Polarimetry/H-jet/Run11: Difference between revisions

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(Created page with "= Final results (255 GeV) Note: These values have changed now that the full analysis is complete, and the A_N combined for all of the runs is used instead of the A_N measured fi...")
 
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= Final results (255 GeV)
= Final results (255 GeV) =


Note: These values have changed now that the full analysis is complete, and the A_N combined for all of the runs is used instead of the A_N measured fill-by-fill. The previous values were systematically incorrect, due to assumed Gaussian errors on the run-by-run A_N used in the denominator, which causes problems when the errors are large. In addition to using the combined A_N, these new results use a higher order calculation of the mean and standard deviation of the ratio of the asymmetries with respect to the beam and target (See http://www.stat.cmu.edu/~hseltman/files/ratio.pdf)
Note: These values have changed now that the full analysis is complete, and the A_N combined for all of the runs is used instead of the A_N measured fill-by-fill. The previous values were systematically incorrect, due to assumed Gaussian errors on the run-by-run A_N used in the denominator, which causes problems when the errors are large. In addition to using the combined A_N, these new results use a higher order calculation of the mean and standard deviation of the ratio of the asymmetries with respect to the beam and target (See http://www.stat.cmu.edu/~hseltman/files/ratio.pdf)
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15467    0.0443 +- 0.0011    0.4493 +- 0.0256    0.0434 +- 0.0014    0.3777 +- 0.0305
15467    0.0443 +- 0.0011    0.4493 +- 0.0256    0.0434 +- 0.0014    0.3777 +- 0.0305
15470    0.0437 +- 0.0013    0.4263 +- 0.0289    0.0444 +- 0.0014    0.4005 +- 0.0306
15470    0.0437 +- 0.0013    0.4263 +- 0.0289    0.0444 +- 0.0014    0.4005 +- 0.0306
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Latest revision as of 10:12, 10 February 2015

Final results (255 GeV)

Note: These values have changed now that the full analysis is complete, and the A_N combined for all of the runs is used instead of the A_N measured fill-by-fill. The previous values were systematically incorrect, due to assumed Gaussian errors on the run-by-run A_N used in the denominator, which causes problems when the errors are large. In addition to using the combined A_N, these new results use a higher order calculation of the mean and standard deviation of the ratio of the asymmetries with respect to the beam and target (See http://www.stat.cmu.edu/~hseltman/files/ratio.pdf) 

