1 / 36

New Opportunities in the Physics Landscape at CERN

10-13 May 2009. New Opportunities in the Physics Landscape at CERN. Antiproton Decelerator (AD) Summary and Prospects. Klaus Jungmann, KVI, University of Groningen, NL. Physics Motivation Unique Possibilities Tests of Fundamental Theories Precision Measurements

gizela
Download Presentation

New Opportunities in the Physics Landscape at CERN

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. 10-13 May 2009 New Opportunities in the Physics Landscape at CERN Antiproton Decelerator (AD) Summary and Prospects Klaus Jungmann, KVI, University of Groningen, NL • PhysicsMotivation • Unique Possibilities • Tests of Fundamental Theories • Precision Measurements • Novel Techniques and Instrumentation • Applications • High Visibility  ? P P

  2. Physics Motivation

  3. Sir Isaac Newton (1642 - 1727) Basic Principles on which Scientists work in Physics  First Theory on Gravity How do we work in Physics ?

  4. FANTOM Study Week Gent 2007 • A Theory is only as good as it is experimentally verified. • A Theory without experimental verification has no standing.

  5. The Standard Model(s) Dark Matter – Dark Energy … • Excellent Description of • ALL Observations • However, many Open Questions • Why 3 generations ? • Why some 30 parameters? • Why one electric charge ? • What about CP violation ? • Why matter-antimatter asymmetry? • ….. • Gravitynot included • NoCombindTheoryofGravityand • Quantum Mechanics. • Contents of the Cosmos • What’s the other 96% beyond matter ?

  6. ? Physics within the Standard Model: complex systems, spectra, lifetimes… + - u u d d u d N S zX e- m- b+ ne Standard Model in Particle Physics Gravitation Grand Unification Electro- Electro - Weak Magnetism Magnetism Standard Model Electricity ? Weak Strong Strong • Speculative Models: • Supersymmetry, Cold dark matter, Tachyons, Radiativemuon generation, • Technicolor, Leptoquarks, Extra gauge bosons, Extra dimensions, • LeftRight Symmetry, Compositeness, Lepton flavour violation, …. • No Status in Physics , yet: “Not Even Wrong” not yet known? Physics outside the Standard Model: new phenomena, new particles…

  7. Experiments at the Frontiers of Standard Theory Direct Search Frontier Precision Frontier  complementary approaches

  8. Test of Fundamental Symmetries PrecisonMeasurements

  9. Since then CERN has a HIGHLY PUBLICLY VISIBLEprogram on Low Energy Precision Testsof most fundamental theories

  10. Precision requires Time pbar-p q/m 45 years electron g-2 60 years muon g-2 45 years muonium 1s-2s 15 years Highly precise CPT & Gravity Tests  Proton and Antiproton q/m compare to 0.1 ppb Clock Comparisons  Proton and Antiproton gravitational accceleration equal to 1 ppm p and pbar charge to mass ratio (circles) p and pbar inertial mass ratio (squares)

  11. Verifications of CPTSymmetry • Tests of particle/antiparticle symmetry (PDG) • Inconsistent definition of figure of merit: comparison difficult • Pattern of CPT violation unknown (P: weak interaction, CP: mesons) • → Arbitrary number joggling to get • “accuracy” better than experiments !!!

  12. CPT– Violation & Lorentz Invariance Violation • Kosteleckyet al.: • Interaction with a finite strength • Figure of merit energy based • → Completely different systems appear much more interesting !

  13. Mass [eV] Verifications of CPT symmetry Using the Kosteleckyet al. Standard Model Extension scheme • Tests of particle/antiparticle symmetry (PDG)

  14. Different methods available to produce Antihydrogen

  15. ATHENA Scientists Create 'Star Trek' Antihydrogen in QuantityBy Alex DominguezAssociated Pressposted: 02:59 pm ET18 September 2002 ATRAP Physical Review Letters 89, 213401 online (2002)

  16. (Anti-)Hydrogen CPT Tests DnHFS= cons. *a2 R+eQED+enucl +eweak + eCPT Laser spectroscopy 1s-2s -------- Microwave spectroscopy 1s Hyperfine Structure Dn1s2s= ¾ *R+eQED+enucl +eweak + eCPT “Long distance” Interaction “Contact” interaction R= mec2 *a2/2 h

  17. Line center accuracy in absence of systematic errors: • n = Dnexp. / (Sign./Noise) Dnexp. /  Nparticles (Anti-)Hydrogen Spectroscopy* Hydrogen 1s-2s Saturation Intensity Is = 0.9 W/cm2 Excitation Rate Re = 4p*84*(I/W/s*cm2)2/Dn/Hz Photo Ionization Rate Rp = 9*I/W/s*cm2 Zeeman shift dnZ = 9.3*B Hz/T ac Stark shift dnac = 1.7*I Hz /W*cm2 Velocity at 1mK V1K = 4 m/s Time-of-flight broadening DnTOF= 3 kHz (1 mK, 600 mm beam diam.) Lyman a detection efficiency 10-6 =  * effMCP (= 10-4 * 10-2) 1011 H-atoms (MIT Bose condensation)dn/n1s2s = 10-13(1s integration time) Just one Problem: Lyman-a detection via field quenching => atoms can be used once only (all 1s, mF states get equally populated) Antihydrogenexperiments benefit from more particles * numbers verified with L. Willmann

