touschek polarimeter for beam energy measurement of vepp ... · outline 1 introduction 2 resonance...

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Touschek polarimeter for beam energy measurement of VEPP-4M collider Ivan Nikolaev Budker Institute of Nuclear Physics Novosibirsk, Russia Frascati Spring School ”Bruno Touschek” May 12-16 2008 Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M collider LNFSS-08 1 / 16

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Page 1: Touschek polarimeter for beam energy measurement of VEPP ... · Outline 1 Introduction 2 Resonance depolarization method (RDM) 3 Intra-beam scattering 4 VEPP-4M accelerating-storage

Touschek polarimeter for beam energy measurement ofVEPP-4M collider

Ivan Nikolaev

Budker Institute of Nuclear PhysicsNovosibirsk, Russia

Frascati Spring School ”Bruno Touschek”May 12-16 2008

Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M colliderLNFSS-08 1 / 16

Page 2: Touschek polarimeter for beam energy measurement of VEPP ... · Outline 1 Introduction 2 Resonance depolarization method (RDM) 3 Intra-beam scattering 4 VEPP-4M accelerating-storage

Outline

1 Introduction

2 Resonance depolarization method (RDM)

3 Intra-beam scattering

4 VEPP-4M accelerating-storage complex

5 Touschek polarimeter

6 Energy calibration

7 Energy interpolation

8 Application of RDM in experiments with KEDR detector

9 Summary

Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M colliderLNFSS-08 2 / 16

Page 3: Touschek polarimeter for beam energy measurement of VEPP ... · Outline 1 Introduction 2 Resonance depolarization method (RDM) 3 Intra-beam scattering 4 VEPP-4M accelerating-storage

Introduction

High precission measurement of masses of J/ψ, ψ′,ψ′′, D mesons andτ -lepton is very important:

Metrology and spectroscopy

Theory test (QCD and Lepton universality)

Calibration of energy scale of accelerators.

It requires absolute calibration of collider’s energy.

Resonance depolarization method: BINP Novosibirsk Russia, 1975:K±, K 0, ω, φ, J/ψ, ψ′, Υ, Υ′, Υ′′

∆m

m= 10−4 ÷ 4× 10−6

Applied at VEPP-2(M), VEPP-4(M), DORIS-II, CESR, LEP,BESSY-II, SLS, ALS.

Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M colliderLNFSS-08 3 / 16

Page 4: Touschek polarimeter for beam energy measurement of VEPP ... · Outline 1 Introduction 2 Resonance depolarization method (RDM) 3 Intra-beam scattering 4 VEPP-4M accelerating-storage

Resonance depolarization method (RDM)

Spin precession frequency depends on beam energy:

Ωspin = Ω0(1 + γµ′

µ0)

Ω0 — revolution frequency, µ0,µ′ — normal and anomal part ofelectron magnetic moment, γ = E/me

Sokolov-Ternov radiation polarization, 1964:

1

τpol' 5√

3

8

λerec

R3γ5

Polarization is destructed by external electromagnetic field withfrequency Ωdep:

Ωspin = nΩ0 + Ωdep, n ∈ Z

Ωs is measured at the moment of depolarization during Ωdep

frequency scan.Polarization destruction can be detected on jump in the rate ofintra-beam scattering.

Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M colliderLNFSS-08 4 / 16

Page 5: Touschek polarimeter for beam energy measurement of VEPP ... · Outline 1 Introduction 2 Resonance depolarization method (RDM) 3 Intra-beam scattering 4 VEPP-4M accelerating-storage

Intra-beam scattering (Touschek effect)

Cross section of intra-beam scattering depends on polarization ofscattered particles:

dΩ=

4r20

v4

(4

sin4 θ− 3

sin2 θ−

~ζ1 ~ζ2

sin2 θ

)

Scattered particles hit scitillator counters

Counting rate:

N =

√πr2

0 cN2

γ5V (σp/p)3

(I1 + ζ2I2

)Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M colliderLNFSS-08 5 / 16

Page 6: Touschek polarimeter for beam energy measurement of VEPP ... · Outline 1 Introduction 2 Resonance depolarization method (RDM) 3 Intra-beam scattering 4 VEPP-4M accelerating-storage

VEPP-4 accelerating-storage complex

Linear accelerator LINAC(50 MeV).

booster synchrotron(350 MeV).

