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Mul$-­‐Jet	
  Genera$on	
  
-­‐	
  status	
  report	
  -­‐	
  
Yoshitaro	
  Takaesu	
  (KEK)	
  
November	
  16,	
  2013	
   1	
  
In	
  collabora$on	
  with	
  Fabio,	
  Johan,	
  Kaoru	
  and	
  Tim	
  
Importance	
  of	
  mul$-­‐jet	
  at	
  the	
  LHC	
  
Mul2-­‐jet	
  signature	
  	
  
appears	
  in	
  many	
  	
  
New	
  Physics	
  models.	
  
Event	
  Generator	
  	
  
should	
  	
  be	
  able	
  to	
  	
  
generate	
  	
  >	
  4	
  jets.	
  
November	
  16,	
  2013	
   2	
  
Limita$on	
  of	
  MG	
  
Generated	
  Codes	
  (>	
  8MB)	
  cannot	
  be	
  compiled	
  in	
  usual	
  PC.	
  	
  
gg 5g
qg q5g
qq qq4g
November	
  16,	
  2013	
   3	
  
8	
  MB	
  
100
101
102
10
3
104
105
2 3 4 5 6
log10
FileSize(KB)
# of Final State Particles
gg > ng
ug > ug ng
uu > uu ng
The	
  file	
  size	
  of	
  codes	
  for	
  QCD	
  processes	
  
How	
  to	
  overcome	
  	
  
the	
  Limita$on	
  
November	
  16,	
  2013	
   4	
  
gg 5g
qg q5g
qq qq4g
Structure	
  of	
  QCD	
  Amp	
  
November	
  16,	
  2013	
   5	
  
gg gg
= ig2
s[fabe
fcde
( 1 · 3 2 · 4 1 · 4 2 · 3)
+ face
fbde
( 1 · 2 3 · 4 1 · 4 2 · 3)
+ fade
fbce
( 1 · 2 3 · 4 1 · 3 2 · 4)]a
b
c
d
fabc
= 2iTr [Ta
, Tb
]Tc Tr(T a
Tb
) =
1
2
ab
=
P(b,c,d)
Tr(T a
T (b)
T (c)
T (d)
)A(a (b) (c) (d))
= Tr(T a
Tb
Tc
Td
)A(abcd) + Tr(T a
Tb
Td
Tc
)A(abdc)
+ Tr(T a
Tc
Tb
Td
)A(acbd) + Tr(T a
Tc
Td
Tb
)A(acdb)
+ Tr(T a
Td
Tb
Tc
)A(adbc) + Tr(T a
Td
Tc
Tb
)A(adcb)
Color	
  flow	
  
Color	
  Factor	
  
color-­‐ordered	
  amp.	
  
i:	
  Color	
  flow	
  
M =
Ncf
i=1
CiAi Ncf (n 1)!
November	
  16,	
  2013	
   6	
  
color
|M|2
=
Ncf
i,j color
Ci CjAi Aj
M =
Ncf
i=1
CiAi
STRATEGY	
  
Divide	
  
color
Ci Cj
A1
A2
A3
· · ·
ANcf 1
ANcf
• Speed	
  up	
  Amp	
  Evalua$on	
  
• Off-­‐shell	
  Recursive	
  Rela2ons	
  	
  
• 	
  Re-­‐organize	
  Color	
  Summa$on	
  
1/Nc	
  expansion	
  
Speed	
  up	
  Amp	
  Evalua$on	
  
November	
  16,	
  2013	
   7	
  
November	
  16,	
  2013	
   8	
  
Off-­‐shell	
  Recursive	
  Rela$ons	
  	
  
Step	
  #	
  
Time	
  performance	
  
November	
  16,	
  2013	
   9	
  
0
0.05
0.1
0.15
0.2
0.25
0.3
4 5 6 7 8
Time(ms)
Final Gluons
Recursive
Non-Recursive
n3
n
4
November	
  16,	
  2013	
   10	
  
Recursive	
  Rela$ons	
  	
  
for	
  gluonic	
  sub-­‐amplitude	
  	
  
Re-­‐organize	
  Color	
  Sum	
  
November	
  16,	
  2013	
   11	
  
November	
  16,	
  2013	
   12	
  
1/Nc	
  expansion	
  
Polynomial	
  of	
  Nc:	
  	
  
color
|M|2
=
Ncf
i,j color
Ci CjAi Aj
= Nm
c
i
|Ai|2
+
1
N2
c
Ai (Aj1,1 + Aj1,2 + · · · )
+
1
N4
c
Ai (Aj2,1 + Aj2,2 + · · · )
+ · · ·
(m = ng + nq/2)
Mul$-­‐jet	
  event	
  genera$on	
  	
  
•  Generate	
  events	
  with	
  Leading	
  Color	
  
Approxima2on	
  
•  For	
  each	
  event,	
  include	
  higher	
  order	
  
correc2ons	
  into	
  its	
  weight.	
  
