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Dive into the research topics where C. S. Sumithrarachchi is active.

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Featured researches published by C. S. Sumithrarachchi.


Physical Review Letters | 2014

Novel technique for constraining r -process (n, γ) reaction rates

A. Spyrou; S. N. Liddick; Ann-Cecilie Larsen; M. Guttormsen; K. Cooper; A.C. Dombos; D. J. Morrissey; F. Naqvi; G. Perdikakis; S. J. Quinn; T. Renstrøm; J. A. Rodriguez; A. Simon; C. S. Sumithrarachchi; R. G. T. Zegers

A novel technique has been developed, which will open exciting new opportunities for studying the very neutron-rich nuclei involved in the r process. As a proof of principle, the γ spectra from the β decay of ^{76}Ga have been measured with the SuN detector at the National Superconducting Cyclotron Laboratory. The nuclear level density and γ-ray strength function are extracted and used as input to Hauser-Feshbach calculations. The present technique is shown to strongly constrain the ^{75}Ge(n,γ)^{76}Ge cross section and reaction rate.


Physical Review Letters | 2012

High-precision measurement of the 19Ne half-life and implications for right-handed weak currents.

S. Triambak; P. Finlay; C. S. Sumithrarachchi; G. Hackman; G. C. Ball; P. E. Garrett; C. E. Svensson; D. S. Cross; A. B. Garnsworthy; R. Kshetri; J. N. Orce; M. R. Pearson; E. R. Tardiff; H. Al-Falou; R. A. E. Austin; R. Churchman; M. Djongolov; R. D'Entremont; C. Kierans; L. Milovanovic; S. O'Hagan; S. Reeve; S. Sjue; S. J. Williams

We report a precise determination of the (19)Ne half-life to be T(1/2)=17.262±0.007 s. This result disagrees with the most recent precision measurements and is important for placing bounds on predicted right-handed interactions that are absent in the current standard model. We are able to identify and disentangle two competing systematic effects that influence the accuracy of such measurements. Our findings prompt a reassessment of results from previous high-precision lifetime measurements that used similar equipment and methods.


Journal of Physics: Conference Series | 2015

Far from 'Easy' Spectroscopy with the 8π and GRIFFIN Spectrometers at TRIUMF-ISAC

P. E. Garrett; A. J. Radich; J M Allmond; C. Andreoiu; G. C. Ball; P. C. Bender; L. Bianco; V. Bildstein; H. Bidaman; R Braid; C Burbadge; S. Chagnon-Lessard; D. S. Cross; G. A. Demand; A. Diaz Varela; M R Dunlop; R. Dunlop; P. Finlay; A. B. Garnsworthy; G. F. Grinyer; G. Hackman; B. Hadinia; S Ilyushkin; B. Jigmeddorj; D. Kisliuk; K Kuhn; A. T. Laffoley; K. G. Leach; A. D. MacLean; J Michetti-Wilson

The 8 pi spectrometer, installed at the TRIUMF-ISAC facility, was the worlds most sensitive gamma-ray spectrometer dedicated to beta-decay studies. A description is given of the 8 pi spectrometer and its auxiliary detectors including the plastic scintillator array SCEPTAR used for beta-particle tagging and the Si(Li) array PACES for conversion electron measurements, its moving tape collector, and its data acquisition system. The recent investigation of the decay of Cs-124 to study the nuclear structure of Xe-124, and how the beta-decay measurements complemented previous Coulomb excitation studies, is highlighted, including the extraction of the deformation parameters for the excited 0(+) bands in Xe-124. As a by-product, the decay scheme of the (7(+)) Cs-124 isomeric state, for which the data from the PACES detectors were vital, was studied. Finally, a description of the new GRIFFIN spectrometer, which uses the same auxiliary detectors as the 8 pi spectrometer, is given.


