1
μ ! "# $ E n e r g y Time 21 Na 20 Ne stable < 0.05 % contamination After separation 0 50 100 150 200 250 0 50 100 150 200 250 E n e r g y Time Na Ne F O Before separation 21 Ne (p, n) 21 Na 0 50 100 150 200 250 0 50 100 150 200 250 M. Sohani, G.P.A. Berg, U. Dammalapati, S. De, S. Dean, P. Dendooven, O. Dermois, K. Jungmann, G. Onderwater,A. Rogachevskiy, E. Traykov, L. Willmann and H.W. Wilschut Kernfysisch Versneller Instituut, Rijksuniversiteit Groningen, The Netherlands TRIμP - A new facility to produce and trap radioactive isotopes TRIμP Discrete symmetries in nature offer sensitive tests of the Standard Model. Example experiments are -ν correlations in β decay of 21 Na and 19 Ne isotopes as well as searches for permanent Electric Dipole Moments (EDM) in Radium atoms. Main goal is investigation of possible symmetry violations which are prediction in various extension to the Standard Model. Trapped rapped Radioactive adioactive I sotopes: sotopes: μ icro icro - Laboratories for Fundamental aboratories for Fundamental P hysics hysics The dual magnetic separator at the TRIμP facility is in operation since mid 2004. It has various operation modes from fragmentation to gas filled mode. Secondary beam can be obtained with a high degree of purity. RFQ A segmented Radio Frequency Quadropole cooler, confines and bunches the secondary beam. (being commissioned) Recoil Ion Momentum Spectroscopy in a Magneto Optical Trap (MOT) In Standard Model: Weak Interaction is V-A In general β-decay could happen via S , P or T β-decay Limit D 0 New Physics Vector (F) [Tensor] β + ν e Scalar [Axial vector (GT)] β + ν e Advantages of 21 Na Y Trapping of Na is well established Y Short lifetime ( T 1/2 22.48 s ) Y Mixed F and GT transition : sensitivity to TRV R and D test both Time Reversal Violation R scalar and tensor (a and EDM) D measurements gives a, A, b, B First step with a 21 Na Production as a high purity secondary beam has been used to measure beta decay branching ratio. RFQ and low energy beam line Electric Dipole Moment (EDM) EDM violates Parity and Time Reversal 482.7 nm 714 nm 7s2 1S0 7s 7p 1P1 7s 7p 3P 7s 6d 1D2 7s 6d 3D 2 1 0 1438 nm 1488 nm 2.8 μm Radium 3 2 1 Barium 6s 5d 1D2 553.7 nm 791 nm 6s 6p 1P1 6s 6p 3P 2 1 0 1130.6 nm 1500.4 nm 6s 5d 3D 3 2 1 3 μm 1108 nm 6s21S0 Why Radium is a promising candidate ? YDegenerate P & D states of opposite parity enhances EDM signal YSome isotopes have octupole deformation Y Several 10000 enhancement is possible Trapping of Barium (Ba) Y Spectroscopy of Ba to pilot Ra spectroscopy Y Extend cooling and trapping to heavy alkaline earth element GHz Hz 137 Ba Measuring 3 D 1 Æ 1 P 1 transition gives hyperfine splitting of P and D states in 137 Ba. Permanent EDM 0 New Physics

TRI µµP - A new facility to produce and trap ... - CERN

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Page 1: TRI µµP - A new facility to produce and trap ... - CERN

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Time

21Na

20Ne

stable

< 0.05 % contamination

After separation

0 50 100 150 200 250

0

50

1

00

150

20

0

2

50

Ene

r gy

Time

Na

NeF

O

Before separation

21Ne (p, n) 21Na

0 50 100 150 200 250

0

50

10

0

150

20

0

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M. Sohani, G.P.A. Berg, U. Dammalapati, S. De, S. Dean, P. Dendooven, O. Dermois, K. Jungmann,G. Onderwater,A. Rogachevskiy, E. Traykov, L. Willmann and H.W. Wilschut

Kernfysisch Versneller Instituut, Rijksuniversiteit Groningen, The Netherlands

TRIµµµµP - A new facility to produce and trap radioactive isotopes

TRI µµµµPDiscrete symmetries in nature offer sensitive tests of the Standard Model. Example experiments are �

-νννν correlations in ββββ decay of 21Na and 19Ne isotopes as well as searches for permanent Electric Dipole Moments (EDM) in Radium atoms. Main goal is investigation of possible symmetry violations which are prediction in various extension to the Standard Model.

TTrapped rapped RRadioactiveadioactive II sotopes: sotopes: µµicroicro -- LL aboratories for Fundamental aboratories for Fundamental PPhysicshysics

The dual magnetic separator at the TRI µµµµPfacility is in operation since mid 2004. It has various operation modes from fragmentation to gas filled mode. Secondary beam can be obtained with a high degree of purity.

RFQA segmented Radio Frequency Quadropole cooler, confines and bunches the secondary beam. (being commissioned)

Recoil Ion Momentum Spectroscopy in a Magneto Optical Trap (MOT )

In Standard Model: Weak Interaction is V-A

In general ββββ-decay could happen viaS , P or T

ββββ-decay

Limit D � 0 ⇔⇔⇔⇔ New Physics

Vector (F) [Tensor]

ββββ+

ννννe

Scalar [Axial vector (GT)]

ββββ+

ννννe

Advantages of 21Na � Trapping of Na is well established� Short lifetime ( T 1/2 � 22.48 s )� Mixed F and GT transition :

sensitivity to TRV

•R and D test both Time Reversal Violation• R →→→→ scalar and tensor (a and EDM)• D measurements gives a, A, b, B•First step with a

21Na Production as a high purity secondary beam has been used to measure beta decay branching ratio.

RFQ and low energy beam line

Electric Dipole Moment (EDM)

EDM violatesParity and

Time Reversal

482.7 nm

714 nm

7s2 1S0

7s 7p 1P1

7s 7p 3P

7s 6d 1D2

7s 6d 3D

2

1

0

1438 nm

1488 nm≈≈≈≈ 2.8 µµµµm

Radium

321

Barium

6s 5d 1D2

553.7 nm

791 nm

6s 6p 1P1

6s 6p 3P210

1130.6 nm

1500.4 nm

6s 5d 3D

321

≈≈≈≈ 3 µµµµm1108 nm

6s2 1S0

Why Radium is a promising candidate ?�Degenerate P & D states of opposite

parity enhances EDM signal�Some isotopes have octupole deformation� Several 10000 enhancement is possible

Trapping of Barium (Ba)� Spectroscopy of Ba to pilot Ra

spectroscopy� Extend cooling and trapping to

heavy alkaline earth element

GHz

Hz

137Ba

Measuring 3D1����1P1 transition gives hyperfine splitting of P and D states in 137Ba.

Permanent EDM � 0 ⇔⇔⇔⇔ New Physics