The SIDDHARTA experiment kaonic hydrogen and deuterium Xray

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The SIDDHARTA experiment: kaonic hydrogen and deuterium X-ray spectroscopy T. Ishiwatari Stefan Meyer Institut,

The SIDDHARTA experiment: kaonic hydrogen and deuterium X-ray spectroscopy T. Ishiwatari Stefan Meyer Institut, Vienna, Austria SIDDHARTA Collaboration Silicon Drift Detector for Hadronic Atom Research by Timing Applications T. Ishiwatari LNF- INFN, Frascati, Italy SMI- ÖAW, Vienna, Austria IFIN – HH, Bucharest, Romania Politecnico, Milano, Italy MPE, Garching, Germany PNSensors, Munich, Germany RIKEN, Japan 9. Oct. 2007, XII HADRON 07 Univ. Tokyo, Japan XII International Conference on Hadron Spectroscopy - Hadron 07 /23

Kaonic atom X-rays and KN scattering lengths Difficulty Shift ( ) and width (

Kaonic atom X-rays and KN scattering lengths Difficulty Shift ( ) and width ( ) of K-p and K-d gives isospin dependent KN scattering lengths(a 0 and a 1) These scattering lengths provide Low-energy SU(3) QCD: SU(3) chiral symmetry, KN s-term, nature of L(1405), S 0 ( 3115 ) S + (3140) T. Ishiwatari 1. High-background in kaon beams 2. Small X-ray yields (a few% K-p, below 1% K-d) 3. Precise determination of X-ray energy and width X-ray detector with 1. high background rejection, 2. large-area, 3. good resolution in energy and time XII International Conference on Hadron Spectroscopy - Hadron 07 2

Experimental results of kaonic atoms Results of kaonic hydrogen Repulsive shift 2 D No

Experimental results of kaonic atoms Results of kaonic hydrogen Repulsive shift 2 D No data 3 He No data 4 He Large shift Small shift Error on K-p is still large! Accuracy of a few e. V for K-p, First measurement for K-d (as well as 4 He, 3 He) are badly needed! T. Ishiwatari 1000 800 Kp. X 600 Izycki et al, 1980 Attractive shift attractive DEAR 400 200 0 -500 Bird 1983 1 H repulsive Davies New exp. width 1 s [e. V] Katom Old exp. 0 shift 1 s [e. V] 500 Phys. Rev. Lett. 94, 212302 (2005) XII International Conference on Hadron Spectroscopy - Hadron 07 3

DEAR experiment at DAFNE e+e- collider optimized to produce f-meson at rest (1. 020

DEAR experiment at DAFNE e+e- collider optimized to produce f-meson at rest (1. 020 Ge. V) DEAR T. Ishiwatari K- beam at DAFNE 1. Monochromatic 2. Low-energy 3. No hadronic background XII International Conference on Hadron Spectroscopy - Hadron 07 4

DEAR experimental setup APD Cryo-Cooler TMP CCD Electronics Kaon Monitor Cryo. Tiger CCD Cooling

DEAR experimental setup APD Cryo-Cooler TMP CCD Electronics Kaon Monitor Cryo. Tiger CCD Cooling 16 CCD 55 -30 (EEV) Vacuum Chamber T. Ishiwatari -1242 x 1152 pixels - pixel size 22. 5 x 22. 5 mm CCD Pre-Amplifier - total area 7. 24 cm 2 per chip - depletion depth ~30 mm - read-out time 1 min. CCD 55 -Chips - energy resolution ~150 e. V @ 6 ke. V - temperature at 165 K XII International Conference on Hadron Spectroscopy - Hadron 07 5

CCD X-ray detector X-ray events 1 and 2 pixel events Charged particles large pixel

CCD X-ray detector X-ray events 1 and 2 pixel events Charged particles large pixel events background suppression by pixel analysis T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 6

K-p energy spectrum by DEAR CCDs G. Beer et al. , PRL 94, 212302

K-p energy spectrum by DEAR CCDs G. Beer et al. , PRL 94, 212302 (2005) T. Ishiwatari et al. , NIMA 556(2006)509 DEAR results S/N~1: 70 Pa rts of M IP s ~1 , 2 pi xe ls X-ray events X-rays : 1, 2 pixels MIPs : ~ 8 pixels, Some MIPs: ~ 1, 2 pixels �background events on X-ray spectra �Timing needed! = - 193 ± 37 (stat. ) ± 6 (syst. ) 1 s = T. Ishiwatari e. V 249 ± 111 (stat. ) ± 30 (syst. ) e. V XII International Conference on Hadron Spectroscopy - Hadron 07 7

SIDDHARTA experiment (LNF, Italy) Silicon Drift Detectors for Hadronic Atom Research by Timing Application

SIDDHARTA experiment (LNF, Italy) Silicon Drift Detectors for Hadronic Atom Research by Timing Application New SDDs specially designed for SIDDHARTA T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 8

