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Proton Polarimetry at RHIC
K. Oleg Eyserfor the CNI polarimeter group
Newport News, VA, October 25, 2013
2 2
@ RHIC
AGSAGSLINACLINACBOOSTERBOOSTER
Polarized Source
Spin Rotators
200 MeV Polarimeter
Absolute Polarimeter (H jet)
PHENIX
BRAHMS & PP2PP
STAR
Siberian Snakes
Siberian Snakes
Spin Flipper
RHIC pC Polarimeters
Rf Dipole AGS Internal Polarimeter
AGS pC Polarimeter
Strong SnakePartial Snake
Helical Partial Snake
3 3
RHIC Luminosity
Beam momentum100 GeV250 GeV
Consistent luminosity improvement over the years
255 GeV in 2013
Significance: Figure of Merit
or
4 4
Polarization and Asymmetries
𝐴𝑁=𝑑𝜎 𝑙𝑒𝑓𝑡−𝑑𝜎 h𝑟𝑖𝑔 𝑡
𝑑𝜎 𝑙𝑒𝑓𝑡+𝑑𝜎 h𝑟𝑖𝑔 𝑡
S
x
y
NP
Polarization:
𝜀=𝐴𝑁 ∙𝑃=𝑁 𝐿−𝑁𝑅
𝑁 𝐿+𝑁𝑅
𝒔𝒛=𝑵
𝒑=𝑳
left
right
scattering plane
𝑠𝑧=±12ℏ𝑃=𝑛↑−𝑛↓
𝑛↑+𝑛↓
(proton)
(proton)(Carbon)
5 5
Polarimeters in RHIC
Carbon polarimeters
Two per ring
Fast measurement
Beam polarization profile
Hydrogen jet
Polarized target
Continuous operation
per fill
normalization
Carbon polarimeters
Hydrogen jet
beam
6 6
Elastic Signal Identification
𝐸𝑘𝑖𝑛=12𝑚𝑣2=1
2𝑚(𝑑𝑡 )
2
ADC/TDC waveform readout
normalized to peak
ADCmax
TDC0
V10BASELINE
Elastic signal
→ Energy calibration
→ Time offset
7 7
Energy Calibration
𝑐 ∙ 𝐴=𝐸𝑚𝑒𝑎𝑠=𝐸𝑘𝑖𝑛−∆𝐸
∆𝐸𝛼(𝐴𝑚 )=0.72∙∆𝐸𝛼 (𝐺𝑑)
Two different α-sources
Stopping power forα-particles and protons from NIST database
∆𝐸𝑃=0.44 ∙∆𝐸𝛼 (𝐺𝑑) ∙𝐸[𝑀𝑒𝑉 ]−0.64
8 8
Elastic Signal and Background
5 MeV
1 M
eV
signal region background region
atomic jet target
proton beam
9 9
Asymmetry and Polarization
⇒
𝜀=𝜀𝑖𝑛𝑐−𝑟 ∙𝜀𝑏𝑔1−𝑟
What if
𝑃 𝐵𝑒𝑎𝑚=−𝜀𝐵𝑒𝑎𝑚𝜀𝑇𝑎𝑟𝑔𝑒𝑡
𝑃𝑇𝑎𝑟𝑔𝑒𝑡𝑃 𝐵=
𝜀𝐵𝜀𝑇𝑃𝑇𝑃𝑌=
𝜀𝑌𝜀𝑇𝑃𝑇
Polarization independent background
Polarization dependent background
background fraction
+
-
+
- +
-
+
-
+
-
+
-
+
-
+
-
+
+
+
+
+
+
+
-
-
-
-
-
+
+
+
-
abort gaps
10 10
Polarimeter PerformanceKinematic distributions for consistency checks
Fast feedback to RHIC operations
Target P=92%
1 Fill
over 150 RHIC fills in 2013
11 11
Summary
Polarization in RHIC is measured with fast p+C targets for monitoring, polarization profiles,
and polarization decay, a polarized atomic hydrogen jet for normalization.
The 2013 data provides unprecedented possibilities to use the jet polarimeter for background studies.
The jet polarimeter provides fast feedback to RHIC operations.
Final analysis and systematic studies are on-going.
https://wiki.bnl.gov/rhicspin/RHIC_Spin_Group
BACKUP
13 13
Polarization Profile
𝑃𝑐𝑜𝑙𝑙=∫𝑑𝑥𝑑𝑦𝑃 (𝑥 , 𝑦 ) 𝐼𝐵 (𝑥 , 𝑦 ) 𝐼𝑌 (𝑥 , 𝑦)
∫𝑑𝑥𝑑𝑦 𝐼𝐵 (𝑥 , 𝑦 ) 𝐼𝑌 (𝑥 , 𝑦 )
𝑃 𝑗𝑒𝑡=∫𝑑𝑥𝑑𝑦𝑃 (𝑥 , 𝑦 ) 𝐼 𝐵 (𝑥 , 𝑦 )
∫𝑑𝑥𝑑𝑦 𝐼𝐵 (𝑥 , 𝑦 )
𝑃𝑠𝑤𝑒𝑒𝑝=∫𝑑𝑦𝑃 (𝑦 ) 𝐼𝐵 ( 𝑦 )
∫𝑑𝑦 𝐼 𝐵 ( 𝑦 )
jet target polarization is flat
vertical and horizontal Carbon targets available
For Gaussian profiles
Profile parameter