10/6/2006 e. de la cruz burelo, spin 2006, kyoto japan 1 hyperon polarization in a quark-quark...
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10/6/200610/6/2006E. De La Cruz Burelo, SPIN 2006, KyE. De La Cruz Burelo, SPIN 2006, Kyoto Japan oto Japan
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Hyperon polarization in a Hyperon polarization in a quark-quark scattering modelquark-quark scattering model
Eduard De La Cruz BureloEduard De La Cruz Burelo
Homer A. NealHomer A. Neal
10/6/200610/6/2006 E. De La Cruz Burelo, SPIN 2006, Kyoto Japan E. De La Cruz Burelo, SPIN 2006, Kyoto Japan 22
OutlineOutline Hyperon polarization remains a major Hyperon polarization remains a major
open question even at energies of open question even at energies of hundreds of GeVhundreds of GeV
Extraordinary behavior of hyperon Extraordinary behavior of hyperon polarization has no simple explanationpolarization has no simple explanation
Polarization in Polarization in pppp pp pp and and pppp H H + X+ X : : could both be the result of simple quark-could both be the result of simple quark-quark scattering?quark scattering?
A proposed model based on quark-quark A proposed model based on quark-quark scattering.scattering.
The qualitative explanation of the hyperon The qualitative explanation of the hyperon polarization for a variety of processespolarization for a variety of processes
10/6/200610/6/2006 E. De La Cruz Burelo, SPIN 2006, Kyoto Japan E. De La Cruz Burelo, SPIN 2006, Kyoto Japan 33
Hyperon polarizationHyperon polarization
An unresolved question: An unresolved question: What causes the large polarization in What causes the large polarization in
inclusive hyperon production in p-p inclusive hyperon production in p-p collisions?collisions?
Vanishingly small polarizations are Vanishingly small polarizations are predicted in QCD. predicted in QCD.
No model is now able to explain all No model is now able to explain all features of Hyperon polarization at features of Hyperon polarization at the same time.the same time.
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ParticleParticle Quark content* PolarizationPolarization
pN pN H+X H+XΛΛ00 (ud)0 s Negative
ΣΣ00 (ud)1 s Positive
ΣΣ++ (uu)1 s Positive
ΣΣ-- (dd)1 s Positive
ΞΞ-- (ss)1 d Negative
ΞΞ00 (ss)1 u Negative
ΩΩ-- s s s ~Zero
ΛΛ00 (u d)0 s Zero
ΞΞ++ (s s)1 d Negative
ΣΣ-- (ūū)1 s Positive
ΛΛbb(ud)0 b ?
Hyperon polarization Hyperon polarization characteristicscharacteristics
ParticleParticle Quark content* PolarizationPolarization
pN pN H+X H+XΛΛ00 (ud)0 s Negative
ΣΣ00 (ud)1 s Positive
ΣΣ++ (uu)1 s Positive
ΣΣ-- (dd)1 s Positive
ΞΞ-- (ss)1 d Negative
ΞΞ00 (ss)1 u Negative
ΩΩ-- s s s ~Zero
ΛΛ00 (u d)0 s Zero
ΞΞ++ (s s)1 d Negative
ΣΣ-- (ūū)1 s Positive
* (Diquark)J state
J=0 : Negative
J = 1 + s quark:
Positive
2 s-quarks: Negative
Plans to measure it (LHC)
10/6/200610/6/2006 E. De La Cruz Burelo, SPIN 2006, Kyoto Japan E. De La Cruz Burelo, SPIN 2006, Kyoto Japan 55
ΛΛ00: Lowest mass hyperon … : Lowest mass hyperon … more intriguingmore intriguing
Very little dependence on the initial proton energy and in the target material.
Grows negative linearly with pT until a plateau is reached around 1 GeV/c.
For constant xF (=pL/pmax) value, the plateau extends from 1 GeV/c to the highest measured pT.
10/6/200610/6/2006 E. De La Cruz Burelo, SPIN 2006, Kyoto Japan E. De La Cruz Burelo, SPIN 2006, Kyoto Japan 66
Intriguing questions:Intriguing questions:
Why do the Λ0 and Ξ polarizations look similar?
Why is the Σ polarization positive?
Why is the Ω polarization almost ~zero?
