liliana apolinário - cern indico
TRANSCRIPT
!"#$%&$'()*+(,-,. /001$*%23*3"4(15(//(&26(0/(7188343124(&*(*+"(9:;<(;=>?(@>"A1*"B
Jet Quenching from Light to Dense Systems
Liliana Apolinário
L. Apolinário OppO 2021
C D#D#(&26(E%E%(0$"4"2*4(712434*"2*(43F2&*%$"4(15(&(GHD(51$A&*312I(
C EJ3A%*+&8(&2341*$10'(32(2K0&$*378"(71$$"8&*3124(@7188"7*3L"(581MB(
C N27$"&4"(15(4*$&2F"(+&6$124('3"864(@4*$&2F"2"44("2+&27"A"2*B(
C O%00$"44312(15(432F8"(+&6$12(40"7*$&(@"2"$F'(8144B
2
QGP in dense systems
L. Apolinário OppO 2021
C D#D#(&26(E%E%(0$"4"2*4(712434*"2*(43F2&*%$"4(15(&(GHD(51$A&*312I(
C EJ3A%*+&8(&2341*$10'(32(2K0&$*378"(71$$"8&*3124(@7188"7*3L"(581MB(
C N27$"&4"(15(4*$&2F"(+&6$124('3"864(@4*$&2F"2"44("2+&27"A"2*B(
C O%00$"44312(15(432F8"(+&6$12(40"7*$&(@"2"$F'(8144B
2
QGP in dense systems
P
P
L. Apolinário OppO 2021
C D#D#(&26(E%E%(0$"4"2*4(712434*"2*(43F2&*%$"4(15(&(GHD(51$A&*312I(
C EJ3A%*+&8(&2341*$10'(32(2K0&$*378"(71$$"8&*3124(@7188"7*3L"(581MB(
C N27$"&4"(15(4*$&2F"(+&6$124('3"864(@4*$&2F"2"44("2+&27"A"2*B(
C O%00$"44312(15(432F8"(+&6$12(40"7*$&(@"2"$F'(8144B
2
QGP in dense systems
[nucl-ex/0109003]
[PHENIX: Phys.Rev.Lett. 88 (2002) 022301][STAR: Phys. Rev. Lett. 89 (2002) 202301]
[nucl-ex/0109003]
P
P
P
L. Apolinário OppO 2021
C D#D#(&26(E%E%(0$"4"2*4(712434*"2*(43F2&*%$"4(15(&(GHD(51$A&*312I
C EJ3A%*+&8(&2341*$10'(32(2K0&$*378"(71$$"8&*3124(@7188"7*3L"(581MB
C N27$"&4"(15(4*$&2F"(+&6$124('3"864(@4*$&2F"2"44("2+&27"A"2*B
C O%00$"44312(15(432F8"(+&6$12(40"7*$&(@"2"$F'(8144B
C O%00$"44312(15(Q"*(40"7*$&(@"2"$F'(8144B
3
QGP in dense systems
P
P
P
P
[arXiv:1504.04337]
[ATLAS: JHEP 09 (2015) 050]
L. Apolinário OppO 2021
C D#D#(&26(E%E%(0$"4"2*4(712434*"2*(43F2&*%$"4(15(&(GHD(51$A&*312I
C EJ3A%*+&8(&2341*$10'(32(2K0&$*378"(71$$"8&*3124(@7188"7*3L"(581MB
C N27$"&4"(15(4*$&2F"(+&6$124('3"864(@4*$&2F"2"44("2+&27"A"2*B
C O%00$"44312(15(432F8"(+&6$12(40"7*$&(@"2"$F'(8144B
C O%00$"44312(15(Q"*(40"7*$&(@"2"$F'(8144B
C R163537&*312(15(Q"*(4%#4*$%7*%$"
3
QGP in dense systems
P
P
P
P
P
[Adapted from: K. Zapp]
!$&7*312(15("2"$F'(15(Q"*(5$&FA"2*4(@D#D#S00B
T"*($&63&8(0$1538"(@D#D#S00B
[arXiv:1809.08602] [arXiv:1801.04895]
[CMS: PRL 122 (2019) 152001][CMS: Phys. Rev. Lett. 121 (2018) 242301]
L. Apolinário OppO 2021
C O+1$*($%2(15(U"U"(&881M"6(*1(032(61M2(*+"(4&A"("55"7*4I(
C V4(W(XYZZ(["\<(]32*(^(_(`#K.(
C @D#D#(,-.)I(V4(W(XY-,(["\<(]32*(^(.Y)(2#K.B
4
QGP in XeXe
L. Apolinário OppO 2021
C O+1$*($%2(15(U"U"(&881M"6(*1(032(61M2(*+"(4&A"("55"7*4I(
C V4(W(XYZZ(["\<(]32*(^(_(`#K.(
C @D#D#(,-.)I(V4(W(XY-,(["\<(]32*(^(.Y)(2#K.B
4
QGP in XeXe
7188"7*3L"(581M(P
L. Apolinário OppO 2021
C O+1$*($%2(15(U"U"(&881M"6(*1(032(61M2(*+"(4&A"("55"7*4I(
C V4(W(XYZZ(["\<(]32*(^(_(`#K.(
C @D#D#(,-.)I(V4(W(XY-,(["\<(]32*(^(.Y)(2#K.B
4
QGP in XeXe[CMS: JHEP 08 (2011) 141]
[arXiv:1902.03603]
"2"$F'(8144(P
7188"7*3L"(581M(P
L. Apolinário OppO 2021
C O+1$*($%2(15(U"U"(&881M"6(*1(032(61M2(*+"(4&A"("55"7*4I(
C V4(W(XYZZ(["\<(]32*(^(_(`#K.(
C @D#D#(,-.)I(V4(W(XY-,(["\<(]32*(^(.Y)(2#K.B
4
QGP in XeXe[CMS: JHEP 08 (2011) 141]
[arXiv:1902.03603]
"2"$F'(8144(P
7188"7*3L"(581M(P
U"U"(a(D#D#(&*(4&A"(b?0&$*ac
L. Apolinário OppO 2021
C O+1$*($%2(15(U"U"(&881M"6(*1(032(61M2(*+"(4&A"("55"7*4I(
C V4(W(XYZZ(["\<(]32*(^(_(`#K.(
C @D#D#(,-.)I(V4(W(XY-,(["\<(]32*(^(.Y)(2#K.B
4
QGP in XeXe[CMS: JHEP 08 (2011) 141]
[arXiv:1902.03603]
"2"$F'(8144(P
?1(47&832F(M3*+(4&A"(b?0&$*a((@6355"$"2*(7"2*$&83*3"4Bd(
O7&832F(M3*+(0"$K0&$*3730&2*(7+&$F"6K+&6$12(A%8*308373*'e
7188"7*3L"(581M(P
L. Apolinário OppO 2021
[arXiv:1705.04176]
[ATLAS: Eur.Phys.J.C 77 (2017) 6, 428]
212K2"F83F3#8"(581M(+&$A12374
C ;188"7*3L3*'(43F2&*%$"4
5
QGP in pA ?P
L. Apolinário OppO 2021
C ;188"7*3L3*'(43F2&*%$"4
C O*$&2F"2"44("2+&27"A"2*
[ALICE: Nature Physics 13 (2017) 535-539]
+'0"$12K*1K0312($&*314(34((6$3L"2(#'(4*$&2F"2"44(712*"2*(
5
QGP in pA ?P
P
L. Apolinário OppO 2021
C ;188"7*3L3*'(43F2&*%$"4
C O*$&2F"2"44("2+&27"A"2*
C ?1(A163537&*3124(12(+&$6(0$1#"4
5
QGP in pA ?