November	
  16,	
  2013	
   13	
  
color
|M|2
=
i
Nm
c |Ai|2
+
1
N2
c
Ai (Aj1,1 + Aj1,2 + · · · ) +
1
Nc2
2
Ai (Aj2,1 + Aj2,2 + · · · ) + · · ·
color
|M|2
=
i
Nm
c |Ai|2
+
1
N2
c
Ai (Aj1,1 + Aj1,2 + · · · ) +
1
Nc2
2
Ai (Aj2,1 + Aj2,2 + · · · ) + · · ·
= |M|2
d n
Leading	
  color	
  summa$on	
  
Color-­‐flow	
  sampling	
  	
  
Ncf (m 1)! (	
  ~	
  40,000	
  for	
  gg	
  -­‐>	
  7g	
  )	
  
November	
  16,	
  2013	
   14	
  
color
|M|2
=
Ncf
i=1
Nm
c |Ai|2
Too	
  LARGE	
  
	
  Event	
  is	
  a	
  set	
  of	
  momenta,	
  helici$es	
  and	
  a	
  color	
  flow	
  
Results	
  
November	
  16,	
  2013	
   15	
  
November	
  16,	
  2013	
   16	
  
gg_6g NLO diff
Entries 61
Mean -0.9229
RMS 0.5551
-3 -2.5 -2 -1.5 -1 -0.5 0
0
2
4
6
8
10
12
14
gg_6g NLO diff
Entries 61
Mean -0.9229
RMS 0.5551
gg_6g NLO diff
= Nm
c
i
|Ai|2
+
1
N2
c
Ai (Aj1,1 +Aj1,2 +···)
color
|M|2
color
|M|2
=
Ncf
i=1
N(n 2)
c (N2
c 1)|Ai|2
November	
  16,	
  2013	
   17	
  
ug_u3g NLNc diff
Entries 1000
Mean 2.63
RMS 2.916
-100 -80 -60 -40 -20 0 20 40 60 80 100
0
100
200
300
400
500
ug_u3g NLNc diff
Entries 1000
Mean 2.63
RMS 2.916
ug_u3g NLNc diff
ug_u3g LNc diff
Entries 1000
Mean -27.28
RMS 13.15
-100 -80 -60 -40 -20 0 20 40 60 80 100
0
20
40
60
80
100
120
ug_u3g LNc diff
Entries 1000
Mean -27.28
RMS 13.15
ug_u3g LNc diff
color
|M|2
=
Ncf
i=1
(N2
c 1)n 1
Nn 1
c
|Ai|2
November	
  16,	
  2013	
   18	
  
Event	
  Genera$on	
  @LNc	
  	
  
pp	
  >	
  	
   W	
  +	
  2	
  jets	
   W	
  +	
  3	
  jets	
   W	
  +	
  4	
  jets	
  
MG5	
  (pb)	
   10673	
  	
   4807.9	
  ±	
  13.2	
   2913	
  ±	
  7.6	
  
LNc	
  CO	
  (pb)	
   11076	
   4623.8	
  ±	
  11.9	
   2460	
  ±	
  6	
  
• 	
  gg	
  -­‐>	
  3,4,5	
  g	
  process	
  is	
  now	
  generated	
  without	
  	
  
major	
  problem	
  and	
  agree	
  with	
  MG5	
  (3,4g).	
  
pp	
  >	
  W+2,3,4	
  jets	
  is	
  also	
  studied	
  recently	
  	
  
and	
  roughly	
  agree	
  with	
  MG5.	
  	
