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Longitudinal News from HERMES: Features and Byproducts of the D q(x) Reanalysis. Joshua G. Rubin University of Illinois RHIC/AGS Users’ Meeting June 1, 2009. A quick plug!. D g/g at HERMES!. When you can’t measure it from scaling ... ...and open-charm is nowhere to be found ...

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longitudinal news from hermes features and byproducts of the d q x reanalysis

Longitudinal News from HERMES:Features and Byproducts of the Dq(x) Reanalysis

Joshua G. Rubin

University of Illinois

RHIC/AGS Users’ Meeting

June 1, 2009

slide2

A quick plug!

Dg/g at HERMES!

When you can’t measure it from scaling...

...and open-charm is nowhere to be found...

...choose a model (PYTHIA), decompose your high pT data into subprocesses, and solve for Dg/g!

Joshua Rubin - RHIC/AGS - June 1, 2009

slide3

Coming to a theatre near you!

Now Back to “The NewDq(x)”

(Watch for an upcoming publication)

Joshua Rubin - RHIC/AGS - June 1, 2009

slide4

The HERMES Experiment

Event Trigger:

Hodoscopes and Calorimeter

Gas Target:

target = 1014 nuc/cm2

>80% polarization

Tracking Chambers

e

Hadron ID:

96-97 Threshold Cerenkov (p)

98-00 RICH (p, K, P)

Lepton Hadron Separation:

Calorimeter + TRD + Preshower

Joshua Rubin - RHIC/AGS - June 1, 2009

slide5

Deep-Inelastic Scattering and DIS Kinematics at HERMES

  • 27.6 GeV positron beam on deuterium gas target
  • ~ 53% Beam Polarization
  • ~ 82% Target Polarization

Thanks Halzen & Martin!

Joshua Rubin - RHIC/AGS - June 1, 2009

d q x and how to measure it
Dq(x) and How to Measure it

Experimental Asymmetry:

(A|| and A1 are related by depolarization and kinematic factors)

LO expression:

How can we get at Dq(x) then?!

Purity is probability that hadron h came from quark flavor q.

 Use correlation between struck quark and observed hadrons to flavor-tag events

Extract quark contributions withsemi-inclusive analysis

Take advantage of the hadrons!

The semi-inclusive version of A1:

Joshua Rubin - RHIC/AGS - June 1, 2009

to jog the memory the long paper
To jog the memory... “The Long Paper”
  • Highlights
    • First ever 5-flavor Dq(x) extraction
    • 9 x-bins for valence quarks, 7 for sea quarks
    • Rigorous unfolding procedure developed which removes detector and radiative smearing without assuming smoothness

Room for Improvement

    • Overlooked low-momentum deuterium data
    • Semi-inclusive kinematic dimensions unexplored. i.e. zh, ph┴
    • Bin-to-bin correlations and absence of smoothness assumption causes apparent error bar inflation
    • An attempt was made to overestimate the difficult-to-compute purity matrix systematic uncertainty. It was hoped that the subject could be revisited with more rigor.

A. Airapetian et al. Phys. Rev., D71:012003, 2005

Though the reanalysis is not complete, it has already yielded new results!

Joshua Rubin - RHIC/AGS - June 1, 2009

slide8

New Dimensions! (zh and ph┴)

Joshua Rubin - RHIC/AGS - June 1, 2009

slide9

What’s interesting about semi-inclusive kinematic variables?

Each x-bin can be divided into z and ph┴dimensions...

Highest energy hadron & fewest string breaks

Lowest energy hadrons & most string breaks

z and ph┴ yield information about the fragmentation process...

  • We’re looking at two features of this extended binning:
  • Quark-hadron correlations can be enhanced in the purity-based extraction of Dq(x) by identifying leading quark and remnant containing hadrons. Work in progress...
  • A1(ph┴) is interesting in itself! It yields information about the fragmentation pT and intrinsic kT.
  • New result!

