(r16) ExclusiveJetStudy < ATLAS

ATLAS Web>ExclusiveJetStudy (revision 16) (raw view)~~EditAttach~~

---+ Exclusive Jet Study With Kt, AntiKt and Cambridge Aachen Jet Finders
   * Reference used to calculate bin width with respect to Jet Energy Resoultion (Calculated using dijet sample): [[%ATTACHURL%/fig_07.eps][Jet_Energy_Resolution.eps]]
    (Jet_Energy_Resolution.eps was taken from the Jet energy Resolution Group URL https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2010-054/ )

    Legend Info:

   *  Signal - Purple
   *  NP0 - Black
   *  NP1 - Red
   *  NP2 - Green (Also Sum of the Backgrounds)
   *  NP3 - Blue
%TOC%

---++ %MAKETEXT{"Kt Jet Finder"}%
The K<sub>t</sub> jet finding algorithm can be broken down into three steps.

1) For each particle i, j in the event the K<sub>t</sub> distance is calculated d<sub>ij</sub> = min(P^2<sub>ti</sub>,P^2<sub>tj</sub>) &Delta;R ^2<sub>ij</sub> / R
 

 Where &Delta;R <sub>ij</sub>= (&Delta;eta<sub>i</sub> - &Delta;eta<sub>j</sub>)^2 + (&Delta;phi<sub>i</sub> - &Delta;phi<sub>j</sub>)^2

The Kt distance from particle i to the beam is also calculated 

d<sub>ij</sub> = P^2<sub>iB</sub>

2) The next step is to find the dmin value for all dij and diB. (Note there are differences between the Inclusive and Exclusive K<sub>t</sub> Jet algorithms)

   * INCLUSIVE K<sub>t</sub> Jet Algorithm:

If d<sub>ij</sub> is the dmin value then the i, j particles are combined ( the particles four momenta are summed together).

if d<sub>iB</sub>  is the dmin value then the particle i is a final jet and the particle i is removed from the list.


   * Exclusive K<sub>t</sub> Jet Algorithm:

If d<sub>ij</sub> is the dmin value and is less than dcut then the i, j particles are combined ( the particles four momenta are summed together).

if d<sub>iB</sub>  is the dmin value and is less than dcut then the particle i combined with the beam jet.

3) 

   * INCLUSIVE K<sub>t</sub> Jet Algorithm:

This process is repeated until no more particles are left.

   * Exclusive K<sub>t</sub> Jet Algorithm:

This process ends when all d<sub>ij</sub> and d<sub>iB</sub> are above the dcut value.

The dcut variable again varies when considering an inclusive or exclusive event.

When looking at an exclusive n-jet event.

dcut = P<sub>t</sub>min^(2) 

This maintains the jet algorithm ability to factorize the initial-state of the collinear singularities, which allows you to obtain a finite cross-section.

When looking at an inclusive jet event.

dcut = E<sub>t</sub>^(2)


   * Recombination Scheme used:

The recombination scheme is the method the user chooses to combine the particles to one and other. There are a number of schemes to choose from, I have chosen the E-Scheme.


E-scheme:

The E-scheme combines the four momenta of the particles vectorially. Therefore the true rapidity is used instead of the pseudorapidity (since the particles have mass not equaling zero) . This procedure must be used to maintain the longitudinal boost invariance of the recombination procedure.

We need the recombination procedure to be longitudinal boost invariant so that corrections to hadronization won't cause strong effects to the recombination procedure (large jump in jet multiplicity).

<strong> Details of R values used in Kt Algorithm (This will be changed so we can have a direct comparison with the anti-kt algorithm)</strong>

dmin_01 -> R = 0.1,
dmin_12 -> R = 0.2,
dmin_23 -> R = 0.3,
dmin_34 -> R = 0.4,
dmin_45 -> R = 0.5,
dmin_56 -> R = 0.6,
dmin_67 -> R = 0.7,
dmin_78 -> R = 0.8 and
dmin_89 -> R = 0.9

These chosen R values will need to be changed to more suitable values, especially 01 to 23, as the R values are far too small for the corresponding jet multiplicity. Also, I will need to change these to R = 1 to compare with the anti-kt algorithm.

It will also be an interesting study to see the effects on the chosen value of R (how it effects the dmin value, does it increase the discriminant against the background dmins???). 

Note:

Most study's look at jets with R = 0.4 and 0.6.
 