[CMS: HIN-15-004-pas]
[arXiv:1611.01664]
[CMS: JHEP 04 (2017) 039]
P
P
❌
L. Apolinário OppO 2021
C ;188"7*3L3*'(43F2&*%$"4
C O*$&2F"2"44("2+&27"A"2*
C ?1(A163537&*3124(12(+&$6(0$1#"4
5
QGP in pA ?
[CMS: HIN-15-004-pas]
[arXiv:1611.01664]
[CMS: JHEP 04 (2017) 039]
N271+"$"2*(037*%$"d
P
P
❌
?""6(A1$"(83A3*4(12(TG(6"47$30*312e(
L. Apolinário OppO 2021
C R163537&*3124(15(*+"(0&$*12(4+1M"$(326%7"6(#'(*+"(32*"$&7*312(M3*+(&(6"712532"6(4*&*"(15(A&**"$I
6
Jet quenching
L. Apolinário OppO 2021
C R163537&*3124(15(*+"(0&$*12(4+1M"$(326%7"6(#'(*+"(32*"$&7*312(M3*+(&(6"712532"6(4*&*"(15(A&**"$I
6
Jet quenching
=8&4*37(47&**"$32F(0$17"44"4I
T"*
R"63%A($"7138
The Physics Case for sPHENIX What are the inner workings of the QGP?
ments is given in Section 1.5. We note that enhancements in q̂ above the critical temperaturemay be a generic feature of many models, as illustrated by the three conjectured evolutions,and so underscore the need for detailed measurements of quark-gluon plasma propertiesnear the transition temperature.
All measurements in heavy ion collisions are the result of emitted particles integrated overthe entire time evolution of the reaction, covering a range of temperatures. Similar to thehydrodynamic model constraints, the theory modeling requires a consistent temperatureand scale dependent model of the quark-gluon plasma and is only well constrained byprecision data through different temperature evolutions, as measured at RHIC and theLHC.
g*Q2
q
?
QGP
Q2 PT Initial Parton
What scale sets this transition?
Tc
Probe Integrates Over a Range of Q2
pQCDScattering from Point-Like BareColor Charges
µD
pQCD ScatteringFrom Quasiparticles
with size ~ µDebye
Strong CouplingNo Quasiparticles
µDebye ! 0
AdS/CFT
?!
" ?
What scale sets this transition?
Scattering from Thermal Mass Gluons?
Figure 1.7: (Left) Diagram of a quark exchanging a virtual gluon with an unknown object inthe QGP. This highlights the uncertainty for what sets the scale of the interaction and whatobjects or quasiparticles are recoiling. (Right) Diagram as a function of the Q2 for the netinteraction of the parton with the medium and the range of possibilities for the recoil objects.
1.3 What are the inner workings of the QGP?
A second axis along which one can investigate the underlying structure of thequark-gluon plasma concerns the question of what length scale of the medium is beingprobed by jet quenching processes. In electron scattering, the scale is set by the virtualityof the exchanged photon, Q2. By varying this virtuality one can obtain information overan enormous range of scales: from pictures of viruses at length scales of 10�5 meters, to
9
From: PHENIX Collab (15)
L. Apolinário OppO 2021
C R163537&*3124(15(*+"(0&$*12(4+1M"$(326%7"6(#'(*+"(32*"$&7*312(M3*+(&(6"712532"6(4*&*"(15(A&**"$I
6
Jet quenching
N2"8&4*37(47&**"$32F(0$17"44"4I=8&4*37(47&**"$32F(0$17"44"4I
T"*
R"63%A($"7138
The Physics Case for sPHENIX What are the inner workings of the QGP?
ments is given in Section 1.5. We note that enhancements in q̂ above the critical temperaturemay be a generic feature of many models, as illustrated by the three conjectured evolutions,and so underscore the need for detailed measurements of quark-gluon plasma propertiesnear the transition temperature.
All measurements in heavy ion collisions are the result of emitted particles integrated overthe entire time evolution of the reaction, covering a range of temperatures. Similar to thehydrodynamic model constraints, the theory modeling requires a consistent temperatureand scale dependent model of the quark-gluon plasma and is only well constrained byprecision data through different temperature evolutions, as measured at RHIC and theLHC.
g*Q2
q
?
QGP
Q2 PT Initial Parton
What scale sets this transition?
Tc
Probe Integrates Over a Range of Q2
pQCDScattering from Point-Like BareColor Charges
µD
pQCD ScatteringFrom Quasiparticles
with size ~ µDebye
Strong CouplingNo Quasiparticles
µDebye ! 0
AdS/CFT
?!
" ?
What scale sets this transition?
Scattering from Thermal Mass Gluons?
Figure 1.7: (Left) Diagram of a quark exchanging a virtual gluon with an unknown object inthe QGP. This highlights the uncertainty for what sets the scale of the interaction and whatobjects or quasiparticles are recoiling. (Right) Diagram as a function of the Q2 for the netinteraction of the parton with the medium and the range of possibilities for the recoil objects.
1.3 What are the inner workings of the QGP?
A second axis along which one can investigate the underlying structure of thequark-gluon plasma concerns the question of what length scale of the medium is beingprobed by jet quenching processes. In electron scattering, the scale is set by the virtualityof the exchanged photon, Q2. By varying this virtuality one can obtain information overan enormous range of scales: from pictures of viruses at length scales of 10�5 meters, to
9
From: PHENIX Collab (15)
L. Apolinário OppO 2021
C R163537&*3124(15(*+"(0&$*12(4+1M"$(326%7"6(#'(*+"(32*"$&7*312(M3*+(&(6"712532"6(4*&*"(15(A&**"$I
6
Jet quenching
N2"8&4*37(47&**"$32F(0$17"44"4I=8&4*37(47&**"$32F(0$17"44"4I
T"*
R"63%A($"7138
The Physics Case for sPHENIX What are the inner workings of the QGP?
ments is given in Section 1.5. We note that enhancements in q̂ above the critical temperaturemay be a generic feature of many models, as illustrated by the three conjectured evolutions,and so underscore the need for detailed measurements of quark-gluon plasma propertiesnear the transition temperature.
All measurements in heavy ion collisions are the result of emitted particles integrated overthe entire time evolution of the reaction, covering a range of temperatures. Similar to thehydrodynamic model constraints, the theory modeling requires a consistent temperatureand scale dependent model of the quark-gluon plasma and is only well constrained byprecision data through different temperature evolutions, as measured at RHIC and theLHC.
g*Q2
q
?
QGP
Q2 PT Initial Parton
What scale sets this transition?
Tc
Probe Integrates Over a Range of Q2
pQCDScattering from Point-Like BareColor Charges
µD
pQCD ScatteringFrom Quasiparticles
with size ~ µDebye
Strong CouplingNo Quasiparticles
µDebye ! 0
AdS/CFT
?!
" ?
What scale sets this transition?
Scattering from Thermal Mass Gluons?