VEPP-3 storage ring(2 GeV).

VEPP-4M collider

Beam energy 1÷ 6 GeV

Bunch number 2× 2

Luminocity,E = 1.5 GeV: 2× 1030

Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M colliderLNFSS-08 6 / 16

Page 7: Touschek polarimeter for beam energy measurement of VEPP ... · Outline 1 Introduction 2 Resonance depolarization method (RDM) 3 Intra-beam scattering 4 VEPP-4M accelerating-storage

Touschek polarimeter

4 pairs of scintillator counters are located in different places ofVEPP-4M. Due to correlation between counters we use only 2 ofthem.

Counting rate is 50÷ 100 kHz/mA2 per counter.

Total counting rate is 0.5− 1.5 MHz.

Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M colliderLNFSS-08 7 / 16

Page 8: Touschek polarimeter for beam energy measurement of VEPP ... · Outline 1 Introduction 2 Resonance depolarization method (RDM) 3 Intra-beam scattering 4 VEPP-4M accelerating-storage

Energy calibration procedure

Prepare polarized beam in VEPP-3 storage ring ( 2000 sec). Injectit into VEPP-4M.

Prepare unpolarized beam.

Equalize currents in polarized and unpolarized beam.

Monitor relative difference of counting rate of polarized andunpolarized beams.

∆ =Npol − Nunpol

Nunpol

Turn on the depolarizer and change Ωdep in a region where resonancedepolarization expected.

Find and fit jump in counting rate.

Accuracy of single energy calibration

σE = 1 keV ∼ 5× 10−7

Two energy calibrations using same bunches (partial depolarization).

Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M colliderLNFSS-08 8 / 16

Page 9: Touschek polarimeter for beam energy measurement of VEPP ... · Outline 1 Introduction 2 Resonance depolarization method (RDM) 3 Intra-beam scattering 4 VEPP-4M accelerating-storage

Example of energy calibration at τ

Tcount = 13 sec

speed = 0.0003 MeV/sec

step = 0.00075 MeV

initial = 1777.47 MeV

final = 1777.544 MeV

Att = 13 dB

2005-05-12 20:14:10Run 1589

TECU1780.05

H = 1705.919

NEM = 2149.013

SEM = 2138.1

SIM = 2287.158

EM3 = 2474.585

KEDR1 = 6520.76

KEDR2 = -1 RF = 181801194 Hz

U = 323.57 kV J = 7.83 A

Qx = 0.531005 Qz = 0.577331

TZ = -0.126246 mm I1 = 2.224 mA I2 = 2.33 mA

DV4OUT=39.531 C

In = 102.68585 kHz

Out = 61.842769 kHz

33.26 kHz/mA^2

E = (1777.501112+-0.00104)Mev Fd = (-791219.637+-1.94)Hz

0 50 100 150 200 250 3000 50 100 150 200 250 300-0.02

-0.015

-0.01

-0.005

0 / ndf 2χ 11.97 / 17

T 2.1± 157.3 DELTA 0.0009506± 0.01237 CONST 0.0005727± -0.01549 SLOPE1 6.211e-06± 6.555e-06 SLOPE2 9.604e-06± 1.402e-05

/ ndf 2χ 11.97 / 17T 2.1± 157.3 DELTA 0.0009506± 0.01237 CONST 0.0005727± -0.01549 SLOPE1 6.211e-06± 6.555e-06 SLOPE2 9.604e-06± 1.402e-05

delta-1

1777

.469

845

1777

.473

595

1777

.477

345

1777

.481

845

1777

.485

595

1777

.489

345

1777

.493

095

1777

.496

845

1777

.500

595

1777

.505

095

1777

.508

845

1777

.512

595

1777

.516

345

1777

.520

095

1777

.523

845

1777

.528

345

1777

.532

095

1777

.535

845

1777

.539

595

Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M colliderLNFSS-08 9 / 16

Page 10: Touschek polarimeter for beam energy measurement of VEPP ... · Outline 1 Introduction 2 Resonance depolarization method (RDM) 3 Intra-beam scattering 4 VEPP-4M accelerating-storage

Energy interpolation between calibrations

E = αHH(1 + αT ∆T ) +∑

i

αi∆Pi

H - guiding magnetic field in calibrating magnet measured by NMRmethod

∆T = TCM − TRING , TRING - average temperature of acceleratorsmagnets.

