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    User name xqian

    Log entry time 02:25:04 on December 03, 2008

    Entry number 251800

    keyword=BAckground Study

    In this log, I summarized the study of the BigBite Wire Chamber Background. Some main features are summarized in the beginning of this log. More details can be found later.

    1. The rate is higher when the HV is higher. The rate is higher when the threshold is lower. The rate is higher when the target density is high.

    2. Too large raster size lead to high background

    3. The rates is high, when the beam is not stable

    4. Background scale with the current on the same target

    5. At 5 pass, by comparing the empty reference cell and the 3He, we conclude 80% of the background is from reference cell.

    6. Background with sieve in is smaller than the one with sieve out.

    7 The shielding we added and the new collimator (not the one for the beam pipe window) give a 15% effect.

    8. On 3He reference cell, the background rates reduce 30% when we go from 1 pass beam to 2 pass beam. The background rates reduce another 45% when we go from 2 pass beam to 5 pass beam. The total improvement is more than 60% from 1 pass to 5 pass. (This include the 15% improvement for adding new shileding and collimator).

    9. At first pass the rates between C1:C2:C3 is 1.34:1.44:1.0. At second pass, the rates between C1:C2:C3 is 1.1:1.17:1. At 5 pass, the rates between C1:C2:C3 is 0.98:1:23:1.

    10. With magnet off, the rates on first chamber is about 100MHz, however the dark current is still ok.

    11 At five pass, we have C1:C2:C3 = 3.8 MHz: 4.5 MHz : 4.3 MHz per 1 uA for the first cell. The number for the second cell is 3.5 : 4.5 : 4.2 MHz per 1uA. The rate reduce a little bit, since the pressure may be lower for the second cell.

    We will need to take a look at the effect of the new collimator.

    *****************************************************************************

    Details

    Single Carbon

    Second pass Single carbon foils

    runnumber, average current, beam energy, BG1, BG2, BG3

    neglect the last two colums, and BG1 means the background for chamber 1 averaged by the current.

    2846 4.67093 2.396 9.07705 8.98951 5.06022 0.307913 0.00976667

    2845 4.95954 2.396 9.0039 8.91744 5.03631 0.312922 0.00990673

    2844 5.08608 2.396 8.99915 8.93464 5.00908 0.365734 0.0127971

    Multi-Carbon

    The rate is quite similar for multi carbon foils run, no matter that is the current

    3618 0.189525 5.889 13.9597 14.9138 11.9391 0.06458 0.00125333

    2970 4.00758 5.889 12.5164 13.1163 10.3946 0.225802 0.0170668

    2968 1.82162 5.889 14.6876 15.1601 11.3286 0.17869 0.00699746

    2964 4.88924 5.889 12.1036 12.7378 10.2521 0.246867 0.0225933

    2962 2.86983 5.889 13.5171 14.0942 10.9364 0.0574684 0.00175447

    2961 3.01676 5.889 13.4611 14.0407 10.9076 0.0589471 0.00185335

    2960 2.57832 5.889 13.4908 14.0576 10.8973 0.0511141 0.00159296

    2958 2.90622 5.889 13.5348 14.0858 10.9569 0.0585775 0.00185201

    2957 2.78242 5.889 13.5596 14.131 10.9588 0.0564937 0.00178668

    2956 3.00221 5.889 13.4767 14.0683 10.9327 0.060318 0.00209442

    2954 3.14097 5.889 13.5017 14.0457 10.6305 0.180482 0.00764256

    2951 5.299 5.889 11.7728 12.2601 10.0398 0.241593 0.0233067

    2947 3.58248 5.889 12.4172 12.9059 10.3477 0.216497 0.0151698

    2946 3.07062 5.889 12.3233 12.7849 10.3564 0.213195 0.0125622

    2945 2.94226 5.889 12.2306 12.7256 10.2864 0.210188 0.0111418

    2944 1.92255 5.889 13.0215 13.4524 10.6482 0.191016 0.00834138

    2943 2.22537 5.889 12.8363 13.2953 10.6254 0.0406736 0.000980007

    two pass beam rate is similar to five pass

    2886 1.96522 2.396 13.0495 13.1289 10.1344 0.342033 0.00833333

    2885 1.99197 2.396 13.003 13.0946 10.0144 0.344767 0.00854667

    sieve out in first pass, the background is higher than 2nd and 5 pass.