Why is there a plateau in the Λ0 polarization?
10/6/200610/6/2006 E. De La Cruz Burelo, SPIN 2006, Kyoto Japan E. De La Cruz Burelo, SPIN 2006, Kyoto Japan 77
Features we would like to Features we would like to explain:explain:
The shape and magnitude of the The shape and magnitude of the ΛΛ0 0
polarizationpolarization The different signs in the The different signs in the ΛΛ0 0 and and ΣΣ
polarizationpolarization The similarity of the polarization for The similarity of the polarization for
the the ΛΛ0 0 and and ΞΞ The small value of the The small value of the ΩΩ polarization polarization
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q-q scattering: relating pp q-q scattering: relating pp pp pp to pp to pp ΛΛ + X process + X process
Is there any connection between the Is there any connection between the observed polarization in these two observed polarization in these two processes? processes? – They could come from the same source: quark-They could come from the same source: quark-
quark scattering.quark scattering.
udu u
d
s
Λ0pro
tonu
dup
roto
n
u
du p
roto
n udu u
d
s
pro
tonu
dup
roto
n udu p
roto
n
u
ssss ssΛ0
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pppppp in a quark-quark pp in a quark-quark scattering modelscattering model
Neal et al. proposed a q-q scattering model to explain the polarization in elastic p-p scattering:
First region is due to q-q scattering
Second region is due to 2q-2q or q-2q
Subsequent data is consistent with 3q-3q scattering*.
Can we apply the same idea to Can we apply the same idea to
pppp ΛΛ + X process? + X process?
Neal et al. proposed a q-q scattering model to explain the polarization in elastic p-p scattering:
First region is due to q-q scattering
Second region is due to 2q-2q or q-2q
Subsequent data is consistent with 3q-3q scattering*.
Can we apply the same idea to Can we apply the same idea to
pppp ΛΛ + X process? + X process?
H.A. Neal et al.
Phys. Lett. B 51 (1974) 79*) H.A. Neal et al.
Phys. Lett. B 439 (1998) 407
10/6/200610/6/2006 E. De La Cruz Burelo, SPIN 2006, Kyoto Japan E. De La Cruz Burelo, SPIN 2006, Kyoto Japan 1010
pppp ΛΛ + X in a quark-quark + X in a quark-quark scattering modelscattering model
From a preexisting pair in the incoming From a preexisting pair in the incoming proton, the s quark scatters, get highly proton, the s quark scatters, get highly polarized, and end up in the hyperon.polarized, and end up in the hyperon.
Hyperon polarization: PHyperon polarization: PHH=P=Pqq(x,p(x,pTT). ). PPqq(x(xFF,p,pTT) : quark polarization effect due to a ) : quark polarization effect due to a q-q scattering process.q-q scattering process.
ss
10/6/200610/6/2006 E. De La Cruz Burelo, SPIN 2006, Kyoto Japan E. De La Cruz Burelo, SPIN 2006, Kyoto Japan 1111
ΛΛ00 polarization from polarization polarization from polarization in in pppppp (1)pp (1)
Model: Model: PPHH=P=Pqq(x,p(x,pTT))
– In a multiple quark scattering* P In a multiple quark scattering* P ~ mqPq(pT)
*) J. Szwed, Phys. Lett. B 105 (1981) 403.
2
1~
)(
)(0
s
u
m
m
XppP
ppppP
Assuming ms~2mu
)()(2 0 XppPppppP
10/6/200610/6/2006 E. De La Cruz Burelo, SPIN 2006, Kyoto Japan E. De La Cruz Burelo, SPIN 2006, Kyoto Japan 1212
ΛΛ00 polarization from polarization polarization from polarization in in pppppp (2)pp (2)
What pWhat pTT((ΛΛ00)) vs. p vs. pTT(p) should we compare?(p) should we compare?– For a elastic p-p scattering in a q-q region (Neal et al.):
– For pp Λ + X in q-q region:
We should compare at:We should compare at:
)()( qppp TT
)(2
3)()()( 00 TTTT psppsp
Assuming s-quark account for half of the Λ0 mass.
