24
Mitglied der Helmholtz- Gemeinschaft Measurement of the Spin- Dependence of the pp Interaction at the AD Ring Polarizing antiprotons May 12, 2009 Paolo Lenisa and Frank Rathmann PAX collaboration New Opportunities in the Physics Landscape at CERN

May 12, 2009 Paolo Lenisa and Frank Rathmann PAX collaboration

  • Upload
    shea

  • View
    34

  • Download
    0

Embed Size (px)

DESCRIPTION

Measurement of the Spin- Dependence of the pp Interaction at the AD Ring Polarizing antiprotons. May 12, 2009 Paolo Lenisa and Frank Rathmann PAX collaboration New Opportunities in the Physics Landscape at CERN. Introduction. - PowerPoint PPT Presentation

Citation preview

Page 1: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Mitg

lied

der H

elm

holtz

-Gem

eins

chaf

t

Measurement of the Spin-Dependence of the pp Interaction at the AD Ring

Polarizing antiprotons

May 12, 2009 Paolo Lenisa and Frank Rathmann PAX collaboration

New Opportunities in the Physics Landscape at CERN

Page 2: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 2

Introduction

We have proposed a method to polarize antiprotons by

„spin-filtering“

Frank Rathmann

Page 3: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 3

(How) is it possible to provide polarized antiproton beams

in HESR ?High Energy Storage Ring (HESR)

for a beam of antiprotons

Frank Rathmann

Introduction

New initiative, driven by the FAIR-project at GSI

Page 4: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 4Frank Rathmann

Physics Case: Transversity distribution of the nucleon in Drell-Yan:

Last leading-twist missing piece of the QCD description of the partonic structure of the nucleon

Direct measurement of h1q

(x,Q2) of the proton for valence quarks (ATT in Drell-Yan >0.2)

transversely polarized proton beam or target () transversely polarized antiproton beam ()

+ other polarization observables in pp

HESRPAX → Polarized Antiprotons

QCD Physics at FAIR employs unpolarized Antiprotons

Page 5: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 5

Plan of talk

Polarizing antiprotons …

Proposals, ideas, calculations, … Experiments

FILTEX (TSR)ep spin flip cross section measurement at COSYSpin-filtering at AD/CERN

Conclusion

Task taken on by the PAX-collaboration: ~100 members, 16 institutions Spokespersons: P. Lenisa (Ferrara), F. Rathmann (Jülich)

Frank Rathmann

Page 6: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 6

Two Methods: Loss versus spin flip

For an ensemble of spin ½ particles with projections + () and – ()

Frank Rathmann

Page 7: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 7

Proposed methods: Spin flip

→ Need for an experimental test of this idea!

Frank Rathmann

Page 8: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 8

ep spin flip cross section measurement at COSY

No effect observed: measured cross sections at least 6 orders-of-magnitude smaller than predicted 1013 b.

0

4107

|Relative velocity of electrons in proton rest frame| (c)

dep

ol (b

arn)

Nominal proton energy in electron rest frame (keV)0 1 2 3

0 110-3 210-3 310-3

2107

-2107

-4107

Frank Rathmann

D.Oellers et al., Physics Letters B 674 (2009) 269

Meanwhile, Mainz group discovered numerical problems in the calculation → two errata.

Page 9: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 9

Spin-filtering

Polarization build-up of an initially unpolarized particle beam by repeated passage through a polarized hydrogen target in a storage ring:

Frank Rathmann

Page 10: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 10

Spin-filtering at TSR: „FILTEX“ – proof-of-principle

→ Spin filtering works for protons

F. Rathmann et al., PRL 71, 1379 (1993)

Frank Rathmann

PAX submitted new proposal to find out how well spin filtering works for antiprotons: Measurement of the Spin-Dependence of the pp Interaction at the AD Ring

(CERN-SPSC-2009-012 / SPSC-P-337)

Page 11: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 11

PAX at the AD (the only place worldwide)