Joshua Rubin - RHIC/AGS - June 1, 2009

what is p h of a final state hadron good for
What is ph┴of a final state hadron good for?
  • ph┴is interesting, but complicated!
  • It is a convolution of fragmentation pT(string breaks) and intrinsic kT(PDFs)
  • Any flavor dependence of kT unknown
  • Important for transverse momentum dependences (TMDs)
  • x and ph┴are not completely independent variables… apparent ph┴ dependence can result from different <x> in each ph┴bin.

Recent theoretical work:

  • M. Anselmino, A. Efremov, A. Kotzinian, and B. Parsamyan
    • Phys.Rev.D74:074015,2006.

Calculate

Construct

Assume

Joshua Rubin - RHIC/AGS - June 1, 2009

a 1 x p h new result
A1(x, ph┴ ) – New Result!
  • Binned in xandph┴to hold <x> more constant within an x-bin.
  • Points fit with and without ph┴ dependant term:

No significant ph┴ dependence observed

Joshua Rubin - RHIC/AGS - June 1, 2009

slide12

A More Robust Calculation of the Purity Matrix Systematic

Joshua Rubin - RHIC/AGS - June 1, 2009

tuning jetset the fragmentation monte carlo
Tuning JETSET, the Fragmentation Monte Carlo
  • Purity matrices, which encode the correlation between struck quark flavor and observed hadron type, are generated using a JETSET Monte Carlo.
  • JETSET is an implementation of the Lund-string phenomenological fragmentation model based on ~12 tunable parameters.
  • These parameters are tuned by minimizing a c2 comparison of MC to data multiplicities.
  • In the existing publication, the systematic uncertainty related to this tune was conservatively overestimated by comparing several tunes that poorly describe multiplicities in the HERMES kinematic regime. This was a major source of uncertainty in the publication.
  • The (unlikely) possibility of correlated parameters creating an ambiguous c2 minimum was not addressed at the time.

Joshua Rubin - RHIC/AGS - June 1, 2009

slide14

Correlating MC tune and Dq(x) systematic uncertainty

Purities

Dq(x)

1. Scanc2 surface around best Monte Carlo tune. Fit with quadratic Polynomial.

68% Contour

Best MC Tune

  • 2. Find 68% contour. Based on two factors:
    • Height of 68% of d-dimensional Gaussian Distribution.
    • The height of c2 minimum to accommodate model imperfection. PDG does something like this.

c2

c2min+C

c2min

parj b

parj a

3. ComputeDq(x) along contour:

The maximum deviation of Dq(x) from the best tune is the 68% uncertainty!

Joshua Rubin - RHIC/AGS - June 1, 2009

slide15

What locations on the 68% contour should be sampled?

68% Contour

This problem is similar to fitting global PDF parameterizations… Models typically have correlatedparameters.What do those guys do?! Look at CTEQ.

(J. Pumplin et al., JHEP 07 (2002) 012)

  • A & B are correlated parameters. The minimum in one depends on the location of the other
  • Compute Hessian matrix of second derivatives to find uncorrelated directions

Extract Dq(x) where uncorrelated parameter vectors cross 68% certainty contour. The greatest deviations represent Dq(x) tune systematic uncertainty.

Joshua Rubin - RHIC/AGS - June 1, 2009

slide16

The real thing…

  • Scan the c2 surface around the best Monte Carlo tune.
  • Correlations are quite clear between parameters
  • Generate and diagonalize the matrix of 2nd derivatives to find linear combinations that are uncorrelated

Jetset/Lund c2 surface in Fragmentation Parameter Basis

  • Blueellipses represent 68% contour
  • Coloredlines represent uncorrelated parameter directions

Joshua Rubin - RHIC/AGS - June 1, 2009

slide17

Revised Dq(x) uncertainty estimate

Published Dq(x) total systematic

PublishedDq(x) MC systematic

Difference between Dq(x) on 68% contour along Hessian vectors and at the c2 minimum.

We can move the old estimate down to the highest colored point!

In most bins, the tune-related systematic can be greatly reduced.

x

Joshua Rubin - RHIC/AGS - June 1, 2009

new related results on the way
New related results on the way!
  • Hadron charge difference asymmetries...
  • Complete Semi-Inclusive Longitudinal Double-Spin Asymmetries binned simultaneously in x, z, and ph┴

(of potentially more interest to the community than a modest improvement in the precision of Dq(x), right?!)

