study of anti-quark flavor asymmetric via e906
DESCRIPTION
Study of anti-quark flavor asymmetric via E906. Shiuan-Hal Shiu 2009/7/13. Contents. Introduction Hardware operation Fast Monte Carlo simulation Future work. Introduction. Is in the proton?. ?. Proton is composed of three valence quark,gluons and sea - PowerPoint PPT PresentationTRANSCRIPT
Study of anti-quark flavor asymmetric via E906
Shiuan-Hal Shiu 2009/7/13
1
ContentsContents Introduction
Hardware operation
Fast Monte Carlo simulation
Future work
2
3
Proton is composed of three valence quark,gluons and sea
By contrast with other quarks, the up and down quark are very similar.
Because of the similarity, anti-down and anti-up quark distributions in the proton are assumed to be equal.
Is this true……? 4
?
ud
Is in the proton? Is in the proton? du
=
5
Light Antiquark Flavor Light Antiquark Flavor Asymmetry: Brief HistoryAsymmetry: Brief History
Naïve Assumption:
This is a common assumption until
1991
X
6
Light Antiquark Flavor Light Antiquark Flavor Asymmetry: Brief HistoryAsymmetry: Brief History
Naïve Assumption:
Gottfried Sum Rule:
1
2 20
1
0
[( ( ) ( )) / ]
1 2( ( ) ( ))
3 3
( )1
3 p p
p nG
p p
S F x F x x dx
u x d
i
x dx
f u d
New Muon Collaboration (NMC)
, Phys. Rev. D50 (1994) R1
SG = 0.235 ± 0.026
( Significantly lower than 1/3 ! )
xdxxFxF np /1
0 22
7
Light Antiquark Flavor Light Antiquark Flavor Asymmetry: Brief HistoryAsymmetry: Brief History
Naïve Assumption:
Gottfried Sum Rule:
NA51 (Drell-Yan) NA 51 Drell-Yan confirms
d-bar(x) > u-bar(x)
8
Light Antiquark Flavor Light Antiquark Flavor Asymmetry: Brief HistoryAsymmetry: Brief History
Naïve Assumption:
Gottfried Sum Rule:
NA51 (Drell-Yan)
E866/NuSea (Drell-Yan)
E866 ExperimentE866 Experiment The cross section of Drell-Yan process is
Here q1, q2 are the beam, target quark distribution.
Detector acceptance chooses xtarget and xbeam.
9
221122112
21
2
21
2 1
9
4xqxqxqxqe
sxxdxdx
d
xtarget xbeam Xbeam
Xta
rget
u
dud
E866 ExperimentE866 Experiment
10
Cryogenic Target System
Station1
Station2
Station3
SM3 Analyzing Magnet
Hadronic Calorimeter
ElectromagneticCalorime
ter
SM12 Analyzing Magnet
Hadron absorb
er
Ring-Imaging Cherenkov
CounterMuon
Detectors
2
212
1
221
xu
xd
xx
pp
pd
E866 use hydrogen and deuterium target
E866 ExperimentE866 Experiment
11
12
Advantages of 120 GeV Main Advantages of 120 GeV Main InjectorInjector
The past: Fermilab E866/NuSeaFermilab E866/NuSea
Data in 1996-1997 1H, 2H, and nuclear targets 800 GeV proton beam
The future: Fermilab E906Fermilab E906
Data in 2009 1H, 2H, and nuclear targets 120 GeV proton Beam
Fixed Target
Beam lines
Tevatron 800 GeV
Main Injector
120 GeV
221122112
21
2
21
2 1
9
4xqxqxqxqe
sxxdxdx
d
13
Follow basic design of MEast spectrometer :
Where possible and practical, reuse elements of the E866 spectrometer. Tracking chamber electronics Hadron absorber, beam dump, muon ID walls Station 2 and 3 tracking chambers Hodoscope array PMT’s SM3 Magnet
– Two magnet spectrometer – Hadron absorber within first magnet
– Beam dump within first Magnet – Muon-ID wall before final elements
New Elements– 1st magnet (different boost)
– Sta. 1 tracking (rates)
– Scintillator (age)
– Trigger (flexibility)
E866 Meson East Spectrometer
14
256 Hodoscopes
MWPC 5500 Channels
Station 2 & 3Drift Chambers1700 ChannelsMulti-hit TDC’s
Station 4 PropTubes 400 Channels
E906 Spectrometer: Bend Plane E906 Spectrometer: Bend Plane ViewView
Target
M1
M2
Sta.1
Sta
.2
Sta
.3
Sta
.4 M
uon
ID w
all
Measurements with the Drell-Yan Measurements with the Drell-Yan processprocess
Fermilab E906/Drell-Yan will extend these measurements and reduce statistical uncertainty.
