Polarimetry Design Updates

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IPBI 6 April 05 Ken Moffeit Polarimetry Design Updates - Dispersion in upstream chicane - 20mrad extraction line 0.75 mrad beam stay clear location of Synchrotron Radiation Stripe Detector Comments about Shielding Number of Cells for Cerenkov Detector Better R22 etc - 2mrad extraction line R22 issues Energy and Polarimeter Chicanes - aligning the Compton IP Comments about surveying and tolerance for direction at Compton IPs. IPBI Meeting 6 April 05 Ken Moffeit

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Polarimetry Design Updates. IPBI Meeting 6 April 05 Ken Moffeit. - Dispersion in upstream chicane - 20mrad extraction line 0.75 mrad beam stay clear location of Synchrotron Radiation Stripe Detector Comments about Shielding Number of Cells for Cerenkov Detector - PowerPoint PPT Presentation

Transcript of Polarimetry Design Updates

Page 1: Polarimetry Design Updates

IPBI 6 April 05 Ken Moffeit

Polarimetry Design Updates

- Dispersion in upstream chicane - 20mrad extraction line

0.75 mrad beam stay clearlocation of Synchrotron Radiation Stripe DetectorComments about ShieldingNumber of Cells for Cerenkov DetectorBetter R22 etc

- 2mrad extraction line R22 issuesEnergy and Polarimeter Chicanes

- aligning the Compton IPComments about surveying and tolerance for direction at Compton IPs.

IPBI Meeting6 April 05

Ken Moffeit

Page 2: Polarimetry Design Updates

IPBI 6 April 05 Ken Moffeit

Upstream Polarimeter with Dispersion = 5 mm

BPC1s = 711.595 m

BPC2730.695 m K Moffeit 31 Apr 05

UpstreamPolarimeter Chicane

10 cm

10 meters

CerenkovDetector

Compton IP250 GeVx = 5 mm

3 cm

Plan View

Angle = 0.24272 mrad

BPC3738.095 m

BPC4760.195 m

250 GeVAngle = 0.24272 mrad

25 GeVAngle = 2.4272 mrad

35 GeVAngle = 1.73371 mrad

4.5 cm

Page 3: Polarimetry Design Updates

IPBI 6 April 05 Ken Moffeit

Dispersion 5mm > 20mm2 is 16 times larger

R(20mm) = R(5mm)/4R3 (20mm)= R3 (5mm)/32Emittance(20mm) = 45 Emit (5mm)

Slide from Ray Arnold

Upstream Polarimeter Emittance Growth versus Dispersion

Page 4: Polarimetry Design Updates

IPBI 6 April 05 Ken Moffeit

Emittance Growth versus Dispersion

Hor

izon

tal E

mitt

ance

Gro

wth

Chicane Dispersion (mm)

Mark Woodley

0

10%

20%

30%

0 10 20

For eta=20mm & 500 GeV beam: Short bend has pole-tip field of 5.4 kG;

Long bend is half of that.

Magnets ok for higher dispersion.

Page 5: Polarimetry Design Updates

IPBI 6 April 05 Ken Moffeit

Upstream Polarimeter with dispersion = 10 mm

BPC1s = 711.595 m

BPC2730.695 m K Moffeit 4 Apr 05

UpstreamPolarimeter Chicane

10 cm

10 meters

CerenkovDetector

Compton IP250 GeV

x = 10 mm

6.14 cm

Plan View

Angle = 0.48544 mrad

BPC3738.095 m

BPC4738.095 m

250 GeVAngle = 0.48544 mrad

25 GeVAngle = 4.8544 mrad

35 GeVAngle = 3.46742 mrad

7.9 cm

3.5 cm

Page 6: Polarimetry Design Updates

IPBI 6 April 05 Ken Moffeit

Space for Laser Beam Insertion/exit

Only 1.4 meters between the inner dipoles is unacceptable. Peter Schuler needs a nominal 8 meters of space (or 14 meter between magnet centers) for the laser beam insertion/exit.This is to accomodate a crossing angle of 10 mrad, and keep the optics away from any synchrotron radiation. These conditions accomodate a vertical beam crossing, but retain a minimal magnet gap height of only 20 mm for all dipoles.

