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  • 8/18/2019 Coherent Noise Task Update

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    Study of Coherent Noise in SiliconStrip Detector at CMS

     

     Atiq ur RahmanDr. Ashfaq Ahmad

      National Centre for Physics, Islamabad

    4/2/16 1Coherent Noise Task 

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    Motivation

    Frameor!

    Measurement of Noise

    Parameteri"ation of coherent noise

    Conclusion

    4/2/16 2Coherent Noise Task 

    Outlines

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    CMS Tracker overview

    4/2/16 Coherent Noise Task  4

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    Module %y&es

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    Motivation

      %o measure coherent noise in silicon stri& detector at

    CM$.

      Develo& a criteria'method to fla( noisy modules in

    $ilicon $tri& %rac!er.

      %he corrections derived is intended to be used durin(trac! reconstruction

      )ould reduce the chance of reconstruction of noisy

    clusters and hel& to (et more &recise A#D data for

    so&histicated analysis.

    64/2/16 Coherent Noise Task 

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    *sin( CM$$)++-+-/&atch D0M and $i$tri& &ac!a(es

    Root

    Identification criteria

    Fec1crate'slot'rin('CC*'M#D*23'22D'I-C etc .

    4''-'56'-'7 vs DetID

    Data1 Pedestal Run

    4/2/16 7Coherent Noise Task 

    Framework

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    Normali"ed Noise difference

    Normali"ed noise difference is assumed to have

    a nominal value hen there is no correlated

    noise and &oints deviatin( from this line are

    considered to be in correlation or anti/correlation

    as a first test.

    =  

    4/2/16 10Coherent Noise Task 

    Noise Calculation Cont!

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    Noise Modes

    De&endin( u&on the different trends of noises

    hich e encounter in $ilicon stri& trac!er, edefine noise modes

    Normal mode

    )in( sus&ect Dead or lo noise mode

    )eird mode

    Normal is one hich is normal trend in trac!er,

    in( mode is >in( ? sha&ed noise trend , Dead

    mode is none res&ondin( and havin( "ero noise

    mode

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    Normal Mode

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    Correlation coefficients for normal mode

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     "in# Mode

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      Correlation Plots for "in# Mode

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    Paraolic or $uadratic fit

    $i"e of >A? decide hether the &arabola is ideor narro.

    Positive >A? shos it is u&ard.

    >@? is the (eneral slo&e in equation of line.

    >C? shift in the &arabola i.e u& or don

    minB/:@'-A;

    minB/

    :min, min; is verte of the &arabolas

    =  

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    Parameteri%ation of correlations coefficients

    4/2/16 17Coherent Noise Task 

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    Map for Parameter &

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    Map for the Parameter '

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    Map for +)min*

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     ()min* vs &

    Only the large value of A do not ensure that thechannel will have large correlation. TheParameter “C” play a decisive role in additionto A . We deicide about the correlated channelwith only !min" not with C or A individually.4/2/16 23Coherent Noise Task 

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     ()min* vs +)min*

    Lager values of !"in# is not hurting

    our results4/2/16 24Coherent Noise Task 

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    & vs +)min*

    All the channels having large value of A parameteralways lies in Physical range of the AP#. $o weshould not worry about the non%physical strips.&asically ' such channels have a almost linear

    distribution of correlation coe(cients. That is why weare ettin the lar e )!min".4/2/16 25Coherent Noise Task 

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    +)min* vs C

    All the anomalous values of the parametersmostly coming in the Physical range of AP#

    $trips.4/2/16 28Coherent Noise Task 

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    Channels in the tail of !min" after the chi%$*uare cut As we have very small windowfor y!min" in the distribution !min"+%.,-

    Channels in the %ails of :min; for 2eft+fit

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    Channels in the Tails of ()min* for ,eft fit

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    Channels in the Tails of ()min* for ,eft-fit

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    Channels in the tails of ()min* for ,eft fit

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    C a e s t e ta s o ) * o e t- t

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    Channels in the tails of ()min* for ,eft fit

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    Channels in the tails of ()min* for ,eft-fit

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    $olution to nois% an& &ea& 'hannel (ro)le"

    As we were getting the noisy as well as thecorrelated channels in the tails of the y!min"which were contaminating our results forcorrelated channels. have /agged the noisy or

    dead strips as not 0tted to our general*uadratic!as well linear model". We haveobtained the distribution of chi s*uare and got agood cut for channels.

    n rest of the channels we get only correlatedchannels in the tails of !min".

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    Chi s*uare &istri)ution )efore an&

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    Chi s*uare &istri)ution )efore an&after 'ut

    12

    The 'hannels in the tail of Left Chi+$*uare)efore the 'ut are (resente& in later sli&es, -t'an .ag even a s"all "issing of stri(s

    4/2/16 35Coherent Noise Task 

    e c anne s n e a s o e %

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    e c anne s n e a s o e $*uare

     we have got almost all the noisy and deadchannels in the tails of chi%s*uare which were in

    the tail of the !min" before the chi%s*uare cut. The Chi s*uare de0nition is highly sensitive forthe channels which have small number of noisystrips.

     The *uadratic 0t model is a general 0t and linear0t is a special case of *uadratic 0t with parameter“A” e*ual to 3ero.

    All the non%Physical )!min" have nominal valuesof parameter A and !min". They do not hurt ourresults. This indicate that they have astonishinglylinear distribution of correlation coe(cients.

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    M f Chi S

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    Map for Chi.S$uare

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    Channels in the tails of chi.S$uare for

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    16

    Channels in the tails of chi S$uare for

    ,eft-fit

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    Channels in the tails of chi/$quare for 2eft+fit

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    174/2/16 39Coherent Noise Task 

    Channels in the tails of chi.S$uare for ,eft-fit

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    89

    $ -

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    Staility of the ()min* in SST TI'

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    y ) *

    Does this y:min; is stable in the other $ub detectorsE

    TI'

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    T0C1

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    T0C

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    TO'

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    TO'

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    Conclusions

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    Conclusions

    %he :min; is used to decide about the correlation of the channels. No

    any individual &arameter can be used to quantify the correlation. >A? and

    >C? are both sensitive but lar(e value of >A? may not decide that thischannel is sensitive for correlation. $imilarly , the only value of >C? do

    not ensure us about correlation only.

    @ut in the case of terribly linear distribution of correlation coefficients, e

    can say that the >C? &arameter becomes same as :min;.

    %he chi/$quare value for the quadratic fit (ives a (ood criteria to

    eliminate the noisy channels. %he channels hose chi/square value for

    the quadratic fit is (reater than to are all noisy.

    %he values of :min; ill be used for fine tune of cluster char(e.

    %his criteria can be used to correct the CM$ data and can reduce the

    chance of noisy clusters. ere is our ti!i &a(e htt&s

    1''ti!i.cern.ch'ti!i'bin'vieauth'CM$'$i$tri&NoiseCorrelation

    https://twiki.cern.ch/twiki/bin/viewauth/CMS/SiStripNoiseCorrelationhttps://twiki.cern.ch/twiki/bin/viewauth/CMS/SiStripNoiseCorrelationhttps://twiki.cern.ch/twiki/bin/viewauth/CMS/SiStripNoiseCorrelationhttps://twiki.cern.ch/twiki/bin/viewauth/CMS/SiStripNoiseCorrelation