introduction to hadronic final state reconstruction in collider experiments (part vi)
DESCRIPTION
Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI). Peter Loch University of Arizona Tucson, Arizona USA. Theoretical Requirements For Jet Finders . collinear sensitivity (2) (signal split into two towers below threshold). infrared sensitivity - PowerPoint PPT PresentationTRANSCRIPT
![Page 1: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/1.jpg)
Intr
oduc
tion
to
Had
roni
c Fi
nal S
tate
Re
cons
truc
tion
in C
ollid
er E
xper
imen
ts
Introduction to Hadronic Final State Reconstruction in Collider Experiments
(Part VI)
Peter LochUniversity of Arizona
Tucson, ArizonaUSA
![Page 2: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/2.jpg)
2P. Loch
U of ArizonaMarch 09, 2010
Theoretical Requirements For Jet Finders
Very important at LHC Often LO (or even NLO) not sufficient to
understand final states Potentially significant K-factors can only be
applied to jet driven spectra if jet finding follows theoretical rules
E.g., jet cross-section shapes Need to be able to compare experiments and theory
Comparison at the level of distributions ATLAS and CMS will unfold experimental effects
and limitations independently – different detector systems
Theoretical guidelines Infrared safety
Adding or removing soft particles should not change the result of jet clustering
Collinear safety Splitting of large pT particle into two collinear
particles should not affect the jet finding
infrared sensitivity(soft gluon radiation merges jets)
collinear sensitivity (2)(signal split into two towers below threshold)
collinear sensitivity (1)(sensitive to Et ordering of seeds)
![Page 3: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/3.jpg)
3P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
![Page 4: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/4.jpg)
4P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2coneR R
![Page 5: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/5.jpg)
5P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2cone
(first protojet)R R
![Page 6: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/6.jpg)
6P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2coneR R
![Page 7: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/7.jpg)
7P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2cone
(second protojet)R R
![Page 8: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/8.jpg)
8P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2cone
(two jets)R R
![Page 9: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/9.jpg)
9P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2coneR R
![Page 10: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/10.jpg)
10P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2coneR R
![Page 11: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/11.jpg)
11P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2coneR R
![Page 12: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/12.jpg)
12P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2cone
(first protojet)R R
![Page 13: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/13.jpg)
13P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2coneR R
![Page 14: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/14.jpg)
14P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2coneR R
![Page 15: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/15.jpg)
15P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2coneR R
![Page 16: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/16.jpg)
16P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2coneR R
![Page 17: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/17.jpg)
17P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2cone
(second protojet)R R
![Page 18: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/18.jpg)
18P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2cone
(second protojet)R R
![Page 19: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/19.jpg)
19P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2cone
(one jet)R R
![Page 20: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/20.jpg)
20P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Use following jet finder rules: Find particle with largest pT above a seed threshold
Create an ordered list of particles descending in pT and pick first particle
Draw a cone of fixed size around this particle Resolution parameter of algorithm
Collect all other particles in cone and re-calculate cone directions from those
Use four-momentum re-summation Collect particles in new cone of same size and find new
direction as above Repeat until direction does not change → cone becomes
stable Take next particle from list if above pT seed threshold Repeat procedure and find next proto-jet
Note that this is done with all particles, including the ones found in previous cones
Continue until no more proto-jets above threshold can be constructed
The same particle can be used by 2 or more jets Check for overlap between proto-jets
Add lower pT jet to higher pT jet if sum of particle pT in overlap is above a certain fraction of the lower pT jet (merge)
Else remove overlapping particles from higher pT jet and add to lower pT jet (split)
All surviving proto-jets are the final jets
2 2cone
(one jet)R R not an infrared safe algorithm!
![Page 21: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/21.jpg)
21P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Other problems with iterative cone finders: “Dark” tower problem
Original seed moves out of cone Significant energy lost for jets
initial cone 1st cone(not stable)
2nd cone(not stable)
3rd cone(stable)
original seed lost for jets!
![Page 22: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/22.jpg)
22P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Other problems with iterative cone finders: “Dark” tower problem
Original seed moves out of cone Significant energy lost for jets
![Page 23: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/23.jpg)
23P. Loch
U of ArizonaMarch 09, 2010
Iterative Seeded Fixed Cone
Advantages Simple geometry based algorithm
Easy to implement Fast algorithm
Ideal for online application in experiment
Disadvantages Not infrared safe
Can partially be recovered by splitting & merging Introduces split/merge pT fraction f (typically 0.50 - 0.75)
Kills “trace” of pertubative infinities in experiment Hard to confirm higher order calculations in “real life” without infinities!
Not collinear safe Used pT seeds (thresholds)
Jets not cone shaped Splitting and merging potentially makes jets bigger than original cone size
and changes jet boundaries
![Page 24: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/24.jpg)
24P. Loch
U of ArizonaMarch 09, 2010
Recursive Recombination
Motivated by gluon splitting function QCD branching happens all the
time Attempt to undo parton
fragmentation Pair with strongest divergence
likely belongs together kT/Durham, first used in e+e-
Catani, Dokshitzer, Olsson, Turnock & Webber 1991
Longitudinal invariant version for hadron colliders Transverse momentum instead of
energy Catani, Dokshitzer, Seymour &
Webber 1993 S.D. Ellis & D. Soper 1993
Valid at all orders!
