%PDF-1.3
1 0 obj
<< /Type /Catalog
/Outlines 2 0 R
/Pages 3 0 R >>
endobj
2 0 obj
<< /Type /Outlines /Count 0 >>
endobj
3 0 obj
<< /Type /Pages
/Kids [6 0 R
10 0 R
12 0 R
14 0 R
16 0 R
18 0 R
20 0 R
22 0 R
24 0 R
26 0 R
]
/Count 10
/Resources <<
/ProcSet 4 0 R
/Font <<
/F1 8 0 R
/F2 9 0 R
>>
>>
/MediaBox [0.000 0.000 612.000 792.000]
>>
endobj
4 0 obj
[/PDF /Text ]
endobj
5 0 obj
<<
/Creator (DOMPDF)
/CreationDate (D:20180623211402+00'00')
/ModDate (D:20180623211402+00'00')
/Title (SGCP Calendar)
>>
endobj
6 0 obj
<< /Type /Page
/Parent 3 0 R
/Contents 7 0 R
>>
endobj
7 0 obj
<<
/Length 3712 >>
stream
0.000 0.000 0.000 rg
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
0.800 0.800 0.800 rg
82.747 558.232 485.320 19.632 re f
0.000 0.000 0.000 RG
0.75 w 0 J [ ] 0 d
83.872 559.357 483.070 17.382 re S
0.000 0.000 0.000 rg
BT 260.650 563.059 Td /F2 14.0 Tf [(Monday, August 17th)] TJ ET
BT 36.266 544.577 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 36.266 521.321 Td /F1 12.0 Tf [(10:00am)] TJ ET
BT 83.497 521.321 Td /F2 12.0 Tf [(Mithat Unsal - SCGP 102)] TJ ET
BT 83.497 488.950 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 488.950 Td /F1 12.0 Tf [(Confinement in compactified SUSY setting )] TJ ET
BT 83.497 460.265 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 460.265 Td /F1 12.0 Tf [(Using the twisted partition function on R3×S1, we argue that the deconfinement phase )] TJ ET
BT 83.497 446.009 Td /F1 12.0 Tf [(transition in pure Yang-Mills theory for all simple gauge groups is continuously connected to a )] TJ ET
BT 83.497 431.753 Td /F1 12.0 Tf [(quantum phase transition that can be studied in a controlled way. We explicitly consider two classes )] TJ ET
BT 83.497 417.497 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 83.497 403.241 Td /F1 12.0 Tf [(and theories without a center symmetry, such as G2 gauge theory. The mechanism governing the )] TJ ET
BT 83.497 388.985 Td /F1 12.0 Tf [(phase transition is universal and valid for all simple groups. The perturbative one-loop potential as )] TJ ET
BT 83.497 374.729 Td /F1 12.0 Tf [(well as monopole-instantons generate attraction among the eigenvalues of the Wilson line. This is )] TJ ET
BT 83.497 360.473 Td /F1 12.0 Tf [(counter-acted by neutral bions — topological excitations which generate eigenvalue repulsion for )] TJ ET
BT 83.497 346.217 Td /F1 12.0 Tf [(all simple groups. The transition is driven by the competition between these three effects. We study )] TJ ET
BT 83.497 331.961 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 83.497 317.705 Td /F1 12.0 Tf [(no change of symmetry, but the expectation value of the Wilson line exhibits a discontinuity. We )] TJ ET
BT 83.497 303.449 Td /F1 12.0 Tf [(also examine the effect of the θ-angle on the phase transition and critical temperature Tc\(θ\). The )] TJ ET
BT 83.497 289.193 Td /F1 12.0 Tf [(critical temperature is a multi-branched function, which has a minimum at θ=π as a result of )] TJ ET
BT 83.497 274.822 Td /F1 12.0 Tf [(topological intereference.)] TJ ET
BT 36.266 231.137 Td /F1 12.0 Tf [(11:00am)] TJ ET
BT 83.497 231.137 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 207.881 Td /F1 12.0 Tf [(11:20am)] TJ ET
BT 83.497 207.881 Td /F2 12.0 Tf [(Ismail Zahed - SCGP 102)] TJ ET
BT 83.497 175.510 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 175.510 Td /F1 12.0 Tf [(Dense instanton-dyon plasma )] TJ ET
BT 36.266 131.825 Td /F1 12.0 Tf [(12:05pm)] TJ ET
BT 83.497 131.825 Td /F2 12.0 Tf [(Yizhuang Liu - SCGP 102)] TJ ET
BT 83.497 99.454 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 99.454 Td /F1 12.0 Tf [(Fermions in a dense instanton-dyon plasma )] TJ ET
BT 36.266 55.769 Td /F1 12.0 Tf [(12:40pm)] TJ ET
BT 83.497 55.769 Td /F2 12.0 Tf [(Lunch - SCGP Cafe)] TJ ET
endstream
endobj
8 0 obj
<< /Type /Font
/Subtype /Type1
/Name /F1
/BaseFont /Times-Roman
/Encoding /WinAnsiEncoding
>>
endobj
9 0 obj
<< /Type /Font
/Subtype /Type1
/Name /F2
/BaseFont /Times-Bold
/Encoding /WinAnsiEncoding
>>
endobj
10 0 obj
<< /Type /Page
/Parent 3 0 R
/Contents 11 0 R
>>
endobj
11 0 obj
<<
/Length 2850 >>
stream
0.000 0.000 0.000 rg
0.000 0.000 0.000 RG
0.75 w 0 J [ ] 0 d
BT 36.266 702.064 Td /F1 12.0 Tf [(2:00pm)] TJ ET
BT 83.497 702.064 Td /F2 12.0 Tf [(Rasmus Larsen - SCGP 102)] TJ ET
BT 83.497 669.693 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 669.693 Td /F1 12.0 Tf [(Classical interactions and numerical studies of the instanton-dyon ensemble )] TJ ET
