P. Finlay
University of Guelph
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Featured researches published by P. Finlay.
Journal of Physics G | 2005
C. E. Svensson; P Amaudruz; C. Andreoiu; A Andreyev; R. A. E Austin; G. C. Ball; D. Bandyopadhyay; A. J. Boston; R. S. Chakrawarthy; A. Chen; R. Churchman; T.E. Drake; P. Finlay; P. E. Garrett; G. F. Grinyer; G. Hackman; B. Hyland; B Jones; R. Kanungo; R Maharaj; J. P. Martin; D. Morris; A. C. Morton; C. J. Pearson; A. A. Phillips; J J Ressler; R. Roy; F. Sarazin; M. A. Schumaker; H. C. Scraggs
The TRIUMF-ISAC gamma-ray escape-suppressed spectrometer (TIGRESS) is a new γ-ray detector array being developed for use at TRIUMFs Isotope Separator and Accelerator (ISAC) radioactive ion beam facility. TIGRESS will comprise 12 32-fold segmented clover-type HPGe detectors coupled with 20-fold segmented modular Compton suppression shields and custom digital signal processing electronics. This paper provides an overview of the TIGRESS project and progress in its development to date.
Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 2003
C. E. Svensson; R. A. E. Austin; G. C. Ball; P. Finlay; P. E. Garrett; G. F. Grinyer; G. Hackman; C.J. Osborne; F. Sarazin; H.C. Scraggs; M. B. Smith; J.C. Waddington
High-resolution γ-ray spectroscopy is one of the most powerful and versatile experimental techniques in low-energy nuclear physics research. With the continuing development of hyper-pure germanium (HPGe) detector technology, including multi-crystal detectors, contact segmentation, and digital signal processing techniques, large γ-ray detector arrays will continue to play a major role in the experimental programs at existing and future radioactive ion beam facilities. This paper provides an overview of recent progress in, and future plans for, the development of large γ-ray spectrometers at such facilities, including the recent commissioning of the 8π spectrometer at ISAC-I and the proposed TRIUMF-ISAC gamma-ray escape suppressed spectrometer array for the ISAC-II facility.
Journal of Physics G | 2005
G. C. Ball; T Achtzehn; D Albers; J S Al Khalili; C. Andreoiu; A Andreyev; S F Ashley; R. A. E Austin; J A Becker; P Bricault; S Chan; R. S. Chakrawarthy; R. Churchman; H Coombes; E S Cunningham; J Daoud; M Dombsky; T.E. Drake; B Eshpeter; P. Finlay; P. E. Garrett; Ch. Geppert; G. F. Grinyer; G. Hackman; V Hanemaayer; B. Hyland; G A Jones; K. A. Koopmans; W. D. Kulp; J Lassen
High-resolution γ-ray spectroscopy is essential to fully exploit the unique, high-quality beams available at the next generation of radioactive ion beam facilities such as the TRIUMF isotope separator and accelerator (ISAC). The 8π spectrometer, which consists of 20 Compton-suppressed HPGe detectors, has recently been reconfigured for a vigorous research programme in weak interaction and nuclear structure physics. With the addition of a variety of ancillary detectors it has become the worlds most powerful device dedicated to β-decay studies. This paper provides a brief overview of the apparatus and highlights from recent experiments.
Physical Review Letters | 2012
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
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.
arXiv: Probability | 2009
G. C. Ball; C. Andreoiu; R. A. E. Austin; D. Bandyopadhyay; John A Becker; P. Bricault; N. Brown; S. Chan; R. Churchman; S. Colosimo; H. Coombes; D. S. Cross; G. A. Demand; T.E. Drake; M. Dombsky; S. Ettenauer; P. Finlay; D. Furse; A. Garnsworthy; P. E. Garrett; K. L. Green; G. F. Grinyer; B. Hyland; G. Hackman; R. Kanungo; W. D. Kulp; J. Lassen; K. G. Leach; J.R. Leslie; C. M. Mattoon
High‐resolution gamma‐ray spectroscopy is essential to fully exploit the unique scientific opportunities at the next generation radioactive ion beam facilities such as the TRIUMF Isotope Separator and Accelerator (ISAC). At ISAC the 8π spectrometer and its associated auxiliary detectors is optimize for β‐decay studies while TIGRESS an array of segmented clover HPGe detectors has been designed for studies with accelerated beams. This paper gives a brief overview of these facilities and also presents recent examples of the diverse experimental program carried out at the 8π spectrometer.In this article we prove the bivariate uniqueness property for a particular “max-type” recursive distributional equation (RDE). Using the general theory developed in [5] we then show that the corresponding recursive tree process (RTP) has no external randomness, more preciously, the RTP is endogenous. The RDE we consider is so called the Logistic RDE, which appears in the proof of the ζ(2)-limit of the random assignment problem [4] using the local weak convergence method. Thus this work provides a non-trivial application of the general theory developed in [5]. AMS 2000 subject classification : 60E05, 60J80, 60K35, 62E10, 82B43.