Review of Scientific Instruments | 2014

A field programmable gate array-based time-resolved scaler for collinear laser spectroscopy with bunched radioactive potassium beams

D. M. Rossi; K. Minamisono; B. R. Barquest; G. Bollen; K. Cooper; M. Davis; K. Hammerton; M. Hughes; P. Mantica; D. J. Morrissey; R. Ringle; J. A. Rodriguez; C. A. Ryder; S. Schwarz; R. Strum; C. S. Sumithrarachchi; D. Tarazona; Shen Zhao

A new data acquisition system including a Field Programmable Gate Array (FPGA) based time-resolved scaler was developed for laser-induced fluorescence and beam bunch coincidence measurements. The FPGA scaler was tested in a collinear laser-spectroscopy experiment on radioactive (37)K at the BEam COoler and LAser spectroscopy (BECOLA) facility at the National Superconducting Cyclotron Laboratory at Michigan State University. A 1.29 μs bunch width from the buncher and a bunch repetition rate of 2.5 Hz led to a background suppression factor of 3.1 × 10(5) in resonant photon detection measurements. The hyperfine structure of (37)K and its isotope shift relative to the stable (39)K were determined using 5 × 10(4) s(-1) (37)K ions injected into the BECOLA beam line. The obtained hyperfine coupling constants A((2)S(1/2)) = 120.3(1.4) MHz, A((2)P(1/2)) = 15.2(1.1) MHz, and A((2)P(3/2)) = 1.4(8) MHz, and the isotope shift δν(39, 37) = -264(3) MHz are consistent with the previously determined values, where available.


Hyperfine Interactions | 2006

The LEBIT facility at MSU. High-precision mass measurements at a fragmentation facility

S. Schwarz; C. Bachelet; M. Block; G. Bollen; D. Davies; M. Facina; C. M. Folden; C. Guénaut; J. Huikari; E. Kwan; A. A. Kwiatkowski; D. J. Morrissey; G. K. Pang; A. Prinke; R. Ringle; J. Savory; P. Schury; C. S. Sumithrarachchi; T. Sun

The low-energy beam and ion trap facility LEBIT at the NSCL at MSU has demonstrated that rare isotopes produced by fast-beam fragmentation can be slowed down and prepared such that precision experiments with low-energy beams are possible. For this purpose high-pressure gas-stopping is employed combined with advanced ion manipulation techniques. Penning trap mass measurements on short-lived rare isotopes have been performed with a 9.4 T Penning trap mass spectrometer. Examples include 66As, which has a half-live of only 96 ms, and the super-allowed Fermi-emitter 38Ca, for which a mass accuracy of 8 ppb (280 eV) has been achieved. The high accuracy of this new mass value makes 38Ca a new candidate for the test of the conserved vector current hypothesis.


Physical Review Letters | 2016

High Precision Determination of the β Decay Q(EC) Value of (11)C and Implications on the Tests of the Standard Model.

K. Gulyuz; G. Bollen; M. Brodeur; R. A. Bryce; K. Cooper; M. Eibach; C. Izzo; E. Kwan; K. Manukyan; D. J. Morrissey; O. Naviliat-Cuncic; Matthew Redshaw; R. Ringle; R. Sandler; S. Schwarz; C. S. Sumithrarachchi; A. A. Valverde; A. C. C. Villari

We report the determination of the Q(EC) value of the mirror transition of (11)C by measuring the atomic masses of (11)C and (11)B using Penning trap mass spectrometry. More than an order of magnitude improvement in precision is achieved as compared to the 2012 Atomic Mass Evaluation (Ame2012) [Chin. Phys. C 36, 1603 (2012)]. This leads to a factor of 3 improvement in the calculated Ft value. Using the new value, Q(EC)=1981.690(61)  keV, the uncertainty on Ft is no longer dominated by the uncertainty on the Q(EC) value. Based on this measurement, we provide an updated estimate of the Gamow-Teller to Fermi mixing ratio and standard model values of the correlation coefficients.


Journal of Physics: Conference Series | 2012

Towards 26Na via (d,p) with SHARC and TIGRESS and a novel zero-degree detector

G. Wilson; W. N. Catford; C. Aa. Diget; N. A. Orr; P. Adsley; H. Al-Falou; R. Ashley; R. A. E. Austin; G. C. Ball; J.C. Blackmon; A. J. Boston; H. J. Boston; S. M. Brown; A. A. Chen; J. Chen; R. Churchman; D. S. Cross; J. Dech; M. Djongolov; T.E. Drake; U. Hager; S. P. Fox; B. R. Fulton; N. Galinski; A. B. Garnsworthy; G. Hackman; D. S. Jamieson; R. Kanungo; K. G. Leach; J. P. Martin

Nucleon transfer experiments have in recent years begun to be exploited in the study of nuclei far from stability, using radioactive beams in inverse kinematics. New techniques are still being developed in order to perform these experiments. The present experiment is designed to study the odd-odd nucleus 26Na which has a high density of states and therefore requires gamma-ray detection to distinguish between them. The experiment employed an intense beam of up to 3×107 pps of 25Na at 5.0 MeV/nucleon from the ISAC-II facility at triumf. The new silicon array SHARC was used for the first time and was coupled to the segmented clover gamma-ray array TIGRESS. A novel thin plastic scintillator detector was employed at zero degrees to identify and reject reactions occurring on the carbon component of the (CD)2 target. The efficiency of the background rejection using this detector is described with respect to the proton and gamma-ray spectra from the (d,p) reaction.