Frank Rathmann

PAX target sectionElectron cooler

Siberian snake

Page 12: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 12Frank Rathmann

Experimental Setup

Atomic Beam Source

Six additional quadrupolesBreit-Rabi

Polarimeter

Target chamber:Detector system + storage cell

Page 13: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 13

Expected Polarizations after filtering for two lifetimestransverse

A

D

Frank Rathmann

longitudinal

d (mm) Θacc (mrad)

8 8.610 10.812 13.0

• Measurement of the buildup equivalent to the determination of σ1 and σ2 • Once a polarized antiproton beam is available, differential double-spin

observables can be measured (50-500 MeV) → pp potential.• Protonium gave already first information about pp potential at rest.

Page 14: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 14

Time plan (once approved)

Frank Rathmann

Phase Time Description

1 Shutdown 2009/102010

Installation of six magnets for the low-β insertion.Commissioning of the low-β section, carried out parasitically.

2a

2b

Shutdown 2010/112 weeks in 20113 weeks in 2011Shutdown 2011/122 weeks in 2012

Installation of the target chamber. Machine acceptance studies. Stacking studies (split in sessions).Installation of ABS, BRP, and detector system.Measurement of H target polarization with antiproton beam.

3 6 weeks in 2012 Spin-filtering measurements using H and D target up to 70 MeV with transverse beam polarization.

4 Shutdown 2012/13

4 weeks in 2013

Shutdown possibly extended up to six months. Implementation and commissioning of electron cooler upgrade to 300 keV.Commissioning of the electron cooler with beam.

5 6 weeks in 2013 Spin-filtering measurements using H and D target up to 430 MeV with transverse beam polarization.

6 Shutdown 2013/14 Implementation of the Siberian snake.

7 8 weeks in 2014 Spin-filtering measurements with H and D target up to 430 MeV with longitudinal beam polarization.

• PAX ready to set sequence into motion by installing low-β section into the AD end of this year!

Proof of compatibility with the other AD users.

Page 15: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 15

Conclusions

• Clear task • Technically feasible• Expertise and commitment by PAX-collaboration• First measurements/achievements• High discovery potential

Now and here or never!

Frank Rathmann

Page 16: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 16

Spare transparencies

Frank Rathmann

Page 17: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 17Frank Rathmann

Page 18: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

18

Expected antiproton beam polarization(in an ideal machine)

• AD machine acceptance: Ax=180 m, Ay=200 m

• Cooled 2 beam emittance = 1 m

• Realistic calculation of acc(mrad) using AD lattice functions and triangular density distribution in storage cell

• Model A: T. Hippchen et al., Phys. Rev. C 44, 1323 (1991)

• Model D: V. Mull, K. Holinde, Phys. Rev. C 51, 2360 (1995)

Polarizing antiprotonsFrank Rathmann

0 2 4 6 8 100

10

20

Storage cell radius (mm)

Acc

epta

nce

angl

e (m

rad)

8

Page 19: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 19

Beam lifetime

Frank Rathmann

d (mm) Θacc (mrad)

8 8.610 10.812 13.0

Page 20: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 20

Target chamber, cell and detector system

Frank Rathmann

Storage cellSilicon strip detectors

Atomic beam

Stored beam

Page 21: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 21

Phase 1

• Central quadrupole magnet (QDN15) remains in place until compatibility of the AD operation with other users is shown.

Frank Rathmann

Page 22: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 22

Hadron Physics „Dream Machine“ for FAIR:

… an asymmetric (double-polarized) proton (15 GeV/c) – antiproton (3.5 GeV/c) collider

using HESR, CSR and APR

Frank Rathmann

Page 23: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 23

Quark Transversity Distribution in Drell-Yan:

Double transverse spin asymmetry:

llqq *

First direct measurement: No competitive processes

Frank Rathmann

Page 24: May 12, 2009  Paolo  Lenisa and  Frank  Rathmann PAX  collaboration

Polarizing antiprotons 24

Proposed methods (1): Some history …

EPAC 1988

Stern-Gerlach splitting never tried (huge effort)

Frank Rathmann