---++++%MAKETEXT{"Signal and Background Comparisons (Bin Width 100 GeV^2)"}%
---++++++%MAKETEXT{"Signal and Background Comparisons Not Normalized"}%
Fig1.1 <img src="%ATTACHURLPATH%/AllDminSigBckKtUnNorm.png" alt="AllDminSigBckKtUnNorm.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckKtUnNorm.eps][AllDminSigBckKtUnNorm.eps]]: 
---++++++%MAKETEXT{"Signal and Background Comparisons Normalized (1/sigma dsigma/dDmin [GeV-2] )"}%
Fig2.1 <img src="%ATTACHURLPATH%/AllDminSigBckKtNorm.png" alt="AllDminSigBckKtNorm.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckKtNorm.eps][AllDminSigBckKtNorm.eps]]: 
---++++++%MAKETEXT{"Signal and Background Comparisons Normalized (dsigma/dDmin [pb/GeV^2] )"}%
Fig3.1 <img src="%ATTACHURLPATH%/AllDminSigBckKtNormLuminosityBinWidth.png" alt="AllDminSigBckKtNormLuminosityBinWidth.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckKtNormLuminosityBinWidth.eps][AllDminSigBckKtNormLuminosityBinWidth.eps]]: 
---++++++%MAKETEXT{"Signal and Sum of Background Comparisons Normalized (dsigma/dDmin [pb/GeV^2] )"}%
Fig4.1 <img src="%ATTACHURLPATH%/AllDminSigBckKtNormLuminosityBinWidth.png" alt="AllDminSigBckKtNormLuminosityBinWidth.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckKtSumNormLuminosityBinWidth.eps][AllDminSigBckKtSumNormLuminosityBinWidth.eps]]:
---++++%MAKETEXT{"Signal and Background Comparisons (Binned in Log(Dmin))"}%
---++++++%MAKETEXT{"Signal and Background Comparisons Not Normalized"}%
Fig5.1 <img src="%ATTACHURLPATH%/AllDminSigBckktUnNormLog10.png" alt="AllDminSigBckktUnNormLog10.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckktUnNormLog10.eps][AllDminSigBckktUnNormLog10.eps]]

---++++++%MAKETEXT{"Signal and Background Comparisons Normalized (1/sigma dsigma/dDmin [GeV-2] )"}%
Fig6.1  <img src="%ATTACHURLPATH%/AllDminSigBckktNormLog10.png" alt="AllDminSigBckktNormLog10.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckktNormLog10.eps][AllDminSigBckktNormLog10.eps]]

---++++++%MAKETEXT{"Signal and Background Comparisons Normalized (dsigma/dDmin [pb/GeV^2] )"}%
Fig7.1 <img src="%ATTACHURLPATH%/AllDminSigBckktNormLuminosityBinWidthLog10.png" alt="AllDminSigBckktNormLuminosityBinWidthLog10.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckktNormLuminosityBinWidthLog10.eps][AllDminSigBckktNormLuminosityBinWidthLog10.eps]]
---++++++%MAKETEXT{"Signal and Sum of Background Comparisons Normalized (dsigma/dDmin [pb/GeV^2] )"}%
Fig8.1 <img src="%ATTACHURLPATH%/AllDminSigBckKtSumNormLuminosityBinWidthLog10.png" alt="AllDminSigBckKtSumNormLuminosityBinWidthLog10.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckKtSumNormLuminosityBinWidthLog10.eps][AllDminSigBckKtSumNormLuminosityBinWidthLog10.eps]]

---++++++%MAKETEXT{"Signal and Sum of Background Comparisons Normalized (1/sigma dsigma/dDmin [GeV-2] )"}%
Fig9.1 <img src="%ATTACHURLPATH%/AllDminSigBckKtSumNormUnityLog10.png" alt="AllDminSigBckKtSumNormUnityLog10.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckKtSumNormUnityLog10.eps][AllDminSigBckKtSumNormUnityLog10.eps]]

---++ %MAKETEXT{"AntiKt Jet Finder"}%
The Anti-Kt Algorithm follows the same procedure as the K<sub>t</sub> algorithm explained above. The differences between these two algorithms are the definitions for d<sub>ij</sub> and d<sub>iB</sub>.

d<sub>ij</sub> = min(1/P^2<sub>ti</sub>,1/P^2<sub>tj</sub>) &Delta;R ^2<sub>ij</sub> / R

and

d<sub>ij</sub> = 1/P^2<sub>iB</sub>


<strong>More detailed points on the behavior of the anti-kt algorithm:</strong>


If we have a hard particle and a soft particle we find the d<sub>ij</sub> value is dominated by the hard particle. When considering the soft particles we find the d<sub>ij</sub> value to be much larger. Therefore the harder particles will cluster with the softer particles long before they cluster with each other.

