! Hypernuclear spectroscopy in Hall A. ! Experimental issues. ! Prospectives (Hall A & Hall C collaboration)

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1 High-Resolution Hypernuclear Spectroscopy ElectronScattering at JLab, Hall A F. Garibaldi HYP Barcelona - October 2012! Hypernuclear spectroscopy in Hall A! 12 C, 16 O, 9 Be, H! E ! Experimental issues! Prospectives (Hall A & Hall C collaboration)

2 HYPERNUCLEAR PHYSICS! Hypernuclei are bound states of nucleons with a strange baryon (Λ)! Extension of physics on N-N interaction to system with S#0! Internal nuclear shell are not Pauli-blocked for hyperons! Spectroscopy This impurity can be used as a probe to study both the structure and properties of baryons in the nuclear medium and the structure of nuclei as baryoni many-body systems Ideal laboratory to study Λ-N interaction, mirror hypernuclei,csb, Λ binding energy

3 Hypernuclear investigation Few-body aspects and YN, YY interaction Short range characteritics ofbb interaction Short range nature of the ΛΝ interaction, no pion exchange: meson picture or quark picture? Spin dependent interactions Spin-orbit interaction,. ΛΣ mixing or the three-body interaction Mean field aspects of nuclear matter A baryon deep inside a nucleus distinguishable as a baryon? Single particle potential Medium effect? Tensor interaction in normal nuclei and hypernuclei Probe quark de-confinement with strangeness probe Astrophysical aspect Role of strangeness in compact stars Hyperon-matter, SU(3) quark-matter, YN, YY interaction information

4

5 H.-J. Schulze, T. Rijken PHYSICAL REVIEW C 84, (2011)

6 BNL 3 MeV KEK336 2 MeV Improving energy resolution ~ 1.5 MeV and new aspects of hyernuclear structure production of mirror hypernuclei energy resolution ~ 500 KeV 635 KeV 635 KeV using electromagnetic probe High resolution, high yield, and systematic study is essential

7 V (r) ΛN interaction Δ S Λ S N Τ Each of the 5 radial integral (V, Δ, S Λ, S N, T) can be phenomenologically determined from the low lying level structure of p-shell hypernuclei most of information is carried out by the spin dependent part doublet splitting determined by Δ, σ Λ, T

8 YN, YY Interactions and Hypernuclear Structure Free YN, YY interaction Constructed from limited hyperon scattering data (Meson exchange model: Nijmegen, Julich) G-matrix calculation YN, YY effective interaction in finite nuclei (YN G potential) Hypernuclear properties, spectroscopic information from structure calculation (shell model, cluster model ) v ( r) = ( a + b k + c k )exp( r / β ) ΛN Energy levels, Energy splitting, cross sections Polarizations, weak decay widths high quality (high resolution & high statistics) spectroscopy plays a significant role i i i F i F i

9 ELECTROproduction of hypernuclei e + A -> e + K + + H in DWIA (incoming/outgoing particle momenta are 1 GeV) ψ H Z i= 1 χ γ χ * K J µ ( i) ψ A - J m (i) elementary hadron current in lab frame (frozen-nucleon approx) - χ γ virtual-photon wave function (one-photon approx, no Coulomb distortion) - χ Κ distorted kaon w. f. (eikonal approx. with 1 st order optical potential) - Ψ Α (Ψ Η ) - target nucleus (hypernucleus) nonrelativistic wave functions (shell model - weak coupling model)

10 reasonable counting rates forward angle 1. ΔE beam /E : 2.5 x ΔP/P : ~ Straggling, energy loss ~ 600 kev septum magnets good energy resolution do not degrade HRS minimize beam energy instability background free spectrum unambiguous K identification High P k /high E in (Kaon survival) RICH detector

11 Kaon collaboration JLAB Hall A Experiment E E94107 COLLABORATION A.Acha, H.Breuer, C.C.Chang, E.Cisbani, F.Cusanno, C.J.DeJager, R. De Leo, R.Feuerbach, S.Frullani, F.Garibaldi*, D.Higinbotham, M.Iodice, L.Lagamba, J.LeRose, P.Markowitz, S.Marrone, R.Michaels, Y.Qiang, B.Reitz, G.M.Urciuoli, B.Wojtsekhowski, and the Hall A Collaboration and Theorists: Petr Bydzovsky, John Millener, Miloslav Sotona 16 O(e,e K + ) 16 Λ N 12 C(e,e K + ) 12 Λ Β 9 Be(e,e K + ) 9 Λ Li H(e,e K + )Λ,Σ 0 E beam = 4.016, 3.777, GeV P e = 1.80, 1.57, 1.44 GeV/c P k = 1.96 GeV/c θ e = θ K = 6 W 2.2 GeV Q 2 ~ 0.07 (GeV/c) 2 Beam current : <100 µa Target thickness : ~100 mg/cm 2 Counting Rates ~ counts/peak/hour Ε Electroproduction of Kaons up to Q2=3(GeV/c)2 (P. Markowitz, M. Iodice, S. Frullani, G. Chang spokespersons) E The angular dependence of 16 O(e,e K + ) 16 N and H(e,e K + )Λ (F. Garibaldi, M.Iodice, J. LeRose, P. Markowitz spokespersons) (run : April-May 2012)

12 Hall A deector setup RICH Detector aerogel first generation hadron arm septum magnets aerogel second generation electron arm To be added to do the experiment

