1. Searches for double partons Lee Pondrom University of Wisconsin July 23, 2012

2. Rick Field’s definition of the ‘underlying event’

3. Single vertex dijet or Z+jet event

4. Charged tracks in the transverse region R Field studied the underlying event and tuned Pythia to match the charged track activity observed in the transverse region. (PRD 82, 034001,(2010). Track p T >.5 GeV, track |η|<1 Parameters track multiplicity, scalar sum track p T. He looked at Z D-Y data to define the transverse region.

5. RField’s Z transverse data X XX X X =jet20,50,70, and 100 data

6. Use jets to define the axis and check Field’s Z results

7. Transverse track activity depends slowly on p TZ or jet1 E T About 90% of the ∑p T and track number plots are energy independent. Underlying event activity is the same for p TZ ≈ jet1E T If double parton hard scattering exists, a good place to look for it would be in the transverse region. Try scalar ∑transverse track p T >15 GeV as a ‘trigger’

8. To see if it works, try jet events with two vertices Use jet100 jet50, and jet20 data Require jets one and two to be on the first vertex. Exactly two vertices per event. Extra jets three and four can be anywhere Separate the two vertices by at least 10 cm. Require vtx2 to have at least 3 charged tracks, with p T >.5 GeV and |η|<1. Second vtx σ ≈ 6 mb.

9. Two vertex event with 2 jets on primary vtx and 2 jets on 2 nd vtx

10. Second vertex is ‘minbias’ CDF minbias defined by the CLC σ ≈ 36 mb Track requirements here are different, in particular |η|<1, so σ is smaller, although 6 mb is a soft number – it depends on instantaneous luminosity taken to be 2E32. For the jet stntuples analyzed, the avge probability of two vertices is 30%.

11. Transverse tracks on primary and secondary vertices

12. Transverse track activity The first vertex transverse tracks are defined with respect to the azimuth φ of the highest E T jet:  /3<Δφ(jet-track)<2  /3 second vertex transverse tracks are defined in the same way with respect to the same jet – highest E T jet on vtx1, track on vtx2. Jet activity ‘triggered’ by ∑transtrackp T >15 GeV is similar in jet20 and on 2 nd vtx. ~90% of all ‘triggers’ have a third jet E T >5 GeV

13. Fraction of ∑transtrackp T >15GeV vs E T jet1

14. ∑transtrackp T >15 GeV Note that the fraction increases from.001 to.015 going from minbias (plotted as E T =5GeV) to jet20. Using σ ≈ 6 mb for the 2 nd vertex, the cross section for the ∑p T >15 GeV ‘trigger’ is σ ≈ 6  b. about 5 times larger than the effective cross section for jet20.

15. Jet activity ‘triggered’ by ∑p T >15 GeV – 2 nd vtx and jet20

16. Jet activity ‘triggered’ by ∑p T >15 GeV 2 nd vtx compared to jet20 Jet4 is similar 2 nd vtx compared to jet20 Δφ12 is the azimuthal angular correlation for the two leading jets. For the 2 nd vtx the ‘trigger’ has no effect on Δφ12, which is on the other vertex. But with transverse tracks on the same vertex, Δφ12 is totally wiped out for jet20. Effect for jet100 is less traumatic.

17. Δφ dijet angular correlations-main jet on vtx 1, jets 3&4 on vtx 2

18. Δφ jet-jet angular correlations after transtrack ∑p T >15 GeV Δφ23 is shifted into the transverse region. The third jet appears near 90 degrees to the second one. Jet 2 and jet 3 are on different vertices. Δφ14 shows a similar shift. Relative to the primary axis, jets 3 and 4, on the second vertex, are in the ‘transverse’ region.

19. Δφ for jets 3&4 on 2 nd vtx, selected by ∑transtrackp T >15GeV

20. Δφ34 with transtrack∑p T >15 GeV For the 2 nd vtx Δφ34 has a distinct peak near . (Sum 2.4<φ<  )/all events=3.5E-4 Jets 3&4 are not required to be on vtx2. Events with Δφ<1 are probably on vtx1 Δφ12 for jet20 data without the ∑p T >15 GeV requirement is shown for comparison of the jet-jet angular correlation. Jet20 is sharper – the average jet E T ’s are higher.