  18. pH Ground-state Hyperfine Structure SIMULATION Need less particles ( 2 pH / s ) because of narrow natural linewidth from B. Juhasz

  19. pHe+ Atom – a naturally occurring trap for antiprotons • • Serendipitously discovered by Tokyo group at KEK • • 3-body system, Metastable • • ~ 3% of stopped antiprotons survive with average lifetime of ~ 3 ms • • Precision laser spectroscopy by ASACUSA: • - best test of 3-body QED theories • - proton-antiproton mass & charge comparison(PDG) • Enters CODATA constant adjustment significantly Hayano, Yamazaki et al.

  20. Progress in atomcule spectroscopy year

  21. CPT Tests @CERN AD • At the CERN AD a number of unique, important CPT tests • were already conducted and improved ones are on their way : • ASACUSApHe , pHe+ , pH , p • ATRAP p , pH • ALPHA pH • One can expect significant steering of Model Building and • High Visibility next to a robust discovery potential.

  22. (Anti-)Hydrogen Gravity Tests F= - m*g ? The Remaining eagerly awaited GravityTest Hydrogen F=m*g ? F=m*g • Lyman –a laser required • Lyman –a laser developed Unique Possibility

  23. Gravity Tests @CERN AD • At the CERN AD is the place to answer the most urgent • question on antimatter gravity : • AEGIS pH • ATRAP pH • Free Fall pH • One can expect an answer to a most fundamental question • to question, which only can be answered by experiment! • High Visibility next to a robust discovery potential.

  24. Standard Model Physics Applications

  25. ASACUSA using RFQD &MUSAHI Antiprotonic Radioactive Atoms • VOLUME 87, NUMBER 8 P H Y S I C A L R E V I E W L E T T E R S 20 AUGUST 2001 • Neutron Density Distributions Deduced from Antiprotonic Atoms • A. Trzcin´ska, J. Jastrze ¸bski, and P. Lubin´ski • Heavy Ion Laboratory, Warsaw University, PL-02-093 Warsaw, Poland • F. J. Hartmann, R. Schmidt, and T. von Egidy • Physik-Department, TechnischeUniversitätMünchen, D-85747 Garching, Germany • B. Klos • Physics Department, Silesian University, PL-40-007 Katowice, Poland • (Received 28 March 2001; published 2 August 2001) Highest Uncertainty Arising from Theory

  26. Antiproton Radio-Therapy A significant win (factor ~4) in a sensitive window for tumor treatment and healthy tissue sparing Carbon Antiprotons

  27. Physics within Standard Model and Applied Research @CERN AD • At the CERN AD also SM physics and Applied Research is • conducted: • ASACUSAp-nucleus annihilation, atomic collisions • Double-Strangeness p-nucleus dedicated experiment • Production • PAX p polarization, p – p interactions • ACE p radiation-therapy • …… • One can expect deeper insights and the development of • novel techniques to the benefit of physics and society.

  28. Antiproton Sources

  29. Antiproton Decelerator (AD) @ CERN • Started operation July 6, 2000 • Antiproton capture, deceleration, cooling • Pulsed extraction • Many Experiments • ASACUSA • ATRAP • ALPHA • AEGIS • Free Fall • PAX • ACE • ….. • Request for more and • better antiproton beams • To speed up progress • To boost accuracy •  ELENA

  30. Consequent Future Development ELENA@CERN ELENAprovides 10-100 times more particles ?Possible Option?TSR@MPIK(Heidelberg)  ELENA ??

  31. FLAIR @ /FAIR Factor 100 more pbar trapped or stopped in gas targets than now FLAIR NESR

  32. New Facilities @CERN AD or GSI/FAIR • New Facilities can provide up to 100 times more particles: • MUSASHI ASACUSA ‘s device to recycle p’s • ELENA Generic low cost CERN solution, • Start possible now • FLAIR GSI/FAIR solution not before 2015 • One can expect faster progress and better results from more p’s • → CERN and GSI should synchronize

  33. Summary and Conclusions • Highly Motivated Urgent Antiproton Experiments • with robust Discovery Potential and High Visibility • CPT, Gravity, Determination of Fundamental Constants, • SM Physics, Applications (Therapy) • Unique Facility worldwide until beyond 2015 • Creative and Innovative Increasing Community • Young people • Novel Techniques and Novel Technology • Physics Program good on Time Path • Physics Program needs more particles • →ELENAwell motivated • Productive and Prosperous Future Ahead Low Energy Antiproton contributions to Physics just started Precision takes Time Care and Particles

  34. Thank YOU !

More Related