BT 83.497 641.008 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 641.008 Td /F1 12.0 Tf [("Instanton-dyons, also known as instanton-monopoles or instanton-quarks, are )] TJ ET
BT 83.497 626.752 Td /F1 12.0 Tf [(topological constituents of the instantons at nonzero temperature and holonomy. Classical )] TJ ET
BT 83.497 612.496 Td /F1 12.0 Tf [(interactions of the dyons have been found and included in numerical simulations of the ensemble of )] TJ ET
BT 83.497 598.240 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 83.497 583.984 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 83.497 569.728 Td /F1 12.0 Tf [(dyons and their classical interactions. The free energy has been calculated as a function of the )] TJ ET
BT 83.497 555.472 Td /F1 12.0 Tf [(holonomy and the dyon densities, using standard Metropolis Monte Carlo and integration over )] TJ ET
BT 83.497 541.216 Td /F1 12.0 Tf [(parameter methods. It is observed that as the temperature decreases and the dyon density grows, the )] TJ ET
BT 83.497 526.960 Td /F1 12.0 Tf [(minimum of the free energy indeed moves from small holonomy to the value corresponding to )] TJ ET
BT 83.497 512.589 Td /F1 12.0 Tf [(confinement.")] TJ ET
BT 36.266 468.904 Td /F1 12.0 Tf [(2:40pm)] TJ ET
BT 83.497 468.904 Td /F2 12.0 Tf [(Tin Sulejmanpasic - SCGP 102)] TJ ET
BT 83.497 436.533 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 436.533 Td /F1 12.0 Tf [(Instanton interactions in \(SUSY\) quantum mechanics )] TJ ET
BT 36.266 392.848 Td /F1 12.0 Tf [(3:20pm)] TJ ET
BT 83.497 392.848 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 369.592 Td /F1 12.0 Tf [(3:40pm)] TJ ET
BT 83.497 369.592 Td /F2 12.0 Tf [(Dmitri Kharzeev - SCGP 102)] TJ ET
BT 83.497 337.221 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 337.221 Td /F1 12.0 Tf [(Overview of the chiral magnetic effect )] TJ ET
BT 36.266 293.536 Td /F1 12.0 Tf [(4:30pm)] TJ ET
BT 83.497 293.536 Td /F2 12.0 Tf [(Huan Huang - SCGP 102)] TJ ET
BT 83.497 261.280 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 261.280 Td /F1 12.0 Tf [(Experimental Searches for Chirality and Magnetic Field Effects in Heavy Ion Collisions at )] TJ ET
BT 83.497 246.909 Td /F1 12.0 Tf [(RHIC)] TJ ET
BT 36.266 203.224 Td /F1 12.0 Tf [(5:00pm)] TJ ET
BT 83.497 203.224 Td /F2 12.0 Tf [(Michael Ogilvie - SCGP 102)] TJ ET
endstream
endobj
12 0 obj
<< /Type /Page
/Parent 3 0 R
/Contents 13 0 R
>>
endobj
13 0 obj
<<
/Length 3941 >>
stream
0.000 0.000 0.000 rg
0.000 0.000 0.000 RG
0.75 w 0 J [ ] 0 d
BT 83.497 732.214 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 732.214 Td /F1 12.0 Tf [(A holistic approach to instantons on R^3 x S^1 )] 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 [(Abelianizing deformations provide important tools for understanding the phase structure )] TJ ET
BT 83.497 689.273 Td /F1 12.0 Tf [(and topological excitations in both continuum and lattice field theories. Such deformations typically )] TJ ET
BT 83.497 675.017 Td /F1 12.0 Tf [(produce a rich phase structure, and allow additional analytic control over nonperturbative effects. In )] TJ ET
BT 83.497 660.761 Td /F1 12.0 Tf [(lattice models, Abelianizing deformations typically lead to the emergence of the constituents of )] TJ ET
BT 83.497 646.505 Td /F1 12.0 Tf [(instantons as primary objects. They can also provide a stabilizing mechanism for classically )] TJ ET
BT 83.497 632.249 Td /F1 12.0 Tf [(conformal theories, removing problems in the naive instanton expansion. Finally, Abelianizing )] TJ ET
BT 83.497 617.993 Td /F1 12.0 Tf [(deformations play a crucial role in phenomenological models of QCD at nonzero temperature and )] TJ ET
BT 83.497 603.622 Td /F1 12.0 Tf [(density, thus providing a bridge between theory and phenomenology.)] TJ ET
0.800 0.800 0.800 rg
82.747 516.195 485.320 19.632 re f
0.75 w 0 J [ ] 0 d
83.872 517.320 483.070 17.382 re S
0.000 0.000 0.000 rg
BT 260.258 521.021 Td /F2 14.0 Tf [(Tuesday, August 18th)] TJ ET
BT 36.266 502.540 Td /F1 12.0 Tf [(9:00am)] TJ ET
BT 83.497 502.540 Td /F2 12.0 Tf [(Ernst-Michael Ilgenfritz - SCGP 102)] TJ ET
BT 83.497 470.284 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 470.284 Td /F1 12.0 Tf [(Signatures of dyons or KvBLL calorons from lattice gluodynamics at nonzero temperature )] TJ ET
BT 83.497 456.028 Td /F1 12.0 Tf [(Abstract 1: We will present an overview of attempts and results of a Berlin-ITEP \(Moscow\) )] TJ ET