  	
  	
  	
  	
  	
  
Preliminary	
  
0.9
1
2 3 4 5 6 7
ratio
Final particles
107
108
10
9
1010
10
11
1012
CrossSection(fb)
gg -> ng Cross Section
CFS (LCA)
COMIX
MG5
November	
  16,	
  2013	
   19	
  
November	
  16,	
  2013	
   20	
  
0
20000
40000
60000
80000
100000
120000
140000
160000
180000
0 50 100 150 200 250 300 350
dXsec/dpT1(pb)
pT1 (GeV)
gg > 4g pT1
MG5 Exact
CFsamp LNc
0
5000
10000
15000
20000
25000
30000
35000
-3 -2 -1 0 1 2 3
dXsec/dy1(pb)
y1 (GeV)
gg > 4g y1
MG5 Exact
CFsamp LNc
10
100
1000
10000
100000
1e+06
0 50 100 150 200 250 300 350
dXsec/dpT1(pb)
pT1 (GeV)
gg > 4g pT1
MG5 Exact
CFsamp LNc
100
1000
10000
100000
0.5 1 1.5 2 2.5 3 3.5 4 4.5 5
dXsec/ddR12(pb)
dR12 (GeV)
gg > 4g dR12
MG5 Exact
CFsamp LNc
pT 1
(Linear	
  scale)	
  
pT 1
(Log	
  scale)	
  
1 R12
gg gggg
November	
  16,	
  2013	
   21	
  
dxadxbd n =
2
s
1
4 2n 2
dy1 · · · dyndp2
T 1 · · · dp2
T n 1
d 1
2
· · ·
d n 1
2
A	
  liee	
  bit	
  of	
  	
   Phase	
  Space	
  Study	
  
Alterna2ve	
  parameteriza2on	
  for	
  MadEvent:	
  	
  
suitable	
  for	
  kinema2cal	
  cuts	
  ,	
  e.g.,	
  p_T	
  cut	
  or	
  rapidity	
  cut.	
  
November	
  16,	
  2013	
   22	
  
2
3
4
5
6
7
8
0 50 100 150 200 250 300 350 400 450 500
MG5
3ch
tch
4
5
6
7
-5 -4 -3 -2 -1 0 1 2 3 4 5
MG5
3ch
tch
pT 1
1
5
6
7
0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5
MG5
3ch
tch
R23
3
4
5
6
7
8
0 200 400 600 800 1000 1200 1400 1600
MG5
3ch
tch
M12
gg ggg (3.5	
  %	
  unweigh2ng	
  eff.)	
  
November	
  16,	
  2013	
   23	
  
-4
-3
-2
-1
0
1
0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5
MG5
3ch
tch
-4
-3
-2
-1
0
1
0 200 400 600 800 1000 1200 1400 1600
MG5
3ch
tch
-2
-1
0
1
2
800 1000 1200 1400 1600 1800 2000
MG5
3ch
tch
-3
-2
-1
0
1
-3 -2 -1 0 1 2 3
MG5
3ch
tch
pT 1
1
R23
M12
gg ggg
pT 1 > 1000GeV
November	
  16,	
  2013	
   24	
  
Amplitude	
  
Phase	
  
Space	
  	
  
Color	
  
Sum	
  
Recursive	
  Rela$ons	
  
Channels	
  	
  
For	
  fast	
  mul$-­‐jet	
  genera$on	
  	
  
OutLook	
  
•  Efficient	
  Phase	
  Space	
  integra2on	
  
•  Include	
  higher	
  order	
  correc2ons	
  in	
  1/Nc.	
  