Figure 1.7: (Left) Diagram of a quark exchanging a virtual gluon with an unknown object inthe QGP. This highlights the uncertainty for what sets the scale of the interaction and whatobjects or quasiparticles are recoiling. (Right) Diagram as a function of the Q2 for the netinteraction of the parton with the medium and the range of possibilities for the recoil objects.
1.3 What are the inner workings of the QGP?
A second axis along which one can investigate the underlying structure of thequark-gluon plasma concerns the question of what length scale of the medium is beingprobed by jet quenching processes. In electron scattering, the scale is set by the virtualityof the exchanged photon, Q2. By varying this virtuality one can obtain information overan enormous range of scales: from pictures of viruses at length scales of 10�5 meters, to
9
R"63%AK326%7"6($"40124"
From: PHENIX Collab (15)
L. Apolinário OppO 2021
C R163537&*3124(15(*+"(0&$*12(4+1M"$(326%7"6(#'(*+"(32*"$&7*312(M3*+(&(6"712532"6(4*&*"(15(A&**"$I
6
Jet quenching
N2"8&4*37(47&**"$32F(0$17"44"4I=8&4*37(47&**"$32F(0$17"44"4I
T"*
R"63%A($"7138
The Physics Case for sPHENIX What are the inner workings of the QGP?
ments is given in Section 1.5. We note that enhancements in q̂ above the critical temperaturemay be a generic feature of many models, as illustrated by the three conjectured evolutions,and so underscore the need for detailed measurements of quark-gluon plasma propertiesnear the transition temperature.
All measurements in heavy ion collisions are the result of emitted particles integrated overthe entire time evolution of the reaction, covering a range of temperatures. Similar to thehydrodynamic model constraints, the theory modeling requires a consistent temperatureand scale dependent model of the quark-gluon plasma and is only well constrained byprecision data through different temperature evolutions, as measured at RHIC and theLHC.
g*Q2
q
?
QGP
Q2 PT Initial Parton
What scale sets this transition?
Tc
Probe Integrates Over a Range of Q2
pQCDScattering from Point-Like BareColor Charges
µD
pQCD ScatteringFrom Quasiparticles
with size ~ µDebye
Strong CouplingNo Quasiparticles
µDebye ! 0
AdS/CFT
?!
" ?
What scale sets this transition?
Scattering from Thermal Mass Gluons?
Figure 1.7: (Left) Diagram of a quark exchanging a virtual gluon with an unknown object inthe QGP. This highlights the uncertainty for what sets the scale of the interaction and whatobjects or quasiparticles are recoiling. (Right) Diagram as a function of the Q2 for the netinteraction of the parton with the medium and the range of possibilities for the recoil objects.
1.3 What are the inner workings of the QGP?
A second axis along which one can investigate the underlying structure of thequark-gluon plasma concerns the question of what length scale of the medium is beingprobed by jet quenching processes. In electron scattering, the scale is set by the virtualityof the exchanged photon, Q2. By varying this virtuality one can obtain information overan enormous range of scales: from pictures of viruses at length scales of 10�5 meters, to
9
R"63%AK326%7"6($"40124"
C >"4%8*32F("55"7*4I("2"$F'(8144<(A163537&*312(15(Q"*(4%#4*$%7*%$"<(A"63%AK326%7"6(&7108&2&$3*'
From: PHENIX Collab (15)
L. Apolinário OppO 2021
C R163537&*3124(15(*+"(0&$*12(4+1M"$(326%7"6(#'(*+"(32*"$&7*312(M3*+(&(6"712532"6(4*&*"(15(A&**"$I
6
Jet quenching
N2"8&4*37(47&**"$32F(0$17"44"4I=8&4*37(47&**"$32F(0$17"44"4I
T"*
R"63%A($"7138
The Physics Case for sPHENIX What are the inner workings of the QGP?
ments is given in Section 1.5. We note that enhancements in q̂ above the critical temperaturemay be a generic feature of many models, as illustrated by the three conjectured evolutions,and so underscore the need for detailed measurements of quark-gluon plasma propertiesnear the transition temperature.
All measurements in heavy ion collisions are the result of emitted particles integrated overthe entire time evolution of the reaction, covering a range of temperatures. Similar to thehydrodynamic model constraints, the theory modeling requires a consistent temperatureand scale dependent model of the quark-gluon plasma and is only well constrained byprecision data through different temperature evolutions, as measured at RHIC and theLHC.
g*Q2
q
?
QGP
Q2 PT Initial Parton
What scale sets this transition?
Tc
Probe Integrates Over a Range of Q2
pQCDScattering from Point-Like BareColor Charges
µD
pQCD ScatteringFrom Quasiparticles
with size ~ µDebye
Strong CouplingNo Quasiparticles
µDebye ! 0
AdS/CFT
?!
" ?
What scale sets this transition?
Scattering from Thermal Mass Gluons?
Figure 1.7: (Left) Diagram of a quark exchanging a virtual gluon with an unknown object inthe QGP. This highlights the uncertainty for what sets the scale of the interaction and whatobjects or quasiparticles are recoiling. (Right) Diagram as a function of the Q2 for the netinteraction of the parton with the medium and the range of possibilities for the recoil objects.
