parton distribution functions and quark orbital motion petr závada institute of physics, prague the...
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Parton distribution functions Parton distribution functions and quark orbital motionand quark orbital motion
Parton distribution functions Parton distribution functions and quark orbital motionand quark orbital motion
Petr ZávadaInstitute of Physics, Prague
The 6th Circum-Pan-Pacific Symposium on High Energy Spin PhysicsJuly 30 - August 2, 2007
Vancouver BC
The 6th Circum-Pan-Pacific Symposium on High Energy Spin PhysicsJuly 30 - August 2, 2007
Vancouver BC
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IntroductionIntroduction
Presented results are based on the covariant QPM. Intrinsic motion, reflecting orbital momenta of quarks, is consistently taken into account. Due to covariance, transversal and longitudinal momenta appear on the same level. [P.Z. Phys.Rev.D65, 054040(2002) and D67, 014019(2003)].
In present LO version, no dynamics, but “exact” kinematics effective tool for separating effects due to dynamics (QCD) and kinematics. This viewpoint well supported by our previous results e.g:
sum rules WW, Efremov-Leader-Teryaev, Burkhard-Cottingham the same set of assumptions implies substantial dependence Γ1 on
kinematical effects Calculation g1 and g2 from valence distributions – very good agreement with
data some new relations between structure functions, including transversity
[A.Efremov, O.Teryaev and P.Z., Phys.Rev.D70, 054018(2004) and arXiv: hep-ph/0512034].
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Previous papers: What is the dependence of the structure
functions on intrinsic motion of the quarks?
In this talk further questions: How can one extract information about intrinsic
motion from the structure functions? What is the role of the orbital momentum of
quarks, which is a particular case of intrinsic motion?
[full version in arXiv: hep-ph/0706.2988 and Eur.Phys.J. C – August2007].
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ModelModel
e-e-
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Structure functionsStructure functions
Input:Input:
3D distributionfunctions in the
proton rest frame
Result:Result:
structure functions
(x=Bjorken xB !)
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F1, F2 - manifestly covariant form:
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g1, g2 - manifestly covariant form:
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CommentsComments
In the limit of static quarks, for p→0, which is equivalent to the assumption p=xP, one gets usual relations between the structure and distribution functions like
Obtained structure functions for m→0 obey the known sum rules:
Sum rules were obtainedfrom:
1) Relativistic covariance2) Spheric symmetry3) One photon exchange
In this talk In this talk m→0 is assumed.is assumed.
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Comments
SStructure functions are represented by integrals from tructure functions are represented by integrals from probabilistic distributions:probabilistic distributions:
This form allows integral transforms:
1) g1 ↔ g2 or F1 ↔ F2 (rules mentioned above were example).2) With some additional assumptions also e.g. integral relation
g1 ↔ F2 can be obtained (illustration will be given).3) To invert the integrals and obtain G or G from F2 or g1 (aim
of this talk).
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g1, g2 from valence quarks
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g1, g2 from valence quarks
Calculation - solid line, data - dashed lineCalculation - solid line, data - dashed line (left) and circles (right)(left) and circles (right)
E155E155
g1 fit of world data by E155 Coll., Phys.Lett B 493, 19 (2000).
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TransversityTransversity In a similar way also the transversity was calculated; see In a similar way also the transversity was calculated; see [A.Efremov, O.Teryaev and P.Z., Phys.Rev.D70, 054018(2004)]. Among others we . Among others we obtainedobtained
- which follows- which follows from covariant kinematics!from covariant kinematics!
Obtained transversities were used for the calculation of double spin Obtained transversities were used for the calculation of double spin asymmetry in the lepton pair production in proposed PAX experiment; asymmetry in the lepton pair production in proposed PAX experiment; see see [A.Efremov, O.Teryaev and P.Z., arXiv: hep-ph/0512034)]. .
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2007: Extraction from the data(for the first time)
2007: Extraction from the data(for the first time)
2004: Our calculation
2004: Our calculation
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Double spin asymmetry in PAX experiment
1.1. 2.2.
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Momentum distributions from structure function F2Momentum distributions from structure function F2
Deconvolution of F2 :
Remarks:• G measures in d3p, P in the dp/M• pmax=M/2 – due to kinematics in the proton rest frame, ∑p=0• Self-consistency test:
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Momentum distributions in the proton rest frameMomentum distributions in the proton rest frame
<pval>=0.11 (0.083) GeV/c for u (d) quarks
Input q(x)
MRST LO 4GeV2
qval=q-q
—-
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Momentum distributions from structure function g1Momentum distributions from structure function g1
Deconvolution of g1 :
Since G=G++G- and ∆G=G++G-
… obtained from F2 ,g1 and represent distribution of quarks with polarization ±.
dp/Md3p
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Distribution functions f±(x)Distribution functions f±(x)
Let us note: but !!
(equality takes place only in non-covariant IMF approach)
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Momentum distributions in the proton rest frameMomentum distributions in the proton rest frame
2) q(x) & Δq(x)
MRST & LSS LO 4GeV2
Remark:xΔfq(x) are similar to xqval(x)
spin contributioncomes dominatly from valence region
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Intrinsic motion and angular momentumIntrinsic motion and angular momentum Forget structure functions for a moment… Angular momentum consists of j=l+s. In relativistic case l,s are not conserved separately, only j is conserved. So, we can
have pure states of j (j2,jz) only, which are represented by the bispinor spherical waves:
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j=1/2j=1/2
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Spin and orbital motionSpin and orbital motion
<s>, <s>, ΓΓ11: two ways, one result: two ways, one result
-covariant approach is a common basis -covariant approach is a common basis
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CommentsComments
• are controlled by the factor , two extremes:
•massive and static quarks and
• for fixed j=1/2 both the quantities are almost equivalent: more kinetic energy (in proton rest frame) generates more orbital motion and vice versa.
•massless quarks and
-this scenario is clearly preferred for quarks with effective mass on scale of thousandths and momentum of tenths of GeV.
• important role of the intrinsic quark orbital motion emerges as a direct consequence of the covariant approach
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Proton spinProton spin
Second scenario:
implies, that a room for gluon contribution can be rather sensitive to the longitudinal polarization:
For ∆∑≈1/3, 0.3 and 0.2 gluon contribution represents 0, 10 and 40%. Value empirically known ∆∑≈0.2-0.35 does not exclude any of these possibilities.
CQSM-chiral quark soliton model:
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Orbital motion of quarks well fits to other motionslike orbital motion of electrons…Orbital motion of quarks well fits to other motionslike orbital motion of electrons…
He
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…or like orbital motion of nucleons…or like orbital motion of nucleons
He
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Orbital motion of quarksOrbital motion of quarks
He
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Orbital motion of everything…Orbital motion of everything…
He
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SummarySummary
Covariant version of QPM involving quark orbital motion was studied. New (LO) results:
Model allows to calculate 3D quark momenta distributions (in proton rest frame) from the structure functions.
Important role of quark orbital motion, which follows from covariant approach, was pointed out. Orbital momentum can represent as much as 2/3 j. The spin function g1 is reduced correspondingly.
Important consequence for the composition of proton spin was suggested.
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Thank you! Thank you!