E906 expects systematic uncertainty to remain at approx. 1% in cross section ratio.
15
2
212
1
221
xu
xd
xx
pp
pd
16
What is CODA?What is CODA? CODA (CEBAF Online Data Acquisition) is a
software DAQ system.
17VME
EB ET ER
User proc.
Disk
cMsg
RC platform
RUN control GUI
Log messag
e
NetworkEthernet
VME
Single board computer
ROC
ROC
msqld
cMlog DataBa
se
mSQL DataBa
se
TranslateTypical system
chart
COMPUTER
The CODA control panelThe CODA control panel
18
RCPlatform
MSQL Daemon
Event Transfersystem
EBe906
ERe906
GUI
Conceptual design of DAQ based Conceptual design of DAQ based on CODAon CODA
19
Unix host running CODA
Ethernet Hub
Data Storage
Online monitoring
Data Decoder Software
MWPC, HODO, Muon
Coincidence Register System, VME
CAMAC TDC for DC
Interface to VME
Accelerator scalers, VME?
Electronics House
Counting House
ROC1ROC2ROC3
L2 Trigger
CODA toolsCODA tools
20
ROCe906roc1
Ebe906daq2
ERe906daq2
CODA file
CODA toolsCODA tools Dbedit: can edit the information of database
21
CODA toolsCODA tools Xcefdmp:
event monitoring software.
22
View File modeOffline
monitoring
Spy Event modeOnline
monitoring
Installation of CODAInstallation of CODA 1. Setup a user account with the proper environment.
2. Setup the CODA database.
3. Setup MVME6100.
4. Transfer the ROC to a DAQ crate by downloading the KERNAL and CODA_ROC program on MVME6100.
5. Add a trigger supervisor.
6. Add more VME module.
23
Hardware configuration in IPASHardware configuration in IPAS
24
MVME6100Single board computer
SIS3610Trigger
supervisor
SIS3600Multi
eventsLatch
Trigger supervisor and latch Trigger supervisor and latch modulemodule
Latch module(SIS3600): When this module received
a trigger, it will capture the signal pattern from the input channel
Will not send any interrupt to single board computer
Trigger supervisor(SIS3610): When this module were
triggered it will send an interrupt to single board computer
25
CONTROL I/O
32 Data
Channl
SIS3600
Use .crl file to control CODAUse .crl file to control CODA
Most of the components in a CODA system are pre-defined by CODA and only require configuring
We can easily write CRL code to control CODA.
26
Booted
Configured
Download
Paused Actived
Terminated
Create
Configure
Configure
Prestart
download
Pause
GO
End
Terminate
Control the SIS3600Control the SIS3600 Functions of SIS3610 is well supported in
CODA, but SIS3600 is not. In order to control the SIS3600 we need to
write the driver which compatible with CODA. I consult the driver of SIS3610 and the manual
of SIS3600 to write a driver for SIS3600. By checking the input pattern, the SIS3600
can work correctly.
27
… 1000… 00011000 …
28
About the fast monte carlo About the fast monte carlo simulationsimulation
Base on Fortran language. Modified version of E866/E772 “fast” Monte Carlo
Code to include E906 geometry. Only traces dimuon from Drell-Yan events, and the
decays of J/. Have 2 main parts 1. Muon pair creation2. Detector Magnetic field is simplified, but muon energy loss
and multiple scattering are included.
