Abstract
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.
Similar content being viewed by others
References
E.A. Vesman, Pis'ma Zh. Èksper. Teoret. Fiz. 5 (1967) 113 (JETP Lett. 5 (1967) 91).
V.P. Dzhelepov et al., Zh. Èksper. Teoret. Fiz. 50 (1966) 1235 (Soviet Phys. JETP 23 (1966) 820).
V.M. Bystritsky et al., Phys. Lett. B 94 (1980) 476.
S. Jones et al., Phys. Rev. Lett. 56 (1986) 588.
W.H. Breunlich et al., Phys. Rev. Lett. 58 (1987) 329.
L.I. Ponomarev, Contemporary Physics 31 (1990) 219; J.S. Cohen, in: Review of Fundamental Processes and Applications of Atoms and Ions, ed. C.D. Lin (World Scientific, Singapore, 1993); W.H. Breunlich et al., Ann. Rev. Nucl. Part. Sci. 39 (1989) 311.
M.P. Faifman and L.I. Ponomarev, Phys. Lett. B 265 (1991) 201; M.P. Faifman et al., Hyp. Interact. 101/102 (1996) 179.
Yu.V. Petrov et al., Phys. Lett. B 331 (1994) 266.
B.M. Forster et al., Hyp. Interact. 65 (1990) 1007.
G.M. Marshall et al., Hyp. Interact. 101/102 (1996) 47.
F. Mulhauser et al., this issue.
M.C. Fujiwara et al., this issue.
M.C. Fujiwara, Ph.D. thesis, University of British Columbia (in preparation).
T.A. Porcelli, Ph.D. thesis, University of Victoria (in preparation).
P.E. Knowles et al., Nucl. Instrum. Methods A 368 (1996) 604.
M.C. Fujiwara et al., Nucl. Instrum. Methods A 395 (1997) 159.
F. Mulhauser et al., Phys. Rev. A 53 (1996) 3069.
V.E. Markushin et al., Hyp. Interact. 101/102 (1996) 155.
T.M. Huber et al., this issue.
J. Wozniak et al., Hyp. Interact. 101/102 (1996) 573.
J. Wozniak et al., this issue.
D.J. Abbot et al., Phys. Rev. A 55 (1997) 214.
A. Badertscher et al., Phys. Lett. B 392 (1997) 28.
K.A. Aniol et al., Phys. Rev. A 28 (1983) 2684.
L. Bracci et al., Muon Catal. Fusion 4 (1989) 247.
C. Chiccoli et al., Muon Catal. Fusion 7 (1992) 87.
A. Adamczak et al., Muon Catal. Fusion 7 (1992) 309.
A. Adamczak, this issue.
M. Jeitler et al., Phys. Rev. A 51 (1995) 2881.
Yu.V. Petrov and V.Yu. Petrov, Phys. Lett. B 378 (1996) 1.
GEANT 3.21, CERN Program Library Long Writeup W5013, CERN, Geneva (1993).
M.C. Fujiwara et al., Hyp. Interact. 106 (1997) 257.
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Marshall, G., Porcelli, T., Adamczak, A. et al. Resonant formation measurements of \(dt\mu \) via time of flight. Hyperfine Interactions 118, 89–101 (1999). https://doi.org/10.1023/A:1012636619847
Issue Date:
DOI: https://doi.org/10.1023/A:1012636619847