    2659 1.94411 1.23 20.489 21.9047 15.2142 0.621937 0.0111867

    2658 1.93284 1.23 19.3895 20.6775 14.3032 0.626444 0.00948006

    2657 1.94821 1.23 19.4812 20.7358 14.3162 0.492541 0.00840213

    2650 0.848011 1.23 19.9542 20.9911 14.5512 0.00606 2.66667e-05

    This run is magnet off. lots of low energy stuff, but not large dark current is fine. (Interesting)

    2641 0.921394 1.23 117.177 116.958 18.3003 0.591873 0.0900667

    sieve in The background level is smaller than sieve out run

    2585 4.31146 1.23 13.8508 14.6175 7.48015 0.459563 0.0137201

    2582 4.39544 1.23 13.9492 14.7142 7.51946 0.461113 0.0150333

    reference cell H2

    4014 11.2568 5.889 3.46187 4.34246 3.65098 0.1909 0.00975333

    4013 11.5656 5.889 3.46019 4.34517 3.64553 0.19404 0.01004

    4012 11.3866 5.889 3.46016 4.34748 3.64713 0.191867 0.00972667

    3942 11.3847 5.889 3.2796 4.12238 3.35871 0.191755 0.00946673

    3941 11.394 5.889 3.28403 4.12752 3.35887 0.191867 0.00906

    3940 11.787 5.889 3.27488 4.11238 3.35655 0.194073 0.00954

    These runs are due to beam tuning

    3286 2.07093 5.889 5.43633 6.03216 4.76275 0.00704667 6e-05

    3285 2.05185 5.889 5.45389 6.05477 4.78058 0.00658667 3.33333e-05

    3284 1.7647 5.889 5.54211 6.21772 4.97923 0.00575333 2e-05

    3283 1.96107 5.889 5.39789 5.95359 4.68159 0.00588135 2.85502e-05

    second pass sieve out, rate is higher than 5 pass

    2904 3.84276 2.396 5.1373 5.29868 3.87372 0.349704 0.00422823

    2903 4.19423 2.396 5.09348 5.27208 3.85028 0.379347 0.00471333

    2902 3.45685 2.396 5.11872 5.30457 3.84334 0.0680536 0.000493653

    2897 3.92018 2.396 5.16858 5.34033 3.89882 0.347107 0.00444

    2896 3.8155 2.396 5.17255 5.3535 3.89401 0.344553 0.00416

    2893 4.05718 2.396 5.14688 5.32725 3.89671 0.3489 0.00417333

    2892 3.7534 2.396 5.18307 5.36327 3.91999 0.340373 0.00382667

    sieve in, rate is lower than the sieve out run

    2869 4.94867 2.396 4.03241 4.03225 2.17442 0.34586 0.00304667

    2868 4.96316 2.396 3.92173 3.90732 2.14529 0.338487 0.0028

    2866 4.72024 2.396 4.03556 4.0295 2.16925 0.3355 0.00236

    2865 4.86636 2.396 4.03456 4.03245 2.15682 0.337853 0.00250667

    2864 4.72289 2.396 4.05494 4.05329 2.19683 0.22746 0.00189333

    2852 1.93914 2.396 4.91344 4.83092 2.52551 0.360967 0.00289333

    2851 2.01945 2.396 4.91049 4.83286 2.52667 0.363253 0.00276

    2850 1.98518 2.396 4.92125 4.82522 2.51028 0.359407 0.0028

    2847 7.3492 2.396 4.63892 4.63796 2.49262 0.188801 0.00296002

    These are the threshold and HV scan, rates are higher when the HV is higher or the threshold is lower