29
WantWantOriginal
We want to observe events of low We want to observe events of low massmass
30
Mass (GeV)
Mass (GeV)
acce
ptan
ce ac
cept
anc
e
The mass and the magnet currentThe mass and the magnet current
31
M1
M2
32
The mass and the magnet currentThe mass and the magnet current
M1
M2
33
The mass and the magnet currentThe mass and the magnet current
M1
M2
34
The mass and the magnet currentThe mass and the magnet current
M1
M2
Configure M1 and M2Configure M1 and M2
Configuration file
35
M1M1M2M2
How to obtain the acceptanceHow to obtain the acceptance The top diagram is
the mass distribution of generated dimuon pairs.
The middle diagram is the mass distribution of reconstructed dimuon pairs.
The bottom diagram “Acceptance” as a function of dimuon mass. 36
Thrown
Reconstruction
Acceptance
Acc
epta
nce
Cou
nts
Cou
nts
GeV
GevGeV
GeV
The result of varying M1 The result of varying M1 currentcurrent
The mass region of generated dimuon pairs is from 1Gev to 15Gev
Green line is the acceptance value with the original M1 current setting.
By increasing the current we find that the peak of acceptance is shifting to high mass end.
Reducing the M1 current can increase the acceptance in the low-mass region.37
M1x0.1
M1x0.5
M1x1.0
M1x1.5
M1x2.0
GeV
Acc
epta
nce
FIX M1*1.5 varying M2FIX M1*1.5 varying M2
M2*1.5 M2*1 M2*0.5
38
Reconstruction
Thrown
M2x0.5
M2x1.0
M2x1.5
Acc
epta
nce
Cou
nts
Cou
nts
GeV GeV GeV
Acc
epta
nce
GeV
Reconstruction
Reconstruction
Thrown Thrown
Acceptance
Acceptance
Acceptance
M2*1.5 M2*1 M2*0.5
39
FIX M1*1 varying M2FIX M1*1 varying M2
M2x0.5
M2x1.0
M2x1.5
GeV GeV GeV
Acc
epta
nce
Cou
nts
Cou
nts
Acc
epta
nce
GeV
Reconstruction
Thrown
Reconstruction
Reconstruction
Thrown Thrown
Acceptance
Acceptance
Acceptance
M2*1.5 M2*1 M2*0.5
40
FIX M1*0.1 varying M2FIX M1*0.1 varying M2
M2x0.5
M2x1.0
M2x1.5
GeV GeV GeV
Acc
epta
nce
Cou
nts
Cou
nts
Acc
epta
nce
GeV
Reconstruction
Thrown
Reconstruction
Reconstruction
Thrown Thrown
Acceptance
Acceptance
Acceptance
Conclusion Reducing the M1 current can increase the
acceptance of low mass region dimuons.
Adjusting the M2 current does not change the acceptance region significantly.
Howerer, adjusting M2 current can change the acceptance.
41
Dump/Target separationDump/Target separationM1x1M1x1
Software cuts conditionsPurple: all events
Green: xF>0 and M>4.5 GeV and pz>20 GeV
Blue: Green and |ytrack|>2.25 in at z=0 (zdump)
Red: Blue and |ytrack|<10.0 in at z=-60 (zstart)
42
Thrown
Count
sC
ounts
Reconstruction
ZTarge
tTarge
tDum
pDum
p
Dump/Target separationDump/Target separation
43
Thrown
Reconstruction
Z
Count
sC
ount
s
Thrown
Reconstruction
Z
Count
sC
ount
s
M1x0.5M1x0.5 M1x0.1M1x0.1
Mass cut > 4.5
Dump/Target separationDump/Target separation
44
Thrown
Reconstruction
Z
Count
sC
ount
s
Thrown
Reconstruction
Z
Count
sC
ount
s
M1x0.5M1x0.5 M1x0.1M1x0.1
Mass cut < 4.5
Dump/Target separationDump/Target separationM1x0.5M1x0.5
45
Counts
Counts
Counts
Counts
ZZ
Z Z
1
2
3
4
Counts
Counts
Counts
Counts
No cut
Z
Z Z
Z
Green+
Y(zdump)>2.25
Xf>0Retrace M<4.5Pz>10
Blue+
Y(zstart)>10
1
2
3
4
Mass cut < 4.5
Reducing the M1 current will lead the z resolution worse.