BT 83.497 441.772 Td /F1 12.0 Tf [(collaboration to establish evidence for Kraan-van Baal/Lee-Lu calorons and fordyon structures in )] TJ ET
BT 83.497 427.516 Td /F1 12.0 Tf [(lattice gauge field ensembles, whichhas begun more than 10 years ago. Some attempts are )] TJ ET
BT 83.497 413.145 Td /F1 12.0 Tf [(alsodescribed to perform simulations of confinement within corresponding models. )] TJ ET
BT 36.266 369.460 Td /F1 12.0 Tf [(9:50am)] TJ ET
BT 83.497 369.460 Td /F2 12.0 Tf [(Michael Muller-Preussker - SCGP 102)] TJ ET
BT 83.497 337.204 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 337.204 Td /F1 12.0 Tf [(Determining the topological susceptibility in lattice QCD at nonzero temperature Abstract 2: )] TJ ET
BT 83.497 322.948 Td /F1 12.0 Tf [(We would like to present an overview of recent determinations of the topological suceptibility in )] TJ ET
BT 83.497 308.692 Td /F1 12.0 Tf [(lattice QCD using \(and comparing\) various smoothing methods, in particular the gradient flow. )] TJ ET
BT 83.497 294.436 Td /F1 12.0 Tf [(How the latter works will be first demonstrated in the simple one-dimensional quantum mechanical )] TJ ET
BT 83.497 280.180 Td /F1 12.0 Tf [(case of an \(un\)harmonic oscillator. Finally we will focus on the topological susceptibility in full )] TJ ET
BT 83.497 265.809 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 36.266 222.124 Td /F1 12.0 Tf [(10:40am)] TJ ET
BT 83.497 222.124 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 198.868 Td /F1 12.0 Tf [(11:00am)] TJ ET
BT 83.497 198.868 Td /F2 12.0 Tf [(Leonid Glozman - SCGP 102)] TJ ET
BT 83.497 166.497 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 166.497 Td /F1 12.0 Tf [(Hadrons with and without zero-mode-zone )] TJ ET
BT 36.266 122.812 Td /F1 12.0 Tf [(11:50am)] TJ ET
BT 83.497 122.812 Td /F2 12.0 Tf [(Ivan Horvath - SCGP 102)] TJ ET
endstream
endobj
14 0 obj
<< /Type /Page
/Parent 3 0 R
/Contents 15 0 R
>>
endobj
15 0 obj
<<
/Length 3705 >>
stream
0.000 0.000 0.000 rg
0.000 0.000 0.000 RG
0.75 w 0 J [ ] 0 d
BT 83.497 732.214 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 732.214 Td /F1 12.0 Tf [(Studies of fermionic zero-mode-zone states )] 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 discuss elements of a long-term effort to characterize QCD vacuum \(and its thermal )] TJ ET
BT 83.497 689.273 Td /F1 12.0 Tf [(states\) in a model-independent manner using lattice QCD. Local behavior of topological density )] TJ ET
BT 83.497 675.017 Td /F1 12.0 Tf [(and properties of \(overlap\) Dirac eigenmodes are given a particular attention. Regarding the latter, )] TJ ET
BT 83.497 660.761 Td /F1 12.0 Tf [(construction of non-Pearson correlations describing chiral polarization of modes will be covered in )] TJ ET
BT 83.497 646.505 Td /F1 12.0 Tf [(some detail, including the proposed equivalence between chiral symmetry breaking and )] TJ ET
BT 83.497 632.249 Td /F1 12.0 Tf [(condensation of local chirality defined accordingly. In the last part of the talk, recent developments )] TJ ET
BT 83.497 617.993 Td /F1 12.0 Tf [(suggesting connections between the properties of Dirac modes and confinement are discussed, )] TJ ET
BT 83.497 603.737 Td /F1 12.0 Tf [(emphasizing the existence of deconfined phase with broken valence chiral symmetry in thermal )] TJ ET
BT 83.497 589.366 Td /F1 12.0 Tf [(QCD, and in systems with many light fundamental flavors.)] TJ ET
BT 36.266 509.416 Td /F1 12.0 Tf [(12:40pm)] TJ ET
BT 83.497 509.416 Td /F2 12.0 Tf [(Lunch - SCGP Cafe)] TJ ET
BT 36.266 486.160 Td /F1 12.0 Tf [(2:00pm)] TJ ET
BT 83.497 486.160 Td /F2 12.0 Tf [(Sayatan Sharma - SCGP 102)] TJ ET
BT 83.497 453.789 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 453.789 Td /F1 12.0 Tf [(The axial U\(1\) anomaly and topological structures in finite temperature QCD )] TJ ET
BT 83.497 425.104 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 425.104 Td /F1 12.0 Tf [(The magnitude of axial U\(1\) symmetry breaking is believed to affect nature of Nf = 2 )] TJ ET
BT 83.497 410.848 Td /F1 12.0 Tf [(QCD chiral phase transition. The explicit breaking of chiral symmetry due to realistic light quark )] TJ ET
BT 83.497 396.592 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 83.497 382.336 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 83.497 368.080 Td /F1 12.0 Tf [(our recent study of the eigenvalue spectrum of QCD with two different lattice fermion )] TJ ET
