1 / 10

IDS120j with and without Resistive Magnets: Pion and Muon Studies within Taper Region, III (20 cm Gaps between Cryostats

This study investigates the spreading of muons within the taper region and beyond in IDS120j geometry with or without resistive magnets. The magnetic field and muon distributions are analyzed, along with neutron energy cutoff and proton beam power.

donnaroberts
Download Presentation

IDS120j with and without Resistive Magnets: Pion and Muon Studies within Taper Region, III (20 cm Gaps between Cryostats

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. IDS120j WITH AND WITHOUT RESISTIVE MAGNETS PION AND MUON STUDIES WITHIN TAPER REGION, III ( 20 cm GAPS BETWEEN CRYOSTATS ) Nicholas Souchlas, PBL (9/4/2012) 1

  2. IDS120j GEOMETRY, WITH/WITHOUT RESISTIVE COILS: WITH 20 cm GAPS *********************************************************** # MUONS SPREADING WITHIN THE TAPER REGION AND BEYOND. # MUONS DETECTED WITHIN 40 cm RADIUS IN z PLANES ALONG THE TAPER REGION AND BEYOND. # MAGNETIC FIELD FOR IDS120j WITH AND WITHOUT THE RS MAGNETS WILL BE USED. (ONLY SC MAGNETS ARE LEFT IN THE GEOMETRY FOR THE MARS SIMULATIONS). # BEAM PIPES WITH TAPERING FROM z = 0.0 cm TO z = 1,500 cm [ BASELINE ] USED FOR BOTH CASES ALTHOUGH THE MAGNETIC FIELD IS NOT 1.5 T AT THE END POINT. *********************************************************** >SIMULATIONS CODE:mars1512 >NEUTRON ENERGY CUTOFF:10-11 MeV >PROTON BEAM POWER: 4 MW >PROTON ENERGY: E = 8 GeV >PROTON BEAM PROFILE: GAUSSIAN, σx = σy = 0.12 cm (P12 POINT) >EVENTS IN SIMULATIONS : Np = 200,000 2 IDS120j GEOMETRY, NO RESISTIVE COILS: WITH 20 cm GAPS *********************************************************** # SIMULATIONS USING LOWEST GRADE W BEADS IN SHIELDING ( OF 15.8 g/cc ) # BP#2 SEGMENTATION STUDIES WITHIN THE FIRST CRYOSTAT AND RIGHT FLANGE OF Hg POOL INNER VESSEL. *********************************************************** >SIMULATIONS CODE:mars1512 ( USING MCNP CROSS SECTION LIBRARIES ) >NEUTRON ENERGY CUTOFF:10-11 MeV >SHIELDING: 60% W + 40% He( WITH STST VESSELS) >PROTON BEAM POWER: 4 MW >PROTON ENERGY: E = 8 GeV >PROTON BEAM PROFILE: GAUSSIAN, σx = σy = 0.12 cm

  3. IDS120j: REPLACING RESISTIVE MAGNETS AND FILLING UPPER HALF OF Hg POOL WITH SHIELDING. GENERAL OVERVIEW (LEFT), POOL REGION DETAILS (RIGHT). [20 cm GAPS] SH#3 SH#1 SH#1A SH#1 SH#4 SH#2 BEAM PIPE EXTENDS HALF WAY UPSTREAM TO THE POOL SH#1A Hg POOL 2 cm THICK STST BEAM PIPE Hg POOL CRYO#4 CRYO#3 CRYO#2 CRYO#1 SH#1 10 cm THICK STST RIGHT FLANGE SH#1 2 cm THICK STST OUTER TUBE Hg POOL STARTS ~ 85 cm AND EXTENDS ALL THE WAY TO THE END OF THE FIRST CRYOSTAT ~ 370 cm. SHVS WALLS, Hg POOL VESSEL DOUBLE WALLS, Be WINDOW, He GAP IN Be WINDOW AND IN HG POOL HAVE NOMINAL VALUES FOR THEIR THIKNESS. STRESS FORCES ANALYSIS AND LOCAL DPD DISTRIBUTION WILL BE USED TO DETERMINE THEIR VALUES. 3

