2. TRI  P presentatie voor RUG College van Bestuur 17 februari 2003 Klaus Jungmann

3. Services to external & internal users Projectruimte Others EU € Programs/Projects AGOR Nuclear Structure and its Nuclear Structure and its Implications for Astrophysics Implications for Astrophysics Interacting Hadrons Interacting Hadrons TRI  P TRI  P..... € €... People € € €... The KVI “company” good science* education of people Two main products: * good science * education of people AGOR

4. project  program 2001  2013 2001  2013 TRI  P T R I  P TRI  P T rapped R adioactive I sotopes:  icrolaboratories for Fundamental P hysics Theory Nuclear Physics Experiment Nuclear Physics Atomic Physics people (scientists) : people (scientists) : G. Berg, U. Dammalapati, P. Dendooven, O. Dermois, A. Dieperink, M.N. Harakeh, R. Hoekstra, K. Jungmann, R. Morgenstern, A. Rogachevskiy, M. Sanchez-Vega, O.Scholten, R. Timmermans, E. Traykov, M. van Veenhuizen, H. Warringa, L. Willmann, H.W. Wilschut + many morefunding:

5. Fundamental Interactions – Standard Model Physics outside Standard Model Searches for New Physics Physics within the Standard Model

6. TRI  P Some Questions related to TRI  P Physics Origin of Parity Violation in Weak Interactions Origin of Parity Violation in Weak Interactions (nature prefers lefthandedness) (nature prefers lefthandedness)  details of  -decays  details of  -decays Na, Ne isotopes Na, Ne isotopes Dominance of Matter over Antimatter in Universe ? Dominance of Matter over Antimatter in Universe ? CP - Violation, Time Reversal Symmetry, Parity Violation CP - Violation, Time Reversal Symmetry, Parity Violation  permanent electric dipole moments ?  permanent electric dipole moments ? Ra isotopes Ra isotopes

7. TRI  P Possibilities to Test New Models  Low Energies & Precision Measurement High Energies & direct observations

8. New Interactions in Nuclear and Muon  -Decay In Standard Model: Weak Interaction is V-A In general  -decay could be also S, P, T Vector [Tensor] ++ e [ ] Scalar [Axial vector] ++ e [ ]

9. TRI  P Radium Permanent Electric Dipole Moment EDMs violate - Parity - Time Reversal -CP Symmetry Advantage over “best“ atom so far ( 199 Hg) - close states of opposite parity  several 10 000 enhancement possible  several 10 000 enhancement possible - some nuclei strongly deformed  may give nuclear enhancement  may give nuclear enhancement 6

10. Key Experiments TRI  P TRI  P will be a user facility TRI  P will be a user facility  open to outside users KVI will concentrate first on KVI will concentrate first on  electroweak tests  electroweak tests *  - decay ( 20,21 Na, 19 Ne) *  - decay ( 20,21 Na, 19 Ne) * electric dipole moments (Ra) * electric dipole moments (Ra)  applications  applications * ALCATRAZ (rare Ca isotope detection) * ALCATRAZ (rare Ca isotope detection) (R. Hoekstra, R. Morgenstern) (R. Hoekstra, R. Morgenstern) Networks will jointly address Networks will jointly address  technology and science issues  technology and science issues * NIPNET, KVI coordinator (H.W. Wilschut) * NIPNET, KVI coordinator (H.W. Wilschut) ION Catcher ION Catcher VIDI grant for spectroscopy on Radium (L. Willmann) VIDI grant for spectroscopy on Radium (L. Willmann)

11. TRI  P Atomic Physics Nuclear Physics Particle Physics

12. TRI  P Atomic Physics Nuclear Physics Particle Physics Target

13. TRI  P x-ray counts [arb.] x-ray energy [channels] raw data fitted x-ray spectra extracted Fr x-rays A. Rogachevsky, H. Wilschut, S. Kopecky, V. Kravchuk, K. Jungmann + AGOR team C Tl C N Ra First TRI  P Tests 15 N + 205 Tl  213 Ra + 7n 213 Fr Fr x-rays

14. TRI  P Atomic Physics Nuclear Physics Particle Physics

15. TRI  P Primary beam from AGOR cyclotron target position in fragment separator mode target position in recoil-separatormode beam of radioactive isotopes to decelerator and traps Combined Fragment and Recoil Separator

16. TRI  P

17. Separator Hall Cooling and Trapping Hall The Wall variety of traps RFQ

18. TRI  P Infrastructure is being prepared for arrival of magnet hardware  A. van den Berg &Co

19. TRI  P Atomic Physics Nuclear Physics Particle Physics

20. TRI  P ION Catcher

21. TRI  P RFQ Cooler Technologically Novel Approach Appears to Work

22. TRI  P Atomic Physics Nuclear Physics Particle Physics

23. TRI  P Magneto-Optical Trap (MOT) Laser beam atoms coldatoms ~1 million Na atoms Temperature < 1 mK

24. TRI  P Diode Laser Hardware & Electronics Several diode lasers operating Several diode lasers operating mechanical parts from KVI mechanical parts from KVI precision electronics precision electronics built at KVI built at KVI optical laboratory built up optical laboratory built up I 2 spectroscopy successful I 2 spectroscopy successful Ba optical trap under way Ba optical trap under way Ti:sapphire, dye, pump lasers Ti:sapphire, dye, pump lasers ordered ordered …. ….

