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1 Electric Field for the dEDM Experiment at the BNL AGS Vasily Dzhordzhadze SPIN 2008, Charlotesvelle October 10, 2008

Electric Field for the dEDM Experiment at the BNL AGS

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Electric Field for the dEDM Experiment at the BNL AGS. Vasily Dzhordzhadze SPIN 2008, Charlotesvelle October 10, 2008. 1. dEDM Experiment at BNL AGS. Presented at the SPIN 2008 Conference by Y.Semetzidis, G.Onderwater, M. Silva, F.Lin - PowerPoint PPT Presentation

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Electric Field for the dEDM Experiment at the BNL AGS

Vasily DzhordzhadzeSPIN 2008, Charlotesvelle

October 10, 2008

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dEDM Experiment at BNL AGS

• Presented at the SPIN 2008 Conference by Y.Semetzidis, G.Onderwater, M. Silva, F.Lin

• Goal: Measurement of the deuteron electric dipole moment at 10-29 e.cm level

• Principle: Polarize; • Interact with a E-Field; • Analyze Spin as a function of time

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Clock Wise (CW) and Counter Clock Wise (CCW) injections

• CW and CCW injections to cancel all T-reversal preserving effects as, e.g., the out of plane <E-field>. EDM is T-violating and behaves differently.

• Issue: Stability as a function of time• Solution: Use the 2-in-1 magnet design for

simultaneous CW and CCW storage (Morse) or Gupta’s common coil magnet.

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E-field Plates Specs• E-field: 120KV/cm with 2cm plate separation. The

design should restrict E-field<=120KV/cm everywhere• Two beams stored at the same time. They should not

influence each other electrically: min distance between the two beams is >15 cm.

• E-field uniformity: quad component < 1ppm distance from end > 10cm; align plates to 1um.

• E-field stability requires temperature stability

dT<10-3K; strong, sturdy plates• Need to operate in a magnetic field: study and

eliminate trapping effects

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E-field Plates• 2 cm apart

• Plate thickness: ~1.5cm, Stainless steel

• Height: 40-60cm, may be taller

• Length ~3.3m/ea, 32 plates (16 pairs) total around the ring

• Radius of curvature: ~8.5m

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E-field plates: ~60cm high

• Aim for 10-5K/m temperature uniformity

Vacuum chamber

Stainless steel support

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POISSON Simulation of E-Fields

2 cm separation , r=2 cm 2 cm separation , r=5 cm

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Common Coil Design for EDM

Aperture #1

Aperture #2

Coils

Coils

Iron Yoke

From R. Gupta’s presentation

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E-field strength

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E-field strength

The field emission with and without high pressure water rinsing (HPR).

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• Electro polishing (EP)• Buffered Chemical Polishing -> Surface

treatment by chemical solutions of NHO3, HF, H3PO4 (1: 1: 2): removal of 150 m for 90 minutes or 30 m for 20 minutes

• Surface roughness measurements by profilometer (2m)

• High Pressure Water Rinsing

Metal finishing

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ELECTROPOLISHING

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Before EPBefore EPBefore EP

After EP

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High Pressure Water Rinsing

Consist of High pressure pump, a spray wand and custom Nozzles. Systems are used as the final step in the surface Preparation. Uses ultra pure water with a pressure of ~1000psi to remove all remnants of the mechanical finishing. Output pressure can reach 3000 psi. Water supply ~500 gallons. Rinsing process is fully programmable by a PC running LabView.

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High Pressure Water Rinsing

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E-field strength, Electrostatic Separators at Tevatron

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E-field strength, Electrostatic Separators at Tevatron

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E-field strength, Electrostatic Separators at Tevatron

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E-field strength, Electrostatic Separators at Tevatron

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• FNAL 170 KV/late: no sparks in 7 days• Scaled to 2cm: gives 107 KV/cm, conditioned at

114 KV/cm. Scaled to 1.4cm : 128 KV/cm conditioned at 136KV/cm

• Using HPWR we expect to achieve the 120 KV/cm strength at 2cm and certainly at 1.4 cm

• O. Prokofiev (FNAL): It will require work but it can be done

E-field strength choice: 12 MV/m

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Measuring gravity direction with inclinometer of 10-10 rad sensitivity

Caution:Moon’s max gravitationaleffect is ±3.5rad!Distance: 60 times earth’s radius and mass ~1% ofearth’sWe need to take it into account when using the inclinometer!

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• We launched two programs for using BNL facilities for testing of the E-Field and gravitational stability

• We will use a clean room available at a new Center for Functional Nanomaterials to assembly the vacuum chamber with plates and test them later.

• We will get vibration free and strict temperature controlled room for our gravitational and position tests using inclinometer

• Later tests will start immediately• Vacuum Chamber tests will start January 2009• Expected first experimental results by Aril 2009

Summary