1.3 What are the inner workings of the QGP?
A second axis along which one can investigate the underlying structure of thequark-gluon plasma concerns the question of what length scale of the medium is beingprobed by jet quenching processes. In electron scattering, the scale is set by the virtualityof the exchanged photon, Q2. By varying this virtuality one can obtain information overan enormous range of scales: from pictures of viruses at length scales of 10�5 meters, to
9
R"63%AK326%7"6($"40124"
C >"4%8*32F("55"7*4I("2"$F'(8144<(A163537&*312(15(Q"*(4%#4*$%7*%$"<(A"63%AK326%7"6(&7108&2&$3*'
f+37+(1#4"$L"4(&$"(A14*(4"243*3L"(*1("&7+(g%"27+32F("55"7*cFrom: PHENIX Collab (15)
L. Apolinário OppO 2021
C [1M&$64(&2(&77%$&*"(6"*"$A32&*312(15(GHD(7+&$&7*"$34*374I(
C [$&240&$"27'(*1(*+"(0&44&F"(15(&(+3F+(A1A"2*%A(0&$*378"(@=FI*$&2401$*(71"55373"2*<(g+&*B(
C ;12434*"2*(6"47$30*312(15(432F8"(+&$6(&26(A%8*308"(415*(47&**"$32F($"F3A"
7
Energy Loss
[Feal et al: 1911.01309]
[Feal, Salgado, Vasquez (19), Andrés, LA, Dominguez (20)]
[Heavy-quarks: S. Cao et al (19)]
L. Apolinário OppO 2021
C [1M&$64(&2(&77%$&*"(6"*"$A32&*312(15(GHD(7+&$&7*"$34*374I(
C [$&240&$"27'(*1(*+"(0&44&F"(15(&(+3F+(A1A"2*%A(0&$*378"(@=FI*$&2401$*(71"55373"2*<(g+&*B(
C ;12434*"2*(6"47$30*312(15(432F8"(+&$6(&26(A%8*308"(415*(47&**"$32F($"F3A"
7
Energy Loss
[Feal et al: 1911.01309]
[Feal, Salgado, Vasquez (19), Andrés, LA, Dominguez (20)]
[Heavy-quarks: S. Cao et al (19)]
R16"8K6"0"26"2*(0&$&A"*"$4I(g+&*<(6"#'"(A&44c
L. Apolinário OppO 2021
C [1M&$64(&2(&77%$&*"(6"*"$A32&*312(15(GHD(7+&$&7*"$34*374I(
C [$&240&$"27'(*1(*+"(0&44&F"(15(&(+3F+(A1A"2*%A(0&$*378"(@=FI*$&2401$*(71"55373"2*<(g+&*B(
C ;12434*"2*(6"47$30*312(15(432F8"(+&$6(&26(A%8*308"(415*(47&**"$32F($"F3A"
7
Energy Loss
[Feal et al: 1911.01309]
[Feal, Salgado, Vasquez (19), Andrés, LA, Dominguez (20)]
[Heavy-quarks: S. Cao et al (19)]
R16"8K6"0"26"2*(0&$&A"*"$4I(g+&*<(6"#'"(A&44c
[Caucal, Iancu, Soyez (21), Adhya, Salgado, Spousta, Tywoniuk (20)]
=L18%*312(M3*+(5&4*("h0&2632F(A"63%Ac
[Salgado, Wiedemann (02, 03), Zakharov (07)]
L. Apolinário OppO 2021
C [1M&$64(&(712434*"2*(*$"&*A"2*(15(A%8*3KF8%12("A344312(0$17"44(
C N6"2*3537&*312(15(32KA"63%A(A163537&*3124(15(G;i(0&$*12(4+1M"$
8
Jet Substructure [Casalderrey-Solana et al (10)][ALICE PLB 802 (2020) 135227]
[arXiv:1905.02512]
L. Apolinário OppO 2021
C [1M&$64(&(712434*"2*(*$"&*A"2*(15(A%8*3KF8%12("A344312(0$17"44(
C N6"2*3537&*312(15(32KA"63%A(A163537&*3124(15(G;i(0&$*12(4+1M"$
8
Jet Substructure [Casalderrey-Solana et al (10)][ALICE PLB 802 (2020) 135227]
[arXiv:1905.02512]
[arXiv:1905.02512]
L. Apolinário OppO 2021
C [1M&$64(&(712434*"2*(*$"&*A"2*(15(A%8*3KF8%12("A344312(0$17"44(
C N6"2*3537&*312(15(32KA"63%A(A163537&*3124(15(G;i(0&$*12(4+1M"$
8
Jet Substructure [Casalderrey-Solana et al (10)][ALICE PLB 802 (2020) 135227]
[arXiv:1905.02512]
?1(43F23537&2*(6355"$"27"(#"*M""2(A16"84(*+&*(&771%2*(1$(21*(51$(
71+"$"27"("55"7*4d
[arXiv:1905.02512]
L. Apolinário OppO 2021
C [1M&$64(&(712434*"2*(*$"&*A"2*(15(A%8*3KF8%12("A344312(0$17"44(
C N6"2*3537&*312(15(32KA"63%A(A163537&*3124(15(G;i(0&$*12(4+1M"$(
C G;i("L18%*312("g%&*3124(*+&*(3278%6"(71$$"7*3124(6%"(*1(*+"(32*"$5"$"27"(15(4%#4"g%"2*("A3**"$4Y(
9
Jet Substructure[Domíngez, et al (20)]
[Barata, Domínguez, Salgado, Vila (21)]
L. Apolinário OppO 2021
C [1M&$64(&(712434*"2*(*$"&*A"2*(15(A%8*3KF8%12("A344312(0$17"44(
C N6"2*3537&*312(15(32KA"63%A(A163537&*3124(15(G;i(0&$*12(4+1M"$(
C G;i("L18%*312("g%&*3124(*+&*(3278%6"(71$$"7*3124(6%"(*1(*+"(32*"$5"$"27"(15(4%#4"g%"2*("A3**"$4Y(
9
Jet Substructure
f+&*(34(*+"(0+"21A"2181F37&8(A&235"4*&*312c
[Domíngez, et al (20)][Barata, Domínguez, Salgado, Vila (21)]
L. Apolinário OppO 2021
C T"*(#$1&6"232F(832j"6(*1("2"$F'(8144(0$17"44"4(
C k%*(34(&841(32*$32437(*1(G;i(L&7%%A($&63&*312d
10
Acoplanarity[D’Eramo, et al (13), D’Eramo, et al (19)]
[Chen et al (17)]
D$1#ſ*'(15(532632F(&(0&$*12(M3*+(0A32S[(L"(&2(&2F8"(𝛉A32
[D’Eramo et al: 1808.03250]
N271A32F(F8%12(15(Z-(H"\
k$37jI([(W(Z--(R"\<(9(W(_(5A
/%*F132F(@6"58"7*"6B(0&$*12(
M3*+(0<𝛉
L. Apolinário OppO 2021
C T"*(#$1&6"232F(832j"6(*1("2"$F'(8144(0$17"44"4(
C k%*(34(&841(32*$32437(*1(G;i(L&7%%A($&63&*312d
11
Acoplanarity
[STAR: 1702.01108]
[CMS (20), ALICE JHEP 09 (2015)][STAR Phys.Rev.C 96 (2017) 2, 024905]
[CMS: HIN-19-006-pas]
lmT"*
634*$3#%*312(15($"7138(Q"*47+&$F"6(0&$*378"4(&M&'(5$1A(l(63$"7*312
+&6$12(m(Q"*
L. Apolinário OppO 2021
C T"*(#$1&6"232F(832j"6(*1("2"$F'(8144(0$17"44"4(
C k%*(34(&841(32*$32437(*1(G;i(L&7%%A($&63&*312d
11
Acoplanarity
[STAR: 1702.01108]
!3$4*(+32*4(15(Q"*(#$1&6"232F(0+'4374c
[CMS (20), ALICE JHEP 09 (2015)][STAR Phys.Rev.C 96 (2017) 2, 024905]
[CMS: HIN-19-006-pas]
lmT"*
634*$3#%*312(15($"7138(Q"*47+&$F"6(0&$*378"4(&M&'(5$1A(l(63$"7*312
+&6$12(m(Q"*
L. Apolinário OppO 2021
C T"*(#$1&6"232F(832j"6(*1("2"$F'(8144(0$17"44"4(
C k%*(34(&841(32*$32437(*1(G;i(L&7%%A($&63&*312d
11
Acoplanarity
[STAR: 1702.01108]
!3$4*(+32*4(15(Q"*(#$1&6"232F(0+'4374c
[CMS (20), ALICE JHEP 09 (2015)][STAR Phys.Rev.C 96 (2017) 2, 024905]
[CMS: HIN-19-006-pas]
lmT"*
634*$3#%*312(15($"7138(Q"*47+&$F"6(0&$*378"4(&M&'(5$1A(l(63$"7*312
+&6$12(m(Q"*
/$(RDN(m(A"63%A($"40124"c
[Chen et al (21)]