2
min(2
( ), )
( , 1)
i j
j
i
ijs Aj g g g j
j i i
j ij
j
dE dCE E
dk M k
E E
cut
2
2 2
2
2 2, T ,
2 2
combine and , else st
Distance between all particles and
Drop normalization to (not fixed in pp)
2min( , )(1 cos )
min( , ) ,
( ) (
op
i j ijij
ij ij i j ij i j i j
j
ij i j i
iy y
E Ey
Q
y d d d R d p
R y y
Q
i j
i j
cu
2
2 2
t
Inclusive longitu
combine and , else stop
di(exclusive
nal invari kT)
ant
)
m
cl
in( ,
us g
)
terin
j
ij i j ij
ijd d i
d d d R R
j
![Page 25: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/25.jpg)
25P. Loch
U of ArizonaMarch 09, 2010
Recursive Recombination
Motivated by gluon splitting function QCD branching happens all the
time Attempt to undo parton
fragmentation Pair with strongest divergence
likely belongs together kT/Durham, first used in e+e-
Catani, Dokshitzer, Olsson, Turnock & Webber 1991
Longitudinal invariant version for hadron colliders Transverse momentum instead of
energy Catani, Dokshitzer, Seymour &
Webber 1993 S.D. Ellis & D. Soper 1993
Valid at all orders!
2
min(2
( ), )
( , 1)
i j
j
i
ijs Aj g g g j
j i i
j ij
j
dE dCE E
dk M k
E E
cut
2
2 2
2
2 2, T ,
2 2
combine and , else st
Distance between all particles and
Drop normalization to (not fixed in pp)
2min( , )(1 cos )
min( , ) ,
( ) (
op
i j ijij
ij ij i j ij i j i j
j
ij i j i
iy y
E Ey
Q
y d d d R d p
R y y
Q
i j
i j
cu
2
2 2
t
Inclusive longitu
combine and , else stop
di(exclusive
nal invari kT)
ant
)
m
cl
in( ,
us g
)
terin
j
ij i j ij
ijd d i
d d d R R
j
![Page 26: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/26.jpg)
26P. Loch
U of ArizonaMarch 09, 2010
Recursive Recombination
Motivated by gluon splitting function QCD branching happens all the
time Attempt to undo parton
fragmentation Pair with strongest divergence
likely belongs together kT/Durham, first used in e+e-
Catani, Dokshitzer, Olsson, Turnock & Webber 1991
Longitudinal invariant version for hadron colliders Transverse momentum instead of
energy Catani, Dokshitzer, Seymour &
Webber 1993 S.D. Ellis & D. Soper 1993
Valid at all orders!
2
min(2
( ), )
( , 1)
i j
j
i
ijs Aj g g g j
j i i
j ij
j
dE dCE E
dk M k
E E
cut
2
2 2
2
2 2, T ,
2 2
combine and , else st
Distance between all particles and
Drop normalization to (not fixed in pp)
2min( , )(1 cos )
min( , ) ,
( ) (
op
i j ijij
ij ij i j ij i j i j
j
ij i j i
iy y
E Ey
Q
y d d d R d p
R y y
Q
i j
i j
cu
2
2 2
t
Inclusive longitu
combine and , else stop
di(exclusive
nal invari kT)
ant
)
m
cl
in( ,
us g
)
terin
j
ij i j ij
ijd d i
d d d R R
j
![Page 27: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/27.jpg)
27P. Loch
U of ArizonaMarch 09, 2010
Recursive Recombination
Motivated by gluon splitting function QCD branching happens all the
time Attempt to undo parton
fragmentation Pair with strongest divergence
likely belongs together kT/Durham, first used in e+e-
Catani, Dokshitzer, Olsson, Turnock & Webber 1991
Longitudinal invariant version for hadron colliders Transverse momentum instead of
energy Catani, Dokshitzer, Seymour &
Webber 1993 S.D. Ellis & D. Soper 1993
Valid at all orders!
