t585 analysis status 3

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T585 analysis status 3 2006/2/2 HIDEYUKI SAKAMOTO Contents On small light yield problem checked by Aron’s i nformation • Tracking status • Transverse and Longitudinal momentum dis tribution • Comparison of DATA with MC • Photo electron distribution • Next to do

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T585 analysis status 3. Contents On small light yield problem checked by Aron’s information Tracking status Transverse and Longitudinal momentum distribution Comparison of DATA with MC Photo electron distribution Next to do. 2006/2/2 HIDEYUKI SAKAMOTO. - PowerPoint PPT Presentation

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T585 analysis status 32006/2/2

HIDEYUKI SAKAMOTO

Contents• On small light yield problem checked by Aron’s information

• Tracking status

• Transverse and Longitudinal momentum distribution

• Comparison of DATA with MC

• Photo electron distribution

• Next to do

P.E as a function of waveguide

This shows that

The problem has also at station side .

From Aron’s check

Track reconstruction -- This is last talk• Based on Uniform B-Field and NO scattering• Chi2 to be minimized

– Input: xi,yi, i=1,4– Output: x0,y0,p0,R,L– Degree of freedom: 8-5=3

2

2fiti

2

2fiti

i

2 )y(y)x(x

]/LRcos[zxx 0ifit 0

/(0.3B)p R T

/(0.3B)p L L

]/L[zRsin yy 0ifit 0 x0, y0

0

#4#3

#2

#1R

Checking of tool -- This is last talk• Input = hit position by GEANT

Vertical: residual (%)

Horizontal: fit parameters

Transverse momentum (pt)

Longitudinal momentum (pz)

MC v.s. reconstructed pt & pz-- This is last talk

MC

Reconst.

Why is Reconst. longitudinal momentum so broad?

•Bug?

•Effect of scattering?

NOW checking this.

Broadness of fitted Pz

• This problem occurs when turning angle, becomes small– z L -1 = z 0.3 B Pz -1 – Small Small B or Large Pz

• In MICE– B=4T,Pz=200MeV/c L=17cm => (z=1m)=337d

eg <= NO Problem

• In T585– B=1T,Pz=400MeV/c..etc.. 1/8 times as MICE=42deg– For analysis, using TOF for Pz reconstruction

#1

#2

#3#4

Event display – MC –

x=0

True

With x

Fitted

Pz=416MeV/c

z=95cm)=39 deg

UpdatedSetup of fiber sheet for MC• Scifi.

– Diameter=350um=>(#)core:350umx94%=>(#)clad:350umx6%

– Pitch=420um– Distance=280um– Material=scinti.

=>(#)core:scinti.(Polythylene)=>(#)clad:PMMA

(#) from Kuraray catalogue• View

– Distance=0.63mm– Material=Air

=> polyurethane adhesive(PSILRA1000) (temporary)

• Mylar– Thickness=25um– Material=(Polyethylene terephthalate) [C10

H8]n

0.4

2m

m0.3

5m

m0.2

8

mm

0.63mm+25um

Sta

tion

Bod

yMylar

X W V

Filled withAdhesive

Difference for View material

There is no significant difference because input momentum is 3GeV/c pion, MIPS

Deposit energy

E1

E2

E3

E4

E5

E4+ E5

E1, E2

E3

E1+E2

E4+ E5

E4+ E5E3

E3

3GeV/c pion

L1A cut

L1A & residue

cut

Photo electron distribution –DATA—

Timing(L1A) Residual

cm

RUN#1255

STATION1

X-VIEW

!! NO CLUSTERING

DATA

Photo electron distribution – MC–

Distributed by POISSON and Gausian

Calibrated by eye (w/o fit)

MC

MCDATA

Station 1 X-VIEW (with Adhesive and Mylar)

!! NO CLUSTERING

Next to do

• Mapping– stopped for while..+My Request (as said e-mail to Aron)“Checking scifi alignment with my modified list”, making after checking by beam DATA.

• Tracking– Reconstruction using TOF for T585 analysis– Estimating errors of reconst. Momentums

• ADC distribution– Including “clustering”– Adjusting : Eye => Fitting