L. Apolinário OppO 202112
QGP onset scale
D#D#U"U"0D#
00
E88(GHD(43F2&*%$"4(P(P(P
N271278%43L"($"4%8*4(P(P(❌
L. Apolinário OppO 202112
QGP onset scale
D#D#U"U"0D#
00
N4(*+"$"(Q"*(g%"27+32F(32(83F+*(4'4*"A4c
E88(GHD(43F2&*%$"4(P(P(P
N271278%43L"($"4%8*4(P(P(❌
L. Apolinário OppO 202112
QGP onset scale
D#D#U"U"0D#
00
N4(*+"$"(Q"*(g%"27+32F(32(83F+*(4'4*"A4c
E88(GHD(43F2&*%$"4(P(P(P
N271278%43L"($"4%8*4(P(P(❌
L. Apolinário OppO 2021
C R&F23*%6"(15(T"*(g%"27+32F(6"0"264(12(4'4*"A(43J"I(
C D"$30+"$&8(7188343124I("h0"7*"6(41A"("2"$F'(8144
13
Light Systems
Studies of System Size dependence
D#( D#( D#(
L. Apolinário OppO 2021
C R&F23*%6"(15(T"*(g%"27+32F(6"0"264(12(4'4*"A(43J"I(
C D"$30+"$&8(7188343124I("h0"7*"6(41A"("2"$F'(8144
13
Light Systems
Studies of System Size dependence
D#( D#( D#(
O"L"$&8(7+&2F"4(&*(*+"(4&A"(*3A"I("2"$F'(8144<(2%78"&$(1L"$8&0<d(
@*11(A&2'(L&$3"4B(
[Citron, Dainese et al (19)]
[JEWEL: Zapp (14)]
[arXiv: 1812.06772]
L. Apolinário OppO 2021
C R&F23*%6"(15(T"*(g%"27+32F(6"0"264(12(4'4*"A(43J"I(
C 93F+*"$(2%78"3(&881M(*1(53h(F"1A"*$'
14
Light Systems
Studies of System Size dependence (always fixing geometry - [0-10]%)
E$(E(W(Z-
/(E(W(.n(U"(
E(W(.,oD#(E(W(,-n
L. Apolinário OppO 2021
C R&F23*%6"(15(T"*(g%"27+32F(6"0"264(12(4'4*"A(43J"I(
C 93F+*"$(2%78"3(&881M(*1(53h(F"1A"*$'
14
Light Systems
Studies of System Size dependence (always fixing geometry - [0-10]%)
E$(E(W(Z-
/(E(W(.n(U"(
E(W(.,oD#(E(W(,-n
[arXiv:2007.13754]
[Huss, Kurkela, Mazeliauskas, Paatelainen, Van der Schee, Widemann (20)]
L. Apolinário OppO 2021
C R&F23*%6"(15(T"*(g%"27+32F(6"0"264(12(4'4*"A(43J"I(
C 93F+*"$(2%78"3(&881M(*1(53h(F"1A"*$'
14
Light Systems [arXiv:2007.13754]
[Huss, Kurkela, Mazeliauskas, Paatelainen, Van der Schee, Widemann (20)]
/(E(W(.n(U"(
E(W(.,oD#(E(W(,-n
L. Apolinário OppO 2021
C N278%43L"(Q"*('3"86(326"0"26"2*(15(2%78"&$(1L"$8&0I
15
Energy Loss in OO
<latexit sha1_base64="o3ipC2DmG8xokcN4UxSRmRqmKFs=">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</latexit>
Rh,jAA(pT , y) =
1
hTAAi(1/Nev)dN
h,jAA/dpT dy
d�h,jpp /dpT dy
L. Apolinário OppO 2021
C N278%43L"(Q"*('3"86(326"0"26"2*(15(2%78"&$(1L"$8&0I
15
Energy Loss in OO
<latexit sha1_base64="o3ipC2DmG8xokcN4UxSRmRqmKFs=">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</latexit>
Rh,jAA(pT , y) =
1
hTAAi(1/Nev)dN
h,jAA/dpT dy
d�h,jpp /dpT dy
[Huss, Kurkela, Mazeliauskas, Paatelainen, Van der Schee, Widemann (20)]
[arXiv:2007.13754]
O""(:%44p4(*&8j
L. Apolinário OppO 2021
C N278%43L"(Q"*('3"86(326"0"26"2*(15(2%78"&$(1L"$8&0I
15
Energy Loss in OO
<latexit sha1_base64="o3ipC2DmG8xokcN4UxSRmRqmKFs=">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</latexit>
Rh,jAA(pT , y) =
1
hTAAi(1/Nev)dN
h,jAA/dpT dy
d�h,jpp /dpT dy
[Huss, Kurkela, Mazeliauskas, Paatelainen, Van der Schee, Widemann (20)]
[arXiv:2007.13754]
2Di!4(08&'(&2(3A01$*&2*($18"(M+"2(&44"4432F(4A&88(Q"*(g%"27+32F("55"7*4e(
@4""(D&&jj32"2p4(*&8jB
O""(:%44p4(*&8j
L. Apolinário OppO 2021
C O3F2&*%$"4(15("2"$F'(8144(32(l(m(Q"*(7132736"27"4c
16
Jet Coincidences [Citron, Dainese et al (19)]
[arXiv: 1812.06772]
T=f=9(@21($"71384B(m(kQ1$j"2(=h0&24312(m(O*"5&2Kk18*JA&22(83A3*
[B. Silva MsC (19)]
[JEWEL: Zapp (14)]
L. Apolinário OppO 2021
C O3F2&*%$"4(15("2"$F'(8144(32(𝜸(m(Q"*(7132736"27"4c
17
Jet Coincidences
[arXiv: 1809.07280]
[ATLAS: Phys.Lett.B 789 (2019) 167-190]
L. Apolinário OppO 2021
C O3F2&*%$"4(15("2"$F'(8144(32(𝜸(m(Q"*(7132736"27"4c
17
Jet Coincidences
[arXiv: 1809.07280]
[ATLAS: Phys.Lett.B 789 (2019) 167-190]
D1443#383*'(51$(//($%2(@$"g%3$"4(4*&*34*374Bd
L. Apolinário OppO 2021
C 911j32F(32436"(15(Q"*4(32*$32437(7124*3*%*312(
C E881M4(*1(4"8"7*($"F3124(15(0+&4"(40&7"(M+"$"(A"63%A("55"7*4(&$"("2+&27"6
18
Jet substructure [Andrews et al (20)]
[Andrews et al: 1808.03689]
[Andrews et al: 1808.03689]
L. Apolinário OppO 2021
C 911j32F(32436"(15(Q"*4(32*$32437(7124*3*%*312(
C E881M4(*1(4"8"7*($"F3124(15(0+&4"(40&7"(M+"$"(A"63%A("55"7*4(&$"("2+&27"6
18
Jet substructure[Dominguez et al (20), Caucal et al (18), Caucal, Iancu, Soyez (20)]
[Andrews et al (20)]
[Caucal et al: 2012.01457][Dominguez et al: 1907.03653]
R"63%A(A163537&*312(5&7*1$
L. Apolinário OppO 2021
C 911j32F(32436"(15(Q"*4(32*$32437(7124*3*%*312(
C E881M4(*1(4"8"7*($"F3124(15(0+&4"(40&7"(M+"$"(A"63%A("55"7*4(&$"("2+&27"6
18
Jet substructure[Dominguez et al (20), Caucal et al (18), Caucal, Iancu, Soyez (20)]
[Andrews et al (20)]
[ALICE: 2002.05307]
[ALICE: Nucl.Phys.A 1005 (2021) 121906]
[Dominguez et al: 1907.03653]
R"63%A(A163537&*312(5&7*1$
L. Apolinário OppO 2021
C 911j32F(32436"(15(Q"*4(32*$32437(7124*3*%*312(
C E881M4(*1(4"8"7*($"F3124(15(0+&4"(40&7"(M+"$"(A"63%A("55"7*4(&$"("2+&27"6
18
Jet substructure[Dominguez et al (20), Caucal et al (18), Caucal, Iancu, Soyez (20)]
N27$"&4"(0$"734312(*1(4*%6'(A"63%AK326%7"6("55"7*4
[Andrews et al (20)]
[ALICE: 2002.05307]
[ALICE: Nucl.Phys.A 1005 (2021) 121906]
[Dominguez et al: 1907.03653]
R"63%A(A163537&*312(5&7*1$
L. Apolinário OppO 2021
C N278%43L"(Q"*(40"7*$&(34(&8M&'4(&(A3h*%$"(15(6355"$"2*(A&F23*%6"4(15(g%"27+32F(
C D1443#383*'(*1(4"8"7*(Q"*4(M+14"(0&$*12(4+1M"$(323*3&*"6(&*("&$8'(4*&F"4(@4*$12F8'(A16353"6Bc
19
Jet spacetime structure
D&$*12(O+1M"$
G.