13 The PID Challenge Very forward angle ---> high background of π and p - TOF and 2 aerogel in not sufficient for unambiguous K identification! Kaon Identification through Aerogels p k π p h = 1.7 : 2.5 GeV/c π All events k p Pions AERO1 AERO2 n=1.015 n=1.055 = A1 A2 k Kaons = A1 A2 Protons = A1 A2

14 RICH PID Effect of Kaon selection Coincidence Time selecting kaons on Aerogels and on RICH AERO K AERO K && RICH K π P K Pion rejection factor ~ 1000

15 12 C(e,e K) 12 B Λ M.Iodice et al., Phys. Rev. Lett. E052501, 99 (2007)

16 The WATERFALL target: reactions on 16 O and 1 H nuclei Be windows H 2 O foil Η 2 Ο foil

17 Results on the WATERFALL target - 16 O and 1 H 1 H (e,e K)Λ 1 H (e,e K)Λ,Σ Λ Σ 16 O(e,e K) 16 N Λ Ø Ø Water thickness from elastic cross section on H Precise determination of the particle momenta and beam energy using the Lambda and Sigma peak reconstruction (energy scale calibration)

18 Results on 16 O target Hypernuclear Spectrum of 16 N Λ Fit 4 regions with 4 Voigt functions χ 2 /ndf = 1.19 Theoretical model based on : SLA p(e,e K + )Λ (elementary process) ΛN interaction fixed parameters from KEK and BNL 16 Λ O spectra Four peaks reproduced by theory The fourth peak (Λ in p state) position disagrees with theory. This might be an indication of a large spin-orbit term S Λ 0.0/13.76±0.16

19 Results on 16 O target Hypernuclear Spectrum of 16 N Λ Fit 4 regions with 4 Voigt functions χ 2 /ndf = 1.19 Binding Energy B L =13.76±0.16 MeV Measured for the first time with this level of accuracy (ambiguous interpretation from emulsion data; interaction involving Λ production on n more difficult to normalize) Within errors, the binding energy and the excited levels of the mirror hypernuclei 16 O Λ and 16 N Λ (this experiment) are in agreement, giving no strong evidence of charge-dependent effects 0.0/13.76±0.16

20 9 Be(e,e K) 9 Li Λ Experimental excitation energy vs Monte Carlo Data (red curve) and vs Monte Carlo data with radiative Effects turned off (blue curve) Radiative corrected experimental excitation energy vs theoretical data (thin curve). Thick curve: three gaussian fits of the radiative corrected data Radiative corrections do not depend on the hypothesis on the peak structure producing the experimental data

21

22 Results on H target The p(e,e K)Λ Cross Section p(e,e'k + )Λ on Waterfall Production run W=2.2 GeV p(e,e'k + )Λ on LH 2 Cryo Target Calibration run Expected data from E07-012, study the angular dependence of p(e,e K)Λ and 16 O(e,e K) 16 N Λ at low Q 2 è None of the models is able to describe the data over the entire range è New data is electroproduction could longitudinal 10/13/09 amplitudes dominate?

23 Why? In this kinematical region models for the K + - Λ electromagnetic production on protons differ drastically The interpretation of the hypernuclear spectra is difficult because of the lack of relevant information about the elementary process. The ratio of the hypernuclear and elementary cross section measured at the same kinematics is almost model independent at very forward kaon scattering angles The ratio of the hypernuclear and elementary cross section doesn t depend strongly on the electroproducion model and contains direct information on hypercnulear structure and production mechanism How? Hall A experimental setup (septum magnets, waterfall target, excellent energy resolution AND Particle Identification ) give unique opportunity to measure, simultaneously, hypernuclear process AND elementary process

24 The results differ not only in the magnitude of the X-section (a factor 10) but also in the angular dependence (given by a different spin structure of the elementary amplitudes for smaller energy (1.3 GeV) where the differences are smaller than at 2 GeV Measuring the angular dependence of the hypernuclear cross section, we may discriminate among models for the elementary process. the information from the hypernucleus production, when the cross sections for productionof various states are measured, is reacher than the ordinary elementary cross section

25 Hypernuclear spectroscopy prospectives at Jlab Collaboration meeting - F. Garibaldi Jlab 13 December 2011 Future mass spectroscopy Decay Pion Spectroscopy to Study Λ-Hypernuclei

26 - Put HKS behind a Hall A style septum magnet in Hall A - Enhance setup in Hall A over HRS2 + Septum - No compromise of low backgrounds - Independently characterize the optics of each arm using elastic scattering - The HKS+Septum arm would replace present Hall A Kaon arm (Septum+HRS) - Keep the ability to use waterfall target or cryotargets

27 Conclusions E94-107: systematic study of p shell light hypernuclei Ø The experiment required important modifications on the Hall A apparatus.new experimental equipment showed excellent performance. Ø Data on 12 C show new information. For the first time significant strength and resolution on the core excited part of the spectrum Ø Prediction of the DWIA shell model calculations agree well with the spectra of 12 B Λ and 16 N Λ for Λ in s-state. In the p Λ region more elaborate calculations are needed to fully understand the data. Ø Interesting results from 9 Be, interpretation underway Ø Elementary reaction needs further studies Ø More to be done in 12 GeV era (few body, Ca-40,Ca-48,Pb )

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