   * R value dependence on jet shape:

If a hard particle has no other hard particles within a distance of 2R then the hard particle will merge with all the surrounded soft particles producing a conical jet shape.

If we have 2 hard particles within R < &Delta;<sub>12</sub> < 2R then we will have two hard jets. These will produce conical and partially conical jets (due to the overlapping getting taken away). The shapes of these two jets are determined by the jets P<sub>t</sub>^2.
   * P<sub>t1</sub>^2 >> P<sub>t2</sub>^2 Then jet 1 will be conical and jet 2 will be partially conical (since it will miss the overlapping with jets)
   * P<sub>t1</sub>^2 = P<sub>t2</sub>^2  Neither jet is conical and the overlapping part of the jet will be split by a straight line equally between the two.

If we have 2 hard particles with &Delta;<sub>12</sub> < R then there will be 1 jet produced. The conical jet will be centered around the jet with the highest P<sub>t</sub>^2. However if the two gets have similar P<sub>t</sub>^2 then the jet shape will be more complex. The shape will be a union of cones with a radius < R around each hard particle plus a cone centered around the final jet with a radius < R.


<strong>Getting the dmin value for n+1 jets into n jets from the anti-kt jet algorithm:</strong>

With the anti-kt algorithm the exclusive jet algorithm does not make physical sense. Since the exclusive jets undoes the last n steps of the clustering and returns whatever objects were left in the cluster sequence after undoing those steps. With the anti-kt algorithm those are often soft objects (low pt, hence large diB or dij, hence clustered late) and bear no relation to the hard structure of the event. 

To over come this, I used the constituents that were clustered with the anti-kt algorithm and used them to be clustered with the kt-algorithm allowing me to access the dmin variables.

***************** These plots are for R=1 *********************************************

---++++%MAKETEXT{"Signal and Background Comparisons (Bin Width 100 GeV^2)"}%
---++++++%MAKETEXT{"Signal and Background Comparisons Not Normalized "}%
Fig10.1 <img src="%ATTACHURLPATH%/AllDminSigBckAntktUnNorm.png" alt="AllDminSigBckAntktUnNorm.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckAntktUnNorm.eps][AllDminSigBckAntktUnNorm.eps]]:
---++++++%MAKETEXT{"Signal and Background Comparisons Normalized (1/sigma dsigma/dDmin [GeV-2] )"}%
Fig11.1 <img src="%ATTACHURLPATH%/AllDminSigBckAntktNorm.png" alt="AllDminSigBckAntktNorm.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckAntktNorm.eps][AllDminSigBckAntktNorm.eps]]:
---++++++%MAKETEXT{"Signal and Background Comparisons Normalized (dsigma/dDmin [pb/GeV^2] )"}%
Fig12.1 <img src="%ATTACHURLPATH%/AllDminSigBckAntktNormLuminosityBinWidth.png" alt="AllDminSigBckAntktNormLuminosityBinWidth.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckAntktNormLuminosityBinWidth.eps][AllDminSigBckAntktNormLuminosityBinWidth.eps]]:
---++++++%MAKETEXT{"Signal and Sum of Background Comparisons Normalized (dsigma/dDmin [pb/GeV^2] )"}%
Fig13.1 <img src="%ATTACHURLPATH%/AllDminSigBckAntktSumNormLuminosityBinWidth.png" alt="AllDminSigBckAntktSumNormLuminosityBinWidth.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckAntktSumNormLuminosityBinWidth.eps][AllDminSigBckAntktSumNormLuminosityBinWidth.eps]]:
---++++%MAKETEXT{"Signal and Background Comparisons (Binned in Log(Dmin))"}%
---++++++%MAKETEXT{"Signal and Background Comparisons Not Normalized"}%
Fig14.1 <img src="%ATTACHURLPATH%/AllDminSigBckKtAntUnNormLog10.png" alt="AllDminSigBckKtAntUnNormLog10.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckKtAntUnNormLog10.eps][AllDminSigBckKtAntUnNormLog10.eps]]
---++++++%MAKETEXT{"Signal and Background Comparisons Normalized (1/sigma dsigma/dDmin [GeV-2] )"}%
Fig15.1 <img src="%ATTACHURLPATH%/AllDminSigBckAntKtNormLog10.png" alt="AllDminSigBckAntKtNormLog10.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckAntKtNormLog10.eps][AllDminSigBckAntKtNormLog10.eps]]
---++++++%MAKETEXT{"Signal and Background Comparisons Normalized (dsigma/dDmin [pb/GeV^2] )"}%
Fig16.1 <img src="%ATTACHURLPATH%/AllDminSigBckAntktNormLuminosityBinWidthLog10.png" alt="AllDminSigBckAntktNormLuminosityBinWidthLog10.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckAntktNormLuminosityBinWidthLog10.eps][AllDminSigBckAntktNormLuminosityBinWidthLog10.eps]]
---++++++%MAKETEXT{"Signal and Sum of Background Comparisons Normalized (dsigma/dDmin [pb/GeV^2] )"}%
Fig17.1 <img src="%ATTACHURLPATH%/AllDminSigBckAntktSumNormLuminosityBinWidthLog10.png" alt="AllDminSigBckAntktSumNormLuminosityBinWidthLog10.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckAntktSumNormLuminosityBinWidthLog10.eps][AllDminSigBckAntktSumNormLuminosityBinWidthLog10.eps]]

