NuMI NBI03 November 7-11, 2003 FNAL thin beam windows Jim Hylen / FNAL Page 1 FNAL experience with thin beam windows Issue is: Survival of window in high.

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Presentation transcript:

NuMI NBI03 November 7-11, 2003 FNAL thin beam windows Jim Hylen / FNAL Page 1 FNAL experience with thin beam windows Issue is: Survival of window in high power proton beam Windows described in this talk: FNAL Anti-proton production target station experience – Information provided by Patrick Hurh and James Morgan NuMI prototype-target test window experience NuMI Decay Pipe Window calculations

NuMI NBI03 November 7-11, 2003 FNAL thin beam windows Jim Hylen / FNAL Page 2 Titanium window on proton beamline for pbar production Tri-clad transition ring and weld backup ring 1.5 mil thick Titanium grade 2 foil Run I era: beam sigma of 0.4 mm 3E12 protons per 1.6  sec pulse failure every year or two Run II era:(~1 – 2 E18 protons/month) beam sigma 0.3 mm on window increasing from 4E12 to 5.25E12 per pulse failures at 3 months, 1 month, 2 weeks

NuMI NBI03 November 7-11, 2003 FNAL thin beam windows Jim Hylen / FNAL Page 3 Titanium window on proton beamline for pbar production Failure mode: Develop vacuum leak (~ 10-7 torr litre /sec) See no signs of cracks on the Ti window under a microscope See some oxidation (similar to picture later in talk) Failure mechanism not known, but have a supposition failure is earlier than probably expected from radiation damage peak temperatures are above "alpha/beta transus", so high temperature and rapid cooling could be inducing micro-structural changes, decreasing ductility, making titanium brittle Ti window was replaced with Be window last year

NuMI NBI03 November 7-11, 2003 FNAL thin beam windows Jim Hylen / FNAL Page 4 Beryllium window on proton beamline for pbar production in beam for about a year now 0.3 mm RMS spot size ~5e12 protons/pulse accumulated about 1.7E19 protons with no failures can see spot where beam heating has caused oxidation having to clean-up mixed waste ( after a wrench-meets-window incident NOT at pbar ) induced installation of a catcher (pair of Ti windows with air break where spot size is 4 mm) which would limit spread of Be contamination upstream in case of catastrophic window failure

NuMI NBI03 November 7-11, 2003 FNAL thin beam windows Jim Hylen / FNAL Page 5 Beryllium Window beamline window versus pbar SEM 10 mil thick Be foil in beamline window Be window used on pbar target SEM is even better test has held vacuum longer (for about 7 years ) with spot size about half that listed for Ti window (recently about 5e12 at ~0.2 mm rms spot size)

NuMI NBI03 November 7-11, 2003 FNAL thin beam windows Jim Hylen / FNAL Page 6 NuMI Prototype Target Test target can Beryllium window During the NuMI target prototype test, an even more intense spot was generated for a short period of time protons/ 10  sec pulse 0.21 mm x 0.16 mm spot size No visible damage to beryllium window ( however target was not run at a high vacuum, only a few milli-torr, so a small leak could have gone unnoticed )

NuMI NBI03 November 7-11, 2003 FNAL thin beam windows Jim Hylen / FNAL Page 7 NuMI Upstream Decay Pipe Window Steel at large radius Transition ring Aluminum thin window 1/16” thick 6061-T6 Al 46 m after target (Downstream window is ¼” steel)

NuMI NBI03 November 7-11, 2003 FNAL thin beam windows Jim Hylen / FNAL Page 8 Decay Pipe Window (accident condition –beam misses target) Accident condition: 4x10 13 proton/spill ~2.5 mm RMS beam spot Air pressure pre-stresses vacuum window Beam heating temporarily reduces stress at center of window Normal running condition: ~4x10 12 proton/spill through target ~11 mm RMS beam spot at window Expect radiation damage at ~ 4x10 19 proton/mm 2 ~ one century of running

NuMI NBI03 November 7-11, 2003 FNAL thin beam windows Jim Hylen / FNAL Page 9 Decay Pipe Window (accident condition –beam misses target) Temperature rise after many beam cycles is small ( 1 pulse / 1.87 seconds)

NuMI NBI03 November 7-11, 2003 FNAL thin beam windows Jim Hylen / FNAL Page 10 Conclusions Performance of Beryllium windows is adequate for NuMI near the target, ( 4e13 protons/pulse at 1 mm rms spot size) while Titanium would not be The ES&H aspect of Beryllium has to be dealt with during design (plan for containment and/or clean-up considered) Aluminum appears adequate for the decay pipe window, where beam conditions are not as harsh