G, G_
GZ GX Gn Gq
T"*
. Z, _
L. Apolinário OppO 2021
C N278%43L"(Q"*(40"7*$&(34(&8M&'4(&(A3h*%$"(15(6355"$"2*(A&F23*%6"4(15(g%"27+32F(
C D1443#383*'(*1(4"8"7*(Q"*4(M+14"(0&$*12(4+1M"$(323*3&*"6(&*("&$8'(4*&F"4(@4*$12F8'(A16353"6Bc
19
Jet spacetime structure
D&$*12(O+1M"$
G.
G, G_
GZ GX Gn Gq
T"*
. Z, _!&4*(=h0&2632F(A"63%A(R"63%AK326%7"6($&63&*312
E663*312&8(0&$*378"4(*1(#"(78%4*"$"6(32(*+"(Q"*(+34*1$'
L. Apolinário OppO 2021
C N278%43L"(Q"*(40"7*$&(34(&8M&'4(&(A3h*%$"(15(6355"$"2*(A&F23*%6"4(15(g%"27+32F(
C D1443#383*'(*1(4"8"7*(Q"*4(M+14"(0&$*12(4+1M"$(323*3&*"6(&*("&$8'(4*&F"4(@4*$12F8'(A16353"6Bc
19
Jet spacetime structure
D&$*12(O+1M"$
G.
G, G_
GZ GX Gn Gq
T"*
. Z, _!&4*(=h0&2632F(A"63%A(R"63%AK326%7"6($&63&*312
E663*312&8(0&$*378"4(*1(#"(78%4*"$"6(32(*+"(Q"*(+34*1$'
ccccc
L. Apolinário OppO 2021
C N278%43L"(Q"*(40"7*$&(34(&8M&'4(&(A3h*%$"(15(6355"$"2*(A&F23*%6"4(15(g%"27+32F(
C D1443#383*'(*1(4"8"7*(Q"*4(M+14"(0&$*12(4+1M"$(323*3&*"6(&*("&$8'(4*&F"4(@4*$12F8'(A16353"6Bc
20
Jet spacetime structure [LA, Cordeiro, Zapp (20)]
dij = min(p2pt,i, p2pt,j)
�R2ij
R2<latexit sha1_base64="wKK30y+eMCLYOEiAc/RsdFnnYak=">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</latexit>
diB = p2pt,i<latexit sha1_base64="cfzX9SCuCYOofNktoSnifTJj8H8=">AAACJXicbVDLSsNAFJ34tr6q4srNYBFcSEmqoBtBKojLCrYKbQ2TyY0dOpmEmRuhhHyMK0G/xZ0IrvwOd04fC18HLhzOuRfOPUEqhUHXfXempmdm5+YXFktLyyura+X1jZZJMs2hyROZ6JuAGZBCQRMFSrhJNbA4kHAd9M+G/vU9aCMSdYWDFLoxu1MiEpyhlfzyVujnol7QE5r6Oe6L4javpYVfrrhVdwT6l3gTUiETNPzyZydMeBaDQi6ZMW3PTbGbM42CSyhKncxAynif3UHbUsViMN18FL+gu1YJaZRoOwrpSP1+kbPYmEEc2M2YYc/89obiv56xUXoQWu8cBipmiqoER4//DITRcTcXKs0QFB/niTJJMaHDymgoNHCUA0sY18K+RHmPacbRFluyXXm/m/lLWrWqd1CtXR5WTuuT1hbINtkhe8QjR+SUXJAGaRJOcvJAnsiz8+i8OK/O23h1ypncbJIfcD6+AGNepRA=</latexit>
0(W( -YX(@𝜏Bdij ⇠ pT,i
�R2ij
R2⇠ pT ✓
2 ⇠ 1
⌧form<latexit sha1_base64="Nm1iQqftl4F+ojBi2pccHT2vifo=">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</latexit>
<latexit sha1_base64="aWwaeP+7nXwzNcv7MuI7QSTVDok=">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</latexit>
⌧form ⇡ E
Q2⇡ 1
2Ez(1� z)(1� cos ✓12)
[arXiv. 2012.02199]
L. Apolinário OppO 2021
C N278%43L"(Q"*(40"7*$&(34(&8M&'4(&(A3h*%$"(15(6355"$"2*(A&F23*%6"4(15(g%"27+32F(
C D1443#383*'(*1(4"8"7*(Q"*4(M+14"(0&$*12(4+1M"$(323*3&*"6(&*("&$8'(4*&F"4(@4*$12F8'(A16353"6Bc
20
Jet spacetime structure [LA, Cordeiro, Zapp (20)]
[arXiv. 2012.02199]
L. Apolinário OppO 2021
C N278%43L"(Q"*(40"7*$&(34(&8M&'4(&(A3h*%$"(15(6355"$"2*(A&F23*%6"4(15(g%"27+32F(
C D1443#383*'(*1(4"8"7*(Q"*4(M+14"(0&$*12(4+1M"$(323*3&*"6(&*("&$8'(4*&F"4(@4*$12F8'(A16353"6Bc
20
Jet spacetime structure
;+11432F(&(#"**"$(0$1h'("2+&27"4(0$"734312(&26(&881M4(*1(4"8"7*(6355"$"2*(Q"*(78&44"4((@#&4"6(12(g%"27+32F(A&F23*%6"B
[LA, Cordeiro, Zapp (20)]
[arXiv. 2012.02199]
L. Apolinário OppO 2021
C R&7+32"(8"&$232F(*"7+23g%"4(A3F+*(&841(+"80(*1(4"8"7*(4*$12F8'(A16353"6(Q"*4(
C =hI(7&81$3A"*$37(Q"*(3A&F"4
21
Machine Learning[LA, Castro, Crispim, Milhano, Pedro, Peres (under preparation)]
[Du, Pablos, Tywoniuk (20)]
C T"M"8(l(k1412(@A%124B(m(T"*(r(XY-,(["\(@21($"71384B(
C l(0*(aW(o-(
C >(W(-YX($"713832F(Q"*(@qS)(𝞹B(&26(0*(a(_-
L. Apolinário OppO 2021
C R&7+32"(8"&$232F(*"7+23g%"4(A3F+*(&841(+"80(*1(4"8"7*(4*$12F8'(A16353"6(Q"*4(
C =hI(7&81$3A"*$37(Q"*(3A&F"4
21
Machine Learning[LA, Castro, Crispim, Milhano, Pedro, Peres (under preparation)]
[Du, Pablos, Tywoniuk (20)]