---++++++%MAKETEXT{"Signal and Sum of Background Comparisons Normalized (1/sigma dsigma/dDmin [GeV-2] )"}%
Fig18.1 <img src="%ATTACHURLPATH%/AllDminSigBckAntktSumNormUnityLog10.png" alt="AllDminSigBckAntktSumNormUnityLog10.png" width='596' height='572' />
   * [[%ATTACHURL%/AllDminSigBckAntktSumNormUnityLog10.eps][AllDminSigBckAntktSumNormUnityLog10.eps]]


-- Main.MichaelWright - 2010-10-06

Attachments

Topic attachments
I	Attachment	History	Action	Size	Date	Who
jpg	ANTIKTDMIN.jpg	r1	manage	22.8 K	2010-10-06 - 13:18	MichaelWright
eps	AllDminSigBckAntKtNormLog10.eps	r1	manage	262.0 K	2010-11-19 - 17:43	MichaelWright
png	AllDminSigBckAntKtNormLog10.png	r1	manage	36.8 K	2010-11-19 - 17:43	MichaelWright
eps	AllDminSigBckAntktNorm.eps	r2 r1	manage	115.9 K	2010-11-17 - 20:45	MichaelWright
jpg	AllDminSigBckAntktNorm.jpg	r1	manage	38.9 K	2010-11-09 - 17:40	MichaelWright
png	AllDminSigBckAntktNorm.png	r2 r1	manage	22.2 K	2010-11-17 - 20:46	MichaelWright
eps	AllDminSigBckAntktNormLuminosity2fb-1.eps	r1	manage	92.8 K	2010-11-11 - 12:19	MichaelWright
jpg	AllDminSigBckAntktNormLuminosity2fb-1.jpg	r2 r1	manage	41.6 K	2010-11-09 - 17:40	MichaelWright
png	AllDminSigBckAntktNormLuminosity2fb-1.png	r1	manage	22.4 K	2010-11-11 - 12:18	MichaelWright
eps	AllDminSigBckAntktNormLuminosityBinWidth.eps	r2 r1	manage	117.4 K	2010-11-17 - 20:47	MichaelWright
png	AllDminSigBckAntktNormLuminosityBinWidth.png	r2 r1	manage	23.3 K	2010-11-17 - 20:47	MichaelWright
eps	AllDminSigBckAntktNormLuminosityBinWidthLog10.eps	r1	manage	289.2 K	2010-11-19 - 17:44	MichaelWright
png	AllDminSigBckAntktNormLuminosityBinWidthLog10.png	r2 r1	manage	37.4 K	2010-11-19 - 18:07	MichaelWright
eps	AllDminSigBckAntktSumNormLuminosity2fb-1.eps	r1	manage	59.5 K	2010-11-11 - 12:20	MichaelWright
jpg	AllDminSigBckAntktSumNormLuminosity2fb-1.jpg	r2 r1	manage	32.3 K	2010-11-09 - 17:41	MichaelWright
png	AllDminSigBckAntktSumNormLuminosity2fb-1.png	r1	manage	17.9 K	2010-11-11 - 12:20	MichaelWright
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png	AllDminSigBckAntktSumNormLuminosityBinWidth.png	r2 r1	manage	19.5 K	2010-11-17 - 20:48	MichaelWright
eps	AllDminSigBckAntktSumNormLuminosityBinWidthLog10.eps	r1	manage	135.7 K	2010-11-19 - 17:44	MichaelWright
png	AllDminSigBckAntktSumNormLuminosityBinWidthLog10.png	r1	manage	26.6 K	2010-11-19 - 17:45	MichaelWright
eps	AllDminSigBckAntktSumNormUnityLog10.eps	r1	manage	132.6 K	2010-11-22 - 11:06	MichaelWright
png	AllDminSigBckAntktSumNormUnityLog10.png	r1	manage	26.8 K	2010-11-22 - 11:06	MichaelWright