Comparison of X-ray detectors used for kaonic X-ray experiments SDD Si(Li) T. Ishiwatari Experiment

Comparison of X-ray detectors used for kaonic X-ray experiments SDD Si(Li) T. Ishiwatari Experiment Kp. X Detector Si(Li) Area [mm 2] Thickness DEAR E 570 CCD SDD 200 724 100 [mm] 5 0. 03 0. 30 D E (FWHM) [e. V] 410 170 185 D t (FWHM) [ns] 290 - 430 T. Ishiwatari NIMA in printing XII International Conference on Hadron Spectroscopy - Hadron 07 9

Triple coincidence technique e+ K+ Triple coincidence: SDDX * Scint. K r SDD to

Triple coincidence technique e+ K+ Triple coincidence: SDDX * Scint. K r SDD to r to illa int Target Sc X-ray K- illa int Φ K+ + K - Sc F S/N =1: 70 (CCD) 10: 1 (SDD) for kaonic Hydrogen T. Ishiwatari e- XII International Conference on Hadron Spectroscopy - Hadron 07 10

Temperature 22 K Pressure max. 5 bar 216 SDDs with 1 cm 2 per

Temperature 22 K Pressure max. 5 bar 216 SDDs with 1 cm 2 per SDD Side wall: Kapton 75 µm Kaon entrance Window: Kapton 150 mm T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 11

SDDs electronics Cryogenic target cell Kaon entrance window T. Ishiwatari XII International Conference on

SDDs electronics Cryogenic target cell Kaon entrance window T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 12

SIDDHARTA Setup on DAFNE SIDDHARTA Kaon monitor T. Ishiwatari focusing quads XII International Conference

SIDDHARTA Setup on DAFNE SIDDHARTA Kaon monitor T. Ishiwatari focusing quads XII International Conference on Hadron Spectroscopy - Hadron 07 lead shield 13

SIDDHARTA: Schedule • Tuning of setup / optimization 100 pb-1 • Precision measurement of

SIDDHARTA: Schedule • Tuning of setup / optimization 100 pb-1 • Precision measurement of kaonic hydrogen 400 pb-1 • Measurement of kaonic deuterium 600 pb-1 • Further options: Kaonic helium studies (3 He and 4 He) T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 14

Monte Carlo simulation background suppression W/o coincidence MIPs (e+/e-) in SDD Background suppression >103

Monte Carlo simulation background suppression W/o coincidence MIPs (e+/e-) in SDD Background suppression >103 Kaon decays With coincidence of K+, K-, X-ray Signal rate ~ 2. 2 x 10 -3 /s 130 /d (duty cycle=2/3 of d. ) Energy (ke. V) Asynchronous background (e-, e+) : negligible Synchronous background (K-p reaction, kaon decay) dominant T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 15

Energy spectra in SIDDHARTA (Monte Carlo) Kaonic deutrium Kα Kβ Kaonic hydrogen Kg, .

Energy spectra in SIDDHARTA (Monte Carlo) Kaonic deutrium Kα Kβ Kaonic hydrogen Kg, . . . S/N=1: 1 S/N=10: 1 Energy (ke. V) K-p: ε 1 s = 193 e. V, Γ 1 s = 249 e. V, Y(Kα )=2% precision: ε 1 s ± 3 e. V Γ 1 s ± 5 e. V K-d: ε 1 s = 325 e. V, Γ 1 s = 630 e. V, Y(Kα )=0. 2% precision: ε 1 s ± 18 e. V Γ 1 s ± 45 e. V Signal rate ~ 2. 2 x 10 -3 /s 30 days data taking 130 /d (duty cycle=2/3 of d. ) XII International Conference on Hadron Spectroscopy - Hadron 07 T. Ishiwatari 16

Expected results in SIDDHARTA Shift and width of kaonic hydrogen 1000 400 Kp. X

Expected results in SIDDHARTA Shift and width of kaonic hydrogen 1000 400 Kp. X SIDDHARTA DEAR 200 0 -500 T. Ishiwatari Izycki et al, 1980 M. Iwasaki et al, 1997 Bird et al, 1983 600 Kp. X (KEK) Davies et al, 1979 width 1 s [e. V] 800 0 shift 1 s [e. V] XII International Conference on Hadron Spectroscopy - Hadron 07 500 17

Tests of vacuum chamber and target Leak check, pressure tests, Power consumption tests, etc.

