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Dive into the research topics where P. E. Knowles is active.

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Featured researches published by P. E. Knowles.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1996

A windowless frozen hydrogen target system

P. E. Knowles; G. Beer; J. L. Beveridge; J Douglas; G. M. Marshall; F. Mulhauser; M Maier; M. C. Fujiwara; A. R. Kunselman; J. Zmeskal

Abstract A cryogenic target system has been constructed in which gaseous mixtures of all three hydrogen isotopes have been frozen onto a thin, 65 mm diameter gold foil. The foil is cooled to 3 K while inside a 70 K radiation shield, all of which is mounted in a vacuum system maintained at 10−9 Torr. Stable multi-layer hydrogen targets of known uniformity and thickness have been maintained for required measurement times of up to several days. To date, hundreds of targets have been successfully used in muon-catalyzed fusion experiments at TRIUMF.


Hyperfine Interactions | 1993

Experiments with energetic [mu]d and [mu]t emitted from solid hydrogen

G. M. Marshall; J. L. Beveridge; J. M. Bailey; G. Beer; P. E. Knowles; G. R. Mason; A. Olin; J. H. Brewer; B. M. Forster; T. M. Huber; B. Pippitt; R. Jacot-Guillarmod; L. Schellenberg; P. Kammel; J. Zmeskal; A. R. Kunselman; C. J. Martoff; C. Petitjean

A set of experiments is reviewed which makes use of the emission of muonic deuterium from the surface of a layer of solid hydrogen. The behaviour of muons in a solid target system has been studied via detection of muon decay electrons, muonic X-rays, and fusion products (neutrons and charged particles). The emission of muonic deuterium is understood to result from the Ramsauer-Townsend scattering minimum. The energy distribution of the emitted atoms ranges from tenths of eV to about 10 eV, and can be controlled to some extent. A proposal is described to use muonic tritium emission to measure the energy dependence of muonic molecular formation.


Physical Review A | 1997

Muon catalyzed fusion in 3-K solid deuterium

P. E. Knowles; Gerald A. Beer; G. R. Mason; T.A. Porcelli; A. Adamczak; J. M. Bailey; J. L. Beveridge; G. M. Marshall; A. Olin; M. C. Fujiwara; T. M. Huber; R. Jacot-Guillarmod; F. Mulhauser; P. Kammel; Johann Zmeskal; S. K. Kim; A. R. Kunselman; C. J. Martoff; C. Petitjean

Muon catalyzed fusion in deuterium traditionally has been studied in gaseous and liquid targets. The TRIUMF solid-hydrogen-layer target system has been used to study the fusion reaction rates in the solid phase of D{sub 2} at a target temperature of 3 K. Products of two distinct branches of the reaction were observed: neutrons by a liquid organic scintillator and protons by a silicon detector located inside the target system. The effective molecular formation rate from the upper hyperfine state of {mu}d and the hyperfine transition rate have been measured: {tilde {lambda}}{sub (3)/(2)}=2.71(7){sub stat}(32){sub syst}{mu}s{sup {minus}1} and {tilde {lambda}}{sub (3)/(2)(1)/(2)}=34.2(8){sub stat}(1){sub syst}{mu}s{sup {minus}1}. The molecular formation rate is consistent with other recent measurements, but not with the theory for isolated molecules. The discrepancy may be due to incomplete thermalization, an effect that was investigated by Monte Carlo calculations. Information on branching ratio parameters for the s and p wave d+d nuclear interaction has been extracted. {copyright} {ital 1997} {ital The American Physical Society}


Hyperfine Interactions | 1996

Muon molecular formation and transfer rate in solid hydrogen-deuterium mixtures

R. Jacot-Guillarmod; J. M. Bailey; G. Beer; J. L. Beveridge; M. C. Fujiwara; T. M. Huber; P. Kammel; P. E. Knowles; A. R. Kunselman; G. M. Marshall; C. J. Martoff; G. R. Mason; F. Mulhauser; A. Olin; C. Petitjean; J. Woźniak; J. Zmeskal

In an experiment at TRIUMF to study muon-catalyzed fusion and associated atomic and molecular effects, negative muons were stopped in a solid protium hydrogen layer containing a small amount of deuterium. Most of the resulting µp atoms disappeared by formation of ppµ molecules or by muon transfer to a deuteron. The µd can drift almost freely through the hydrogen layer due to the Ramsauer-Townsend effect and may even leave the layer. If a thin neon layer is frozen atop the hydrogen, the exiting muonic atoms will very rapidly release their muon to a neon atom. The analysis of the time structure of the neon X-rays is used to determine the rates of the slower processes involved in the evolution of the µp. This analysis has been performed with the help of Monte Carlo calculations, which simulate the kinetics of both µp and µd atoms in the hydrogen mixtures.