21. Jet E T on 2nd vertex with ∑trackp T >15 GeV ‘trigger’

22. Jet20 Data Stntuple gjt1bk & gjt1bj 3E6 events Require only one vertex Require at least two jets with |η| 20 GeV. Other jet E T >5 GeV Apply level 5 jet energy corrections Events Jet1&2 Jet3 Jet4 Lum(live) 110203 61769 21174 151694/nb 56% 19% Prescaled σ ≈ 0.7 nb; unprescaled σ≈1.2  b

23. Jet20 data Jet E T

24. Jet20 data Δφ distributions

25. Following Rick Field, define the transverse region relative to jet1φ Look at charged tracks with |η|.5 GeV, and with  /3<Δφ<2  /3, where Δφ is the azimuthal angle between the track and the highest E T (trigger) jet. These tracks are sensitive to the underlying event, and hence at least in part depend on multiparton interactions.

26. Jet20 data properties of the transverse tracks

27. Jet20 transverse track p T cut Based on the idea that the transverse region has some sensitivity to what is going on in the event other than the two primary jets, we make a cut on the scalar sum of track p T >15 GeV. This cut leaves 1611events – 1.5% of all dijets. The fraction increases with jet energy. The cut moves jet3 into the Δφ region of the tracks.

28. Effect of the ∑transtrackp T >15GeV on the jet φ distributions

29. Effect of the ∑transtrack p T >15 GeV cut on jet φ Of the 1611events, 1495, or 93%, have jet3E T >5 GeV, and these jets are clustered around  /2 relative to the trigger jet. 15 GeV is too high relative to the main jet activity, so the correlation Δφ12 is strongly perturbed.

30. Δφ34 and the high p T transverse tracks The idea is that jets 3 and 4 could be result of independent scattering of two other partons. If that is true, a good place to look is in the Δφ region of the underlying event. The ∑transtrack p T >15 GeV serves as a ‘trigger’. Δφ34 should peak near .

31. Δφ34 and jet3E T before and after track∑p T >15 GeV cut

32. Enhancement near Δφ=  ? Normalizing the two distributions to Δφ<1.5 gives a difference 2.4<Δφ<3.2 of -8±17 events. Transverse jet energies for jets3 and 4 are increased by the track p T cut

33. Look at jet100 data 1E6 events gjt4bk & Pythia bt0stb Same requirements: only one good vertex, trigger jet E T >100 GeV, level5 jetECorr Yields for 1E6 events Jet1&2 jet3 jet4 p T >15GeV Lum 170710 101231 35034 10247 126342/nb Jet3 and jet4 fractions same as jet20 p T >15 GeV fraction 4x larger than jet20 σ ≈ 1.3 nb no prescale

34. Jet100 data and Pythia E T

35. Jet100 & Pythia transtrack p T and Δφ12

36. Jet100 data effect of the transverse tracks on Δφ12 and Δφ13

37. Jet100 effect of transverse tracks on jetE T 3 and Δφ34

38. Jet100 & Pythia effect of ∑p T >15 GeV cut on transverse tracks

39. Jet100 effect of transverse tracks Jet100 similar to jet20. Pythia & data agree. Perturbation of Δφ12 considerably less than for jet20. Δφ13 shifts so that jet3 is  /2 away from jet1 Jet3 E T shifts to larger values

40. Compare jet100 and Pythia Δφ34 before and after ∑p T >15GeV cut

41. Jet100 data and Pythia Δφ34 The data and Pythia agree qualitatively in the shapes of the Δφ34 angular distributions before and after the ∑p T >15 GeV cut on the scalar sum of transverse tracks. Near Δφ34≈  Pythia has a smaller excess than the data.

42. Now compare Δφ34 before and after ∑p T >15 GeV cut

43. Excess near Δφ34≈  Normalize the plots to.5<Δφ34<1.5 Subtract (after cut)-(before cut) 2.4<Δφ34<3.2. Jet100 data difference = 295±50 events Pythia difference = 54±30 events

44. Does this excess mean anything? There are 170710 jet100 good dijet events So the excess 2.4<Δφ34<  is 0.0017±0.0003. Pythia excess is smaller: 0.0007±0.0004. If the number of MPI’s per hard scatter is 5, which comes from Field’s analysis of Drell Yan (PRD 82,034001(2010)), the probability of a second hard scatter is 0.00034±0.00005, or about 3.5E-4 for the jet100 data.

