ll spin correlations and spin selected hbt
DESCRIPTION
LL spin correlations and spin selected HBT. Fei Du, Sandweiss’ group, Yale. Outline: Lambda and its decay Spin correlations Spin selected HBT. L and its decay. L (uds) m = 1115.683 ± 0.006 MeV c t = 7.9 cm Asymmetry in decay. L detection at STAR. - PowerPoint PPT PresentationTRANSCRIPT
DOE review, 09/15/2003 1
spin correlations and spin selected HBT
Fei Du, Sandweiss’ group, Yale
Outline:• Lambda and its decay• Spin correlations• Spin selected HBT
DOE review, 09/15/2003 2
and its decay
(uds)– m = 1115.683 ± 0.006 MeV– c = 7.9 cm
Asymmetry in decay
cos64.01cos
d
dw
p
DOE review, 09/15/2003 3
detection at STAR
Topological method: pair up decay products (p and ) with geometry and invariant mass cuts
Preliminary
DOE review, 09/15/2003 4
How to find out the spin
Two transformations:
• 1st: transform to the CMS of the di- pair
• 2nd: transform each proton to the rest frame of its parent .
• Take the proton momentum direction as an indicator of the spin direction.
DOE review, 09/15/2003 5
spin correlations
• Spin correlation at low : due to Fermi-Dirac statistics.
• For system, at low Q, s-wave state (l=0) dominates (symmetrical space wavefunction), thus total spin S = 0. (↑↓-↓↑)
• Spins are anti-aligned.
221 )( qqQ
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Complication I – Q is never 0
• Finite Q → source radius
3/
3/2
3/
2
onscontributi 1 offraction :
onscontributi 0 offraction :
10
11
10
00
1
0
FF
FC
FF
FC
SF
SF
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Complication II – spin direction is not perfectly measured
Calculation done by G. Alexander et. al.:Use of Spin-Correlations to Study Low Energy and Space Symmetries and Resonances, Phys. Lett. B352:162, 1995
)1( 1374.01
)0( 4122.01
cos
trans.2after protons obetween tw angle :
Sydy
dN
Sydy
dN
y
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Spin correlation golden formula
Q
Qy
dy
dN
Q
Qe
y
yydy
dN
Qr
,1
0 ,4122.01
,4/3
0 ,0 ),1(
4
3
)3
41(4122.01
)1374.01()4122.01)(1(
22
DOE review, 09/15/2003 9
ALEPH data
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Preliminary
PreliminaryPreliminary
Preliminary
PreliminaryPreliminary
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Fit dN/dy to 1 + ky
Q (MeV) k
0 – 200 -0.15 ± 0.14
200 – 400 -0.25 ± 0.06
400 – 600 -0.03 ± 0.04
600 – 800 0.003 ± 0.03
800 – 1000 -0.009 ± 0.03Preliminary
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HBT (Bose-Einstein correlation)
)1()()(
)()(
][2
1
22
12212211
21
2,12,12
)()(12
Qr
rkrkirkrki
eNkPkP
kkPkkC
ee
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HBT (Fermi-Dirac correlation)
• Aligned spins: • Anti-aligned spins:
DOE review, 09/15/2003 14
Better treatment
22
12212211
1)(
][2
1 )()(012
Qr
rkrkirkrkiS
eQC
ee
22
12212211
1)(
][2
1 )()(112
Qr
rkrkirkrkiS
eQC
ee
22
2222
5.01
)1(75.0)1(25.0)(Qr
QrQr
e
eeQC
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HBT with spin selection
< /2
(y > 0)
/2
(y < 0)
triplet 0.534 0.466
singlet 0.397 0.603
222222
6.01)1(8.0)1(2.0)(
2.0)0|0( ,8.0)0|1(QrQrQr eeeQC
ySPySP
DOE review, 09/15/2003 16
aligned)-(anti 06.005.0
(aligned) 12.028.0
pairs) (all 08.016.0
1)(22
QreQC
Preliminary
PreliminaryPreliminary
DOE review, 09/15/2003 17
Outlook
• With next year’s data (~ 20x more statistics than shown in the plots here), things will become much clearer.
• Also we can use tighter cut on spin alignment with more statistics.