1 Impact de l’effet faisceau-faisceau sur la precision de la mesure de la luminosité à l’ILC Cécile Rimbault, LAL Orsay SOCLE,19-20 Novembre 2007, Clermont-Ferrand

Cécile Rimbault, LAL Orsay Principe de la mesure de luminosité via la diffusion Bhabha Modifications induites par l’effet faisceau-faisceau Conséquences sur la précision accessible pour la luminosité Dépendance avec les paramètres du faisceau et l’énergie de la collision Conclusions Impact de l’effet faisceau-faisceau sur la precision de la mesure de la luminosité à l’ILC

Bhabha particles are detected in coincidence in the luminosity monitor LumiCal covering a range of 26.2 to 82 mrad. L= N Bh /  Bh from counting rate  integrated luminosity Measurement of energy and scattering angle of the Bhabhas  luminosity spectrum reconstruction Physics needs:  L/L : Luminosity measurement in the LumiCal using Bhabha scattering at small angles

Bhabhas are produced with BHLUMI, √s = 500 GeV, 25<  <90 mrad, ISR include Beam-Beam effect treatment with GUINEA-PIG (Nominal beam param. used for simul.) Modification of initial state: Beamstrahlung  √s’≤√s,  ini ≠ 0, E elec ≠ E posit Modification of final state: Electromagnetic deflections  bhabha angle reduction (~10 -2 mrad) + small energy losses Beam-Beam effects on Bhabha scattering

5 First study with the following selection cuts : E beam  Suppression of Bhabha particles within selection cuts: the bias is defined as (N theor – N exp )/N theor Due to modification of initial state = beamstrahlung: (-3.78 ± 0.04)% Due to modification of final state = EM deflections: (-0.65 ± 0.02)% Total BHabha Suppression Effect (BHSE): (-4.41 ± 0.05)% Why is there such an important Bias ? Consequences on integrated luminosity measurement: Reduction of Bhabha counting rate - 1

6 Bhabha0 Bhabha1 Beamstrahlung  enhancement of acollinearity:    = 1.27 mrad    = 2.00 mrad The angular cut should not be symmetric: new asymmetrical cuts 30 mrad<  -+ <75 mrad & 26.2 mrad<  +- <82 mrad ref. A. Stahl LC-DET Reduction of Bhabha counting rate - 2 Angular cuts optimization

7 Beamstrahlung & EM deflections: Bhabha energy reduction + energy asymmetry enhancement  use global energy cut: E + + E - > 0.8√s BHSE from Beamstrahlung BHSE from EM deflections Total BHSE Reduction of Bhabha counting rate - 3 Energy cuts optimization

8 Suppression of Bhabha particles inside the selection cuts E beam : Due to modification of initial state = beamstrahlung: (-3.78 ± 0.04)% Due to modification of final state = EM deflections: (-0.65 ± 0.02)% Total BHabha Suppression Effect : (-4.41 ± 0.05)% Suppression of Bhabha particles inside the optimized selection cuts 30 mrad 0.8√s : Due to modification of initial state = beamstrahlung: (-1.03 ± 0.04)% Due to modification of final state = EM deflections: (-0.48 ± 0.02)% Total BHabha Suppression Effect : (-1.51 ± 0.05)%  The bias on integrated luminosity measurement is reduced about a factor 3 with asymmetric angular cuts and global energy cut. Consequences on integrated luminosity measurement: Reduction of Bhabha counting rate - 4

9 Reconstruction of luminosity spectrum from lumical Experimentally, EMdeflections have no impact on the reconstructed lumi spectrum.  Beamstrahlung can still be measured with lumi spectrum  EMdeflections can not be controlled directly...    ISR ISR+BS ISR+BS+EMdef x exp from K. Mönig ref. LC-PHSM TESLA

10 Sensitivity of BHSE to the beam parameters BHSE is not sensitive to beam offsets,  x and  y,, to longitudinal shifts of the bunch waist and to vertical size of the bunch. BUT BHSE has strong dependence on bunch length,  z, and horizontal size,  x BHSE from Beamstrahlung BHSE from EM deflections Total BHSE  z (  m)  x (nm)

11 Sensitivity of BHSE to energy - 1 ILC should enable physics runs initially for energies from the Z boson mass to 500 GeV  In this energy range beam-beam effects are strongly modified BHSE from Beamstrahlung BHSE from EM deflections Total BHSE With constant beam optical parameters

12 Sensitivity of BHSE to energy - 2 ILC should enable physics runs initially for energies from the Z boson mass to 500 GeV  In this energy range beam-beam effects are strongly modified BHSE from Beamstrahlung BHSE from EM deflections Total BHSE Constant luminosity At low energy, EM contribution of BHSE becomes dominant, reaching few 100*10 -4 Constant beam parameters

13 Summary & Conclusions - 1 Beam-beam effects on Bhabha scattering increase acollinearity (+0.7 mrad) and energy asymmetry on the Bhabha particles  Need to find a compromise with background suppression cuts This leads to a bias on the integrated luminosity measurement of the order of , depending on selection cuts and beam parameters BHabha Suppression Effect mainly arises from beamstrahlung (for Nominal ILC) The reconstructed luminosity spectrum in the LumiCal is almost not modified by EM deflections  beamstrahlung can be measured from the lumi spectrum reconstruction Main dependencies are from the horizontal and longitudinal sizes of the bunch. A precision of 20% is needed on their knowledge to limit the error on BHSE from EM deflections to about To reach a precision of on luminosity, a precision better that 5% is needed on  x and  z.

14 Summary & Conclusions - 2 No direct way to control experimentally the bias from EM deflections, but measurements of beam angular divergence in extraction line could provide a way to monitor lumi bias from  x variations. For  z ?  Need to use a simulation tool: CAIN, GUINEA-PIG and GUINEA-PIG++ for further studies. For the GigaZ option, a precision of is needed for the luminosity, while the bias from EM deflections is >100 x  need more complete studies. “Impact of beam-beam effects on precision luminosity measurements at ILC”, C. Rimbault, P. Bambade, K. Mönig, D. Schulte, EuroTeV-Report , JINST 2 P09001.