45. Compare to the 2 nd vertex Δφ34 The 2.4<Δφ<  fraction for 2 nd vtx =3.5E-4, which agrees with the peak fraction observed in the jet100 data (but not in Pythia). The dip in Δφ34 near 1.7 radians for the ‘trigger’ events in jet100 is of unknown origin, but is reproduced by Pythia. Subtract (after ∑p T –before ∑p T ) and compare to 2 nd vertex peak.

46. Compare jet100 excess with 2 nd vertex

47. Look at Jet50 data and Pythia Jet20 data are too low E T relative to the ∑transtrackp T >15 GeV cut. Jet50 data are higher, and the Pythia file bt0srb has 4.5E6 events, while bt0stb (jet100) has only 1E6 events, so we have better statistics for the monte carlo. Same procedure as jet20 and jet100

48. Jet transverse energies after level5 jet energy corrections

49. Jet-jet Δφ correlations jet50 and Pythia

50. Jet50 data and Pythia

51. Jet50 data and Pythia after ∑transtrackp T >15 GeV cut

53. Δφ34 for jet50 data and Pythia w/wo ∑transtrackp T >15 GeV

54. Jet50 data and Pythia agree well The excess near Δφ34 =  when the transverse track ‘trigger’ is applied now appears in both the data and Pythia. The excess normalized to the number of events is: jet50 jet100 Data 0.0016±0.0002 0.0017±0.0003 Pythia 0.0009±0.0002 0.0007±0.0004

55. So what? ∑p T >15 GeV trigger gives back to back low E T jets on the second vertex ∑p T >15 GeV trigger also gives an enhancement in Δφ34≈  in jet100 and jet50 data. Pythia jet50 shows about ½ the effect. Pythia jet100 lacks statistics. The enhancement is consistent with the 2 nd vertex, if there are 5 2 nd vertices inside a jet100 or jet50 event.

56. Effective cross section Some folks like to quote an effective cross section, defined by the ratio σ DP =σ A σ B /σ eff. Divide by σ A : ε = σ B /σ eff, or σ eff =σ B /ε, where σ B = 6  b = cross section for the second vertex, and ε = 0.0016±0.0002. ε is energy independent-same for jet50 and jet100, which is consistent with DPI. These numbers give σ eff =3.8±0.5 mb,Δφ=2  /3 Scaling in φ, σ eff =11.4±1.5 mb, in agreement with D0 (PRD 81 052012 (2010)).

57. Extend the study to Drell-Yan  pairs Use high p T muon trigger stntuples 5E8 events total available. 1E6 events takes about 4 hours to analyze So 5E8 would take 3 months of steady computing, unless I can speed things up. 5E7, or 10%, analyzed so far

58.  ± pair yields from high p T muon trigger Stntuples Require two muons opposite charge |η|<1. Eliminate events with cosmic rays Require at least one CMU*CMP muon Require at least one jet E T >5 GeV 48894 events 30GeV<m  <130GeV 40567 events 80GeV<m  <100 GeV 28811 events Z pair p T >10 GeV

59. D-Y mass and p T plots

60. D-Y mass and p T Gauss fit to peak at 90.8 GeV, width 3.8 GeV Pair p T compared to recoil jet E T with level5 jet energy corrections is much harder than jet20 E T spectrum

61. Compare to Pythia D-Y

62. Δφ and ΔE T for track pair and recoil jets

63. Data compared to Pythia D-Y

64. Δφ and ΔE T for track pair and recoil jets Pair p T >10GeV. Central Δφ peak consistent with jet-jet Δφ12 for jet20 data. Δφ=|(recoil jetsφ) – tracksφ| -  is asymmetric, with a tail towards negative values, ie jets and tracks in the same quadrant. ΔE T is nearly symmetric, with a shift such that jet E T is about 4 GeV low relative to the tracks, even with level5 jetEcorr. Pythia agrees with both plots.

