Title: Expected vacuum performance in LHCb
1Expected vacuum performance in LHCb
- Adriana Rossi
- With thanks to J.R. Knaster
2Contents
- LHCb layout
- Vacuum stability for ion induced desorption
- Expected dynamic pressure profile
- General comments to the current design
- Main open questions for LHCb
- Conclusions
3LHCb layout
- Vertex Tank (Al) - Larger lateral gap
- Approximated to cylinders of same lateral pumping
- Cone (NEG coated)
- Approximated to cylinders
- Lumped pumps
- Sputter ion pumps (SIP) on Vertex Tank
- SIP sublimation pumps at 19.7 m from IP (cone
end) - Geometry for calculations
- From -1.2 m to 21.5 m from IP considered
- Section upstream to be defined (freedom)
4LHCb layout
5Vacuum stability for ion induced desorption
- Assumptions
- Vertex Tank
- Unbaked
- Ion desorption yield (hi) as for unbaked surface,
with ion incident energy 300 eV. - Cone
- Saturated not pumping
- hi as for baked surface, ion incident energy
300 eV. - hi as for unbaked surface, ion incident energy
300 eV - To be verified - measurements on going.
- Weak dependence of ion energy with b function
neglected
6Vacuum stability for ion induced desorption
- Results Critical current
- Calculated with the single gas model, in the
VD closed position - The vacuum is said to be stable if
- Icrit gt 3.4 A
7Vacuum stability for ion induced desorption
- Results (2)
- The vacuum is unstable if the saturated NEG hi is
as large as for an not conditioned stainless
steel. - Baking of the Vertex Tank at T 150ºC is being
included in the new design. Main advantages
longer time to saturate the NEG and lower hi ?
stability - The pump at the end of the cone ( 19.7 m from
IP) is indispensable for vacuum stability.
The pump _at_ cone end may be removed after
experience with ops
8Expected dynamic pressure profile
- Assumptions
- Vertex Tank
- Photon desorption yield as for unbaked surface,
with photon incident energy 12 eV - Cone
- Photon desorption yield as for baked and glow
discharge cleaned surface (to be verified -
measurements on going), with ion incident energy
300 eV. - Electron induced desorption not taken into
account Assumption valid in the absence of
electron multipacting -
9Expected dynamic pressure profile
- Results
- Note There is no stringent request on vacuum
performance from the LHCb experiment
10General comments to the current design(1)
- Visit to NIKHEF and to DESY - Hera-B
- Report to be issued
- NIKHEF
- Concerns expressed by LHC/VAC taken into
consideration. Solutions have been proposed. - Vacuum scenarios (pump-down, venting and beam
operations) outlined. - VD foil feasibility and tests on going.
- CO2 2 phases also at ambient temperature ? no
overpressure foreseen due to T changes. - Calculations show cooling capillaries can
withstand several hundreds bars.
11General comments to the current design(2)
- HERA-B
- Similar concept.
- No safety system in between primary and secondary
vacua. - Vacuum issues less critical.
- Baking not possible.
- Long pump-down at beginning of operations (due to
secondary vacuum pressure) but faster (1/2 day)
after following venting. - No vacuum accidents.
12Main open questions for LHCb (1)
- VD foil thicknessWaiting for calculations and
test results. Critical pressure to be decided
depending on the criteria chosen by CERN/LHC.
Accident scenario (for plastic deformation and
rupture) to be described, with the consequences
on machine running. - Gravity valvesDynamic response in realistic
geometry to be tested. Limits to be assessed. - Pump-down and venting scenarioPrototype and
tests requested. - Secondary vacuum outgassingMeasurements
requested
Fear that 15mbar not enough
13Main open questions for LHCb (2)
- Seal between primary and secondary vacuumIn
present design one all metal seal and one Viton
seal. - Baking demonstration
- Cooling system reliabilityMain concern vacuum
brazing on 0.1 mm Stainless Steel tubes for 15
bar CO2 circulation. - Bellow between primary and secondary vacua
- Fast shutters foreseen after the low b quads
- Electron cloud study for the LHCb
geometryCoating of the VD Al foil with low SEY
materials (NEG, TiN, in situ Ti evaporation or
others) may result necessary
14Conclusions
- The LHC/VAC group accepts
- Foil not withstanding atmospheric pressure -
compromise between safety and physics
performances. - 2 phases CO2 cooling system in secondary vacuum.
- Provided that
- Risk assessment complies with LHC standards.
- Design developments in close collaboration/supervi
sion with CERN. - Prototype and testing prove principles.
- Replacement vacuum chamber in the case of major
accident. - Machine and other experiments agree.