Physical Review C | 2009
M. A. Schumaker; C. E. Svensson; D. Bandyopadhyay; G. A. Demand; P. Finlay; P. E. Garrett; K. L. Green; G. F. Grinyer; K. G. Leach; A. A. Phillips; J. Wong; D. Cline; A. B. Hayes; A. Whitbeck; G. Hackman; C. J. Pearson; A. N. Andreyev; G. C. Ball; L. Buchmann; R. Churchman
The low-energy structure of the proton dripline nucleus {sup 20}Na has been studied using Coulomb excitation at the TRIUMF-ISAC radioactive ion beam facility. A 1.7-MeV/nucleon {sup 20}Na beam of {approx}5x10{sup 6} ions/s was Coulomb excited by a 0.5-mg/cm{sup 2nat}Ti target. Scattered beam and target particles were detected by the BAMBINO segmented Si detector while {gamma} rays were detected by two TIGRESS HPGe clover detectors set perpendicular to the beam axis. Coulomb excitation from the 2{sup +} ground state to the first excited 3{sup +} and 4{sup +} states was observed, and B({lambda}L) values were determined using the 2{sup +}{yields}0{sup +} de-excitation in {sup 48}Ti as a reference. The resulting B({lambda}L){down_arrow} values are B(E2;3{sup +}{yields}2{sup +})=55{+-}6 e{sup 2} fm{sup 4} (17.0{+-}1.9 W.u.), B(E2;4{sup +}{yields}2{sup +})=35.7{+-}5.7 e{sup 2} fm{sup 4} (11.1{+-}1.8 W.u.), and B(M1;4{sup +}{yields}3{sup +})=0.154{+-}0.030 {mu}{sub N}{sup 2} (0.086{+-}0.017 W.u.). These measurements provide the first experimental determination of B({lambda}L) values for this proton dripline nucleus of astrophysical interest.
Physical Review C | 2005
F. Sarazin; Jim Al-Khalili; G. C. Ball; G. Hackman; P. M. Walker; R. A. E. Austin; B. Eshpeter; P. Finlay; P. E. Garrett; G. F. Grinyer; K. A. Koopmans; W. D. Kulp; J.R. Leslie; D. Melconian; C. J. Osborne; M. A. Schumaker; H. C. Scraggs; J. Schwarzenberg; M. B. Smith; C. E. Svensson; J.C. Waddington; J. Wood
The β-decay of 11Li has been studied at ISAC/TRIUMF using the 8pi spectrometer, an array of 20 Compton-suppressed high-purity germanium detectors. Most of the 11Li β-decay strength is observed to proceed through unbound states in 11Be, which subsequently decay by one-neutron emission to 10Be. This results in the observation of a γ-spectrum dominated by the decay of the excited states in 10Be. These transitions exhibit characteristic Doppler broadened lineshapes, due to the the recoiling effect induced by the neutron emission. A Monte-Carlo simulation was developed to analyze the complex shape of these γ-lines. Both the half-lives of states in 10Be and the energies of the β-delayed neutrons feeding those states were obtained. It was also possible to determine the excitation energies of the parent states in 11Be. The present contribution was the subject of a publication in a scientific journal (F. Sarazin et al., Phys. Rev. C 70, 031302(R)(2004) )shortly before the conference. It was judged not appropriate to submit for peerreviewing a contribution with nearly the same content. The reader is therefore invited to read the original publication.
Physics Letters B | 2018
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
D. S. Jamieson; P. E. Garrett; G. C. Ball; G. A. Demand; T. Faestermann; P. Finlay; K. L. Green; R. Hertenberger; K. G. Leach; A. A. Phillips; C. S. Sumithrarachchi; S. Triambak; H.-F. Wirth
The nuclear structure of Cd-112 has been investigated with the Cd-111((d)over-right-arrow, p)Cd-112 reaction. Isotopically enriched targets of Cd-111 were bombarded with 22 MeV polarized deuterons, and reaction products were analyzed with a magnetic spectrograph. Angular distributions and analyzing powers were determined for 129 states, 49 of which are newly observed, up to approximately 4.2 MeV in excitation energy. The observed angular distributions were compared with distorted wave Born approximation (DWBA) and adiabatic distorted wave approximation (ADWA) calculations to extract the spectroscopic factors. Two-quasineutron configurations involving coupling to the s(1/2) orbital are suggested. The sum of spectroscopic strengths extracted by using the ADWA for the individual l transfers are combined with previous results from the Cd-111((d)over-right-arrow, t) reaction and show good agreement with the 2j + 1 sum rule, whereas those extracted with the DWBA calculations are significantly less.