Dump/Target separationDump/Target separationM1x0.1M1x0.1
46
Counts
Counts
Counts
Counts
No cut
Z 1
Z Z
Z
2
3
4
Green+
Y(zdump)>2.25
Xf>0Retrace M<4.5Pz>10
Blue+
Y(zstart)>10
Mass cut < 4.5
Change the target locationChange the target location
47
50 inche
s
Change the target locationChange the target location
48
130 inche
s
Change the target locationChange the target location
1
2
3
4
M1*0.5
49
Counts
Counts
Counts
Counts
Z
Z Z
Z
No cutGreen
+Y(zdump)>2.
25
Blue+
Y(zstart)>10
Xf>0Retrace M<4.5Pz>10
1
2
3
4
Mass cut < 4.5
Change the target locationChange the target location
1
2
3
4
M1*0.1
Changing target location can slightly improve the z resolution.50
Counts
Counts
Counts
Counts
Z
Z Z
Z
No cut
Green+
Y(zdump)>2.25
Blue+
Y(zstart)>10Xf>0Retrace M<4.5Pz>10
1
2
3
4
Mass cut < 4.5
Check the relations of retrace Check the relations of retrace mass and retrace zmass and retrace z After applied the
cut(mass >4.5 Gev) , we can see that the events are almost spread in the region which less than z=0.
51
18
Z(inches)
161412108
6
4
2
00
-20
-60
-80
-40
-100
20
40
60
100
80
mass
(GeV
) M1x1M1x1
Check the relations of retrace Check the relations of retrace mass and retrace zmass and retrace z
After applied the cut (mass <4.5 Gev), we can see that the events are still scattered throughout the x axis.
52
M1x0.5M1x0.518
Z(inches)
161412108
6
4
2
00
-20
-60
-80
-40
-100
20
40
60
100
80
mass
(GeV
)
Check the relations of retrace Check the relations of retrace mass and retrace zmass and retrace z
53
18
Z(inches)
161412108
6
4
2
00
-20
-60
-80
-40
-100
20
40
60
100
80
mass
(GeV
) M1x0.1M1x0.1
Conclusion Conclusion
After reducing the M1 current, more and more events can not get a correct retraced Z value.
Changing target location can slightly improve the Dump/Target separation rate.
Low mass events are affected by the multiple scattering seriously.
Low mass events generally have small opening angle, this will increase the difficulty to retrace the Z position.
54
55
Drell-Yan decay angular Drell-Yan decay angular distributionsdistributions
A general expression for Drell-Yan decay angular distributions:
2 21 31 cos sin 2 cos sin cos 2
4 2
d
d
Production plane
Decay plane
Collins-Soper frame is defined in dimuon CMS.
The Z-axis is the bisector of Pbeam and –Ptarget .
Θ is the angle between Pμ+ and Z-axis .
Φ is the angle between production plane and decay plane .
Pbea
m
Ptarge
t
Y
X
Z
Pμ+
Angular distribution reconstructAngular distribution reconstruct The top diagram
is the cosΘ distribution of generated events.
The middle diagram is the reconstructed cosΘ.
The bottom diagram “Acceptance” is obtained by
56
Counts
Counts
Counts
Counts
Acc
epta
nce
Thrown
Reconstruction
Acceptance
cosΘ (cs)
thrown
tionreconstrucacceptance
Testing the fast monte carlo Testing the fast monte carlo simulation programsimulation program Thrown a
shape angular distribution.
Fit the reconstruction data using function:
Check the fitting result λ within error bar is consist with the input value or not.