  4. IDS120j: WITHOUT RESISTIVE MAGNETS. DETAILS OF THE DOUBLE STST Hg POOL VESSEL (LEFT, MIDDLE) AND THE DOUBLE Be WINDOW (RIGHT). [20 cm GAPS] TWO 0.5 cm THICK Be WINDOWS AT THE END OF CRYO#1 WITH 0.5 cm He GAP BETWEEN THEM FOR COOLING. 2 cm THICK STST INNER Hg POOL VESSEL WITH 1 cm He GAP FOR COOLING. 10 cm THICK STST RIGHT / LEFT FLANGE OF SHVS#4, SHVS#1 / SHVS#2 WITH 20 cm GAP BETWEEN THEM. 4

  5. IDS120j: DETAILS OF THE DOUBLE WALL Hg POOL VESSEL ENVISIONED BY VAN GRAVE. ( PLOTS ARE FROM VAN GRAVE'S 8 / 9 / 2012 PRESENTATION ) He GAS WILL BE FLOWING BETWEEN THE TWO WALLS FOR COOLING. VESSEL FILLED WITH He COOLED THE BEAM PIPE IN THAT AREA WILL BE PART OF THE POOL VESSEL W BEADS FOR SCs SHIELDING. AND REMOVING THE HEAT LOAD WILL BE A CHALLENGING TASK. SEGMENTATION ANALYSIS WILL BE PERFORMED TO DETERMINE THE AZIMUTHAL DPD DISTRIBUTION. 5

  6. IDS120j: FOR THE PIONS AND MUONS DISTRIBUTIONS STUDIE WITHIN THE TAPER REGION ONLY THE SCs ARE PRESENT IN MARS SIMULATIONS [ LEFT ]. BEAM PIPE PROFILE WITH / WITHOUT RS WITH END OF TAPER AT z = 15 m [ RIGHT ]. 6

  7. MUONS RADIAL DISTRIBUTION HISTOGRAMS z (IN m) = 1 (BLACK), 5 (RED), 10 (GREEN), 15 (BLUE), 20 (PINK) FOR 15 T ( LEFT ) AND 20 T ( RIGHT ) MAGNETIC FIELD IN THE TARGET REGION. [ 40 < Ekin < 180 MeV ] SUPRESSION SUPRESSION PIONS AND MUONS DISTRIBUTIONS DEPEND ON: RELATIVE POSITIONS OF PROTON BEAM AND Hg JET ( --> PIONS INITIAL CONDITIONS ), DECAY ( PIONS ) / GENERATION ( MUONS ) OF PARTICLES, THE MAGNETIC FIELD. ONE CAN SEE THE EFFECT ( SENSITIVITY ) ON MUONS YIELDS, DISRTIBUTIONS OF A STRONGER MAGNETIC FIELD IN THE TARGET REGION. IN BOTH CASES THE TAIL HAS REACH A LIMIT AT ~ 15 m AND IS CLEARLY MORE SUPRESSED IN THE 20 T FIELD CASE. ONE CAN ALSO SEE HOW THE CENTER OF THE DISTRIBITION CHANGES WITH z [ <r> ~ 5 / 3 cm --> 10 / 7 cm ( 15 / 20 T ) ] . 7 x/Rap AND y/Rap [BOTH 15 / 20 T] HAVE ONLY A SMALL DIFERENCE. SMALLER RADIAL SPREADING WITH 20 T FIELD [ ~ FIXED DIFFERENCE 15-20 T]. SLOWER DECREASE BETWEEN ~ 2 AND ~ 4 m. FAST DECREASE OF r_max/Rap WITHIN FIRST 8-9 m, MUCH LARGER FOR 20 T FOR ~ 1 -3 m. TAIL PIONS WILL FOCUS FAST WITHIN ~ 10 m [NEED TO TAKE INTO ACCOUNT THE NUMBER OF PARTICLES REPRESENTED BY THESE 20 EVENTS, RATIOS MAY HAVE TO BE MULTIPLIED WITH # PARTICLES WEIGHT FOR 1-20 m POINTS TO EXTRACT MORE CLEAR INFO]. (sig_r/Rap)(15 m/15 T)~0.36 (sig_r/Rap)(15 m/20 T)~0.34 [ GAUSSIAN DISTRIBUTION ? ]