BT 83.497 353.824 Td /F1 12.0 Tf [(discretizations which retain a remnant of the continuum chiral symmetry, using exact chiral overlap )] TJ ET
BT 83.497 339.568 Td /F1 12.0 Tf [(fermions as probes. From the eigenvalue spectrum of the overlap operator, we do not observe any )] TJ ET
BT 83.497 325.312 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 83.497 311.056 Td /F1 12.0 Tf [(observed to persist even at 1.5Tc which are primarily responsible for its breaking. These )] TJ ET
BT 83.497 296.800 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 83.497 282.544 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 83.497 268.173 Td /F1 12.0 Tf [(gas ensemble already setting in at 1.5 Tc.)] TJ ET
BT 36.266 224.488 Td /F1 12.0 Tf [(2:45pm)] TJ ET
BT 83.497 224.488 Td /F2 12.0 Tf [(Maria Lombardo - SCGP 102)] TJ ET
endstream
endobj
16 0 obj
<< /Type /Page
/Parent 3 0 R
/Contents 17 0 R
>>
endobj
17 0 obj
<<
/Length 3898 >>
stream
0.000 0.000 0.000 rg
0.000 0.000 0.000 RG
0.75 w 0 J [ ] 0 d
BT 83.497 732.329 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 732.329 Td /F1 12.0 Tf [(Scale separation, walking dynamics and approach to criticality in QCD with varying number )] TJ ET
BT 83.497 717.958 Td /F1 12.0 Tf [(of flavors. )] TJ ET
BT 83.497 689.273 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 689.273 Td /F1 12.0 Tf [(QCD with Nf fundamental fermions has a rich phase structure which has been explored )] TJ ET
BT 83.497 675.017 Td /F1 12.0 Tf [(with analytic and numerical studies. In the massless case and at zero temperature an essential )] TJ ET
BT 83.497 660.761 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 83.497 646.505 Td /F1 12.0 Tf [(reflected by Miransky scaling of infrared observables. In turn, the conformal phase can be seen as )] TJ ET
BT 83.497 632.249 Td /F1 12.0 Tf [(the zero temperature limit of a \(strongly\)interactive quark gluon plasma when the number of flavors )] TJ ET
BT 83.497 617.993 Td /F1 12.0 Tf [(approach its critical value. In lattice simulations a nonzero quark mass is usually included, and )] TJ ET
BT 83.497 603.737 Td /F1 12.0 Tf [(conformality is explicitely broken, with two main consequences: a\) The would-be conformal phase )] TJ ET
BT 83.497 589.481 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 83.497 575.225 Td /F1 12.0 Tf [(anomalous dimension are still observable below the critical number of flavors; b\)The critical )] TJ ET
BT 83.497 560.969 Td /F1 12.0 Tf [(singularity disappears however ratios of homogeneous observables still carry an imprinting of the )] TJ ET
BT 83.497 546.713 Td /F1 12.0 Tf [(critical dynamics. The talk is a brief overview of these phenomena, elucidated by the behaviour of )] TJ ET
BT 83.497 532.457 Td /F1 12.0 Tf [(the \(pseudo\)critical temperature, mass spectrum, string tension and Wilson flow in the )] TJ ET
BT 83.497 518.086 Td /F1 12.0 Tf [(preconformal region.)] TJ ET
BT 36.266 438.136 Td /F1 12.0 Tf [(3:30pm)] TJ ET
BT 83.497 438.136 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 414.880 Td /F1 12.0 Tf [(4:00pm)] TJ ET
BT 83.497 414.880 Td /F2 12.0 Tf [(Kenji Fukushima - SCGP 102)] TJ ET
BT 83.497 382.509 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 382.509 Td /F1 12.0 Tf [(QCD under curvature and magnetic effects )] TJ ET
BT 36.266 338.824 Td /F1 12.0 Tf [(5:15pm)] TJ ET
BT 83.497 338.824 Td /F2 12.0 Tf [(Vasily Sazonov - SCGP 102)] TJ ET
BT 83.497 306.453 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 306.453 Td /F1 12.0 Tf [(Convergent Series)] TJ ET
0.800 0.800 0.800 rg
82.747 255.291 485.320 19.632 re f
0.75 w 0 J [ ] 0 d
83.872 256.416 483.070 17.382 re S
0.000 0.000 0.000 rg
BT 250.927 260.117 Td /F2 14.0 Tf [(Wednesday, August 19th)] TJ ET
BT 36.266 241.636 Td /F1 12.0 Tf [(9:00am)] TJ ET
BT 83.497 241.636 Td /F2 12.0 Tf [(Misha Shifman - SCGP 102)] TJ ET
BT 83.497 209.265 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 209.265 Td /F1 12.0 Tf [(Topological defects in Yang-Mills with non-abelian moduli and their implications. )] TJ ET
BT 83.497 180.580 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 180.580 Td /F1 12.0 Tf [("I discuss developments of the last decade in Yang-Mills theories \(including those at )] TJ ET
BT 83.497 166.324 Td /F1 12.0 Tf [(strong coupling\) with or without supersymmetry. I focus on the progress in understanding non-)] TJ ET