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5r
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
1/N
dN
/dr
Vacuum Medium
CNN output < 0.6 CNN output > 0.6
*Preliminary*
*Preliminary*
L. Apolinário OppO 2021
C R&7+32"(8"&$232F(*"7+23g%"4(A3F+*(&841(+"80(*1(4"8"7*(4*$12F8'(A16353"6(Q"*4(
C =hI(7&81$3A"*$37(Q"*(3A&F"4
21
Machine Learning[LA, Castro, Crispim, Milhano, Pedro, Peres (under preparation)]
[Du, Pablos, Tywoniuk (20)]
D$1A3432F(4"8"7*312(15(A"63%AKA16353"6(Q"*4(@*$&32"6(12(A16"8(6"0"26"2*(5"&*%$"4dB
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5r
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
1/N
dN
/dr
Vacuum Medium
CNN output < 0.6 CNN output > 0.6
*Preliminary*
*Preliminary*
L. Apolinário OppO 2021
C GHDK83j"("55"7*4(32(4A&88(4'4*"A4I(
C E$"(*+"'(&88($"8&*"6(*1(*+"(4&A"(0+"21A"2&c(
C !81M(&26(4*$&2F"2"44(5$1A(212KGHD(0+'4374c
22
Soft and Hard Scales[Andrés, Armesto, Niemi, Paatelainen, Salgado(19)]
[Andrés et al: 1902.03231]
L. Apolinário OppO 2021
C GHDK83j"("55"7*4(32(4A&88(4'4*"A4I(
C E$"(*+"'(&88($"8&*"6(*1(*+"(4&A"(0+"21A"2&c(
C !81M(&26(4*$&2F"2"44(5$1A(212KGHD(0+'4374c
22
Soft and Hard Scales[Andrés, Armesto, Niemi, Paatelainen, Salgado(19)]
?12K*$3L3&8(7122"7*312(@.(["\(sK(.(H"\B(
>EE(M3*+(L,(7&2(0$1L36"(5%$*+"$(7124*$&324
[Andrés et al: 1902.03231]
L. Apolinário OppO 2021
C GHDK83j"("55"7*4(32(4A&88(4'4*"A4I(
C E$"(*+"'(&88($"8&*"6(*1(*+"(4&A"(0+"21A"2&c(
C !81M(&26(4*$&2F"2"44(5$1A(212KGHD(0+'4374c
22
Soft and Hard Scales[Andrés, Armesto, Niemi, Paatelainen, Salgado(19)]
?12K*$3L3&8(7122"7*312(@.(["\(sK(.(H"\B(
>EE(M3*+(L,(7&2(0$1L36"(5%$*+"$(7124*$&324
[Andrés et al: 1902.03231]
[Katz, Prado, Noronha-Hostler, Suaide (20)]
O""(?1$12+&K:14*8"$p4(*&8j
[Katz et al: 1907.03308]
L. Apolinário OppO 2021
C /h'F"2($%24I(%2817j(Q"*(g%"27+32F(4*%63"4(#'(L&$'32F(4'4*"A(43J"(M3*+32(*+"(4&A"(7"2*$&83*'(F"1A"*$'
C H"1A"*$'(32(83F+*(4'4*"A4(L4(F"1A"*$'(32(0D#c
23
Summary/Outlook
L. Apolinário OppO 2021
C /h'F"2($%24I(%2817j(Q"*(g%"27+32F(4*%63"4(#'(L&$'32F(4'4*"A(43J"(M3*+32(*+"(4&A"(7"2*$&83*'(F"1A"*$'
C H"1A"*$'(32(83F+*(4'4*"A4(L4(F"1A"*$'(32(0D#c
C T"*(g%"27+32F(32(4A&88(4'4*"A4I
C ;+&88"2F32FI($"g%3$"(*+"1$"*37&8(712*$18(1L"$(212K"2"$F'(8144(@2Di!4B
C :1M(M"88(7&83#$&*"6(34(1%$($"5"$"27"c
23
Summary/Outlook
L. Apolinário OppO 2021
C /h'F"2($%24I(%2817j(Q"*(g%"27+32F(4*%63"4(#'(L&$'32F(4'4*"A(43J"(M3*+32(*+"(4&A"(7"2*$&83*'(F"1A"*$'
C H"1A"*$'(32(83F+*(4'4*"A4(L4(F"1A"*$'(32(0D#c
C T"*(g%"27+32F(32(4A&88(4'4*"A4I
C ;+&88"2F32FI($"g%3$"(*+"1$"*37&8(712*$18(1L"$(212K"2"$F'(8144(@2Di!4B
C :1M(M"88(7&83#$&*"6(34(1%$($"5"$"27"c
C !3$4*($%2(M388(%2817j(3278%43L"(Q"*(A"&4%$"A"2*4<(#%*(7132736"27"4(M388(83j"8'(#"(83A3*"6d
C >EEI(4"8"7*312(#3&4(@12(0[(15(Q"*Bc
C T"*(4%#4*$%7*%$"I(36"2*35'(78&44"4(15(t"&$8'Sg%"27+"6u(Q"*4Y(9%A32143*'(7124*$&32*4c
23
Summary/Outlook
L. Apolinário OppO 2021
C /h'F"2($%24I(%2817j(Q"*(g%"27+32F(4*%63"4(#'(L&$'32F(4'4*"A(43J"(M3*+32(*+"(4&A"(7"2*$&83*'(F"1A"*$'
C H"1A"*$'(32(83F+*(4'4*"A4(L4(F"1A"*$'(32(0D#c
C T"*(g%"27+32F(32(4A&88(4'4*"A4I
C ;+&88"2F32FI($"g%3$"(*+"1$"*37&8(712*$18(1L"$(212K"2"$F'(8144(@2Di!4B
C :1M(M"88(7&83#$&*"6(34(1%$($"5"$"27"c
C !3$4*($%2(M388(%2817j(3278%43L"(Q"*(A"&4%$"A"2*4<(#%*(7132736"27"4(M388(83j"8'(#"(83A3*"6d
C >EEI(4"8"7*312(#3&4(@12(0[(15(Q"*Bc
C T"*(4%#4*$%7*%$"I(36"2*35'(78&44"4(15(t"&$8'Sg%"27+"6u(Q"*4Y(9%A32143*'(7124*$&32*4c
23
Summary/Outlook
Thank you!