Page 7: Polarimetry Design Updates

IPBI 6 April 05 Ken Moffeit

10 mm dispersion and 8m for laser input

BPC1s = 711.595 m

BPC2730.695 m K Moffeit 4 Apr 05

UpstreamPolarimeter Chicane

10 cm

10 meters

CerenkovDetector

Compton IP250 GeV

x = 10 mm

6.14 cm

Plan View

Angle = 0.48544 mrad

BPC3~745 m

BPC4~767 m

250 GeVAngle = 0.48544 mrad

25 GeVAngle = 4.8544 mrad

35 GeVAngle = 3.46742 mrad

7.9 cm

3.5 cm

8meters

Page 8: Polarimetry Design Updates

IPBI 6 April 05 Ken Moffeit

20 mrad Extraction Line

Eight Cerenkov Cells 1 cm wide Six cover the region between 36 GeV (12 cm from beam line) 25.1 GeV (17.8 cm)And 2 outside the kinematic limit

Location of Synchrotron Detector

Cerenkov Detector Shielding issues:Cells closest to beam pipe will see Synchrotron Radiation (below 10 MeV?)

250 GeV

25 GeV

45.59 GeV

K Moffeit 4 Apr 05

2 mradenergystripe

2 mradenergystripeBVX1

z=59.69 m

3 mradenergystripe

3 mradenergystripe

Shielding

Energy Chicane

Polarimeter Chicane

10 cm

10 meters

SynchrotronStripe Detector

SynchrotronStripe Detector

CerenkovDetector

Wiggler

Low Field

25.1 GeV

BVX2z=61.99 m

BLEXz=64.29 m

BLEXz=66.89 m

WEX1z=65.59 m

0.75mrad

BVX3z=68.19 m

BVX4z=70.49 m

BVX5z=72.79 m

BVX6z=75.09 m

BLEXz=77.39 m

BLEXz=79.99 m

WEX1z=78.69 m

BVX7z=81.29 m

BPM BPM

BVX8z=83.59 m

BVX9z=100.59 m

BVY1z=120.59 m

BVY2z=132.59 m

BVY3z=152.59 m

Compton IP

17.8cm

QFX4z=156.59 m

0.75mrad

35.7 GeV 12.0cm

Synchrotron StripeDetector z=143.69 m

Page 9: Polarimetry Design Updates

IPBI 6 April 05 Ken Moffeit

LCWS Mar 05 Yuri Nosochkov

Original Optics Improved R22 Optics

bad

Good

Page 10: Polarimetry Design Updates

IPBI 6 April 05 Ken Moffeit

Yuri Nosochkov (5 April 05)

Most Recent Optics LCWS Improved R22 Optics

GoodNot Good > Lose 1cm at Cerenkov Det1st Cell starts at 13 cm instead of 12 cm2 mrad synchrotrotron swipe barely gets out of 0.75 mrad beam stay clear

Page 11: Polarimetry Design Updates

IPBI 6 April 05 Ken Moffeit

2mrad extraction line R22 issues Energy and Polarimeter Chicanes

K Moffeit 12 Mar 05

Polarimeter ChicanePlan View

10 m

10 cm

BHEX3Az=180.06 mx=106.20 cm

BHEX3Bz=182.36 mx=107.57 cm

BHEX3Cz=184.66 mx=108.56 cm

BHEX4Bz=198.96 mx=111.81 cm

BHEX4Az=196.67 mx=111.12 cm

BHEX4Cz=201.26 mx=112.88 cm

BHEX4Dz=203.56 mx=114.35 cm

BHEX4Ez=205.86 mx=116.22 cm

Compton IPAngle 8.850 mrad

Angle 7.138 mrad

Angle 5.425 mrad

Angle 3.712 mradAngle 2.0 mrad

Angle 3.621 mrad

Angle 5.242 mrad

Angle 6.863 mrad

Angle 2.0 mradat IR

Focusz=191.66 mx=110.12 cm

25 GeV

CerenkovDetector

Optics ImprovementR22 ~ 1.3 nowNeed R22 ~ 0.5

Expand 2 mrad section to include Energy chicane Polarimeter chicane

Page 12: Polarimetry Design Updates

IPBI 6 April 05 Ken Moffeit

Aligning the Compton IP

Precision surveying should be good to <50 micro radians

Can precision gyroscopes be used to achieve better accuracy?Perhaps <25 micro radians