BT 83.497 152.068 Td /F1 12.0 Tf [(Abelian dynamics, 2D-4D correspondence and various applications. In the supersymmetric case )] TJ ET
BT 83.497 137.697 Td /F1 12.0 Tf [(remarkable exact results ensue.")] TJ ET
BT 36.266 94.012 Td /F1 12.0 Tf [(10:00am)] TJ ET
BT 83.497 94.012 Td /F2 12.0 Tf [(Gerald Dunne - SCGP 102)] TJ ET
endstream
endobj
18 0 obj
<< /Type /Page
/Parent 3 0 R
/Contents 19 0 R
>>
endobj
19 0 obj
<<
/Length 3588 >>
stream
0.000 0.000 0.000 rg
0.000 0.000 0.000 RG
0.75 w 0 J [ ] 0 d
BT 83.497 732.214 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 732.214 Td /F1 12.0 Tf [(Overview of the resurgence program )] TJ ET
BT 36.266 688.529 Td /F1 12.0 Tf [(11:00am)] TJ ET
BT 83.497 688.529 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 665.273 Td /F1 12.0 Tf [(11:20am)] TJ ET
BT 83.497 665.273 Td /F2 12.0 Tf [(Ariel Zhitnitsky - SCGP 102)] TJ ET
BT 83.497 632.902 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 632.902 Td /F1 12.0 Tf [(Vacuum energy, contact term and all that in gauge systems with nontrivial holonomy )] TJ ET
BT 83.497 604.217 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 604.217 Td /F1 12.0 Tf [( I present few highly nontrivial features of the gauge theories when the configurations )] TJ ET
BT 83.497 589.961 Td /F1 12.0 Tf [(with nontrivial holonomy play the crucial role in dynamics. First example is the computation of the )] TJ ET
BT 83.497 575.705 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 83.497 561.449 Td /F1 12.0 Tf [(configurations with nontrivial holonomy saturate the contact term which was conjectured for )] TJ ET
BT 83.497 547.193 Td /F1 12.0 Tf [(strongly coupled QCD long ago by Witten and Veneziano. Second example is computations of the )] TJ ET
BT 83.497 532.937 Td /F1 12.0 Tf [(contact term in nontrivial curved hyperbolic background. I argue that correction to the energy is )] TJ ET
BT 83.497 518.681 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 83.497 504.425 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 83.497 490.169 Td /F1 12.0 Tf [(understanding of the observed cosmological dark energy, which is interpreted in this framework as )] TJ ET
BT 83.497 475.798 Td /F1 12.0 Tf [(the modification of the QCD vacuum energy in topologically nontrivial background. )] TJ ET
BT 36.266 432.113 Td /F1 12.0 Tf [(12:05pm)] TJ ET
BT 83.497 432.113 Td /F2 12.0 Tf [(Yachao Qian - SCGP 102)] TJ ET
BT 83.497 399.742 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 399.742 Td /F1 12.0 Tf [(Spin Asymmetries and P-odd Effects through QCD Instantons)] TJ ET
BT 36.266 356.057 Td /F1 12.0 Tf [(12:50pm)] TJ ET
BT 83.497 356.057 Td /F2 12.0 Tf [(Juven Wang \(IAS Princeton\) - SCGP 102)] TJ ET
BT 83.497 323.686 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 323.686 Td /F1 12.0 Tf [(Quantum Statistics, Spacetime Topology and Lattice Chiral Fermions of Condensed Matter )] TJ ET
BT 36.266 280.001 Td /F1 12.0 Tf [(1:35pm)] TJ ET
BT 83.497 280.001 Td /F2 12.0 Tf [(Lunch - SCGP Cafe)] TJ ET
0.800 0.800 0.800 rg
82.747 249.268 485.320 19.632 re f
0.75 w 0 J [ ] 0 d
83.872 250.393 483.070 17.382 re S
0.000 0.000 0.000 rg
BT 256.366 254.095 Td /F2 14.0 Tf [(Thursday, August 20th)] TJ ET
BT 36.266 235.613 Td /F1 12.0 Tf [(9:00am)] TJ ET
BT 83.497 235.613 Td /F2 12.0 Tf [(Jeff Greensite - SCGP 102)] TJ ET
BT 83.497 203.242 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 203.242 Td /F1 12.0 Tf [( Confinement via center vortices )] TJ ET
BT 83.497 174.557 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 174.557 Td /F1 12.0 Tf [( I review the motivation and numerical evidence for the center vortex confinement )] TJ ET
BT 83.497 160.186 Td /F1 12.0 Tf [(mechanism.)] TJ ET
BT 36.266 116.501 Td /F1 12.0 Tf [(10:00am)] TJ ET
BT 83.497 116.501 Td /F2 12.0 Tf [(Kej-Ichi Kondo - SCGP 102)] TJ ET
endstream
endobj
20 0 obj
<< /Type /Page
/Parent 3 0 R
/Contents 21 0 R
>>
endobj
21 0 obj
<<
/Length 4601 >>
stream
0.000 0.000 0.000 rg
0.000 0.000 0.000 RG
0.75 w 0 J [ ] 0 d
BT 83.497 732.214 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 732.214 Td /F1 12.0 Tf [(Monopoles and confinement )] 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 [(We give a review on the recent developments on quark confinement from the viewpoint )] TJ ET
BT 83.497 689.273 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 83.497 675.017 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 83.497 660.761 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 83.497 646.505 Td /F1 12.0 Tf [(Mills theory without the scalar field. Second, we give a new framework for reformulating the )] TJ ET