Journal of Instrumentation | 2011

Commissioning the DANTE array of BaF2 detectors at TRIUMF-ISAC using a fast-timing lifetime measurement

D. S. Cross; G. C. Ball; P. E. Garrett; S. Triambak; S. J. Williams; C. Andreoiu; R. Churchman; A. B. Garnsworthy; G. Hackman; J.R. Leslie; J. N. Orce; C. S. Sumithrarachchi; C. E. Svensson

The Di-pentagonal Array for Nuclear Timing Experiments (DANTE) is an array of ten BaF2 detectors used in conjunction with the 8π gamma-ray spectrometer at the TRIUMF-ISAC radioactive-ion beam facility. DANTE is used to conduct direct lifetime measurements of nuclear excited states in the picosecond - nanosecond range. This, in turn, will aid in probing the collective structures of deformed nuclei. The capability of DANTE to measure nanosecond-scale lifetimes is demonstrated by using a 152Eu source. The half-life of the Iπ = 21+ state of 152Sm is measured to be 1.426 ± 0.018 ns.


Physics Letters B | 2018

Reorientation-effect measurement of the first 2+ state in 12C : Confirmation of oblate deformation

M. Kumar Raju; J. N. Orce; Petr Navratil; G. C. Ball; T.E. Drake; S. Triambak; G. Hackman; C. J. Pearson; K.J. Abrahams; E.H. Akakpo; H. Al Falou; R. Churchman; D.S. Cross; M. Djongolov; N. Erasmus; P. Finlay; A. B. Garnsworthy; P. E. Garrett; D. Jenkins; R. Kshetri; K. G. Leach; S. Masango; D.L. Mavela; C.V. Mehl; M.J. Mokgolobotho; C. Ngwetsheni; G.G. O'Neill; E. T. Rand; S. Sjue; C. S. Sumithrarachchi

Abstract A Coulomb-excitation reorientation-effect measurement using the TIGRESS γ−ray spectrometer at the TRIUMF/ISAC II facility has permitted the determination of the 〈 2 1 + ‖ E 2 ˆ ‖ 2 1 + 〉 diagonal matrix element in 12C from particle−γ coincidence data and state-of-the-art no-core shell model calculations of the nuclear polarizability. The nuclear polarizability for the ground and first-excited (2 1 + ) states in 12C have been calculated using chiral NN N4LO500 and NN+3NF350 interactions, which show convergence and agreement with photo-absorption cross-section data. Predictions show a change in the nuclear polarizability with a substantial increase between the ground state and first excited 2 1 + state at 4.439 MeV. The polarizability of the 2 1 + state is introduced into the current and previous Coulomb-excitation reorientation-effect analyses of 12C. Spectroscopic quadrupole moments of Q S ( 2 1 + ) = + 0.053 ( 44 ) eb and Q S ( 2 1 + ) = + 0.08 ( 3 ) eb are determined, respectively, yielding a weighted average of Q S ( 2 1 + ) = + 0.071 ( 25 ) eb, in agreement with recent ab initio calculations. The present measurement confirms that the 2 1 + state of 12C is oblate and emphasizes the important role played by the nuclear polarizability in Coulomb-excitation studies of light nuclei.


Physical Review C | 2018

Precision mass measurements of neutron-rich Co isotopes beyond N=40

C. Izzo; G. Bollen; M. Brodeur; M. Eibach; K. Gulyuz; J. D. Holt; J. M. Kelly; Matthew Redshaw; R. Ringle; R. Sandler; S. Schwarz; S. R. Stroberg; C. S. Sumithrarachchi; A. A. Valverde; A. C. C. Villari

The region near Z=28, N=40 is a subject of great interest for nuclear structure studies due to spectroscopic signatures in

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D. J. Morrissey

Michigan State University

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K. G. Leach

Colorado School of Mines

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S. Schwarz

Michigan State University

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G. Bollen

Michigan State University

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R. Ringle

Michigan State University

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G. C. Ball

Chalk River Laboratories

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