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Dive into the research topics where R.J. Miller is active.

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Featured researches published by R.J. Miller.


Physics Letters B | 1976

KLo interactions at 550 MeV/c☆

Y. Cho; M. Derrick; R.J. Miller; R.P. Smith; A. Engler; G. Keyes; R.W. Kraemer; J. Schlereth; M. Tanaka

Abstract Differential and channel cross sections and hyperon polarizations are presented for the reactions KLop → KSop, π+Λo, and π+Σo at an average beam momentum of 550 MeV/c. These data provide constraints on KN and K N amplitudes obtained from charged kaon reactions and reject one of the S = +1, I = 0 and one of the S = -1, I = 1 phase shift solutions.


Physical Review D | 1978

Measurement of the f/sub +/ form factor in K/sup 0//sub L/. -->. pi. /sup + -/e/sup - +/v decays using a large hydrogen bubble chamber

A. Engler; G. Keyes; R.W. Kraemer; M. Tanaka; Y. Cho; M. Derrick; D. Lissauer; R.J. Miller; J. L. Schlereth

The decay K/sup 0//sub L/ ..-->.. ..pi..e..nu.. was studied in an experiment using the Argonne 12-ft bubble chamber exposed to a K/sup 0//sub L/ beam of momentum 550 +- 35 MeV/c. Use of the monochromatic beam and the large chamber volume allowed the selection of about 12 000 K/sup 0//sub e/3 events, containing a small ((5.3 +- 0.5) %) and well understood background from K/sup 0//sub mu3/ decay. The main feature of this experiment is the good acceptance over the Dalitz plot which minimizes possible systematic errors in the determination of the vector form factor f/sub +/(q/sup 2/). We find that the data are adequately described by a linear q/sup 2/ parameterization, f/sub +/(q/sup 2/) = f/sub +/(0)(1 + lambda/sub +/q/sup 2// m/sub ..pi..//sup 2/), with the slope parameter lambda/sub +/ = 0.028 +- 0.004 before radiative corrections are made. Direct application of radiative corrections, as calculated by Ginsberg, yields lambda/sub +/ = 0.025 +- 0.005. Our result is in good agreement with other recent experiments and with the assumption of K* (890) dominance.


Physics Letters B | 1976

Energy dependence of the reactions KLop→KSop,π+Λ, π+Σo from 1540 to 1610 MeV

A. Engler; G. Keyes; R.W. Kraemer; J. Schlereth; M. Tanaka; Y. Cho; M. Derrick; D. Lissauer; R.J. Miller; R.P. Smith

Abstract The reactions K L o p→K S o p, π + Λ , π + Σ o have been measured for center-of-mass energies from 1540 to 1610 MeV. Channel cross sections and coefficients of the Legendre polynomial expansion of the differential cross sections and hyperon polarizations are presented. We see no evidence in the πΛ channel for the suggested 3 2 − resonance at 1580 MeV. The cross section for the K S o p channel shows an energy dependence which is not predicted by the existing phase shift solutions based on charged kaon data.


Particles and Fields-1977: Annual Meeting of the American Physical Society Division of Particles and Fields | 2008

High resolution measurement of τp elastic scattering near 90° c.m.

L. E. Price; K. A. Jenkins; R. Klem; R.J. Miller; P. Schreiner; H. Courant; Y. Makdisi; M. L. Marshak; E. A. Peterson; K. Ruddick

Large angle π±p elastic scattering cross sections have been measured between 2 and 9 GeV/c in fine intervals of incident momentum and scattering angle. The data are used to test predictions of the quark parton model and the statistical bootstrap model.


Physical Review D | 1977

Measurement of K L 0 → π + π − π 0 decay parameters

Y. Cho; M. Derrick; D. Lissauer; R.J. Miller; A. Engler; G. Keyes; R.W. Kraemer; J. Schlereth; M. Tanaka

The decay


Physical Review D | 1977

Measurement of K/sup 0//sub L/. -->. pi. /sup +/. pi. /sup -/. pi. /sup 0/ decay parameters. [Branching ratio, isospin, decay amplitude]

Y. Cho; M. Derrick; D. Lissauer; R.J. Miller; A. Engler; G. Keyes; R.W. Kraemer; J. L. Schlereth; M. Tanaka

{K}_{L}^{0}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\pi}}^{0}


Physical Review D | 1976

A Measurement of K0(L) --> pi+ pi- pi0 Decay Parameters

Y. Cho; J. L. Schlereth; R.J. Miller; R.W. Kraemer; D. Lissauer; A. Engler; M. Derrick; G. Keyes; M. Tanaka

has been studied in an experiment using the Argonne 12-ft hydrogen bubble chamber exposed to a


Physical Review D | 1978

Properties of the hadronic system resulting fromν¯μpinteractions

M. Derrick; P. Gregory; L. Hyman; K. Jaeger; D. Lissauer; R.J. Miller; B. Musgrave; J. J. Phelan; P. Schreiner; R. Singer; S.J. Barish; A. Engler; G. Keyes; T. Kikuchi; R.W. Kraemer; V. E. Barnes; D.D. Carmony; A. F. Garfinkel; A. T. Laasanen

{K}_{L}^{0}


Physical Review Letters | 1976

Study of high-energy antineutrino-proton interactions

M. Derrick; T. Dombeck; L. Hyman; K. Jaeger; D. Lissauer; R.J. Miller; B. Musgrave; J.J. Phelan; P. Schreiner; R. Singer; S.J. Barish; A. Engler; G. Keyes; R.W. Kraemer; J. L. Schlereth

beam of momentum 550 \ifmmode\pm\else\textpm\fi{} 35 MeV/c. After radiative corrections to the data, a fit using a matrix element of the form


Physical Review Letters | 1978

Fluctuations in large-angle. pi. /sup + -/elastic scattering

K. A. Jenkins; L. E. Price; R. Klem; R.J. Miller; P. Schreiner; H. Courant; Y. Makdisi; M. L. Marshak; E. A. Peterson; K. Ruddick

{|M|}^{2}\ensuremath{\propto}1+\frac{g({s}_{3}\ensuremath{-}{s}_{0})}{{{m}_{{\ensuremath{\pi}}^{+}}}^{2}}+h{[\frac{({s}_{3} \ensuremath{-} {s}_{0})}{{{m}_{{\ensuremath{\pi}}^{+}}}^{2}}]}^{2} + k{[\frac{({s}_{1} \ensuremath{-} {s}_{2})}{{{m}_{{\ensuremath{\pi}}^{+}}}^{2}}]}^{2}

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A. Engler

Carnegie Mellon University

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R.W. Kraemer

Carnegie Mellon University

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G. Keyes

Carnegie Mellon University

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D. Lissauer

Brookhaven National Laboratory

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M. Tanaka

Carnegie Mellon University

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P. Schreiner

Argonne National Laboratory

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Y. Cho

Argonne National Laboratory

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J. L. Schlereth

Argonne National Laboratory

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M. Derrick

Argonne National Laboratory

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B. Musgrave

Argonne National Laboratory

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