65. Scalar sum p T for transverse tracks Z data, jet20data, and Pythia

66. Transverse track scalar ∑p T relative to the  pair axis The trans track ∑p T distributions for D-Y  pairs and for QCD jet20 dijets look very similar. p TZ > 10 GeV required to define ‘transverse track’. Again Pythia agrees well with the data

67. Effect of p TZ on recoil jet E T

68. Effect of p TZ on recoil dijet invariant mass

69. Effect of p TZ on jet E T There are plenty of dijets with E T >5 GeV in events with p TZ <10 GeV Requiring p TZ >10 GeV suppresses the low E T jets, particularly for jet 1. Dijet invariant mass for recoil jets 1&2 depends on p TZ ; jets 2&3 not so much. p TZ =15.6; =12.7 (GeV) p TZ >10 =22.3; =14.7 (GeV)

70. Effect of p TZ on recoil jets Δφ distributions

71. Closer look at recoil jet Δφ12

72. Closer look at Δφ12 near  Normalizing the blue curve to the black from 0 10 GeV. Too large to be DP. The difference in the two histograms is compared to jet20 data in the second plot. It is possible for two jets to be created in D-Y events where the p T of the  pair is less than 10 GeV. For very low  pair p T the two jets have to balance each other.

73. scalar∑transtrack p T >15 GeV For Z->  data with p TZ >10 GeV define the transverse tracks after all muons have been removed as those tracks with p T >.5 GeV and |η|<1 at  /3<Δφ<2  /3 relative to p TZ.. Then require the scalar ∑p T of these tracks to be >15GeV, as a ‘trigger’ analogous to the jet20 and jet100 analyses.

74. Effect of ∑transtrackp T >15 GeV on recoil jets E T

75. Effect of ∑transtrackp T >15 GeV

76. Effect of ∑transtrackp T >15 GeV on recoil jet Δφ distributions

77. Compare D-Y Z->  data and Jet20 data, p TZ >10 GeV

78. Compare D-Y Z->  and Jet20 data, p TZ >10 GeV

79. Discussion Remember that jet1 in the jet20 and jet100 data becomes the Z in the D-Y data, so jet20 jet2->D-Y jet1, jet20 jet3->D-Y jet2, etc. Jet20 Δφ34 is similar to D-Y Δφ23 Jet20 Δφ23 is dominated by gluon radiation off jet 2 to form jet3, while for D-Y Δφ12 is dominated at low jetE T by ISR from initial quarks, so they don’t look similar.

80. D-Y and jet20 for scalar∑transtrackp T >15 GeV

81. More discussion However, there is no sign of an enhancement in Δφ(jets2-3) near . In fact, Δφ(jets2-3) looks more isotropic with the ∑p T >15 GeV cut than without it. This represents about 10% of the total available high p T muon data, but 30% of the integrated luminosity (3/fb)

82. Keep looking -79927 Z-> 

83. More Δφ plots 79927 Z’s

84. The last set including Δφ34

85. High statistics PYTHIA runs-new histograms

86. High statistics Pythia runs

87. Pythia Δφ jets1&2 and Δφ jets 2&3

88. Subtract (with-without) the ∑transtrackp T requirement

89. Jets 1 and 2 align in the transverse region to balance the p TZ

90. No sign of double parton scattering The behavior of the ∑transtrackp T >15 GeV trigger on the Z sample affects jets 1 and 2. jet 3 moves near jet2, to help conserve p T. Jets 1 and 2 move into the transverse region of φ, and Δφ12~2*  /3, resulting in a cancellation of p TZ. Hence there is no evidence for two independent hard scatters.

91. Pythia recoil jet E T for jets1&2

92. Pythia recoil jet3 E T and Δφ

93. Pythia E T jets 1,2&3 Notice how much broader the E T distributions are with the ∑transtrackp T >15 GeV ‘trigger’. This is counter to the notion of a second independent hard scatter, which would result in steeper falling E T distributions, like jet20.

94. Still no effect, even with jets 3 and 4 Try cutting harder p TZ >20 GeV, to see if that helps the Δφ(pair-jets_total) plot. Try using the entire D-Y mass range 30- 130 GeV. Look at Δφ for the jets – muon pair, as well as jet-jet.