    1650 + 3.5 V

    2685 1.72291 1.23 12.2057 13.3082 9.50286 0.480219 0.00400117

    1650 + 4.0V

    2684 2.0892 1.23 11.4936 12.5096 8.84428 0.495099 0.00413549

    1650 + 4.5V

    2683 2.04255 1.23 11.1484 12.1435 8.5713 0.500836 0.00415233

    1650 + 5.0V

    2682 1.81637 1.23 11.0712 12.0718 8.44012 0.507425 0.00333214

    1550 + 5.0V

    2681 1.82323 1.23 8.86306 9.42724 6.60712 0.483394 0.0017937

    1550 + 4.5V

    2680 1.97943 1.23 9.0395 9.70446 6.85989 0.51719 0.00264319

    1550 + 4.0V

    2679 1.75381 1.23 9.42102 10.1693 7.13414 0.542088 0.00271599

    1550 + 3.5V

    2678 1.75899 1.23 9.67786 10.4546 7.34888 0.54923 0.00329754

    1550 + 3.0V

    2677 1.79008 1.23 9.9638 10.7769 7.58926 0.542637 0.00326192

    1500 + 3.0V

    2676 2.30766 1.23 8.48994 9.09366 6.51045 0.44623 0.00248046

    1500 + 4.0V

    2674 2.29701 1.23 7.65378 8.02825 5.77458 0.210723 0.00064744

    1500 + 4.5V

    2673 2.21942 1.23 7.24323 7.5164 5.38512 0.118234 0.000270072

    1500 + 5.0V

    2672 2.06816 1.23 6.86352 7.07275 5.02221 0.057475 6.69203e-05

    1600 + 5.0V

    2671 1.78938 1.23 10.0348 10.8669 7.67328 0.542029 0.00334943

    1600 + 4.5V

    2670 1.97533 1.23 10.1546 10.9842 7.77619 0.541571 0.00399294

    1600 + 4.0V

    2669 1.89475 1.23 10.4294 11.2939 8.01602 0.533764 0.00410295

    1600 + 3.0V 2668 1.9056 1.23 11.0937 12.0601 8.56418 0.512073 0.00401645

    1600 + 3.5V sieve out 2666 1.85109 1.23 10.7801 11.7277 8.29799 0.522674 0.0041606