25. TRI  P Atomic Physics Nuclear Physics Particle Physics

26. AGOR is preparing for TRI  P Various upgrades and adaptations New Beams New Beams e.g. 208 Pb e.g. 208 Pb new sources (metals) new sources (metals) improved transmission improved transmission vacuum improvement vacuum improvement ….. ….. High Power (TRI  P would appreciate 1 kW) High Power (TRI  P would appreciate 1 kW) new extraction new extraction beam stops beam stops beam monitoring beam monitoring ….. …..  S. Brandenburg &Co  S. Brandenburg &Co

27.  P-related upgrades of AGOR-facility TRI  P requirements –high intensity (10 12 pps) –very heavy ions (e.g. Pb) –low energy upgrades –rearrange beamlines –AGOR cyclotron –ECR ion source

28. ECR ion source boost intensity –improve magnet configuration: new hexapole magnet  collaboration with LBNL(USA) and JYFL (Finland) beams of metallic ions –internal oven and sputtering system optimize transmission to AGOR cyclotron –redesign low energy beamline

29. AGOR cyclotron vacuum – –limit beam transmission – –improve factor 10 – –cryogenic pumps extraction system – –limit beam intensity heat dissipation – –redesign ESD & EMC2

30. TRI  P Atomic Physics Nuclear Physics Particle Physics

31. TRI  P Theory is Essential guidance on what to measure guidance on what to measure detailed calculations detailed calculations strong local group needed strong local group needed external contacts external contacts

32. TRI  P TRAPS 2002: NIPNET - ION Catcher - HITRAP Meeting Meeting in Groningen, May 2002 International Embedding

33. TRI  P TRI  P has already generated some interest some 15 invited conference some 15 invited conference talks of TRI  P scientists interest in collabortion interest in collabortion TRI  P expertise outside KVI TRI  P expertise outside KVI Collaborations at KVI Collaborations at KVI

34. TRI  P TRI  P Organization (Physics) TRI  P Organization (Physics) Program leader: K. Jungmann TRI  P management: H. Wilschut Program leader: K. Jungmann TRI  P management: H. Wilschut KVI Staff Experimentalists: KVI Staff Experimentalists: G.P. Berg, P. Dendooven, O. Dermois, M.N. Harakeh, R. Hoekstra, K. Jungmann, R. Morgenstern, L. Willmann, H. Wilschut (focus:  -decays, edm‘s; ground work) R. Morgenstern, L. Willmann, H. Wilschut (focus:  -decays, edm‘s; ground work) KVI Staff Theorists: KVI Staff Theorists: A. Dieperink, O. Scholten, R. Timmermans Postdocs: Postdocs: S. Kopecky, + M. Sanchez-Vega + N.N. PhD Students: PhD Students: V. Kravchuk, E. Traykov, U. Dammalapati, A. Rogachewskiy, T. Hoogeveen + N.N. ‘s Master Students: Master Students: H. Waringa M. van Veenhuizen, H. Waringa External Experimentalists: External Experimentalists: TUNL, NIPNET, ION CATCHER, discussions now: BNL, BU, IUCF, Osaka, Urbana, Yale... discussions now: BNL, BU, IUCF, Osaka, Urbana, Yale... (edm experiment) PARIS, Texas A&M PARIS (parity violation), Texas A&M (  -decays)

35. TRI  P TRI  P Organization (Technical) TRI  P Organization (Technical) Separator MOT & Laser Laboratory Separator MOT & Laser Laboratory (production stage) (design stage/ production stage) (production stage) (design stage/ production stage) project leader: Otto Dermois /Georg Berg project leader: Lorenz Willmann ass. proj. lead: Harry Kiewiet ass. proj. lead: Jan Mulder slow control : Dick Damstra slow control : Henk van der Duin design:Lambertus Slatius design:Bastian Duinsveld vaccum:Harry Timersma vaccum:Henk Gorter optics&lasers:Gerald Ebberink optics&lasers:Gerald Ebberink RFQ cooler and LEB Infrastructure RFQ cooler and LEB Infrastructure (design stage, test experiments) (being done right now) (design stage, test experiments) (being done right now) project leader :Lorenz Willmann project leader: Ad van den Berg ass. proj. lead: Leo Huismann radiation safety:Hans Beijers slow control : Peter Kroon design:Bastian Duinsveld design:Lambertus Slatius building services: Jans Sijbring vaccum:Henk Gorter cooling:Steven van der Veen electronics:Martin Stokroos electro-technics:Piet Wieringa Targets Targets (orientaton phase) (orientaton phase) project leader :Hans Wilschut

36. TRI  P Goals of TRI  P Goals of TRI  P Study fundamental interactions using radioactive isotopes Study fundamental interactions using radioactive isotopes in traps in traps A facility will be created for in house and outside users A facility will be created for in house and outside users General Time Lines General Time Lines Project started 2001; setup facility in 4 years Project started 2001; setup facility in 4 years TRI  P became a managed program in July 2001 TRI  P became a managed program in July 2001 Exploitation of facility until 2013 Exploitation of facility until 2013 TRI  P will evolve into a 50% user of AGOR TRI  P will evolve into a 50% user of AGOR Midterm review in 2008 Midterm review in 2008

37. NOW WE ARE LOOKING FORWARD TO NEW SCIENTIFIC RESULTS IN A COUPLE OF YEARS TRI  P