Top Banner
Proton spin Proton spin structure structure and intrinsic motion and intrinsic motion of constituents of constituents Petr Závada Inst. of Physics, Prague
29

Proton spin structure and intrinsic motion of constituents

Dec 30, 2015

Download

Documents

joel-mays

Proton spin structure and intrinsic motion of constituents. P etr Z ávada Inst. of Physics, Prague. DIS2004. Introduction. - PowerPoint PPT Presentation
Welcome message from author
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Page 1: Proton spin structure  and intrinsic motion of constituents

Proton spin structure Proton spin structure and intrinsic motionand intrinsic motion

of constituentsof constituents

Petr ZávadaInst. of Physics, Prague

Page 2: Proton spin structure  and intrinsic motion of constituents

IntroductionIntroduction

Presented results follow from QPM, in which (valence) quarks are considered as quasifree fermions on mass shell, with effective mass x0=m/M. Momenta distributions describing intrinsic quark motion have spherical symmetry and constraint J=1/2 is applied. The model is constructed in consistently covariant way [for details see P.Z. Phys.Rev.D65,054040(2002) and D67,014019(2003)]. In this talk some properties of spin functions obtained in the model will be discussed:

Sum rules for g1,g2 g1,g2 from valence quarks, comparison with experimental

data Discussion about Γ1 and standard naïve QPM model Transversity

Page 3: Proton spin structure  and intrinsic motion of constituents

ModelModel

Input:

Page 4: Proton spin structure  and intrinsic motion of constituents

Output:

Model

Page 5: Proton spin structure  and intrinsic motion of constituents

CommentsComments

…procedure complex, but unambiguous, task is well-defined.

As a result there is a naïve QPM, improved not by QCD dynamic, but in kinematics: covariance + spheric symmetry constrained by J=1/2.

We shall try to demonstrate, that it is also very important...

Page 6: Proton spin structure  and intrinsic motion of constituents

Sum rulesSum rules Basis:

Page 7: Proton spin structure  and intrinsic motion of constituents

Sum rules

Page 8: Proton spin structure  and intrinsic motion of constituents

Sum rules

Page 9: Proton spin structure  and intrinsic motion of constituents

CommentComment

… all these rules were here obtained from covariant kinematics and rotational symmetry, J=1/2.

Page 10: Proton spin structure  and intrinsic motion of constituents

Valence quarksValence quarks

Page 11: Proton spin structure  and intrinsic motion of constituents

Valence quarks

Page 12: Proton spin structure  and intrinsic motion of constituents

Valence quarks

Page 13: Proton spin structure  and intrinsic motion of constituents

Valence quarksValence quarks

Calculation - solid line, data - dashed lineCalculation - solid line, data - dashed line (left) and circles (right)(left) and circles (right)

E155E155

Page 14: Proton spin structure  and intrinsic motion of constituents

g1 - analysisg1 - analysis

Integrating g1 gives:

… …so, it seems: more motion=less spin? so, it seems: more motion=less spin?

How to understand it?How to understand it?

staticstaticquarksquarks

masslessmasslessquarksquarks

Page 15: Proton spin structure  and intrinsic motion of constituents

Lesson of QMLesson of QM Forget structure functions for a while and calculate another task. Remember, that 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 relativistic spherical waves:

Page 16: Proton spin structure  and intrinsic motion of constituents

Lesson of QM

Page 17: Proton spin structure  and intrinsic motion of constituents

Lesson of QM

Page 18: Proton spin structure  and intrinsic motion of constituents

Spin and intrinsic motionSpin and intrinsic motion

j=1/2j=1/2 j=1/2j=1/2

m=pm=p00m≈0m≈0

j=l+sj=l+s1≥1≥‹‹ss››/j≥1/3/j≥1/3

QM:QM:ForFor pp00>m >m there there mustmust bebe some some

orbital momentum!orbital momentum!

Page 19: Proton spin structure  and intrinsic motion of constituents

Comparison with standard approachComparison with standard approach

Page 20: Proton spin structure  and intrinsic motion of constituents

CommentComment

Results suggest, that proton structure functions g1 and g2 can have a simple and natural interpretation even in terms of a naive QPM, provided that the model is based on a consistently covariant formulation, which takes into account intrinsic motion and spheric symmetry connected with the constraint J=1/2. This is not satisfied for standard formulation of QPM, which is based on simplified one-dimensional kinematics related only to the preferred reference system (infinite momentum frame). As a result, there is e.g. the known fact, that function g2 has no well-defined meaning in the standard naive QPM. In this case it is just result of simplified kinematics and not because of absence of dynamics.

Page 21: Proton spin structure  and intrinsic motion of constituents

SummarySummary

Page 22: Proton spin structure  and intrinsic motion of constituents
Page 23: Proton spin structure  and intrinsic motion of constituents

Transversity(preliminary, P.Z.+A.Efremov, O.Teryaev)

First, remind our procedure for g1, g2 :

Page 24: Proton spin structure  and intrinsic motion of constituents

Transversity may be related to auxiliary polarized process described by interference of axial vector and scalar currents. (see G.R.G.R. Goldstein, R.L.Goldstein, R.L. Jaffe and X.D.Jaffe and X.D. Ji, Phys. Rev. D 52, 5006 Ji, Phys. Rev. D 52, 5006 (1995);(1995); B.L.B.L. Ioffe and A.Ioffe and A. Khodjamirian, Phys. Rev. D 51, 3373 Khodjamirian, Phys. Rev. D 51, 3373 (1995)(1995)). We try to use simplest form of such vector, giving:

Page 25: Proton spin structure  and intrinsic motion of constituents

Using technique of integral transforms gives: Using technique of integral transforms gives:

Page 26: Proton spin structure  and intrinsic motion of constituents

Dashed line – from g1 Full line – from qv Dotted – calculation by P.Schweitzer, D.Urbano, M.V.Polyakov,

C.Weiss, P.V.Pobylitsa and K.Goeke, Phys.Rev. D 64, 034013 (2001).

CalculationCalculation

Page 27: Proton spin structure  and intrinsic motion of constituents

But generally, obtained functions (in particular d-quarks) may not satisfy Soffer inequality. Why? One should consistently take into account interference nature of transversity…

Page 28: Proton spin structure  and intrinsic motion of constituents

Transversity based on the expression…Transversity based on the expression…

satisfies Soffer bound, in fact it satisfies a new, more strict limit…satisfies Soffer bound, in fact it satisfies a new, more strict limit…

Page 29: Proton spin structure  and intrinsic motion of constituents

Calculation Dashed line – Soffer bound Full line – δqmax Both limits are equivalent either for static quarks or for

pure states with polarization +.