    2664 1.93926 1.23 10.5676 11.499 8.11036 0.5265 0.00366667

    2660 1.87621 1.23 10.4002 11.3256 7.91279 0.463586 0.00343694

    2663 2.03858 1.23 10.4459 11.3048 8.00073 0.52568 0.00362667

    2662 1.99827 1.23 10.5103 11.3971 8.03963 0.527653 0.00385333

    sieve in run in first pass, the rate is lower than sieve out run

    2633 1.78828 1.23 7.82255 7.95385 4.18372 0.46388 0.00145333

    2632 0.90210 1.23 8.11132 8.26986 4.19264 0.463633 0.00109333

    2629 0.99101 1.23 8.40817 8.63248 4.46425 0.463493 0.00113333

    2624 0.28064 1.23 8.28214 8.70947 4.47389 0.0413149 0.000142301

    2604 5.01666 1.23 8.50572 8.95142 4.53239 0.263297 0.00256372

    beam tuning

    2620 0.96540 1.23 9.35927 9.52543 5.3044 0.115473 0.000526667

    2614 0.94302 1.23 10.7585 10.8503 5.6252 0.57156 0.00178

    2613 0.99403 1.23 11.044 11.105 5.76637 0.575413 0.00211333

    2612 1.04271 1.23 10.8427 10.92 5.68454 0.57802 0.0019

    2611 1.01808 1.23 10.9225 10.9927 5.6719 0.578347 0.00208

    2610 0.98875 1.23 11.366 11.4142 6.03939 0.579447 0.00218

    N2data

    pressure 20psig

    4010 11.6932 5.889 4.0198 5.04793 4.45353 0.220955 0.0164734

    4009 11.2016 5.889 4.04732 5.09582 4.48859 0.215167 0.0155733

    4008 9.67266 5.889 4.11216 5.18183 4.55485 0.207271 0.0140085

    3939 11.6724 5.889 4.15517 5.23129 4.64779 0.222408 0.0182801

    3934 11.3273 5.889 4.16782 5.2588 4.664 0.2193 0.0175867

    3931 11.2677 5.889 4.16432 5.21655 4.64402 0.216659 0.0174006

    pressure 100psig

    3282 1.96958 5.889 10.473 11.693 10.8406 0.0262333 0.000406667

    3281 2.26364 5.889 10.3199 11.4844 10.5732 0.0305933 0.00052

    3279 2.18303 5.889 9.71474 10.6823 9.54764 0.0277916 0.00034266

    pressre 50psig

    2918 1.99368 2.396 8.11019 8.47274 6.8722 0.360018 0.0058254

    2917 1.98579 2.396 8.06489 8.46214 6.82837 0.0148484 0.000179137

    2916 2.04135 2.396 8.0489 8.44301 6.82444 0.0154467 0.000126667

    2915 1.88838 2.396 8.14762 8.56423 6.92097 0.381732 0.00616915

    2914 2.09692 2.396 7.9709 8.45287 6.72433 0.0140575 0

    2913 2.04483 2.396 8.1729 8.5239 6.66991 0.0172702 0

    2907 1.91982 2.396 8.16135 8.54129 6.88152 0.36134 0.00532667

    1st pass trig!! pressure scan

    2559 5.29056 1.23 7.60471 7.4369 4.14489 0.0177333 0.00143333

    N2 pressure ~ 246 torr

    2524 4.69149 1.23 9.89994 10.4611 6.43899 0.0212735 0.000353336

    N2 pressure ~ 510 torr

    2523 4.35171 1.23 10.2622 10.8647 6.7714 0.0689538 0.000813339

    765 torr

    2522 4.66098 1.23 11.4481 12.1992 7.94162 0.0825006 0.00167334

    950 torr

    2521 4.68852 1.23 12.3153 13.1583 8.7502 0.131701 0.00385336

    950 torr

    2520 4.71689 1.23 12.3971 13.1556 8.7613 0.0948951 0.00282426

    950 torr

    2519 4.34867 1.23 12.8662 13.6869 9.11378 0.0802706 0.00210276

    515 torr.

    2517 4.72041 1.23 9.80474 10.3065 6.59345 0.0747272 0.00102001

    507 torr.

    2516 4.74451 1.23 9.53598 9.99812 6.35487 0.0688805 0.000873339

    266 torr

    2515 4.41825 1.23 9.46317 9.91849 6.27052 0.06824 0.00078

    ure 3 torr.

    2514 4.55156 1.23 9.21638 9.62683 5.9756 0.0618537 0.00054667

    re 749 torr

    2513 4.61167 1.23 10.2039 10.7289 6.96307 0.0773472 0.00112001

    reference 3He data 3 energy runs from first pass to 5 pass, improve more than a factor of 2.

    2564 4.61776 1.23 10.0454 10.8125 7.48501 0.114647 0.00432

    2563 4.88235 1.23 10.9602 11.6051 7.14126 0.09366 0.00408667

    4005 10.8809 5.889 3.38005 4.23468 3.48439 0.192887 0.0104067

    3949 11.3533 5.889 3.31355 4.161 3.38478 0.189388 0.00950006

    3946 11.8713 5.889 3.30076 4.13643 3.37455 0.196387 0.01006

    3945 11.5341 5.889 3.30051 4.14206 3.37517 0.194193 0.00984

    2922 1.97366 2.396 7.11114 7.57777 6.48057 0.31718 0.00384667

    2921 1.99182 2.396 7.10596 7.54307 6.4787 0.318627 0.00374

    2920 1.81167 2.396 7.14193 7.58229 6.49638 0.29748 0.00372

    2919 1.9698 2.396 7.15823 7.56401 6.48512 0.311813 0.00342

    empty reference raster size change

    3x4 raster size

    4007 11.4213 5.889 2.76085 3.44538 2.51669 0.2132 0.0077526

    4006 10.5255 5.889 2.776 3.47252 2.51562 0.18469 0.00621703

    3929 4.89064 5.889 2.74376 3.40178 2.44653 0.186893 0.00352667

    3923 5.01379 5.889 2.93821 3.79588 2.6847 0.194133 0.00390667

    different beam position? slightly higher than above

    3541 1.86719 5.889 3.28279 3.75036 2.96604 0.232715 0.00299335

    3540 1.80735 5.889 3.21022 3.70337 2.91882 0.258592 0.00278288

    3539 1.8739 5.889 3.22734 3.72941 2.95936 0.264549 0.00266255

    3538 1.9824 5.889 3.17856 3.6735 2.83333 0.296809 0.0037938

    N2 in the cell

    3930 5.03349 5.889 3.7956 4.73739 4.03699 0.177433 0.00626624

    5*6.5 raster

    3927 1.89417 5.889 3.2603 4.21602 2.90328 0.00497952 0

    3926 1.95549 5.889 3.16921 4.15467 2.75569 0.0058361 6.68256e-05

    3925 1.96553 5.889 3.13285 4.07754 2.7371 0.00556575 2.03874e-05

    beam trip!!