  8. MUONS DISTRIBUTION HISTOGRAMS IN x, z (IN m) = 1 (BLACK), 5 (RED), 10 (GREEN), 15 (BLUE), 20 (PINK) FOR 15 T ( LEFT ) AND 20 T ( RIGHT ) MAGNETIC FIELD IN THE TARGET REGION. [ 40 < Ekin < 180 MeV ] SUPRESSION THE CENTER OF THE DISTRIBUTIONS IS IN THE NEGATIVE x DIRECTION ( -1 ≲ <x> ≲ 0 cm ) AND DOES NOT VARY MUCH WITH z, IT ALSO LOOKS LIKE MOST OF THE SUPRESSION IN THE DISTRIBUTIONS TAILS IS IN THE +x DIRECTION WHEN 15 --> 20 T. ** POSSIBLE CANCELLING EFFECTS BETWEEN POSITIVE AND NEGATIVE MUONS x DISTRIBUTIONS ? ** 8 POSITIVE PIONS x, y AND r DEVIATIONS AS FUNCTIONS OF AXIAL DISTANCE. 7 x AND y SPREADING HAVE ONLY A SMALL DIFERENCE. FROM THE RADIAL SPREADING WITHIN THE FIRST 10 m OR SO IT APPEARS A PORTION OF THE PARTICLES COULD BE LOST IN THE BEAM PIPE AND SHIELDING MATERIAL. THE RADIAL SPREADING HAS REACH ITS LIMIT VALUE OF ~ 11 cm AT z ~ 10 cm. SAME CONCLUSIONS AS THOSE FOR POSITIVE PIONS CAN BE DRAWN FROM ABOVE PLOTS FOR NEGATIVE PIONS.

  9. MUONS DISTRIBUTION HISTOGRAMS IN y, z (IN m) = 1 (BLACK), 5 (RED), 10 (GREEN), 15 (BLUE), 20 (PINK) FOR 15 T ( LEFT ) AND 20 T ( RIGHT ) MAGNETIC FIELD IN THE TARGET REGION. [ 40 < Ekin < 180 MeV ] SHIFT SUPRESSION THE CENTER OF THE DISTRIBUTIONS IS IN THE POSITIVE y DIRECTION ( 0 ≲ <y> ≲ 1 cm INITIALLY). THERE IS A WEAK INCREASE WITH z FOR THE 15 T FIELD AND A RELATIVELY STRONGER INCREASE FOR THE 20 T. [ FROM ~ 1 cm FOR 15 / 20 T TO ~ 2 cm FOR 15 T AND ~ 6 cm FOR 20 T CASE. IT ALSO LOOKS LIKE MOST OF THE SUPRESSION IN THE DISTRIBUTIONS TAILS IS IN THE - y DIRECTION WHEN 15 --> 20 T. ** POSSIBLE CANCELLING EFFECTS BETWEEN POSITIVE AND NEGATIVE MUONS y DISTRIBUTIONS ? ** 9 SAME CONCLUSIONS CAN BE DRAWN FROM ABOVE PLOT FOR NEGATIVE PIONS TOO. NEGATIVE PIONS x, y AND r DEVIATIONS AS FUNCTIONS OF AXIAL DISTANCE. 8

  10. NUMBER OF PIONS AND MUONS PER INCIDENT PROTON AS FUNCTIONS OF AXIAL DISTANCE [ LEFT ] AND FOR MUONS ONLY [ RIGHT ]. MOST SIGNIFICANT DIFFERENCE IS IN THE YIELD OF POSITIVE MUONS (FROM 15 TO 20 T) AND STARTS AT ~ 10 cm. 10 MUONS RADIAL SPREADING HAS A FASTER INCRAESE WITHIN FIRST FEW METERS SINCE MORE AND MORE PIONS DECAY TO MUONS INCREASING THEIR NUMBER AND THEIR SPREADING . PIONS AND MUONS RADIAL SPREADING COMPARISON. 11

More Related