Pi are:

Temperature of VEPP-4M tunnel.

Temperature of cooling distilled water

Average radial orbit

Air,tech water temperatures,. . .

Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M colliderLNFSS-08 10 / 16

Page 11: Touschek polarimeter for beam energy measurement of VEPP ... · Outline 1 Introduction 2 Resonance depolarization method (RDM) 3 Intra-beam scattering 4 VEPP-4M accelerating-storage

Examples of energy interpolation

VEPP-4M energy in tau mass experiment.

200626/12

200627/12

200628/12

200629/12

200630/12

200631/12

200701/01

1776.6

1776.8

1777.0

1777.2

1777.4

VEPP-4M energy reconstructed energy

energy calibrations

CBS

Difference between interpolated energy and the measured energy with allaperiodic dependeces accounted (J/ψ mass experiment)

Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M colliderLNFSS-08 11 / 16

Page 12: Touschek polarimeter for beam energy measurement of VEPP ... · Outline 1 Introduction 2 Resonance depolarization method (RDM) 3 Intra-beam scattering 4 VEPP-4M accelerating-storage

Application of RDM in experiments with KEDR detector

Charmonium masses

2002: Scan of J/ψ (40 nb−1)

2002: Scan of ψ′ (76nb−1)

2005: J/ψ (230nb−1)

2004-2006: 3 scan of ψ′ (230nb−1)

2004: ψ(3770)

Tau mass

2005-2007: 5.2pb−1

Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M colliderLNFSS-08 12 / 16

Page 13: Touschek polarimeter for beam energy measurement of VEPP ... · Outline 1 Introduction 2 Resonance depolarization method (RDM) 3 Intra-beam scattering 4 VEPP-4M accelerating-storage

KEDR detector

1 Vacuum chamber2 Vertex detector3 Drift chamber4 Aerogel Cherenkov

counters5 TOF scintillation

counters6 LKr barrel calorimeter7 Superconducting coil (6

kGs)8 Magnet yoke9 Muon tubes10 CsI end cap calorimeter11 Compensating solenoid12 Quadrupole

Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M colliderLNFSS-08 13 / 16

Page 14: Touschek polarimeter for beam energy measurement of VEPP ... · Outline 1 Introduction 2 Resonance depolarization method (RDM) 3 Intra-beam scattering 4 VEPP-4M accelerating-storage

J/ψ , ψ′,ψ′′ mesons mass measurement.

MJ/ψ = 3096.917± 0.01± 0.007 MeV (2002)

Mψ(2S) = 3686.117± 0.012± 0.015 MeV (preliminary)

Mψ(3770) = 3773.5± 0.9± 0.6 MeV (preliminary)

Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M colliderLNFSS-08 14 / 16

Page 15: Touschek polarimeter for beam energy measurement of VEPP ... · Outline 1 Introduction 2 Resonance depolarization method (RDM) 3 Intra-beam scattering 4 VEPP-4M accelerating-storage

Tau mass measurement

Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M colliderLNFSS-08 15 / 16

Page 16: Touschek polarimeter for beam energy measurement of VEPP ... · Outline 1 Introduction 2 Resonance depolarization method (RDM) 3 Intra-beam scattering 4 VEPP-4M accelerating-storage

Summary

Accuracy of single energy calibration is around 1 keV 5× 10−7

More than 2k calibrations done.

Touschek polarimeter is succesfuly applied for high precisioncharmonium and tau masses measurement with KEDR detector.

Accuracy of VEPP-4M energy interpolation is 7 keV for charmoniummass measurement and 30 keV for tau mass measurement.

Ivan Nikolaev (BINP SB RAS) Touschek polarimeter for beam energy measurement of VEPP-4M colliderLNFSS-08 16 / 16