BT 83.497 632.249 Td /F1 12.0 Tf [(SU\(N\) Yang-Mills theory using new field variables. This includes the preceding works on field )] TJ ET
BT 83.497 617.993 Td /F1 12.0 Tf [(decompositions given by Cho, Duan and Ge, Faddeev and Niemi, as a special case called the )] TJ ET
BT 83.497 603.737 Td /F1 12.0 Tf [(maximal option in our reformulations. An advantage of the reformulations is that the original Yang-)] TJ ET
BT 83.497 589.481 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 83.497 575.225 Td /F1 12.0 Tf [(the restricted field gives the dominant contribution to quark confinement in the gauge-independent )] TJ ET
BT 83.497 560.969 Td /F1 12.0 Tf [(way. Then, our reformulations can be combined with the non-Abelian Stokes theorem. In the so-)] TJ ET
BT 83.497 546.713 Td /F1 12.0 Tf [(called minimal option, especially, the restricted field is non-Abelian and involves the non-Abelian )] TJ ET
BT 83.497 532.457 Td /F1 12.0 Tf [(magnetic monopole with the stability group U\(N-1\). This suggests the non-Abelian dual )] TJ ET
BT 83.497 518.201 Td /F1 12.0 Tf [(superconductivity picture for quark confinement. This should be compared with the maximal )] TJ ET
BT 83.497 503.945 Td /F1 12.0 Tf [(option: the restricted field is Abelian and involves only the Abelian magnetic monopoles with the )] TJ ET
BT 83.497 489.689 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 83.497 475.433 Td /F1 12.0 Tf [(the reformulations of the SU\(N\) Yang-Mills theory and present the results of the numerical )] TJ ET
BT 83.497 461.177 Td /F1 12.0 Tf [(simulations of the SU\(3\) Yang-Mills theory on a lattice. The numerical simulations include the )] TJ ET
BT 83.497 446.921 Td /F1 12.0 Tf [(derivation of the linear potential for static interquark potential, i.e., non-vanishing string tension, in )] TJ ET
BT 83.497 432.665 Td /F1 12.0 Tf [(which the restricted field dominance and magnetic monopole dominance are established, )] TJ ET
BT 83.497 418.409 Td /F1 12.0 Tf [(confirmation of the dual Meissner effect by measuring the chromoelectric flux tube between quark-)] TJ ET
BT 83.497 404.038 Td /F1 12.0 Tf [(antiquark pair, the induced magnetic-monopole current, and the type of dual superconductivity, etc.)] TJ ET
BT 36.266 324.088 Td /F1 12.0 Tf [(11:00am)] TJ ET
BT 83.497 324.088 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 300.832 Td /F1 12.0 Tf [(11:20am)] TJ ET
BT 83.497 300.832 Td /F2 12.0 Tf [(Chris Korthals-Altes - SCGP 102)] TJ ET
BT 83.497 268.461 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 268.461 Td /F1 12.0 Tf [(The magnetic component of the QCD plasma. )] TJ ET
BT 83.497 239.776 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 239.776 Td /F1 12.0 Tf [(I review the necessity of a magnetic component in the QCD plasma, as seen by lattice )] TJ ET
BT 83.497 225.405 Td /F1 12.0 Tf [(simulations of spatial Wilsonloops.)] TJ ET
BT 36.266 181.720 Td /F1 12.0 Tf [(12:00pm)] TJ ET
BT 83.497 181.720 Td /F2 12.0 Tf [(Peter Petreczky - SCGP 102)] TJ ET
BT 83.497 149.349 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 149.349 Td /F1 12.0 Tf [(The Polyakov loop from the lattice )] TJ ET
BT 36.266 105.664 Td /F1 12.0 Tf [(12:40pm)] TJ ET
BT 83.497 105.664 Td /F2 12.0 Tf [(Lunch: - SCGP Cafe)] TJ ET
BT 36.266 82.408 Td /F1 12.0 Tf [(3:30pm)] TJ ET
BT 83.497 82.408 Td /F2 12.0 Tf [(Coffee Break - SCGP 102)] TJ ET
BT 36.266 59.152 Td /F1 12.0 Tf [(4:00pm)] TJ ET
BT 83.497 59.152 Td /F2 12.0 Tf [(Jinfeng Liao - SCGP 102)] TJ ET
endstream
endobj
22 0 obj
<< /Type /Page
/Parent 3 0 R
/Contents 23 0 R
>>
endobj
23 0 obj
<<
/Length 3799 >>
stream
0.000 0.000 0.000 rg
0.000 0.000 0.000 RG
0.75 w 0 J [ ] 0 d
BT 83.497 692.949 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 692.949 Td /F1 12.0 Tf [(Electric flux tube and thermal monopoles in the deconfined phase )] TJ ET
BT 83.497 664.264 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 664.264 Td /F1 12.0 Tf [(The QCD vacuum structure and the mechanism for confinement provides a persistent )] TJ ET
BT 83.497 650.008 Td /F1 12.0 Tf [(challenge to our understanding of nonperturbative gauge dynamics. One compelling idea is to )] TJ ET
BT 83.497 635.752 Td /F1 12.0 Tf [(consider the vacuum as a monopole condensate and the confinement/deconfinement transition as )] TJ ET
