Atomic Physics Accelerator Facility at Darmstadt, Warsaw, November - - PowerPoint PPT Presentation

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Atomic Physics Accelerator Facility at Darmstadt, Warsaw, November - - PowerPoint PPT Presentation

Polish German Meeting on the New International Atomic Physics Accelerator Facility at Darmstadt, Warsaw, November 24, 2003 Atomic Physics at the New International Accelerator Facility at GSI in Darmstadt Atomic Physics under Extreme


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SLIDE 1

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

Atomic Physics Atomic Physics at the New International Accelerator Facility at GSI in Darmstadt Atomic Physics under Extreme Conditions Andrzej Warczak

Jagiellonian University, Institute of Physics, Kraków, Poland

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SLIDE 2

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

Atomic Physics

ATOMIC PHYSICS WITH HIGHLY CHARGED IONS

LASER DEVELOPMENT & TECHNIQUES X-RAY SPECTROMETRS & DETECTORS REACTION SPECTROMETERS ION TRAP TECHNIQUES STORAGE RING TECHNIQUES COOLING TECHNIQUES

ATOMIC REACTIONS AND DYNAMICS ATOMIC SPECTROSCOPY NUCLEAR GROUND STATE PROPERTIES

ATOMIC PHYSICS WITH HIGHLY CHARGED IONS

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SLIDE 3

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

Extreme Static Fields

1 10 20 30 40 50 60 70 80 90 10

9

10

10

10

11

10

12

10

13

10

14

10

15

10

16

1s

<E> [V/cm] Nuclear Charge, Z

Z = 92

H-like Uranium EK = -132 • 103 eV <E>= 1.8 • 1016 V/cm Hydrogen EK = -13.6 eV <E>= 1 • 1010 V/cm

Z = 1

Quantum Electro- Dynamics

Strongest laser fields : 1022 W/cm2

2p3/2 2p1/2 2s1/2 1s1/2

Lyα1 (E1) Lyα2 (E1) M1 Lamb Shift

1 s

  • g

r

  • u

n d s t a t e : i n c r e a s e

  • f

t h e e l e c t r i c f i e l d s t r e n g t h b y s i x

  • r

d e r s

  • f

m a g n i t u d e

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SLIDE 4

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

1990 1992 1994 1996 1998 2000 2002

420 430 440 450 460 470 480 490 500 510 520

Decelerated Ions: Cooler (our exp.)

Year Lamb Shift [eV]

U

91+

Gasjet Cooler

Decelerated Ions: Jet

Theory: 463,95 ± 1 eV

  • V. A. Yerokhin and V. M. Shabayev(2001)

Experiment: 459.8 ± 4.8 eV

The recently achieved accuracy of 4.8 eV is a considerable improvement by a factor of 3 compared to the most precise value up to now.

U92+ from SIS ESR Experimental Storage Ring NESR New Experimental Storage Ring

0 Joint Papers

The ground state Lamb shift in H-like uranium

About 2

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SLIDE 5

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

Towards an Accuracy of 1 eV Development of x-ray detection techniques

Segmented Ge(i) detectors

30 mm 52 mm 15mm

Transmission crystal spectrometer

GSI–Świerk-Grenoble–Kraków-Kielce-Frankfurt Calorimeters Micro-strip Ge(i) detectors and polarimeters Juelich-GSI–Świerk-Kraków-Kielce-Frankfurt Mainz-GSI Harvard-GSI