...if you trust the following fragmentation function symmetry:

(On the deuteron)

Similar to isoscalar Ds(x) extraction...

Joshua Rubin - RHIC/AGS - June 1, 2009

concluding remarks
Concluding Remarks
  • A1(ph┴ ) -- A first look at this interesting quantity
    • No dependence was observed.
    • Can we differentiate sources ofph┴ ? Can we learn something about flavor-dependence of intrinsic kT? Can we learn something meaningful about fragmentation?
  • Improved fragmentation model tune uncertainty
    • Uncertainty appears to be considerably smaller than published
    • Robust Hessian approach properly handles correlated parameters
  • New Goodies Soon!
    • Hadron Charge Difference Asymmetries  Alternative (Duv+Ddv)/(uv+dv)
    • Final A1h(x,z, ph┴ ) numbers to be made available on Durham.
  • Look out for a Dg/g publication from HERMES soon!

Joshua Rubin - RHIC/AGS - June 1, 2009

slide20

Extra slides…

Joshua Rubin - RHIC/AGS - June 1, 2009

slide21

Addressing Error Bar Inflation: Covariance and Smoothness

Joshua Rubin - RHIC/AGS - June 1, 2009

kinematic unfolding and the interpretation of uncertainties
Kinematic Unfolding and the Interpretation of Uncertainties

Published asymmetries from HERMES long Dq(x) paper fit with:

A1h (x) = C1 + C2 x

Born Bins (j)

  • The bin-to-bin unfolding procedure used in the long Dq(x) paper for A1(x):
    • Corrects radiative and detector smearing by tracking MC event bin migration
    • Makes no assumption of smoothness
  • Side-effect:
    • Statistical errors correlated and considerably larger than those of raw asymmetry

When A1 is fit with a smooth function and statistical covariance is taken into account (blue band), inflated uncertainties are reduced.

Joshua Rubin - RHIC/AGS - June 1, 2009

fits to the quark polarizations
Fits to the Quark Polarizations
  • Helicity densities fitted with xDq(x) = C1 xc2 (1-x)c3
  • Data points have rigorous model-independent uncertainties (and associated covariance)
  • Fits give a more reasonable impression of the true statistical significance of the data taking into account covariance and (reasonably) assuming smooth physics
  • Statistical covariance is crucial when interpreting data. Fit uncertainty can be overestimated without including covariance (pink band). Fit central values are affected as well.
  • Do utilize provided covariance info when interpreting data!

(Simulated data points for illustrative purposes only!)

Joshua Rubin - RHIC/AGS - June 1, 2009

slide25

What do we know about A1(ph┴) so far?

From: Harut Avakian, “Studies on transverse spin effects at Jlab”,

QCD Structure of the Nucleon June 12-16, 2006, Rome

CLAS sees clear ph┴ dependence of A1

  • Some care was taken to correct for the varying x-dependence in in each ph┴ -bin.
  • CLAS result is at a significantly lower W and higher x thanHERMES

Joshua Rubin - RHIC/AGS - June 1, 2009

slide26

The Gluon Polarization

(Thanks Elke!)

Joshua Rubin - RHIC/AGS - June 1, 2009

strategies for accessing d g g in ep
Strategies for accessing Dg/g in ep
  • Q2 Scaling of Asymmetries

Limited Q2 coverage (when compare to unpolarized case!). Gluon polarization poorly constrained

  • Golden channels. i.e. Isolate a single process involving a gluon with a known cross section– e.g. open charm isolates photon-gluon fusion.

Not enough statistics at HERMES kinematics

  • Model the Spectrum of Processes at high pT
    • Enhances perterbative gluon signal processes
    • Suppresses soft processes

Use Monte Carlo (PYTHIA) to do this!

Joshua Rubin - RHIC/AGS - June 1, 2009

processes with sensitivity to d g g
Processes with Sensitivity to Dg/g

PGF

VMD

Anomalous-q

Joshua Rubin - RHIC/AGS - June 1, 2009

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