BT 83.497 621.496 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 83.497 607.240 Td /F1 12.0 Tf [(proposed, namely to understand confinement from above i.e. in the deconfined phase, by studying )] TJ ET
BT 83.497 592.984 Td /F1 12.0 Tf [(the thermal monopole ensemble in the vicinity of Tc. The so-called ``magnetic scenario'' suggests )] TJ ET
BT 83.497 578.728 Td /F1 12.0 Tf [(that an ensemble of abundant and light thermal monopoles emerges above Tc and reaches )] TJ ET
BT 83.497 564.472 Td /F1 12.0 Tf [(condensation condition at Tc thus leading to confinement transition. In this talk we focus on how )] TJ ET
BT 83.497 550.216 Td /F1 12.0 Tf [(such a scenario sheds light on two interesting phenomena: \(1\) the survival of extended electric flux )] TJ ET
BT 83.497 535.960 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 83.497 521.704 Td /F1 12.0 Tf [(the confinement transition parameters on the fermion contents, which provides a unique test of the )] TJ ET
BT 83.497 507.448 Td /F1 12.0 Tf [(the mechanism of confinement as monopole condensation. Lastly we briefly comment upon how )] TJ ET
BT 83.497 493.192 Td /F1 12.0 Tf [(these monopoles behave as a color-opaque low-viscosity matter and help understand a few key )] TJ ET
BT 83.497 478.936 Td /F1 12.0 Tf [(properties of the quark-gluon plasma observed in heavy ion collision experiments. [References: )] TJ ET
BT 83.497 464.680 Td /F1 12.0 Tf [(Jinfeng Liao & Edward Shuryak, PRL109\(2012\)152001; PRD82\(2010\)094007; )] TJ ET
BT 83.497 450.309 Td /F1 12.0 Tf [(PRL101\(2008\)162302; PRC75\(2007\)054907.])] TJ ET
BT 36.266 406.624 Td /F1 12.0 Tf [(4:40pm)] TJ ET
BT 83.497 406.624 Td /F2 12.0 Tf [(Claudia Ratti - SCGP 102)] TJ ET
BT 83.497 374.253 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 374.253 Td /F1 12.0 Tf [(Thermal monopoles and kinetics of sQGP )] TJ ET
BT 36.266 330.568 Td /F1 12.0 Tf [(5:20pm)] TJ ET
BT 83.497 330.568 Td /F2 12.0 Tf [(Shu Lin - SCGP 102)] TJ ET
BT 83.497 298.197 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 298.197 Td /F1 12.0 Tf [(The Polyakov loop potential and semi-QGP )] TJ ET
BT 83.497 269.512 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 269.512 Td /F1 12.0 Tf [(I will discuss lattice results on gauge theory thermodynamics and Polyakov loop. In )] TJ ET
BT 83.497 255.256 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 83.497 241.000 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 83.497 226.744 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 83.497 212.373 Td /F1 12.0 Tf [(effect on gluons and quarks. I will also discuss its phenomenological implications.)] TJ ET
BT 36.266 168.688 Td /F1 12.0 Tf [(6:00pm)] TJ ET
BT 83.497 168.688 Td /F2 12.0 Tf [(Jiechen Xu - SCGP 102)] TJ ET
endstream
endobj
24 0 obj
<< /Type /Page
/Parent 3 0 R
/Contents 25 0 R
>>
endobj
25 0 obj
<<
/Length 4314 >>
stream
0.000 0.000 0.000 rg
0.000 0.000 0.000 RG
0.75 w 0 J [ ] 0 d
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 36.266 409.624 Td /F1 12.0 Tf [(6:30pm)] TJ ET
BT 83.497 409.624 Td /F2 12.0 Tf [(Workshop Banquet)] TJ ET
0.800 0.800 0.800 rg
82.747 378.891 485.320 19.632 re f
0.75 w 0 J [ ] 0 d
83.872 380.016 483.070 17.382 re S
0.000 0.000 0.000 rg
BT 266.488 383.717 Td /F2 14.0 Tf [(Friday, August 21st)] TJ ET
BT 36.266 365.236 Td /F1 12.0 Tf [(9:00am)] TJ ET
BT 83.497 365.236 Td /F2 12.0 Tf [(Adam Szczepaniak - SCGP 102)] TJ ET
BT 83.497 332.865 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 332.865 Td /F1 12.0 Tf [(Couloumb gauge confinement and emerging phenomenology )] TJ ET
BT 36.266 289.180 Td /F1 12.0 Tf [(10:00am)] TJ ET
BT 83.497 289.180 Td /F2 12.0 Tf [(Alexander Turbiner - SCGP 102)] TJ ET
BT 83.497 256.809 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 256.809 Td /F1 12.0 Tf [(Energy gap in quantum mechanics: double well potential )] TJ ET
BT 83.497 228.124 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 228.124 Td /F1 12.0 Tf [(Exploring the Schr\\"odinger equation the locally accurate wave function of the ground )] TJ ET
BT 83.497 213.868 Td /F1 12.0 Tf [(\(and the first excited\) states will be constructed for 1D double well potential for weak, intermediate )] TJ ET
BT 83.497 199.612 Td /F1 12.0 Tf [(and strong coupling. As for 3D case the example of hydrogen molecular ion will be considered )] TJ ET
BT 83.497 185.241 Td /F1 12.0 Tf [(briefly)] TJ ET
BT 36.266 141.556 Td /F1 12.0 Tf [(11:00am)] TJ ET