L. Apolinário OppO 2021
C D#D#(&26(E%E%(0$"4"2*4(712434*"2*(43F2&*%$"4(15(&(GHD(51$A&*312I
26
QGP in dense systems
L. Apolinário OppO 2021
C D#D#(&26(E%E%(0$"4"2*4(712434*"2*(43F2&*%$"4(15(&(GHD(51$A&*312I
C EJ3A%*+&8(&2341*$10'(32(2K0&$*378"(71$$"8&*3124(@7188"7*3L"(581MB
26
QGP in dense systems
P
[arXiv:1808.0395]
[ATLAS: Eur.Phys.J.C 78 (2018) 12, 997]
L. Apolinário OppO 2021
C D#D#(&26(E%E%(0$"4"2*4(712434*"2*(43F2&*%$"4(15(&(GHD(51$A&*312I
C EJ3A%*+&8(&2341*$10'(32(2K0&$*378"(71$$"8&*3124(@7188"7*3L"(581MB
C N27$"&4"(15(4*$&2F"(+&6$124('3"864(@4*$&2F"2"44("2+&27"A"2*B
26
QGP in dense systems
P
P [arXiv:1307.5543]
[ALICE: Phys.Lett.B 734 (2014) 409-410]
L. Apolinário OppO 2021
C D#D#(&26(E%E%(0$"4"2*4(712434*"2*(43F2&*%$"4(15(&(GHD(51$A&*312I
C EJ3A%*+&8(&2341*$10'(32(2K0&$*378"(71$$"8&*3124(@7188"7*3L"(581MB
C N27$"&4"(15(4*$&2F"(+&6$124('3"864(@4*$&2F"2"44("2+&27"A"2*B
C O%00$"44312(15(432F8"(+&6$12(40"7*$&(@"2"$F'(8144B
26
QGP in dense systems[nucl-ex/0109003]
[PHENIX: Phys.Rev.Lett. 88 (2002) 022301][STAR: Phys. Rev. Lett. 89 (2002) 202301]
[nucl-ex/0109003]
P
P
P
L. Apolinário OppO 2021
C D#D#(&26(E%E%(0$"4"2*4(712434*"2*(43F2&*%$"4(15(&(GHD(51$A&*312I
C EJ3A%*+&8(&2341*$10'(32(2K0&$*378"(71$$"8&*3124(@7188"7*3L"(581MB
C N27$"&4"(15(4*$&2F"(+&6$124('3"864(@4*$&2F"2"44("2+&27"A"2*B
C O%00$"44312(15(432F8"(+&6$12(40"7*$&(@"2"$F'(8144B
C O%00$"44312(15(Q"*(40"7*$&(@"2"$F'(8144B
27
QGP in dense systems
P
P
P
P
[arXiv:1504.04337]
[ATLAS: JHEP 09 (2015) 050]
L. Apolinário OppO 2021
C D#D#(&26(E%E%(0$"4"2*4(712434*"2*(43F2&*%$"4(15(&(GHD(51$A&*312I
C EJ3A%*+&8(&2341*$10'(32(2K0&$*378"(71$$"8&*3124(@7188"7*3L"(581MB
C N27$"&4"(15(4*$&2F"(+&6$124('3"864(@4*$&2F"2"44("2+&27"A"2*B
C O%00$"44312(15(432F8"(+&6$12(40"7*$&(@"2"$F'(8144B
C O%00$"44312(15(Q"*(40"7*$&(@"2"$F'(8144B
C R163537&*312(15(Q"*(4%#4*$%7*%$"
27
QGP in dense systems
P
P
P
P
P
[Adapted from: K. Zapp]
!$&7*312(15("2"$F'(15(Q"*(5$&FA"2*4(@D#D#S00B
T"*($&63&8(0$1538"(@D#D#S00B
[arXiv:1809.08602] [arXiv:1801.04895]
[CMS: PRL 122 (2019) 152001][CMS: Phys. Rev. Lett. 121 (2018) 242301]
L. Apolinário OppO 2021
C N6"2*3537&*312(15($"6%7"6(4"*(15(1#4"$L"4(*+&*(&$"(A14*(6347$3A32&2*
28
Multibayesian approach
O1A"(0&3$(15(1#4"$L"4(61(21*(7&$$'(326"0"26"2*(3251$A&*312
[arXiv:2011.01430]
[JETSCAPE (20,21)]
[STRONG 2020 - NA3 (on-going)]
L. Apolinário Quark Matter 2019
C R14*8'(4""2(32(Q"*($&63&8(0$1538"(#%*(43F2&*%$"4(15("&7+(&00$1&7+(34(L"$'(6355"$"2*I
29
Medium Response
[Coupled Jet-Fluid: 1701.07951] [MARTINI:1807.06550][Hybrid: 1609.05842]
[Casalderrey-Solana, Gulhan, Milhano, Pablos, Rajagopal (14;17)][Tachibana, Chang, Qin (17)]
[Park, Jeon, Gale (18)]
L. Apolinário Quark Matter 2019
C R14*8'(4""2(32(Q"*($&63&8(0$1538"(#%*(43F2&*%$"4(15("&7+(&00$1&7+(34(L"$'(6355"$"2*I
29
Medium Response
O"L"$&8(%27"$*&32*3"4d(k%*(4""A4(*1(#"(2"7"44&$'(*1(6"47$3#"("h7"44(15(0&$*378"4(&*(8&$F"(&2F8"4d
[Coupled Jet-Fluid: 1701.07951] [MARTINI:1807.06550][Hybrid: 1609.05842]
[Casalderrey-Solana, Gulhan, Milhano, Pablos, Rajagopal (14;17)][Tachibana, Chang, Qin (17)]
[Park, Jeon, Gale (18)]
L. Apolinário Quark Matter 2019
C :1M"L"$(I
C 9&$F"(712*$3#%*312(15(A"63%A($"40124"(8"&64(*1(&(8&$F"(>(6"0"26"27"(12(Q"*(>EE
C R&F23*%6"(34(&F&32(A16"8(6"0"26"2*
30
Medium response
L. Apolinário Quark Matter 2019
C :1M"L"$(I
C 9&$F"(712*$3#%*312(15(A"63%A($"40124"(8"&64(*1(&(8&$F"(>(6"0"26"27"(12(Q"*(>EE
C R&F23*%6"(34(&F&32(A16"8(6"0"26"2*
C !"&*%$"4(15(*+"(0&$*12(4+1M"$(4""A(*1(6$3L"(#"+&L31%$((15(Q"*(>EE(@>Q"*B(@$&*+"$(*+"2(A"63%A($"40124"B
30
Medium response
L. Apolinário Quark Matter 2019
C :1M"L"$(I
C 9&$F"(712*$3#%*312(15(A"63%A($"40124"(8"&64(*1(&(8&$F"(>(6"0"26"27"(12(Q"*(>EE
C R&F23*%6"(34(&F&32(A16"8(6"0"26"2*
C !"&*%$"4(15(*+"(0&$*12(4+1M"$(4""A(*1(6$3L"(#"+&L31%$((15(Q"*(>EE(@>Q"*B(@$&*+"$(*+"2(A"63%A($"40124"B
C T"*(>&63&8(0$1538"(L4(T"*(>EE
C D%*(4"L"$"(7124*$&324(12(*+"(Q"*K326%7"6(71A012"2*
30
Medium response
@f"(&841(+&L"I(A34432F(0[<(v@$B(M3*+(0[(#32(3251$A&*312<(,K0&$*378"(71$$"8&*3124<dB
L. Apolinário OppO 2021
C R3F+*(&841(&00"&$(32(*+"(2"&$K43J"(lK+&6$12(71$$"8&*312
31
Medium response