2
min(2
( ), )
( , 1)
i j
j
i
ijs Aj g g g j
j i i
j ij
j
dE dCE E
dk M k
E E
cut
2
2 2
2
2 2, T ,
2 2
combine and , else st
Distance between all particles and
Drop normalization to (not fixed in pp)
2min( , )(1 cos )
min( , ) ,
( ) (
op
i j ijij
ij ij i j ij i j i j
j
ij i j i
iy y
E Ey
Q
y d d d R d p
R y y
Q
i j
i j
cu
2
2 2
t
Inclusive longitu
combine and , else stop
di(exclusive
nal invari kT)
ant
)
m
cl
in( ,
us g
)
terin
j
ij i j ij
ijd d i
d d d R R
j
![Page 28: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/28.jpg)
28P. Loch
U of ArizonaMarch 09, 2010
kT –like Algorithms
Classic procedure Calculate all distances dji for list of
particles Uses distance parameter
Calculate di for all particles Uses pT
If minimum of both lists is a dij, combine i and j and add to list Remove i and j, of course
If minimum is a di, call i a jet and remove from list
Recalculate all distances and continue all particles are removed or called a jet
Features Clustering sequence is ordered in
kT Follows jet structure
Alternatives Cambridge/Aachen clustering
Uses angular distances only Clustering sequence follows jet
structure Anti-kT clustering
No particular ordering, sequence not meaningful
2 2
2T
Inclusive longitudinal invariant clu
min
stering
( , )ij i j ij
i i
d d d R R
d p
![Page 29: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/29.jpg)
29P. Loch
U of ArizonaMarch 09, 2010
kT –like Algorithms
Classic procedure Calculate all distances dji for list of
particles Uses distance parameter
Calculate di for all particles Uses pT
If minimum of both lists is a dij, combine i and j and add to list Remove i and j, of course
If minimum is a di, call i a jet and remove from list
Recalculate all distances and continue all particles are removed or called a jet
Features Clustering sequence is ordered in
kT Follows jet structure
Alternatives Cambridge/Aachen clustering
Uses angular distances only Clustering sequence follows jet
structure Anti-kT clustering
No particular ordering, sequence not meaningful
2 2
2T
min( , )
Inclusive longitudinal invariant clustering
Cambridge/Aachen (cluster smallest first until >1
0)
ij i j ij
ni
ij ij
i
d d d R
d
R
dn
p
d
![Page 30: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/30.jpg)
30P. Loch
U of ArizonaMarch 09, 2010
kT –like Algorithms
Classic procedure Calculate all distances dji for list of
particles Uses distance parameter
Calculate di for all particles Uses pT
If minimum of both lists is a dij, combine i and j and add to list Remove i and j, of course
If minimum is a di, call i a jet and remove from list
Recalculate all distances and continue all particles are removed or called a jet
Features Clustering sequence is ordered in
kT Follows jet structure
Alternatives Cambridge/Aachen clustering
Uses angular distances only Clustering sequence follows jet
structure Anti-kT clustering
No particular ordering, sequence not meaningful
2 2
2T
Inclusive longitudinal invariant clustering
Cambridge/Aachcluster smallest first until >1
en ( 0)
Anti-kfollow classic algorith
min( ,
1
)
( )m
T
ij i j ij
ni i
ij ijd d
d d d
dn
p
n
R R
![Page 31: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/31.jpg)
31P. Loch
U of ArizonaMarch 09, 2010
kT Examples
kT, n=1 Anti-kT, n=-1 Cambridge/Aachen, n=0
![Page 32: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/32.jpg)
32P. Loch
U of ArizonaMarch 09, 2010
kT Examples
kT, n=1 Anti-kT, n=-1 Cambridge/Aachen, n=0
![Page 33: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/33.jpg)
33P. Loch
U of ArizonaMarch 09, 2010
kT Examples
kT, n=1 Anti-kT, n=-1 Cambridge/Aachen, n=0
![Page 34: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/34.jpg)
34P. Loch
U of ArizonaMarch 09, 2010
kT Examples
kT, n=1 Anti-kT, n=-1 Cambridge/Aachen, n=0
![Page 35: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/35.jpg)
35P. Loch
U of ArizonaMarch 09, 2010
kT Examples
kT, n=1 Anti-kT, n=-1 Cambridge/Aachen, n=0
![Page 36: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/36.jpg)
36P. Loch
U of ArizonaMarch 09, 2010
kT Examples
kT, n=1 Anti-kT, n=-1 Cambridge/Aachen, n=0
![Page 37: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/37.jpg)
37P. Loch
U of ArizonaMarch 09, 2010
Recursive Recombination Algorithms
![Page 38: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/38.jpg)
38P. Loch
U of ArizonaMarch 09, 2010
Recursive Recombination Algorithms
![Page 39: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/39.jpg)
39P. Loch
U of ArizonaMarch 09, 2010
Recursive Recombination Algortihms
![Page 40: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/40.jpg)
40P. Loch
U of ArizonaMarch 09, 2010
Recursive Recombination Algortihms
![Page 41: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/41.jpg)
41P. Loch
U of ArizonaMarch 09, 2010
Recursive Recombination Algorithms
![Page 42: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/42.jpg)
42P. Loch
U of ArizonaMarch 09, 2010
Recursive Recombination Algorithms
![Page 43: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/43.jpg)
43P. Loch
U of ArizonaMarch 09, 2010
Recursive Recombination Algorithms
![Page 44: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/44.jpg)
44P. Loch
U of ArizonaMarch 09, 2010
Recursive Recombination Algorithms
![Page 45: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/45.jpg)
45P. Loch
U of ArizonaMarch 09, 2010
Recursive Recombination Algorithms
![Page 46: Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part VI)](https://reader035.vdocuments.net/reader035/viewer/2022062323/5681624c550346895dd294c3/html5/thumbnails/46.jpg)
46P. Loch
U of ArizonaMarch 09, 2010
Recursive Recombination Algorithms