Fill      Y_AN                 Y_Pol                B_AN                 B_Pol        
15166     0.0446 +- 0.0015     0.4477 +- 0.0341     0.0439 +- 0.0015     0.4437 +- 0.0335
15170     0.0429 +- 0.0025     0.4099 +- 0.0558     0.0442 +- 0.0027     0.3721 +- 0.0601
15172     0.0453 +- 0.0017     0.4914 +- 0.0390     0.0432 +- 0.0016     0.4922 +- 0.0355
15173     0.0442 +- 0.0022     0.3976 +- 0.0497     0.0447 +- 0.0024     0.3440 +- 0.0526
15190     0.0479 +- 0.0018     0.5165 +- 0.0402     0.0442 +- 0.0019     0.4939 +- 0.0409
15196     0.0450 +- 0.0022     0.5891 +- 0.0487     0.0423 +- 0.0020     0.5161 +- 0.0443
15200     0.0478 +- 0.0035     0.5416 +- 0.0782     0.0461 +- 0.0033     0.6005 +- 0.0736
15202     0.0469 +- 0.0024     0.3876 +- 0.0530     0.0441 +- 0.0023     0.5305 +- 0.0501
15205     0.0506 +- 0.0029     0.6292 +- 0.0654     0.0491 +- 0.0030     0.4913 +- 0.0671
15207     0.0426 +- 0.0019     0.4464 +- 0.0417     0.0448 +- 0.0016     0.4451 +- 0.0349
15208     0.0449 +- 0.0042     0.6189 +- 0.0948     0.0347 +- 0.0042     0.4879 +- 0.0920
15210     0.0443 +- 0.0034     0.5487 +- 0.0749     0.0431 +- 0.0032     0.4603 +- 0.0695
15213     0.0405 +- 0.0022     0.5501 +- 0.0497     0.0447 +- 0.0023     0.4380 +- 0.0504
15233     0.0455 +- 0.0025     0.5240 +- 0.0551     0.0458 +- 0.0028     0.4719 +- 0.0629
15244     0.0434 +- 0.0022     0.5282 +- 0.0489     0.0428 +- 0.0022     0.4085 +- 0.0494
15249     0.0414 +- 0.0032     0.5113 +- 0.0720     0.0412 +- 0.0037     0.7391 +- 0.0819
15251     0.0431 +- 0.0045     0.5331 +- 0.0936     0.0456 +- 0.0044     0.5055 +- 0.0909
15254     0.0462 +- 0.0016     0.5175 +- 0.0366     0.0436 +- 0.0017     0.5936 +- 0.0383
15255     0.0442 +- 0.0015     0.5303 +- 0.0335     0.0420 +- 0.0016     0.4333 +- 0.0364
15256     0.0443 +- 0.0022     0.5627 +- 0.0489     0.0411 +- 0.0031     0.2828 +- 0.0683
15257     0.0466 +- 0.0019     0.4666 +- 0.0434     0.0442 +- 0.0021     0.5303 +- 0.0464
15283     0.0440 +- 0.0025     0.4597 +- 0.0560     0.0460 +- 0.0026     0.5461 +- 0.0565
15284     0.0423 +- 0.0018     0.4720 +- 0.0401     0.0413 +- 0.0024     0.5162 +- 0.0523
15287     0.0508 +- 0.0045     0.5993 +- 0.1013     0.0424 +- 0.0051     0.5310 +- 0.1133
15299     0.0446 +- 0.0018     0.5296 +- 0.0409     0.0442 +- 0.0021     0.3954 +- 0.0470
15314     0.0421 +- 0.0021     0.4458 +- 0.0461     0.0431 +- 0.0025     0.5112 +- 0.0550
15315     0.0416 +- 0.0028     0.4983 +- 0.0615     0.0365 +- 0.0031     0.4445 +- 0.0690
15316     0.0377 +- 0.0020     0.4447 +- 0.0442     0.0407 +- 0.0023     0.4465 +- 0.0484
15322     0.0425 +- 0.0018     0.5188 +- 0.0398     0.0457 +- 0.0016     0.5126 +- 0.0352
15324     0.0405 +- 0.0020     0.6186 +- 0.0449     0.0412 +- 0.0016     0.4655 +- 0.0343
15335     0.0451 +- 0.0013     0.5265 +- 0.0293     0.0423 +- 0.0015     0.5119 +- 0.0341
15337     0.0411 +- 0.0016     0.5530 +- 0.0358     0.0455 +- 0.0015     0.5089 +- 0.0335
15338     0.0409 +- 0.0018     0.4447 +- 0.0403     0.0419 +- 0.0019     0.5079 +- 0.0408
15356     0.0452 +- 0.0017     0.5354 +- 0.0372     0.0433 +- 0.0022     0.5192 +- 0.0479
15357     0.0462 +- 0.0037     0.4089 +- 0.0834     0.0469 +- 0.0043     0.4031 +- 0.0950
15363     0.0409 +- 0.0016     0.4485 +- 0.0361     0.0434 +- 0.0019     0.4079 +- 0.0421
15364     0.0395 +- 0.0018     0.4799 +- 0.0390     0.0433 +- 0.0016     0.5280 +- 0.0362
15365     0.0441 +- 0.0017     0.5227 +- 0.0381     0.0424 +- 0.0018     0.4897 +- 0.0401
