Polarized internal gas target at LHC

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Presentation transcript:

Polarized internal gas target at LHC Paolo Lenisa – University of Ferrara and INFN (& friends) Brainstorming on future fixed targets at LHCb CERN - 21.12.16

The HERMES polarized internal gas target @ DESY-HERA (e+/- E=27 GeV) Polarized atomic beam injected from left Sample beam: QMS (a = molecular fraction). Polarimeter (P = atomic polarization). Sampling corrections to compute polarization seen by beam. Atomic Beam Source Target Gas Analyzer Sample Beam Polarimeter Target B

HERMES H&D target e 27.6 GeV p 920 GeV

The HERMES target now: installation@ COSY-FZJ (p/d E=2 GeV) ABS Breit-Rabi polarimeter Last achievement Target compatible for H and D running (Without vacuum breaks!)

LHC beams p and Pb beams intensities @ LHC Protons: Ip = 3.63∙1018 p/s @ 7 TeV. Lead: IPb = 4.64∙1014 Pb/s @ 2.76 TeV/u.

LHC beams p and Pb beams intensities @ LHC Beam half-life: ≈ 10 h Protons: Ip = 3.63∙1018 p/s @ 7 TeV. Lead: IPb = 4.64∙1014 Pb/s @ 2.76 TeV/u. Beam half-life: ≈ 10 h Parasitic operation requires small reduction of half-life (< 10%)

LHC beams p and Pb beams intensities @ LHC Beam half-life: ≈ 10 h Protons: Ip = 3.63∙1018 p/s @ 7 TeV. Lead: IPb = 4.64∙1014 Pb/s @ 2.76 TeV/u. Beam half-life: ≈ 10 h Parasitic operation requires small reduction of half-life (< 10%) 1s-radius at IP (full energy): < 0.02 mm Negligible compared with the cell radius (> 5 mm) Safety radius at injection (450 GeV for p): > 25 mm “Openable” cell required.

Geometry for a LHC storage cell LHC Requirements: Beam tube Length: 1000 mm (L1 = 500 mm) Closed: D1 = 14 mm (> DVELO = 10 mm). Opened: D1 = 50 mm Feed tube: D2 = 10 mm and L2 = 100 mm Cell temperature: T = 300 K. Conductance: Ci [l/s] = 3.81 √(T/M)∙ Di3 / (Li + 1.33 Di) (M = molecular weight) Density: r0 = I / Ctot with Ctot = C1 + C2 +... (I [part/s] gas flow-rate)

Geometry for a LHC storage cell LHC Requirements: Beam tube Length: 1000 mm (L1 = 500 mm) Closed: D1 = 14 mm (> DVELO = 10 mm). Opened: D1 = 50 mm Feed tube: D2 = 10 mm and L2 = 100 mm Cell temperature: T = 300 K. Conductance: Ci [l/s] = 3.81 √(T/M)∙ Di3 / (Li + 1.33 Di) (M = molecular weight) Density: r0 = I / Ctot with Ctot = C1 + C2 +... (I [part/s] gas flow-rate) Example: H, Ctot = 2 C1 + C2 = 12.81 l/s, I = 6.5∙1016/s (HERMES): r0 = 5.07∙1012/cm3 areal density q = L1∙ r0 = 2.54∙1014/cm2

The HERMES storage cell (realized in the Ferrara-INFN workshop) Material: 75 mm Al with Drifilm coating Size: length: 400mm, elliptical cross section (21 mm x 8.9 mm) Temperature: 100 K ( variable 35 K – 300 K)

Openable storage cell development in Ferrara (Storage cell for 2 GeV p/d beam at COSY (FZ-Juelich)

Polarized 1H gas target performance Polarized H injected into storage cell Areal density: q = 2.54∙1014 H/ cm2 Proton current Ip = 3.63∙1018/s (similar @ TeV) Total luminosity: Lpp = 0.92∙1033/ cm2 s (About 10% of the collider luminosity) (x20 RHIC p-p luminosity) Possibility to cool down the cell to 100 K (q increase by √(300/100) = √3 = 1.73)