Tests of vacuum chamber and target Leak check, pressure tests, Power consumption tests, etc. have been performed. burst pressure ~ 3. 5 bar T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 18

Microscopic tests T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 19

Microscopic tests T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 19

SDD Spectroscopy test T. Ishiwatari w 49/s 01 w 45/s 03 w 40/s 01

SDD Spectroscopy test T. Ishiwatari w 49/s 01 w 45/s 03 w 40/s 01 Performance tests of each SDD are done with an Fe source. The average of the energy resolution is ~140 e. V. XII International Conference on Hadron Spectroscopy - Hadron 07 20

SDD test at BTF Back rejection factor at 50 Hz SDD time resolution Dt(FWHM)=720

SDD test at BTF Back rejection factor at 50 Hz SDD time resolution Dt(FWHM)=720 ns Counts/10 ch/sec No Trigger (without coincidence) Trigger (With coincidence) ADC [ch] T. Ishiwatari TDC [ch] XII International Conference on Hadron Spectroscopy - Hadron 07 21

DAY-1 configuration: mini SIDDHARTA SDD tests with kaon atom X-rays (Nov. and Dec. 2007)

DAY-1 configuration: mini SIDDHARTA SDD tests with kaon atom X-rays (Nov. and Dec. 2007) Install on “KLOE” I. P. New beam pipe New beam technique Reduced X-ray detection system: 8 -12 SDDs First step: Kaonic nitrogen (and 4 He) Kaonic nitrogen: 4000 X-ray events in ~3 days [30 pb-1] Performance tests of SDDs, Check background suppression T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 22

SIDDHARTA plans 2008: 1) ~ e. V level precision measurement of kaonic hydrogen (400

SIDDHARTA plans 2008: 1) ~ e. V level precision measurement of kaonic hydrogen (400 pb-1); 2) first measurement of kaonic deuterium (600 pb-1) 3) Kaonic helium measurement (He 3 and He 4) Under study: 4) Kaon mass precision measurement at the level of 10 ke. V 5) Other light kaonic atoms measurement (Li, Be…); 6) Investigate the possibility of the measurement of other types of hadronic exotic atoms (sigmonic hydrogen ? ) T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 /23

Summary DEAR finished successfully: most precise data on KH shift and width up to

Summary DEAR finished successfully: most precise data on KH shift and width up to now Theoretical studies continue SIDDHARTA is well under way: precison measurements on KH, KD, … T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 24

Thank you very much T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron

Thank you very much T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 25

X-ray transition energies (e. m. ) Kaonic hydrogen Kaonic deuterium T. Ishiwatari (SMI) Kaonic

X-ray transition energies (e. m. ) Kaonic hydrogen Kaonic deuterium T. Ishiwatari (SMI) Kaonic 3 He T. Ishiwatari Kaonic 4 He XII International Conference on Hadron Spectroscopy - Hadron 07 26

Kaonic hydrogen With a 0, a 1 for the I=0, 1 S-wave KN scattering

Kaonic hydrogen With a 0, a 1 for the I=0, 1 S-wave KN scattering lengths in the isospin limit (md = mu), m being the reduced mass of the K-p system, and neglecting isospin-breaking corrections: Deser-type formula „By using the non-relativistic effective Lagrangian approach a complete expression for the isospin-breaking corrections can be obtained; in leading order parameter-free modified Deser-type relations exist and can be used to extract scattering lengths from kaonic atom data“ (Meißner, Raha, Rusetsky, 2004) T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 27

Kaonic deuterium For the determination of the isospin dependent scattering lengths a 0 and

Kaonic deuterium For the determination of the isospin dependent scattering lengths a 0 and a 1 the hadronic shift and width of kaonic hydrogen and kaonic deuterium are necessary Theoretical procedures are needed to connect the observables with the isospin-dependent scattering lengths T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 28

K-p and K-d atom X-rays K-p (K-d) e. m. bound kaonic atoms Bohr radius

K-p and K-d atom X-rays K-p (K-d) e. m. bound kaonic atoms Bohr radius ~80 fm, binding energy ~9 ke. V Kaonic atom e. m. energy of K line (e. V) hydrogen 6479 200 250 deuterium 7820 325* 630* X-ray Yield Kα ~1 -3 % ~0. 2 %** *) A. N. Ivanov, M. Cargnelli, M. Faber, H. Fuhrmann, V. A. Ivanova, J. Marton, N. I. Troitskaya, J. Zmeskal, Eur. Phys. J. A 23 (2005) 79 **) Estimated value T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 29

DEAR – Comparison with theory B. Borasoy, R. Nißler and W. Weise, Phys. Rev.

DEAR – Comparison with theory B. Borasoy, R. Nißler and W. Weise, Phys. Rev. Lett. 94, 213401 (2005) T. Ishiwatari A. N. Ivanov et al. , Eur. Phys. J. A 21 (2004) 11 J. Phys. G 31 (2005) 769 Eur. Phys. J. A 25 (2005) 329 XII International Conference on Hadron Spectroscopy - Hadron 07 30

Silicon Drift Detector high energy resolution at fast shaping times, due to the small

Silicon Drift Detector high energy resolution at fast shaping times, due to the small anode capacitance Small capacitance electrode type anode cathode GND Si(Li) SDD Q = CV = ( S / d ) V UIR UOR UBACK T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 31

T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 32

T. Ishiwatari XII International Conference on Hadron Spectroscopy - Hadron 07 32