eps	AllDminSigBckAntktUnNorm.eps	r2 r1	manage	107.3 K	2010-11-17 - 20:46	MichaelWright
jpg	AllDminSigBckAntktUnNorm.jpg	r1	manage	36.3 K	2010-11-09 - 17:40	MichaelWright
png	AllDminSigBckAntktUnNorm.png	r2 r1	manage	20.1 K	2010-11-17 - 20:46	MichaelWright
eps	AllDminSigBckKtAntUnNormLog10.eps	r1	manage	254.5 K	2010-11-19 - 17:43	MichaelWright
png	AllDminSigBckKtAntUnNormLog10.png	r1	manage	34.2 K	2010-11-19 - 17:44	MichaelWright
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jpg	AllDminSigBckKtNorm.jpg	r1	manage	37.4 K	2010-11-09 - 17:39	MichaelWright
png	AllDminSigBckKtNorm.png	r2 r1	manage	21.0 K	2010-11-17 - 20:49	MichaelWright
eps	AllDminSigBckKtNormLuminosity2fb-1.eps	r1	manage	89.1 K	2010-11-11 - 12:20	MichaelWright
jpg	AllDminSigBckKtNormLuminosity2fb-1.jpg	r2 r1	manage	40.0 K	2010-11-09 - 17:40	MichaelWright
png	AllDminSigBckKtNormLuminosity2fb-1.png	r1	manage	21.5 K	2010-11-11 - 12:21	MichaelWright
eps	AllDminSigBckKtNormLuminosityBinWidth.eps	r2 r1	manage	112.8 K	2010-11-17 - 20:50	MichaelWright
png	AllDminSigBckKtNormLuminosityBinWidth.png	r2 r1	manage	22.5 K	2010-11-17 - 20:51	MichaelWright
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jpg	AllDminSigBckKtSumNormLuminosity2fb-1.jpg	r2 r1	manage	31.4 K	2010-11-09 - 17:40	MichaelWright
eps	AllDminSigBckKtSumNormLuminosityBinWidth.eps	r2 r1	manage	80.4 K	2010-11-17 - 20:51	MichaelWright
png	AllDminSigBckKtSumNormLuminosityBinWidth.png	r2 r1	manage	18.8 K	2010-11-17 - 20:52	MichaelWright
eps	AllDminSigBckKtSumNormLuminosityBinWidthLog10.eps	r1	manage	136.0 K	2010-11-19 - 17:37	MichaelWright
png	AllDminSigBckKtSumNormLuminosityBinWidthLog10.png	r1	manage	26.9 K	2010-11-19 - 17:38	MichaelWright
eps	AllDminSigBckKtSumNormUnityLog10.eps	r1	manage	132.8 K	2010-11-22 - 11:05	MichaelWright
png	AllDminSigBckKtSumNormUnityLog10.png	r1	manage	27.6 K	2010-11-22 - 11:06	MichaelWright
eps	AllDminSigBckKtUnNorm.eps	r3 r2 r1	manage	102.4 K	2010-11-17 - 20:50	MichaelWright
jpg	AllDminSigBckKtUnNorm.jpg	r1	manage	34.8 K	2010-11-09 - 17:39	MichaelWright
png	AllDminSigBckKtUnNorm.png	r2 r1	manage	19.5 K	2010-11-17 - 20:50	MichaelWright
eps	AllDminSigBckktNormLog10.eps	r1	manage	261.7 K	2010-11-19 - 17:36	MichaelWright
png	AllDminSigBckktNormLog10.png	r1	manage	36.5 K	2010-11-19 - 17:36	MichaelWright
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png	AllDminSigBckktNormLuminosityBinWidthLog10.png	r1	manage	36.3 K	2010-11-19 - 17:37	MichaelWright
eps	AllDminSigBckktUnNormLog10.eps	r1	manage	253.3 K	2010-11-19 - 17:36	MichaelWright
png	AllDminSigBckktUnNormLog10.png	r1	manage	36.0 K	2010-11-19 - 17:37	MichaelWright