57
)(cos1 2
Counts
Thrown
cosΘ (cs)
)(cos1 2
acceptance))(cos1( 2
Monte carlo data fitting resultMonte carlo data fitting result
58
)(cos5.01 2 )(cos11 2 cosΘ (cs)
cosΘ (cs)Input function : Input function :
λ=0.687958Err=0.10103
3
λ=0.924215Err=0.0954
346
Monte carlo data fitting resultMonte carlo data fitting result
59)(cos31 2 )(cos21 2 Input function :Input function :
cosΘ (cs)
cosΘ (cs)
λ=1.50516Err=0.125
602
λ=2.34244Err=0.1655
32
ConclusionConclusion The fitting in the case λ=1 is successful, but
fails in the other case.
I will spend more time to checking the fitting program and fast monte carlo program to find out why the fitting fails.
Finally, the goal is adding the φ angular distribution to study the θ and φ acceptance and resolutions for the J/Psi and D-Y events.
60
61
62
Timeline of E906Timeline of E906
2002: E906 Approved by Fermilab PAC 2006: E906 funded by DOE Nuclear Physics 2008, Dec: Stage-II approval by Fermilab Director and
MOU between Fermilab and E906 Collaboration finalized. Construction and installation of spectrometer and readout
electronics to be done in 2009 and upper half of 2010. First beam expected in the fall of 2010!
Man PowerMan Power Institute of Physics, Academia Sinica (IPAS):
Wen-Chen Chang, Ping-Kun Teng, Yen-Chu Chen (stationed at FNAL), Da-Shung Su (engineer)
Shiuan-Hal Shiu (Ph.D. student, preparing his proposal and plan to go to work with Ron Gilman on level-2 trigger afterwards.)
Bo-Ru Lin (research assistant, leaving the group in July and joining Colorado group as Ph.D. student.)
Jia-Ye Chen (Expect to work as postdoc next summer.) Ling-Tung University (LTU):
Ting-Hua Chang Summer-study students: will help on the mass production of
electronics. There are people from “National Kaohsiung Normal
University” (NKNU) who wish to join E906 experiment: Rurng-Sheng Guo (member of FNAL E665 and CDF Collaboration) Su-Yin Wang (Ph.D. student in NKNU, under the supervision of
Rurng-Sheng Guo)
63
Responsibility of Taiwan groupResponsibility of Taiwan group
Build 400 preamplifier-discriminators cards (6400 channels in total) for 5500 tracking channels in Station 1 MWPC and for 400 channels Proportional tubes in Station 4,
Build the readout system for Coincidence Registers (CR), which consists of 110 CR modules (7040 channels in total) for 5500 tracking channels in Station 1 MWPC, for 400 channels of Proportional tubes in Station 4, and for 320 channels of hodoscope planes in all stations,
Participate in the LVL2-Trigger project – two CEAN V1495 FPGA logic units purchased and one Ph.D. student will be available in fall to work on this project.
64
preamplifier-discriminators cardspreamplifier-discriminators cards
65
16
ch
EC
L i
np
uts
16
ch
EC
L i
np
uts
VME Backplane
NIM/ECL ↔ TTL
A24
~A
31
D16
~D
31
Eth
ern
et
10/1
00M
bp
sARM processorAT91SAM9260
64
ch
EC
L t
o T
TL
[2
]
Front panel
TransceiverDM9161
Deb
ug
U
AR
T
COM port
JTAG-ICE
16
ch
EC
L i
np
uts
FPGAActel A3P-1000
VM
E b
us
P1
VM
E b
us
P2
2ch
NIM
I/O
64MB SDRAM
256MB x 16 NAND Flash [5]
Bu
s b
uff
er
x5
[6
]B
us
bu
ffe
r x
3 [
6]
A01
~A
23,
D0~
D15
, D
S, A
S, W
rite
, DT
AC
K
Trigger, Fast clear
Reset
64MB x 32 SDRAM [4]
BusyReady/
- +
16
1
CLKDATAx xx x
6ch
EC
L c
on
tro
l I/O
8ch TTL to ECL [1]JTAG
16
ch
EC
L i
np
uts
64MB SDRAM4Kbit x 32 DP-SRAM [3]
Coincidence Register (CR) modulesCoincidence Register (CR) modules
[1] ON Semiconductor, MC10H124[2] ON Semiconductor, MC10H125[3] IDT, IDT70V24, 4Kbit x16 Dual-Port SRAM[4] Winbond, W9825G6, 256Mbit x16 SDRAM[5] Micron, MT29F2G16AACWP, 2Gb x16 NAND Flash[6] TI, SN74VMEH22501A, VME bus transceiver
A32
, Ad
dre
ssin
g
rota
ry s
wit
ches
Th
e d
efin
itio
n o
f E
CL
co
nn
ecto
r
66
E906 detector readout and DAQ systemE906 detector readout and DAQ system
67
Some information and estimationSome information and estimation Main Injector RF clock frequency: 53 MHz.