Polarized 1H gas target performance Polarized H injected into storage cell Areal density: q = 2.54∙1014 H/ cm2 Proton current Ip = 3.63∙1018/s (similar @ TeV) Total luminosity: Lpp = 0.92∙1033/ cm2 s (About 10% of the collider luminosity) (x20 RHIC p-p luminosity) Possibility to cool down the cell to 100 K (q increase by √(300/100) = √3 = 1.73) spp @ √s = √2MnEp ≈ 100 GeV = 50 mb = 5∙10-26 cm2 Loss rate dN/dt: 4.5∙107/ s Stored protons: N = 3.2∙1014 Max. relative loss rate: (dN/dt)/N = 1.4∙10-7/ s. The H target does not affect the life time of the 7 TeV proton beam.

(with Pb-beam loss rate limited to 10%) Pb on Xe target (with Pb-beam loss rate limited to 10%) Pb lifetime in Pb-Pb collider: tc = 10 h/ 0.693 = 14.4 h Max Induced target life time: tt = 10∙14.4 h = 144 h Loss rate dN/dt = N∙ (N = number Pb ions = 4∙1010): N∙/N = 1/144 h -> N∙ = N/5.18∙105 s = 7.72∙104/s = LPb-Xe ∙ stot (Pb-Xe) shadronic: 7.65 barn -> scaling with nuclear radii: stot (Pb-Xe) = 6.6 barn

(with Pb-beam loss rate limited to 10%) Pb on Xe target (with Pb-beam loss rate limited to 10%) Pb lifetime in Pb-Pb collider: tc = 10 h/ 0.693 = 14.4 h Max Induced target life time: tt = 10∙14.4 h = 144 h Loss rate dN/dt = N∙ (N = number Pb ions = 4∙1010): N∙/N = 1/144 h -> N∙ = N/5.18∙105 s = 7.72∙104/s = LPb-Xe ∙ stot (Pb-Xe) shadronic: 7.65 barn -> scaling with nuclear radii: stot (Pb-Xe) = 6.6 barn Max. Pb-Xe lumi: LPb-Xe = 1.17∙1028/ cm2s (10 x Pb-Pb collider design luminosity (1027/ cm2 s) Xe density q: 2.52∙1013/cm2 Xe flow rate at 300 K: 2.1∙10-5 mbar l/s

Conclusions Storage cell target provides highest areal density at minimum gas input. Internal targets represent a solid technology: > 10 years of run at HERA - 27.6 GeV e+/e- at I = 40 mA presently in use at COSY (2 GeV p/d)

Conclusions Storage cell target provides highest areal density at minimum gas input. Internal targets represent a solid technology: > 10 years of run at HERA - 27.6 GeV e+/e- at I = 40 mA presently in use at COSY (2 GeV p/d) Polarized H gas target: Cell with L=1 m and f = 14 mm assumed (as SMOG/VELO @ LHCb) 1033/cm2 s accessible

Conclusions Storage cell target provides highest areal density at minimum gas input. Internal targets represent a solid technology: > 10 years of run at HERA - 27.6 GeV e+/e- at I = 40 mA presently in use at COSY (2 GeV p/d) Polarized H gas target: Cell with L=1 m and f = 14 mm assumed (as SMOG/VELO @ LHCb) 1033/cm2 s accessible Unpolarized target: p-A and Pb-A collisions with H2, He, Ne, Ar, Kr and Xe Max. Pb-Xe lumi: LPb-Xe = 1.17∙1028/ cm2s

Conclusions Storage cell target provides highest areal density at minimum gas input. Internal targets represent a solid technology: > 10 years of run at HERA - 27.6 GeV e+/e- at I = 40 mA presently in use at COSY (2 GeV p/d) Polarized H gas target: Cell with L=1 m and f = 14 mm assumed (as SMOG/VELO @ LHCb) 1033/cm2 s accessible Unpolarized target: p-A and Pb-A collisions with H2, He, Ne, Ar, Kr and Xe Max. Pb-Xe lumi: LPb-Xe = 1.17∙1028/ cm2s FINAL OBVIOUS (?) REMARK: The implementation of a storage cell in ANY storage ring requires (from the beginning) the highest level of involvement and participation of the accelerator group.