•  Generate	
  events	
  with	
  quarks	
  
•  Detailed	
  study	
  for	
  many	
  distribu2ons	
  of	
  Mul2-­‐
jet	
  	
  events	
  
November	
  16,	
  2013	
   25	
  

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  • 1. Mul$-­‐Jet  Genera$on   -­‐  status  report  -­‐   Yoshitaro  Takaesu  (KEK)   November  16,  2013   1   In  collabora$on  with  Fabio,  Johan,  Kaoru  and  Tim  
  • 2. Importance  of  mul$-­‐jet  at  the  LHC   Mul2-­‐jet  signature     appears  in  many     New  Physics  models.   Event  Generator     should    be  able  to     generate    >  4  jets.   November  16,  2013   2  
  • 3. Limita$on  of  MG   Generated  Codes  (>  8MB)  cannot  be  compiled  in  usual  PC.     gg 5g qg q5g qq qq4g November  16,  2013   3   8  MB   100 101 102 10 3 104 105 2 3 4 5 6 log10 FileSize(KB) # of Final State Particles gg > ng ug > ug ng uu > uu ng The  file  size  of  codes  for  QCD  processes  
  • 4. How  to  overcome     the  Limita$on   November  16,  2013   4   gg 5g qg q5g qq qq4g
  • 5. Structure  of  QCD  Amp   November  16,  2013   5   gg gg = ig2 s[fabe fcde ( 1 · 3 2 · 4 1 · 4 2 · 3) + face fbde ( 1 · 2 3 · 4 1 · 4 2 · 3) + fade fbce ( 1 · 2 3 · 4 1 · 3 2 · 4)]a b c d fabc = 2iTr [Ta , Tb ]Tc Tr(T a Tb ) = 1 2 ab = P(b,c,d) Tr(T a T (b) T (c) T (d) )A(a (b) (c) (d)) = Tr(T a Tb Tc Td )A(abcd) + Tr(T a Tb Td Tc )A(abdc) + Tr(T a Tc Tb Td )A(acbd) + Tr(T a Tc Td Tb )A(acdb) + Tr(T a Td Tb Tc )A(adbc) + Tr(T a Td Tc Tb )A(adcb) Color  flow   Color  Factor   color-­‐ordered  amp.   i:  Color  flow   M = Ncf i=1 CiAi Ncf (n 1)!
  • 6. November  16,  2013   6   color |M|2 = Ncf i,j color Ci CjAi Aj M = Ncf i=1 CiAi STRATEGY   Divide   color Ci Cj A1 A2 A3 · · · ANcf 1 ANcf • Speed  up  Amp  Evalua$on   • Off-­‐shell  Recursive  Rela2ons     •   Re-­‐organize  Color  Summa$on   1/Nc  expansion  
  • 7. Speed  up  Amp  Evalua$on   November  16,  2013   7  
  • 8. November  16,  2013   8   Off-­‐shell  Recursive  Rela$ons     Step  #  
  • 9. Time  performance   November  16,  2013   9   0 0.05 0.1 0.15 0.2 0.25 0.3 4 5 6 7 8 Time(ms) Final Gluons Recursive Non-Recursive n3 n 4
  • 10. November  16,  2013   10   Recursive  Rela$ons     for  gluonic  sub-­‐amplitude    
  • 11. Re-­‐organize  Color  Sum   November  16,  2013   11  
  • 12. November  16,  2013   12   1/Nc  expansion   Polynomial  of  Nc:     color |M|2 = Ncf i,j color Ci CjAi Aj = Nm c i |Ai|2 + 1 N2 c Ai (Aj1,1 + Aj1,2 + · · · ) + 1 N4 c Ai (Aj2,1 + Aj2,2 + · · · ) + · · · (m = ng + nq/2)
  • 13. Mul$-­‐jet  event  genera$on     •  Generate  events  with  Leading  Color   Approxima2on   •  For  each  event,  include  higher  order   correc2ons  into  its  weight.   November  16,  2013   13   color |M|2 = i Nm c |Ai|2 + 1 N2 c Ai (Aj1,1 + Aj1,2 + · · · ) + 1 Nc2 2 Ai (Aj2,1 + Aj2,2 + · · · ) + · · · color |M|2 = i Nm c |Ai|2 + 1 N2 c Ai (Aj1,1 + Aj1,2 + · · · ) + 1 Nc2 2 Ai (Aj2,1 + Aj2,2 + · · · ) + · · · = |M|2 d n
  • 14. Leading  color  summa$on   Color-­‐flow  sampling     Ncf (m 1)! (  ~  40,000  for  gg  -­‐>  7g  )   November  16,  2013   14   color |M|2 = Ncf i=1 Nm c |Ai|2 Too  LARGE    Event  is  a  set  of  momenta,  helici$es  and  a  color  flow  
  • 15. Results   November  16,  2013   15  