Beam structure: 1013 protons in a 5 s slow extraction spill every minute. Beam intensity: 2*1012/sec.
Level-2 trigger latency: Master Trigger OR decision time= 91ns.
Level-1 trigger rate (X): MWPC designed Singles rates:53MHz.(?) The total rate of single muons traversing the detector and
passing the trigger matrix tracking will be approximately 100 kHz with the LH2 target and 150 kHz with the LD2 target (both cases include tracks originating in the beam dump).
Event size of MWPC W/O data reduction: 5500bit=0.8kB
Depth of memory buffer: 53MHz*91ns~ 5 events. Size of total memory to buffer 5 events=0.8kB*5=4kB.
VME transfer throughput:0.8kB*1kHz=0.8MB/per sec << Optic fiber ~100 MB/sec and VME 160 MB/sec. Deadtime-free is possible.68
What I have learned from recent What I have learned from recent works. works. How to write a driver for VME module.
How to install and use CODA DAQ system.
Simulation and analysis methods in high energy physics.
More knowledge about nuclear physics.
69
70
71
backup
72
The physics motivation Why we choose measuring Drell-Yan process. What we can learn from Drell-Yan process.
*The past experiments *The results of E866 Etc.
E906 experiments Introduce the experiment’s framework. Comparing with the past experiments.
73
Why we want to study the low mass region. Introduce the goal we want to reach.
What the simulation program do. Introduce the program.
The detector geometry and configure file. Introduce the detector geometry and the fast
monte carlo simulation flow paht. The results of this simulation.
74
Why we want to study the angle distribution
How I define the axis
The result of this study
75
What is CODA? CODA flow chart.
Introduce sis3610 and sis3600 What is trigger supervisor and latch.
The flow chart of controlling the vme module Make a description of how the data acquisition
work.
76
Introduce the works Taiwan group is going to do.
What parts I will do in the future. What is Level2 trigger.
What I have learned from recent works.
77
What will we learn?
– d-bar/u-bar in the proton– Nuclear effects in the sea quark distributions– High-x valence distributions– Partonic energy loss in cold nuclear matter
78
Momentum Difference(X) (M1*0.5)
79
Momentum Difference(Y) (M1*0.5)
80
Momentum Difference(Z) (M1*0.5)
81
Pt/Pz(positive) (M1*0.5)
82
Pt/Pz(negative) (M1*0.5)
83
Opening angle of muon pairs
fe198v5m101mrtr.le.4.5zrtr.le.0
fe198v5m101mrtr.le.4.5zrtr.ge.0
fe198v5m101_dumpmrtr.le.4.5zrtr.le.0
fe198v5m101_dumpmrtr.le.4.5zrtr.ge.0
84
Momentum Difference(X) (M1*0.1)
85
Momentum Difference(Y) (M1*0.1)
86
Momentum Difference(Z) (M1*0.1)
87
Pt/Pz(positive) (M1*0.1)
88
Pt/Pz(negative) (M1*0.1)
89
Opening angle of muon pairs
fe198v5m101mrtr.le.4.5zrtr.le.0
fe198v5m101mrtr.le.4.5zrtr.ge.0
fe198v5m101_dumpmrtr.le.4.5zrtr.le.0
fe198v5m101_dumpmrtr.le.4.5zrtr.ge.0
90
91
Theta y distribution of positive muon at zstart
92
Theta y distribution of positive muon at zstart
93
Theta y distribution of negative muon at zstart
94
Theta y distribution of negative muon at zstart
95
Momentum distribution of positive muon at zstart
96
Momentum distribution of positive muon at zstart
97
Momentum distribution of negative muon at zstart
98
Momentum distribution of negative muon at zstart
99
X distribution of positive muon at zstart
100
X distribution of positive muon at zstart
101
X distribution of negative muon at zstart
102
X distribution of negative muon at zstart
103
Theta x distribution of positive muon at zstart
104
Theta x distribution of positive muon at zstart
105
Theta x distribution of negative muon at zstart
106
Theta x distribution of negative muon at zstart
107
