QCD strings and )] TJ ET
BT 83.497 408.569 Td /F1 12.0 Tf [(discuss some of the consequences for the nucleus-nucleus \(AA\) and proton-nucleus \(pA\) collisions. )] TJ ET
BT 83.497 394.313 Td /F1 12.0 Tf [(From the academic point of view, the interaction provides new \(high entropy\) regimes of the string )] TJ ET
BT 83.497 380.057 Td /F1 12.0 Tf [(behavior near the Hagedorn point. Among the applications are the onset of the explosive regime in )] TJ ET
BT 83.497 365.801 Td /F1 12.0 Tf [(pA collisions, elliptic flow in pA collisions, jet quenching in the mixed phase, modification of the )] TJ ET
BT 83.497 351.545 Td /F1 12.0 Tf [(particle spectra in high-energy cosmic rays, etc. I will also comment on the evidence of similar )] TJ ET
BT 83.497 337.289 Td /F1 12.0 Tf [(collective phenomena in proton-proton \(pp\) collisions. The talk is based on recent papers )] TJ ET
BT 83.497 322.918 Td /F1 12.0 Tf [(1402.7363 \(PRD\), 1404.1888 \(PRC\), 1503.05213 \(PRC\))] TJ ET
BT 36.266 279.838 Td /F1 12.0 Tf [(4:30pm)] TJ ET
BT 83.497 279.233 Td /F2 12.0 Tf [(Rob Pisarski & Edward Shuryak - SCGP 102)] TJ ET
BT 83.497 249.862 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 249.862 Td /F1 12.0 Tf [(Concluding remarks)] TJ ET
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