BT 83.497 141.556 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 118.300 Td /F1 12.0 Tf [(11:30am)] TJ ET
BT 83.497 118.300 Td /F2 12.0 Tf [(Ismail Zahed - SCGP 102)] TJ ET
BT 83.497 85.929 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 85.929 Td /F1 12.0 Tf [(Holographic Pomeron )] TJ ET
BT 36.266 42.244 Td /F1 12.0 Tf [(12:30pm)] TJ ET
BT 83.497 42.244 Td /F2 12.0 Tf [(Lunch - SCGP Cafe)] TJ ET
endstream
endobj
26 0 obj
<< /Type /Page
/Parent 3 0 R
/Contents 27 0 R
>>
endobj
27 0 obj
<<
/Length 3369 >>
stream
0.000 0.000 0.000 rg
0.000 0.000 0.000 RG
0.75 w 0 J [ ] 0 d
BT 36.266 702.064 Td /F1 12.0 Tf [(2:00pm)] TJ ET
BT 83.497 702.064 Td /F2 12.0 Tf [(Ioannis Iatrakis - SCGP 102)] TJ ET
BT 83.497 669.693 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 669.693 Td /F1 12.0 Tf [(QCD strings and their interactions from the holographic perspective )] TJ ET
BT 36.266 626.008 Td /F1 12.0 Tf [(2:50pm)] TJ ET
BT 83.497 626.008 Td /F2 12.0 Tf [(T. Iritani - SCGP 102)] TJ ET
BT 83.497 593.637 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 593.637 Td /F1 12.0 Tf [(QCD strings on the lattice )] TJ ET
BT 83.497 564.952 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 564.952 Td /F1 12.0 Tf [( In the QCD vacuum, quarks are confined inside hadrons, which can be understood by a )] TJ ET
BT 83.497 550.696 Td /F1 12.0 Tf [(linear rising interquark potential. This linear potential is produced by the string structure of chromo )] TJ ET
BT 83.497 536.440 Td /F1 12.0 Tf [(fields between quarks. We introduce how to observe this phenomenological QCD string in lattice )] TJ ET
BT 83.497 522.184 Td /F1 12.0 Tf [(QCD. Besides the mechanism of quark confinement, QCD string would cause interesting )] TJ ET
BT 83.497 507.928 Td /F1 12.0 Tf [(phenomena. For example, we demonstrate the non-trivial modification of chiral condensate in the )] TJ ET
BT 83.497 493.672 Td /F1 12.0 Tf [(presence of QCD string. We also discuss more precise determination of QCD string features using )] TJ ET
BT 83.497 479.301 Td /F1 12.0 Tf [(gradient flow.)] TJ ET
BT 36.266 435.616 Td /F1 12.0 Tf [(3:30pm)] TJ ET
BT 83.497 435.616 Td /F2 12.0 Tf [(Coffee Break & Workshop Closing - SCGP Cafe)] TJ ET
BT 36.266 412.360 Td /F1 12.0 Tf [(4:00pm)] TJ ET
BT 83.497 412.360 Td /F2 12.0 Tf [(Tigran Kalaydzhyan - SCGP 102)] TJ ET
BT 83.497 379.989 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 379.989 Td /F1 12.0 Tf [(QCD string interactions and implications for high energy collisions )] TJ ET
BT 83.497 351.304 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 135.145 351.304 Td /F1 12.0 Tf [(In this talk I would like to introduce an idea of interaction between QCD strings and )] TJ ET
BT 83.497 337.048 Td /F1 12.0 Tf [(discuss some of the consequences for the nucleus-nucleus \(AA\) and proton-nucleus \(pA\) collisions. )] TJ ET
BT 83.497 322.792 Td /F1 12.0 Tf [(From the academic point of view, the interaction provides new \(high entropy\) regimes of the string )] TJ ET
BT 83.497 308.536 Td /F1 12.0 Tf [(behavior near the Hagedorn point. Among the applications are the onset of the explosive regime in )] TJ ET
BT 83.497 294.280 Td /F1 12.0 Tf [(pA collisions, elliptic flow in pA collisions, jet quenching in the mixed phase, modification of the )] TJ ET
BT 83.497 280.024 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 83.497 265.768 Td /F1 12.0 Tf [(collective phenomena in proton-proton \(pp\) collisions. The talk is based on recent papers )] TJ ET
BT 83.497 251.397 Td /F1 12.0 Tf [(1402.7363 \(PRD\), 1404.1888 \(PRC\), 1503.05213 \(PRC\))] TJ ET
BT 36.266 207.712 Td /F1 12.0 Tf [(4:30pm)] TJ ET
BT 83.497 207.712 Td /F2 12.0 Tf [(Rob Pisarski & Edward Shuryak - SCGP 102)] TJ ET
BT 83.497 175.341 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 114.493 175.341 Td /F1 12.0 Tf [(Concluding remarks)] TJ ET
endstream
endobj
xref
0 28
0000000000 65535 f
0000000008 00000 n
0000000073 00000 n
0000000119 00000 n
0000000347 00000 n
0000000376 00000 n
0000000513 00000 n
0000000576 00000 n
0000004340 00000 n
0000004449 00000 n
0000004557 00000 n
0000004622 00000 n
0000007525 00000 n
0000007590 00000 n
0000011584 00000 n
0000011649 00000 n
0000015407 00000 n
0000015472 00000 n
0000019423 00000 n
0000019488 00000 n
0000023129 00000 n
0000023194 00000 n
0000027848 00000 n
0000027913 00000 n
0000031765 00000 n
0000031830 00000 n
0000036197 00000 n
0000036262 00000 n
trailer
<<
/Size 28
/Root 1 0 R
/Info 5 0 R
>>
startxref
39684
%%EOF