Xf distribution of muon at zstart
108
Xf distribution of muon at zstart
109
X1 distribution of muon at zstart
110
X1 distribution of muon at zstart
111
X2 distribution of muon at zstart
112
X2 distribution of muon at zstart
113
Total momentum distribution of muon at zstart
114
Total momentum distribution of muon at zstart
115
116
Station 1 Chamber RatesOccasionally a muon showers in the
absorber If this happens in the center of the
absorber, no effect is seen as shower is also absorbed
If this happens in the last few inches of the absorber, shower can create extremely large rates in Station 1 (of low momentum particles)
Solution is to have an absorber-free region at the end of the field volume and use field as a sweeper
In Solid Iron magnet, there is no absorber-free sweeper region! (Can we find a wide gap sweeper magnet?)
Requires GEANT MC to see magnitude of effect
Absorber and B Field
Sta. 1
Absorber and B Field
Absorber and B Field
B Field only
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118
119
Data Sources
256 Hodoscopes—bit latches
MWPC 5500 Channels
bit latches
Station 2 & 3Drift Chambers1700 ChannelsMulti-hit TDC’s
Station 4 PropTubes 400 Channels
Bit latches
The problem we meetThe problem we meet There can be thousands to millions of
events occurring per second.
Detectors are very large - containing many thousands of individual channels.
Events are different sizes.
Events occur at random.
Only a few events are interesting.
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cut
121
Use the E906 Fast Monte Carlo simulation for study configuration data.
The configuration file is “fe198v5.dat”.
By changing the entry “current and step to scale” we can adjust the M1 or M2 current.
Fix M2 current and vary M1 currentFix M2 current and vary M1 current
The input to the simulation is decided by Ykick*input/2000 and
the tracking plane from #2 to #13 will affected
by this factor.
The input to the simulation is decided by Ykick*input/2000 and
the tracking plane from #2 to #13 will affected
by this factor.122
Fix the M1 current, and change the M2 current (Ykick).
Fix M1 current and vary M2 currentFix M1 current and vary M2 current
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Cuts conditionsPurple: all events
Green: xF>0 and M>4.5 GeV and pz>20 GeV
Blue: Green and |ytrack|>2.25 in at z=0 (zdump)
Red: Blue and |ytrack|<10.0 in at z=-60 (zstart)
Moving the cut condition at zdump to Station 1 and change the value.
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Original Changed
125
Original Changed
Try |ytrack|>8 in at z=238 (before station1)126
M1*0.5
1
2
3
127
4
M1*0.1
1
2
3
4
Changing cut condition can not improve the z resolution.128
129
Gottfried-Jackson frame(GJ)Gottfried-Jackson frame(GJ) Gottfried-Jackson
frame is defined in dimuon CMS .
The Z-axis is the direction of Pbeam .
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Production plane
Decay plane
Helicity frame(HX)Helicity frame(HX) Helicity frame is
defined in dimuon CMS .
The Z-axis is Pbeam + Ptarget.
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Production plane
Decay plane
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133
134
TriggerSIS3610
VME flow chartVME flow chart
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Reach the event number?
No
Yes
EBCreateevent
CODAStart
Initialize3600/3610
Clear/Reset 3600/3610
End
Events into SIS3600
Setup phase
SIS3610Send
Interrupt toMVME6100
Latch phase
Exit phase
Data to storagephase
MVME6100Take DataFrom 6100
ERET
DISK
No
Yes
EXIT?
Why we need DAQ?Why we need DAQ? The goal of a nuclear physics experiment is to get data
about nuclear interactions.