    3542 1.82395 5.889 1.28077 1.28932 1.02121 0.0721667 0.000893333

    5x6

    3275 2.03877 5.889 5.40557 5.60552 3.50721 0.00624078 0.00020574

    4x5

    3273 1.98153 5.889 4.176 4.4487 3.01578 0.00455057 0

    2.5x3

    3271 1.66312 5.889 3.89525 4.11759 2.71481 0.00380458 1.67602e-05

    3270 1.965 5.889 3.85245 4.09403 2.8398 0.00456533 3.86892e-05

    3x4

    3268 2.03831 5.889 6.3187 6.94812 6.02927 0.013661 0.00082926

    2.5x3

    3267 2.19367 5.889 2.00874 2.14353 1.39417 0.00244494 0

    empty

    beam tune 2509 2.90436 1.23 16.4406 17.5463 12.5161 0.0217135 0.000260002

    2505 2.82326 1.23 17.859 19.0421 13.5373 0.0246203 0.000449236

    2x2

    2325 5.08008 1.23 4.2994 4.53177 2.56811 0.0265267 0

    2324 4.91173 1.23 4.30762 4.53365 2.5644 0.0248138 6.72097e-06

    2323 4.87545 1.23 4.35167 4.5812 2.59184 0.02644 0

    2322 5.08998 1.23 4.35943 4.58319 2.60349 0.0248 6.66667e-06

    2321 4.89342 1.23 4.36836 4.60076 2.62061 0.0247884 6.84763e-06

    2320 4.94491 1.23 4.36208 4.60392 2.62289 0.0262827 7.3109e-06

    2319 5.16267 1.23 4.33874 4.5735 2.61053 0.02582 0

    2318 5.25545 1.23 4.33154 4.57546 2.61615 0.0262562 0

    2317 5.19533 1.23 4.37278 4.60763 2.62919 0.05514 0

    2316 4.97971 1.23 4.39772 4.62156 2.64202 0.0537333 0

    2315 4.77045 1.23 4.41954 4.63722 2.6462 0.05356 2e-05

    real polarized 3He, the average rates is quite similar

    RUN 3556 is with new collimator and shielding. Compared with RUN 3021, the rates reduce by a bout 15%.

    3021 7.97504 5.9 4.68492 5.23143 4.5515 0.256623 0.0116291

    3556 8.28536 5.9 3.77395 4.4809 4.29501 0.204275 0.00916673

    3569 11.3584 5.9 3.65593 4.35755 4.02504 0.20616 0.01124

    3571 11.2944 5.9 3.65142 4.35109 4.0919 0.207993 0.0113867

    RUN 3541, 3542, 3543 is the empty referene cell, and 3544 is the 3He The background rates is about 80% of the 3He rates

    3541 1.86719 5.9 3.28279 3.75036 2.96604 0.232715 0.00299335

    3543 1.94121 5.9 3.18378 3.66135 2.88962 0.239073 0.00302

    3544 1.95769 5.9 3.97802 4.71563 4.52142 0.165533 0.00343333

    Background is very similar, by scanning the current

    3018 1.98209 5.9 5.03532 5.55658 4.83986 0.230573 0.0037012

    3019 3.69325 5.9 4.88407 5.40834 4.71405 0.234663 0.00590446

    3020 5.78568 5.9 4.76234 5.30384 4.62295 0.243494 0.00865559

    3021 7.97504 5.9 4.68492 5.23143 4.5515 0.256623 0.0116291

    3022 9.73255 5.9 4.63156 5.16448 4.52227 0.266201 0.0146022

    3023 9.71271 5.9 4.66147 5.22138 4.5366 0.262625 0.0154721

    different HV settings

    1600V

    3032 2.15946 5.9 5.04022 5.58662 4.84224 0.237825 0.00449471

    1650V

    3033 1.94897 5.9 5.84464 6.42662 5.44551 0.236422 0.00452348

    1700V

    3034 1.95179 5.9 7.03842 7.47304 6.28947 0.234326 0.00497759

    1700V

    3035 1.19218 5.9 7.37401 7.81979 6.57345 0.230152 0.00353357

    1650V

    3036 1.19131 5.9 6.03348 6.56762 5.62791 0.232815 0.00355174

    1600V

    3037 0.95790 5.9 5.32927 5.80697 5.04749 0.227772 0.00305459

    1550V

    3038 0.930574 5.9 4.60269 5.02584 4.38054 0.15725 0.00163984

    new polarized 3He cell

    4079 8 11.5111 3.53784 4.5189 4.21531 0.194212 0.0127401



    A copy of this log entry has been emailed to: jpchen@jlab.org,jiang@jlab.org