15366     0.0445 +- 0.0023     0.4566 +- 0.0511     0.0466 +- 0.0020     0.4960 +- 0.0445
15368     0.0430 +- 0.0017     0.4757 +- 0.0384     0.0420 +- 0.0017     0.5770 +- 0.0371
15370     0.0449 +- 0.0034     0.6006 +- 0.0744     0.0442 +- 0.0031     0.4727 +- 0.0679
15372     0.0408 +- 0.0019     0.4675 +- 0.0427     0.0455 +- 0.0016     0.5061 +- 0.0347
15376     0.0461 +- 0.0017     0.4095 +- 0.0373     0.0430 +- 0.0015     0.4863 +- 0.0338
15378     0.0457 +- 0.0018     0.4029 +- 0.0394     0.0441 +- 0.0015     0.5029 +- 0.0335
15380     0.0450 +- 0.0018     0.4786 +- 0.0393     0.0429 +- 0.0016     0.5181 +- 0.0347
15381     0.0413 +- 0.0034     0.4459 +- 0.0768     0.0434 +- 0.0033     0.4886 +- 0.0736
15386     0.0407 +- 0.0014     0.4226 +- 0.0319     0.0433 +- 0.0015     0.4561 +- 0.0337
15390     0.0459 +- 0.0024     0.5260 +- 0.0556     0.0465 +- 0.0026     0.4805 +- 0.0577
15393     0.0461 +- 0.0014     0.4624 +- 0.0315     0.0404 +- 0.0017     0.3908 +- 0.0370
15397     0.0441 +- 0.0014     0.4008 +- 0.0325     0.0443 +- 0.0015     0.5187 +- 0.0327
15399     0.0418 +- 0.0014     0.4134 +- 0.0319     0.0437 +- 0.0012     0.4469 +- 0.0274
15402     0.0449 +- 0.0030     0.5126 +- 0.0678     0.0425 +- 0.0031     0.4470 +- 0.0693
15403     0.0413 +- 0.0025     0.6038 +- 0.0563     0.0392 +- 0.0025     0.3912 +- 0.0560
15425     0.0429 +- 0.0019     0.4256 +- 0.0430     0.0387 +- 0.0019     0.4420 +- 0.0409
15426     0.0391 +- 0.0027     0.4518 +- 0.0599     0.0417 +- 0.0025     0.5386 +- 0.0563
15427     0.0426 +- 0.0015     0.4750 +- 0.0327     0.0432 +- 0.0014     0.5069 +- 0.0305
15431     0.0452 +- 0.0025     0.5515 +- 0.0563     0.0451 +- 0.0026     0.4558 +- 0.0574
15435     0.0454 +- 0.0016     0.4342 +- 0.0365     0.0459 +- 0.0016     0.4982 +- 0.0358
15436     0.0429 +- 0.0013     0.4328 +- 0.0301     0.0452 +- 0.0013     0.4738 +- 0.0293
15438     0.0435 +- 0.0022     0.4510 +- 0.0499     0.0455 +- 0.0023     0.5637 +- 0.0506
15443     0.0457 +- 0.0014     0.5009 +- 0.0311     0.0448 +- 0.0014     0.5292 +- 0.0302
15452     0.0430 +- 0.0018     0.5279 +- 0.0387     0.0458 +- 0.0019     0.5097 +- 0.0412
15466     0.0484 +- 0.0049     0.5127 +- 0.1090     0.0374 +- 0.0053     0.3861 +- 0.1154
15467     0.0443 +- 0.0011     0.4493 +- 0.0256     0.0434 +- 0.0014     0.3777 +- 0.0305
15470     0.0437 +- 0.0013     0.4263 +- 0.0289     0.0444 +- 0.0014     0.4005 +- 0.0306
Blue beam polarization measured by jet Yellow beam polarization measured by jet
Blue beam, 250 GeV Yellow beam, 250 GeV


beam polarization measured by jet

blue points: blue beam pol., red points: yellow beam pol.


A_N measured by jet

Black points: preliminary run 11 results. Red points: run 9 results


Run11 polarization at injection energy

runs with both beams: 

Y_Pol              B_Pol
0.70 +- 0.038      0.60 +- 0.037

runs with blue beam only: 

B_Pol
0.54 +- 0.034


Ratio of jet to pC, split by blue/yellow beam and upstream/downstream detector and by target used

  • pC/jet ratios - pdf


Polarization by fill for timeslices around the center of the banana plot

As usual, the red points are for the yellow beam, and blue points are for the blue beam

yellow beam blue beam

yellow beam, -3 to -1 ns yellow beam, -1 to 1 ns yellow beam, 1 to 3 ns blue beam, -3 to -1 ns blue beam, -1 to 1 ns blue beam, 1 to 3 ns


Polarization by 2-hour time period in fill

red points for yellow beam, blue for blue Decay.png


Last modified by Oleg on 10-02-2015

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