jpg	AlpgenJimmyttbarlnqqNp0AntiKtDmin.jpg	r1	manage	36.7 K	2010-11-02 - 12:58	MichaelWright
jpg	AlpgenJimmyttbarlnqqNp0KtDmin.jpg	r1	manage	36.1 K	2010-11-02 - 13:08	MichaelWright
jpg	AlpgenJimmyttbarlnqqNp1AntiKtDmin.jpg	r1	manage	37.6 K	2010-11-02 - 13:00	MichaelWright
jpg	AlpgenJimmyttbarlnqqNp1KtDmin.jpg	r1	manage	36.5 K	2010-11-02 - 13:09	MichaelWright
jpg	AlpgenJimmyttbarlnqqNp2AntiKtDmin.jpg	r1	manage	38.3 K	2010-11-02 - 13:00	MichaelWright
jpg	AlpgenJimmyttbarlnqqNp2KtDmin.jpg	r1	manage	36.9 K	2010-11-02 - 13:09	MichaelWright
jpg	AlpgenJimmyttbarlnqqNp3AntiKtDmin.jpg	r1	manage	36.0 K	2010-11-02 - 13:01	MichaelWright
jpg	AlpgenJimmyttbarlnqqNp3KtDmin.jpg	r1	manage	35.9 K	2010-11-02 - 13:09	MichaelWright
jpg	Pythia_ttH120_neglepnu_jj_bb_AntKt_Dmin.jpg	r1	manage	38.1 K	2010-11-02 - 13:07	MichaelWright
jpg	PythiattH120neglepnujjbb.jpg	r1	manage	39.3 K	2010-11-02 - 12:52	MichaelWright
jpg	SignalBckAntiKt01Dmin.jpg	r1	manage	40.9 K	2010-11-02 - 13:16	MichaelWright
jpg	SignalBckAntiKt12Dmin.jpg	r1	manage	41.7 K	2010-11-02 - 13:17	MichaelWright
jpg	SignalBckAntiKt23Dmin.jpg	r1	manage	42.8 K	2010-11-02 - 13:17	MichaelWright
jpg	SignalBckAntiKt34Dmin.jpg	r1	manage	42.0 K	2010-11-02 - 13:17	MichaelWright
jpg	SignalBckAntiKt45Dmin.jpg	r1	manage	40.6 K	2010-11-02 - 13:18	MichaelWright
jpg	SignalBckAntiKt56Dmin.jpg	r2 r1	manage	39.6 K	2010-11-02 - 13:37	MichaelWright
jpg	SignalBckAntiKt67Dmin.jpg	r2 r1	manage	39.7 K	2010-11-02 - 13:38	MichaelWright
jpg	SignalBckAntiKt78Dmin.jpg	r1	manage	39.9 K	2010-11-02 - 13:19	MichaelWright
jpg	SignalBckAntiKt89Dmin.jpg	r1	manage	39.2 K	2010-11-02 - 13:19	MichaelWright
jpg	SignalBckKt01Dmin.jpg	r1	manage	41.9 K	2010-11-02 - 14:44	MichaelWright
jpg	SignalBckKt12Dmin.jpg	r1	manage	41.4 K	2010-11-02 - 14:45	MichaelWright
jpg	SignalBckKt23Dmin.jpg	r1	manage	41.5 K	2010-11-02 - 14:45	MichaelWright
jpg	SignalBckKt34Dmin.jpg	r1	manage	39.5 K	2010-11-02 - 14:45	MichaelWright
jpg	SignalBckKt45Dmin.jpg	r1	manage	40.2 K	2010-11-02 - 14:45	MichaelWright
jpg	SignalBckKt56Dmin.jpg	r1	manage	40.4 K	2010-11-02 - 14:45	MichaelWright
jpg	SignalBckKt67Dmin.jpg	r1	manage	40.5 K	2010-11-02 - 14:46	MichaelWright
jpg	SignalBckKt78Dmin.jpg	r1	manage	39.7 K	2010-11-02 - 14:46	MichaelWright
jpg	SignalBckKt89Dmin.jpg	r1	manage	39.5 K	2010-11-02 - 14:46	MichaelWright
jpg	SignalKTDMIN.jpg	r1	manage	22.4 K	2010-10-06 - 13:16	MichaelWright
eps	fig_07.eps	r1	manage	28.2 K	2010-11-10 - 09:33	MichaelWright
pdf	king_poster.pdf	r1	manage	1328.7 K	2010-11-09 - 17:18	MichaelWright

Topic revision: r16 - 2010-11-23 - MichaelWright

ATLAS