Particles pass through detectors which generate electrical signals contain information about the particles type, energy, trajectory .
The complete set of signals which describe a single nuclear interaction is called an Event.
The data acquisition system digitizes, formats and stores this information in a way which can be retrieved for later analysis.
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The structure of DAQThe structure of DAQ Triggering (choosing events we want)
Readout (digitizing detector signals)
Event formatting (standardize what we’re saving)
Event building (putting fragments together)
Event transport (make events available to all)
Event storage (save data for analysis)
Run Control (configure-start-stop experiments)
Monitoring (tell me what’s going on)
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A DAQ system exampleA DAQ system example
138
Trigger
ReadoutEvent
formattingEvent
building Event
transport
Event storage
Run control
Monitoring
Why using CODA?Why using CODA? CODA is a software toolkit with some specialized
hardware support.
Modular software components use the network for inter-process communication and event transport.
Use open standards and minimize the use of commercial software while maximizing use of commercial hardware.
DAQ systems for each experimental Hall can be “built-up” from common components to fit their needs.
139
VME VME (Versa Module Europa)(Versa Module Europa) VMEbus is a computer bus
standard, originally developed for the Motorola 68000 line of CPUs, but later widely used for many applications.
8/16/24/32/64 bit bus,24/32/64 support BLT(block transfer).
The data is transfering in the back plane bus.
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Angular distribution Angular distribution The angular distribution may be changed by
the detector acceptance.
141
?!!
What is Level 2 triggerWhat is Level 2 trigger
Level 1 trigger
Level 2 trigger
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Backplane bus
SIS3600
Computingmodule
SIS3610
interrupt data
Hardware configuration in IPASHardware configuration in IPAS
143
MVME6100Single board computer
SIS3610Trigger
supervisor
SIS3600Multi
eventsLatch
BackPlane Bus
Change the target locationChange the target location
The target original location is at -70 to -50. We change it to -150 to -130.
144
145
146
147
is more suppressed than in the proton since
(Field and Feynman 197
(pQCD calculati
Paul
ons b
Origins of ( ) ( )?
y Ross and Sachrajda)
(Bag model calculation by Signal, Thomas, Schreib
7
i blocking by the valenc
)
e quarks
u x d x
g uu g dd
p uud
Quark spectrum includes a bound state plus the
polarized negative
er)
(Diakonov
Chiral quark-soli
, Pobylitsa, Poly
and positive D
akov, Wakamats
irac continuu
u, Kubota)
ton model
Instanton m l
m
ode
,
Sta
(Dorokhov, Kochelev)
(Bourrely, Butistical model ccella, Sof
,
f er)
etc. L R R L L R R Lu u d d d d u u
The valence quarks affect the Dirac vacuum and the quark-antiquark sea
質子 p (uud). 中子 n (udd)
148
What is the origin of ?What is the origin of ?du,
In general : 1, 0, 0
Fermilab E866 Measurements
149
800 ( ) / ( )GeV p d X p p X
150
Proton Economics Total of 5.2 X 1018 protons (over 2 years)
Maximum instantaneous rate of 2 X 1012 proton/sec Based on E866 experience with target related rate
dependence—balance systematic and statistical uncertainties Station 1 chamber rates.
Possible delivery scenario: 5 sec spill of 1 X 1013 protons each minute Longer spill (5 sec) desirable over 5-1 sec spills
Leading order structure function
151
],,[, 22222 QxqQxqxeQxF ii
ii
The leading-order structure function F2 is given by quark-momentum distributions in the nucleon
How the fast monte carlo generate muon 1. random create virtual photon mass. 2. random create feynman X 3. determine Pt^2(max), X1, X2 4. determine Pt 5. random phi angle in ? Frame. 6. from dimuon CMS ,the virtual photon average separate it’s mass
to two muons. 7.by the difference mass condition to determine cos(theta). 8.calculate Pl, Pt. 9.boost along Pt and create phimu, phimu is the mu+ with respect
to the pt of the gamma 10.boost along Pl to overall CMS frame, and check Pz grate or less
pmumin. 11.boost to lab.
152