Presentation on theme: "Marina Barbui Trento, Italy, April 7-11, 2014"— Presentation transcript:
1Marina Barbui Trento, Italy, April 7-11, 2014 Exploring the alpha cluster structure of nuclei using the thick target inverse kinematics technique for multiple alpha decays. The 24Mg caseMarina BarbuiTrento, Italy, April 7-11, 2014
2Alpha clustering in Astrophysics Estimated limit N = 10a for self-conjugate nuclei(Yamada PRC 69, )massMany theoretical works have brought to the picture of alpha cluster nuclei described as a diluted gas of alphas in the lowest S state. (PRL 87, ; PRC 75, ).Many experimental works have explored the 8Be and 12C cases, fewer are available on the heavier systems.Excitation energyWe have investigated the 24Mg case with 20Ne+α at 2.9 and 9.7 AMeV using the Thick Target Inverse kinematics Technique (K. Artemov et al., Sov. J. Nucl. Phys. 52, 406 (1990))
3The Thick target inverse kinematics technique Allows covering a large range of incident energies in the same experiment.In the inverse kinematics, the reaction products are focused at forward angles.Allows measuring reaction products emitted at 0o.This Method (K. Artemov et al., Sov. J. Nucl. Phys. 52, 406 (1990)) has been used several times to measure the resonant elastic scattering (Eur. Phys. J. A (2011) 47: 73; Eur. Phys. J. A (2011) 47: 96; AIP Conf. Proc. 1213, 137 (2010) ) and is used here for the first time to detect multiple alpha decays.
4Experimental setup 20Ne beam from the K150 cyclotron at TAMU @ 3.7 AMeV, 2.9 AMeV after the window@ 11 AMeV, 9.7 AMeV after the window48 cmReaction chamber filled with 4He gas at a pressure sufficient to stop the beam before the detectors10.3 PSI with 20Ne AMeVand50 PSI with 20Ne AMeVMeasured quantities:-Energy signals from every detector pad.-Time from the cyclotron radiofrequency.
5Preliminary analysis Energy calibration. Time calibration. Identification of the alpha particles with gates on DE-E and E-Time.Selection of the events with alpha multiplicity 1, 2 and 3 for further analysis.Reconstruction of the interaction point in the gas using the kinematics, the measured alpha energies and the energy loss tables from SRIM (double check with the measured time).Reconstruction of the excitation energy of the 24Mg.
6Events with Alpha Multiplicity 1 Ne 2.9 AMeVThreshold for 6a decayNice energy resolution (about 30 keV at 0o) worsening as we move to larger anglesPossibility to measure the whole excitation function in the same experiment.Comparison with the excitation function measured in keV energy steps in normal kinematics at 168o in the center of mass By R. Abegg and C.A. Davis PRC 43(1991)2523
7Events with alpha multiplicity 2 9.7 AMeV, 2a in the telescope at about 0 degEstimate of the uncorrelated events-PRC 63(2001)034317PRC 57 (1998) 1277This workThreshold for6a decayAfter subtraction of the uncorrelated24Mg*8Be16O
8Events with alpha multiplicity 3 9.7 AMeV, 3a Telescope124Mg*12C112C2aif 12C2 is in the ground stateEx(12C) [MeV]Hoyle state3- state-PRC 63(2001)034317PRC 57 (1998) 1277This work
9We can do betterImprove the statistics by considering events with 2 alphas in the Telescope 1 and the third elsewhere7.6 MeV (0+)2 12C in the Hoyle statewe detect mixed alphas9.6 MeV (3-)11.8 MeV (2-)12.7 MeV (1+)10.8 MeV (1-)
10For each stateRelative energy of the three couples of alpha particles -> Tells us if the decay is proceeding through the 8Be ground state.Dalitz Plot and Sphericity/Coplanatity Plot -> Information about the energy and momentum of the emitted alpha particles. Tell us about the shape of the decaying 12CExcitation energy of the 24Mg
11With selection of events decaying through the 8Begs or not Erelative<220keV through 8BegsErelative>220keV not through 8BegsWith subtraction of uncorrelated events7.6 MeV (0+)9.6 MeV (3-)11.8 MeV (2-)12.7 MeV (1+)Energy[MeV]Through 8BegsNo 8Begs7.659.6411.812.7
12Energy Dalitz Plots Ideal to describe 3 body decays Based on Viviani’s theorem saying that for any point P in an equilateral triangle the sum of the distances of the point from the sides of the triangle is a constant independent of P𝑦=𝑥 3𝐸 1 + 𝐸 2 + 𝐸 3 =𝑐𝑜𝑛𝑠𝑡= 𝐸 𝑡𝑜𝑡P= (𝑃 𝑥 , 𝑃 𝑦 )𝑃 𝑥 = 𝐸 1 +2 𝐸 2 𝐸 𝑚𝑎𝑥 − 3 2E2/EmaxPE3/Emax𝑃 𝑦 = 𝐸 1 𝐸 𝑚𝑎𝑥E1/EmaxIf the decay proceeds through the formation of a 8Be𝐸 𝑚𝑎𝑥 = 2 3 𝐸 𝑡𝑜𝑡Events inside the circle conserve both energy and momentumThe center of the circle is at P=(0.5, 0.5)
