Trigger Criteria for Level 1

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Trigger Criteria for Level 1 Joel Butler

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Trigger Criteria for Level 1. Joel Butler. Objective. The use of the requirement of “N” detached tracks EACH with impact parameter greater then “M” standard deviations as the Level 1 requirement has been with us from the earliest days of the Level 1 Trigger development - PowerPoint PPT Presentation

Transcript of Trigger Criteria for Level 1

Page 1: Trigger Criteria for Level 1

Trigger Criteria for Level 1

Joel Butler

Page 2: Trigger Criteria for Level 1

Objective• The use of the requirement of “N” detached tracks

EACH with impact parameter greater then “M” standard deviations as the Level 1 requirement has been with us from the earliest days of the Level 1 Trigger development

• It is natural to ask whether – Some other criteria would have somewhat improved

efficiency. Possible gains are small for B’s but potentially large for charm where efficiency is low

– What effect this trigger criteria has on the proper time distribution (an effect of the current trigger first observed by Harry Cheung) and whether some other criteria would have a smaller effect.

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Game Plan

• Study the effect on the efficiency and proper time distribution for our usual trigger for “typical states” of B and charm decay

• Study alternatives

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Trigger Efficiency B-->D* for Final Signal Events

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Trigger Efficiency for B-->D* for all signal events

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Level 1 Trigger Efficiency

For generated minbias:

Upper left: 300 MeV/c

Upper right: 500 MeV/c

Lower left: 700 MeVc

NormalTrigger

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Proper time for B-->D*

Affect of proper timeResolution seen clearlyIn untriggered curve to1 ps and to triggeredthrough whole distribution

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Reduced proper time for B-->D*’ = - Nwhere N is the L/ cut

It means you start thedecay clock after N. This works only if doesnot depend on . This is useful for lifetimemeasurements but not formixing where the interactionstarts the clock.The lifetime fit with no trigger

Is very close to the MC value.

Notrigger

L1Trigger

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Fit Results

The result of the fit to the “untriggered” ’ distribution: 1.67ps

The result of the fit to the “triggered” ’ distribution: 1.98ps

The uncertainty is about 0.02. One can probably do a bit betterBy tailoring the ranges, but the f(’) will still not be flat.

Nothing here is fatal but it would be very good to improve the situation

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Conclusion from B study

• The trigger affects the time distribution requiring “f()” corrections. These are always subject to complaint and should be kept as small as possible

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Charm Study

• Study undertaken with directly produced Do--> K.

• Used a “candidate driven” algorithm to build the primary vertex for each candidate D. This is the first time I have a completely “unprompted” analysis. Valid only for all charged final states

• Consider also Pt cut on “detached” candidates

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Level 1 Trigger Efficiency

For generated CCBAR:

Upper left: 300 MeV/c

Upper right: 500 MeV/c

Lower left: 700 MeVc

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Level 1 Trigger Efficiency

For generated D0-->K:

Upper left: 300 MeV/c

Upper right: 500 MeV/c

Lower left: 700 MeVc

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Charm

• Pt cuts cause less trouble than I would have imagined

• The “standard” trigger has an efficiency of around 10%, which is not bad. Roughly, speaking, the “effective” charm luminosity is 15-20% of the B luminosity

• Improvements would be welcome

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In progress

• Change trigger criteria– Require two tracks each with M>3– Require sum of normalized detachment squared

greater than some number, like 72 (2X62) and then explore from there

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Sum of normalized impact parameters

squared for all detached tracks associated with

each primary

Each track must have at least 3 , which for two tracksgives 9, so a sum of 18 min isalready required