  • 16. November  16,  2013   16   gg_6g NLO diff Entries 61 Mean -0.9229 RMS 0.5551 -3 -2.5 -2 -1.5 -1 -0.5 0 0 2 4 6 8 10 12 14 gg_6g NLO diff Entries 61 Mean -0.9229 RMS 0.5551 gg_6g NLO diff = Nm c i |Ai|2 + 1 N2 c Ai (Aj1,1 +Aj1,2 +···) color |M|2 color |M|2 = Ncf i=1 N(n 2) c (N2 c 1)|Ai|2
  • 17. November  16,  2013   17   ug_u3g NLNc diff Entries 1000 Mean 2.63 RMS 2.916 -100 -80 -60 -40 -20 0 20 40 60 80 100 0 100 200 300 400 500 ug_u3g NLNc diff Entries 1000 Mean 2.63 RMS 2.916 ug_u3g NLNc diff ug_u3g LNc diff Entries 1000 Mean -27.28 RMS 13.15 -100 -80 -60 -40 -20 0 20 40 60 80 100 0 20 40 60 80 100 120 ug_u3g LNc diff Entries 1000 Mean -27.28 RMS 13.15 ug_u3g LNc diff color |M|2 = Ncf i=1 (N2 c 1)n 1 Nn 1 c |Ai|2
  • 18. November  16,  2013   18   Event  Genera$on  @LNc     pp  >     W  +  2  jets   W  +  3  jets   W  +  4  jets   MG5  (pb)   10673     4807.9  ±  13.2   2913  ±  7.6   LNc  CO  (pb)   11076   4623.8  ±  11.9   2460  ±  6   •   gg  -­‐>  3,4,5  g  process  is  now  generated  without     major  problem  and  agree  with  MG5  (3,4g).   pp  >  W+2,3,4  jets  is  also  studied  recently     and  roughly  agree  with  MG5.               Preliminary  
  • 19. 0.9 1 2 3 4 5 6 7 ratio Final particles 107 108 10 9 1010 10 11 1012 CrossSection(fb) gg -> ng Cross Section CFS (LCA) COMIX MG5 November  16,  2013   19  
  • 20. November  16,  2013   20   0 20000 40000 60000 80000 100000 120000 140000 160000 180000 0 50 100 150 200 250 300 350 dXsec/dpT1(pb) pT1 (GeV) gg > 4g pT1 MG5 Exact CFsamp LNc 0 5000 10000 15000 20000 25000 30000 35000 -3 -2 -1 0 1 2 3 dXsec/dy1(pb) y1 (GeV) gg > 4g y1 MG5 Exact CFsamp LNc 10 100 1000 10000 100000 1e+06 0 50 100 150 200 250 300 350 dXsec/dpT1(pb) pT1 (GeV) gg > 4g pT1 MG5 Exact CFsamp LNc 100 1000 10000 100000 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5 dXsec/ddR12(pb) dR12 (GeV) gg > 4g dR12 MG5 Exact CFsamp LNc pT 1 (Linear  scale)   pT 1 (Log  scale)   1 R12 gg gggg
  • 21. November  16,  2013   21   dxadxbd n = 2 s 1 4 2n 2 dy1 · · · dyndp2 T 1 · · · dp2 T n 1 d 1 2 · · · d n 1 2 A  liee  bit  of     Phase  Space  Study   Alterna2ve  parameteriza2on  for  MadEvent:     suitable  for  kinema2cal  cuts  ,  e.g.,  p_T  cut  or  rapidity  cut.  
  • 22. November  16,  2013   22   2 3 4 5 6 7 8 0 50 100 150 200 250 300 350 400 450 500 MG5 3ch tch 4 5 6 7 -5 -4 -3 -2 -1 0 1 2 3 4 5 MG5 3ch tch pT 1 1 5 6 7 0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5 MG5 3ch tch R23 3 4 5 6 7 8 0 200 400 600 800 1000 1200 1400 1600 MG5 3ch tch M12 gg ggg (3.5  %  unweigh2ng  eff.)  
  • 23. November  16,  2013   23   -4 -3 -2 -1 0 1 0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5 MG5 3ch tch -4 -3 -2 -1 0 1 0 200 400 600 800 1000 1200 1400 1600 MG5 3ch tch -2 -1 0 1 2 800 1000 1200 1400 1600 1800 2000 MG5 3ch tch -3 -2 -1 0 1 -3 -2 -1 0 1 2 3 MG5 3ch tch pT 1 1 R23 M12 gg ggg pT 1 > 1000GeV
  • 24. November  16,  2013   24   Amplitude   Phase   Space     Color   Sum   Recursive  Rela$ons   Channels     For  fast  mul$-­‐jet  genera$on    
  • 25. OutLook   •  Efficient  Phase  Space  integra2on   •  Include  higher  order  correc2ons  in  1/Nc.   •  Generate  events  with  quarks   •  Detailed  study  for  many  distribu2ons  of  Mul2-­‐ jet    events   November  16,  2013   25