13Sphericity/Coplanarity study Use Energy flow matrix defined as in the references:Physics Letters 110 B (1982) 185Physics Letters B 240 (1990) 28PRL 64(1990) 2246PRL 78 (1997) 2084pi (n) are the momentum components of the particle n, mn is the mass of the particle nli are the eigenvalues of the matrix in ascending order l1 ≤ l2 ≤ l3Disk shapeRod shape
147.6 MeV (0+) Hoyle State mostly decays through 8Begs Consistent with the description of the Hoyle state by other authorsLess than 1.6 % of the events (depending on the cut) decay directly into 3 alphas
159.6 MeV (3-) decays through 8Begs JoP Conference series 111 (2008)012017
16Dalitz Plot (2- at 11.8 MeV) not decaying through 8Begs Comapred with Fynbo’s predictions
17Dalitz Plot (1+ at 12.7 MeV) not decaying through 8Begs Comapred with Fynbo’s predictions
18Simple Monte-Carlo decay simulation to understand something more about the shape of 12C -Conservation of energy and momentum-Classical kinematics-Energy and width of the resonances-In case of decay through 8BeQ1) Q has a flat distribution 2) Q is optimized in order to match the experimental energy distribution and sphericity/coplanarity plot
19ExperimentalHoyle stateQ optimized (gaussian distribution centered at p/3 with sigma p/6 and Q>p/9)Q has a flat distribution
20Experimental(3-) stateQ optimized (gaussian distribution centered at p/2 with sigma p/8)Q has a flat distribution
21Experimental(1+) state at 12.7 MeV decaying through the 8Be excited state (Ex = 2.9 MeV, G=1 MeV )Q optimized (gaussian distribution centered at p/6 with sigma p/12)Q has a flat distribution
22E*(12C1) = 11.83 MeV (2-) Decay without 8Be Through the 8Be excited state E=2.9 MeV, G=1 MeVExperimental DataDecay without 8Be
24Explanation of the peak at 8.6 MeV We see the peak only selecting the events decaying through the ground state of 8BeNo peak for the other selection.Might be due to 24Mg splitting into 2 carbons each in the Hoyle state (reasonable because the Hoyle state is the most populated and mostly decays through the 8Be gs)If so, there should be a systematic effect if we look at the average kinetic energy along the beam axis (the high energy alpha particle in the center of mass is always connected to the less energetic one in the laboratory framework)If we look at the center of mass velocity in the x direction for the known states this has a symmetric distribution around zeroThe 8.6 MeV peak does not.Simple Monte-Carlo simulation to show that this is what actually occurs
25Velocities on the beam direction (3- ) 9.6 MeV state -> SymmetricHoyle State -> Symmetric(2- )11.8 MeV state -> Symmetric8.6 MeV peak -> NOT Symmetric= Something is wrong(1+) 12.7 MeV-> Symmetric
26Simple simulation ingredients: Using the previous simulation for the 12C decayConservation of energy and momentum for the decay of 24MgInputs: E* (24Mg), E*(12C1) , E*(12C2), width of the statesAngular distribution of the carbons proportional to Pl(cos q)2E* (24Mg) = 33.2 MeV (this is found to decay in 2 carbons)First calculation:
27If we mix 2 alphas from C1 and one alpha from C2 The peak at 8.6 MeV appears.There is also a bump at about 10 MeV that we need to take into accountExperimental 8.6 MeV peakThe x component of the velocity in the center of mass shows an asymmetric shape as for the measured 8.6 MeV peak
28How we reconstruct those events In the laboratory we see two alphas from C1 (va1, va2) and one from C2 (va3)va3<va1≈va2In case of the Hoyle state the standard deviation of the 3 alphas energies is very small => the average of v1 and v2 is very close to the velocity of C1, v3 represents the velocity of C2 (overestimated).C1 and C2 are in the Hoyle state and emit 3 alphasva3va2va1In the labWe can calculate the relative energy between C1 and C2E*24Mg = 𝐸 𝑟𝑒 𝑙 𝐶1−𝐶2 + E*C1+ E*C𝐸 𝑟𝑒 𝑙 𝐶1−𝐶2 = 1 2 𝜇 𝑣 𝑟𝑒𝑙 2E*C1= E*C2 = 7.65 MeVQ(24Mg->2 12C) = MeV
29ConclusionsWe observed several resonant states in 24Mg with excitation energy up to 38 MeV, well above the threshold for decaying in 6 alpha particlesWe did not observe any direct decay into 6 alphasThe observed states show alpha cluster properties. Depending on the energy they can decay in 20Ne+a, 16O +8Be, 12C+12C->3a, 12C->3a+12C->3a.Several 12C excited states decaying into 3 a particles were identified and analyzed in detail to obtain information about the decay mode and the shape of the 3 a configuration.
30Thank you for your attention! M. Barbui1, V.Z. Goldberg1, E-J. Kim1, K. Hagel1, G.Rapisarda1, S. Wuenschel1, X. Liu1,2, H. Zheng1, G. Giuliani1, and J.B. Natowitz11 Cyclotron Institute, Texas A&M University, MS3366 College Station, TX2 Institute of modern physics, Chinese Academy of Sciences, Lanzhou, China