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SLIDE 6

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

Atomic Physics – Nuclear Physics

Giessen-GSI-Krakow

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SLIDE 7

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

Extreme Velocities Extreme Dynamic Fields

100meV 10eV 1keV 100GeV 1GeV 10MeV 100keV SIS300 HESR NESR ISR USR HITRAP

η=(γ-1)mc2/EBK=1

γ

100 1

E/u for U92+

10 2

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SLIDE 8

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

Extreme Velocities Lorentz Shifted (γ-boosted) Laser Cooling/ Spectroscopy

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SLIDE 9

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

Extreme Velocities

Precision Measurements of 2s Lamb Shift in Strong Fields of High-Z Li-like Ions

γ=23.9

eV 6 . 280

0 =

ω h

Projectile frame excitation fluorescence

laser excitation 280.6 eV

1s2 2s1/2 1s2 2p1/2

eV

L

87 . 5 = ω h

Lab.System (laser)

fluorescence detection

  • Lab. System

fluorescence

eV

X

13384 = ω h

γ=23.9

The large Doppler shift allows us to use visible laser sources to excite transitions in the energy range up to 280 eV, e.g. 2s-2p transitions in lithium-like heavy ions

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SLIDE 10

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

Extreme Dynamic Fields

Weizsäcker-Williams (1934) E(t) N(ω) Quantization Fourier- Transform

50 500 500 1000

N(ω)

Photon - Field

[keV] [

ħω

Photoionization in strong virtual photon fields with I ≥ 1020 W/cm2

E=γZ/b2 t ≤ 0.1 as E(t)

A t

  • m

„ e x p l

  • d

e s “ i n A t t

  • s

e c

  • n

d P u l s e

  • f

v i r t u a l P h

  • t
  • n

s

A unique light source

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SLIDE 11

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

Extreme Dynamic Fields

Collision times in the sub-attosecond regime (10–22 s < t < 10–18s)

Positive Continuum Negative Energy Continuum

Transfer

Excitation Ionization Free Pair Production + mc

  • mc2

2

e+ e-

e+

Capture

e-

ECPP

High- γ

γ Z b2 ≈

E

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SLIDE 12

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

Photon-Matter Interaction in the Relativistic Regime

Photoionization

e

  • 50

100 150 200 250 300 350 200 400

Lyα

1

K-REC 8

  • REC

M-REC L-REC Lyβ Lyα

2

counts

photon energy (keV )

U92+ => N2, 358 MeV/u

Radiative Electron Capture

e

E KIN 8

E L E K

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SLIDE 13

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

E

hω´

I

6000 6500 7000 7500 8000 3 6 9 counts (arb. units) energy (channels)

I⊥ (∆E+hω´)

∆E

hω´

||

I

6000 6500 7000 7500 8000 3 6 9 counts (arb. units) energy (channels)

I⊥ (∆E+hω´) I(∆E+hω´)

2 0 4 0 6 0 8 0 1 0 0 1 2 0 1 4 0 1 6 0 1 8 0 1 2 3 4 5 6 7 c o m p le te re la tiv is tic c a lc u la tio n s (E ic h le r e t a l.) n o n re la tiv is tic d ip o le d is trib u tio n la b o ra to ry fra m e U 92 += > N 2, 3 0 9 .7 M e V /u

ze ro d e g re e e m iss io n o f e le c tric ra d ia tio n b y e le c tro n c a p tu re in to s -o rb ita ls is fo rb id d e n b y a n g u la r m o m e n tu m c o n s e rv a tio n la w s ze ro d e g re e e m issio n : (α Z )

2 co rre c tio n to th e m a g n e tic e m issio n R ad iative C ap tu re in to th e K -S h ell

dσ/dΩ [arbitrary units]

m a g n e tic tra n s itio n s
  • b s e rv a tio n a n g le θ [d e g ]

0.01 0.1 1 10 100 1000 1 10 100 adiabatisity parameter η cross section per target electron

σ(barn)

0.1 1 10 beam energy [GeV/u] (for Au

79+ ions)

Photon-Matter Interaction in the Relativistic Regime

About 40 Joint Papers

Total cross sections Angular distribution Polarization

Ge(i) Pixel Detector (FZ Jülich)

Frankfurt-GSI-Krakow-Kielce-Świerk Lanzhou-Argonne-Kassel-Berlin

Gas Jet target

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SLIDE 14

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

The HITRAP Project at GSI

cooling trap experiments for slow particles experiments with particles at rest

U92+

post- decelerator EXPERIMENTS WITH HIGHLY-CHARGED IONS AT EXTREMELY LOW ENERGIES:

  • ultra-accurate mass measurements (atomic physics)
  • g-factor measurements (tests of QED)
  • laser and x-ray spectroscopy
  • nuclear polarization
  • surface studies and hollow-atom spectroscopy
  • collisions at very low velocities
  • experiments with antiprotons at the NESR

EXPERIMENTS WITH HIGHLY-CHARGED IONS AT EXTREMELY LOW ENERGIES:

  • ultra-accurate mass measurements (atomic physics)
  • g-factor measurements (tests of QED)
  • laser and x-ray spectroscopy
  • nuclear polarization
  • surface studies and hollow-atom spectroscopy
  • collisions at very low velocities
  • experiments with antiprotons at the NESR

11.4 MeV/u

U73+ SIS

stripper target

NESR

electron cooling and deceleration down to 4 MeV/u

U73+ U92+

4 M e V / u

EXPERIMENTS WITH HIGHLY-CHARGED IONS AT EXTREMELY LOW ENERGIES:

  • ultra-accurate mass measurements (atomic physics)
  • g-factor measurements (tests of QED)
  • laser and x-ray spectroscopy
  • nuclear polarization
  • surface studies and hollow-atom spectroscopy
  • collisions at very low velocities
  • experiments with antiprotons at the NESR

EXPERIMENTS WITH HIGHLY-CHARGED IONS AT EXTREMELY LOW ENERGIES:

  • ultra-accurate mass measurements (atomic physics)
  • g-factor measurements (tests of QED)
  • laser and x-ray spectroscopy
  • nuclear polarization
  • surface studies and hollow-atom spectroscopy
  • collisions at very low velocities
  • experiments with antiprotons at the NESR

The HITRAP project will be a part of FLAIR

FACILITY FOR LOW- ENERGY ANTI-PROTONS and IONS RESEARCH

The HITRAP project will be a part of FLAIR

FACILITY FOR LOW- ENERGY ANTI-PROTONS and IONS RESEARCH

UNILAC

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SLIDE 15

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

Antiproton Factory

SIS100/300 HESR NESR CR AP

New accelerator facility

Parameters: antiprotons up to 30 GeV, stored and cooled

Z – range

  • 1 => 92

Z – range 1 => 92

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SLIDE 16

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

Ultra-Slow and Trapped Antiprotons

Why is there no Antimatter Why is there no Antimatter in the Universe? in the Universe?

Hydrogen Antihydrogen

GSI will GSI will provide provide the Most Intense the Most Intense Source of Antiprotons Source of Antiprotons

Positron Antiproton

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SLIDE 17

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

Ultra-Slow and Trapped Antiprotons

What to Do with FLAIR What to Do with FLAIR

  • Test of fundamental symmetries: CPT
  • Exotic systems: “Atomcules”
  • Interaction of matter with antimatter
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SLIDE 18

Polish – German Meeting

  • n the New International

Accelerator Facility at Darmstadt, Warsaw, November 24, 2003

Atomic Physics

Stored Particles Atomic Research Collaboration

Atomic Physics Group, GSI, Darmstadt, Germany University of Frankfurt, Germany University of Dresden, Germany MPI Heidelberg, Germany University of Heidelberg, Germany University of Mainz, Germany University of Stockholm, Sweden Warsaw University, Warsaw, Poland Lebedev Institute, Moscow, Russia Jagiellonian University , Kraków, Poland Institute of Nuclear Physics, PAN, Kraków, Poland Kansas State University, Kansas, USA Institute of Nuclear Studies, Świerk, Poland Institute of Modern Physics, Lanzhou, China ANL, Argonne, USA Tbilisi State University, Tbilisi, Georgia HMI, Berlin, Germany Świętokrzyska Academy, Kielce, Poland University of Kassel, Germany University of St. Petersburg, Russia University of Giessen, Germany Fudan University, Shanghai, China, LBNL, Berkeley, USA University of Tokyo, Japan LLNL, Livermore, USA