Hyperfine Interactions | 1993

Producing μ−d and μ−t in vacuum

P. E. Knowles; G. Beer; G. R. Mason; A. Olin; J. M. Bailey; J. L. Beveridge; G. M. Marshall; J. H. Brewer; B. M. Forster; T. M. Huber; R. Jacot-Guillarmod; L. Schellenberg; P. Kammel; J. Zmeskal; A. R. Kunselman; C. J. Martoff; C. Petitjean

After the feasibility of vacuum isolated μ−d production was demonstrated at TRIUMF in 1989, development was begun on a target system that would take advantage of the process to aid in the understanding of the muon catalyzed fusion cycle. Minimal neutron backgrounds, the ability to use silicon detectors, and compatibility with tritium were considered important for a very versatile target system. The advantages which the target gives in isolating μCF process will be outlined.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1997

Characterization of solidified gas thin film targets via alpha particle energy loss

M. C. Fujiwara; G. Beer; J. L. Beveridge; J. L. Douglas; T. M. Huber; R. Jacot-Guillarmod; S.K Kim; P. E. Knowles; A. R. Kunselman; M. Maier; G. M. Marshall; G. R. Mason; F. Mulhauser; A. Olin; C. Petitjean; T.A. Porcelli; J. Zmeskal

Abstract A method is reported for measuring the thickness and uniformity of thin films of solidified gas targets. The energy of α particles traversing the film is measured and the energy loss is converted to thickness using the range. The uniformity is determined by measuring the thickness at different positions with an array of sources. Monte Carlo simulations have been performed to study the film deposition mechanism. Thickness calibrations for a TRIUMF solid hydrogen target system are presented.


Archive | 1999

Resonant formation measurements of \(dt\mu \) via time of flight

G. M. Marshall; T.A. Porcelli; A. Adamczak; J.M. Bailey; G. Beer; M. P. Faifman; M. C. Fujiwara; T. M. Huber; R. Jacot-Guillarmod; P. Kammel; S.K. Kim; P. E. Knowles; A. R. Kunselman; M. Maier; V.E. Markushin; G. R. Mason; F. Mulhauser; A. Olin; C. Petitjean; J. Zmeskal

Solid hydrogen in the form of an inhomogeneous layered target offers several experimental advantages when compared with liquid or gas. Beams of non-thermalized muonic hydrogen atoms allow us to explore resonant molecular ion formation processes near eV kinetic energies. Isotopically specific layers make it possible to separate competing and confusing interactions and to employ the time of flight for comparison with predictions based on theoretical energy dependences. Unambiguous charged fusion product detection simplifies absolute intensity measurements.The systematic uncertainties encountered in resonant molecular ion formation measurements, using solid hydrogen target layers, are being investigated with simulations which use the many calculated energy-dependent rates and cross-sections which are now available. The importance of the rates for processes such as muon transfer and elastic scattering are discussed, and results of some recent analyses are presented.


Hyperfine Interactions | 1996

MEASURING STICKING AND STRIPPING IN MUON-CATALYZED DT FUSION WITH MULTILAYER THIN FILMS

M. C. Fujiwara; J. M. Bailey; Gerald A. Beer; J. L. Beveridge; E. Gete; T. M. Huber; R. Jacot-Guillarmod; P. Kammel; Nazir P. Kherani; S. K. Kim; P. E. Knowles; A. R. Kunselman; V. E. Markushin; G. M. Marshall; C. J. Martoff; G. R. Mason; F. Mulhauser; A. Olinc; C. Petitjean; T.A. Porcelli; T. J. Stocki; Johann Zmeskal

We propose a direct measurement of muon sticking to alpha particles in muon-catalyzed dt fusion at a high density. Exploiting the features of a multilayer thin-film target developed at TRIUMF, the sticking is determined directly by detection of charged fusion products. Experimental separation of initial sticking and stripping may become possible for the first time. Monte Carlo simulations, as well as preliminary results of test measurements are described.


Hyperfine Interactions | 1993

Muon transfer from hot muonic hydrogen atoms to neon

R. Jacot-Guillarmod; J. M. Bailey; G. Beer; P. E. Knowles; G. R. Mason; A. Olin; J. L. Beveridge; G. M. Marshall; J. H. Brewer; B. M. Forster; T. M. Huber; P. Kammel; J. Zmeskal; A. R. Kunselman; C. Petitjean

A negative muon beam has been directed on adjacent solid layers of hydrogen and neon. Three targets differing by their deuterium concentration were investigated. Muonic hydrogen atoms can drift to the neon layer where the muon is immediately transferred. The time structure of the muonic neon X-rays follows the exponential law with a disappearance rate corresponding to the one of μ−p atoms in each target. The rates λppμ and λpd can be extracted


Hyperfine Interactions | 1996

Measurement of muon transfer rate λpt and molecular formation rate λppµ, in solid hydrogen targets, in solid hydrogen targets

F. Mulhauser; J. M. Bailey; G. Beer; J. L. Beveridge; J. L. Douglas; M. C. Fujiwara; T. M. Huber; R. Jacot-Guillarmod; P. Kammel; P. E. Knowles; S. K. Kim; A. R. Kunselman; M. Maier; V. E. Markushin; G. M. Marshall; C. J. Martoff; G. R. Mason; A. Olin; C. Petitjean; T.A. Porcelli; J. Zmeskal

The knowledge of muon transfer from protium to tritium is essentially theoretical and the different theoretical values disagree partially. Using solid hydrogen-tritium targets, with different tritium concentrations, we obtained precise experimental results for the transfer rate to tritium and the ppµ molecular formation rate. The time spectra of neutrons and alpha particles produced after dtµ fusion are used to determine the transfer rate λpt and the molecule formation rate λppµ.

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T. M. Huber

Gustavus Adolphus College

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A. Olin

University of Victoria

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G. R. Mason

University of Victoria

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C. Petitjean

Paul Scherrer Institute

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R. Jacot-Guillarmod

University of British Columbia

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G. Beer

University of Victoria

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