)()(3
2 0 TT ppp
10/6/200610/6/2006 E. De La Cruz Burelo, SPIN 2006, Kyoto Japan E. De La Cruz Burelo, SPIN 2006, Kyoto Japan 1313
Comparison of proton and Comparison of proton and ΛΛ00 polarizationpolarization
Proton polarization multiplied by 2
Proton pT multiplied by 2/3
If we let proton data to tell us what values prefer to match Λ0 data, selected values are around to 2 and 2/3.
10/6/200610/6/2006 E. De La Cruz Burelo, SPIN 2006, Kyoto Japan E. De La Cruz Burelo, SPIN 2006, Kyoto Japan 1414
What about the plateau?What about the plateau?
The plateau in the Λ0 polarization can be understood as the saturation of the s quark polarization (P=100%).
Po
lari
zati
on
Po
lari
zati
on
10/6/200610/6/2006 E. De La Cruz Burelo, SPIN 2006, Kyoto Japan E. De La Cruz Burelo, SPIN 2006, Kyoto Japan 1515
Explaining the other featuresExplaining the other features
Why the similar polarization for the Why the similar polarization for the ΛΛ0 0 and and ΞΞ??
If the polarization of both hyperons is due to one s quark becoming highly polarized from the scattering process, then we expect the polarization of both hyperons to be similar.
10/6/200610/6/2006 E. De La Cruz Burelo, SPIN 2006, Kyoto Japan E. De La Cruz Burelo, SPIN 2006, Kyoto Japan 1616
Why the different sign in the Why the different sign in the ΛΛ0 0
and and ΣΣ polarization? polarization?
u d
s
u d
s
Beam quarks does not Beam quarks does not contributed to the contributed to the ΛΛ00 polarizationpolarization
s quark is responsible for the s quark is responsible for the large polarization of the large polarization of the ΛΛ00..
s quark polarization is negative.s quark polarization is negative.
s quark polarization is negative which force the polarization of the u and d quarks to be positive, so overall polarization is positive.
If we assume the s quark being responsible of the polarization, it can be showed that the sign of the Σ polarization is opposite to that of the Λ polarization.
10/6/200610/6/2006 E. De La Cruz Burelo, SPIN 2006, Kyoto Japan E. De La Cruz Burelo, SPIN 2006, Kyoto Japan 1717
Why Why ΩΩ polarization is ~0?polarization is ~0?
One of 3 s quarks get polarized in the scattering, One of 3 s quarks get polarized in the scattering, setting a maximum of 33% to the polarization of setting a maximum of 33% to the polarization of the the ΩΩ..
Should be similar to the Should be similar to the ΛΛ00 polarization in the one polarization in the one quark scattering region.quark scattering region.
Λ0 polarization compared to the Ω polarization. Statistics too low to make strong conclusions.
10/6/200610/6/2006 E. De La Cruz Burelo, SPIN 2006, Kyoto Japan E. De La Cruz Burelo, SPIN 2006, Kyoto Japan 1818
Future tests/ImplicationsFuture tests/Implications
ΛΛb b polarization is planned to be measured polarization is planned to be measured
in LHC (ATLAS & LHCb)in LHC (ATLAS & LHCb) Polarization could be huge if the q-q Polarization could be huge if the q-q
contribution to production is important and contribution to production is important and the Szwed mass scaling holds.the Szwed mass scaling holds.
Simple relation should exist between Simple relation should exist between ΛΛ and and ΛΛbb polarization is our q-q idea is polarization is our q-q idea is
correct.correct.
10/6/200610/6/2006 E. De La Cruz Burelo, SPIN 2006, Kyoto Japan E. De La Cruz Burelo, SPIN 2006, Kyoto Japan 1919
Conclusions:Conclusions:
A model based in a simple q-q scattering A model based in a simple q-q scattering process is proposed:process is proposed:
Polarization due the scattering process PPolarization due the scattering process Pqq(p(pTT) is the ) is the same for all quark species.same for all quark species.
s quark scatters from the incoming proton is the s quark scatters from the incoming proton is the responsible for the large hyperon polarization.responsible for the large hyperon polarization.
ΛΛ and proton polarization seems to have a and proton polarization seems to have a common source.common source.
The model is able to qualitatively address The model is able to qualitatively address all of the main observed features of all of the main observed features of hyperon polarization.hyperon polarization.