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Volumn 61, Issue 7, 2000, Pages

Muonium decay

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EID: 17144408402     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.61.073001     Document Type: Article
Times cited : (38)

References (39)
  • 10
    • 85037216127 scopus 로고    scopus 로고
    • R. Carey and D. Hertzog et al., “A precision measurement of the positive muon lifetime using a pulsed muon beam and μLan detector,” proposal to PSI
    • R. Carey and D. Hertzog et al., “A precision measurement of the positive muon lifetime using a pulsed muon beam and μLan detector,” proposal to PSI.
  • 11
    • 85037188625 scopus 로고    scopus 로고
    • J. Kirkby et al., FAST proposal to PSI, 1999
    • J. Kirkby et al., FAST proposal to PSI, 1999.
  • 12
    • 85037216061 scopus 로고    scopus 로고
    • S. N. Nakamura et al., “Precise measurement of the (Formula presented) lifetime and test of the exponential decay law,” RIKEN-RAL proposal
    • S. N. Nakamura et al., “Precise measurement of the (Formula presented) lifetime and test of the exponential decay law,” RIKEN-RAL proposal.
  • 13
    • 0004226417 scopus 로고
    • C. S. Wu, V. W. Hughes
    • J. Brewer, K. Crowe, F. Gygax, and A. Schenk, in Muon Physics, edited by C. S. Wu and V. W. Hughes (Academic Press, New York, 1977), Vol. 3, p. 1.
    • (1977) Muon Physics , vol.3 , pp. 1
    • Brewer, J.1    Crowe, K.2    Gygax, F.3    Schenk, A.4
  • 14
    • 33744594626 scopus 로고
    • G. Alefeld, J. Völkl
    • A. Seeger, in Topics in Applied Physics, edited by G. Alefeld and J. Völkl (Springer-Verlag, New York, 1978), Vol. 28, p. 349.
    • (1978) Topics in Applied Physics , vol.28 , pp. 349
    • Seeger, A.1
  • 17
  • 18
    • 85037187173 scopus 로고    scopus 로고
    • V. W. Hughes and G. zu Putlitz, in Quantum Electrodynamics, edited by T. Kinoshita (World Scientific, Singapore, 1990), p. 822
    • V. W. Hughes and G. zu Putlitz, in Quantum Electrodynamics, edited by T. Kinoshita (World Scientific, Singapore, 1990), p. 822.
  • 20
    • 85037214451 scopus 로고    scopus 로고
    • The (Formula presented) state of free muonium is metastable
    • The (Formula presented) state of free muonium is metastable 15, decaying to (Formula presented) in about 1/7 sec. The value of (Formula presented) in that configuration leads to a factor of 4 reduction in the corresponding time dilation corrections of Eqs. (101112).
  • 24
    • 85037239768 scopus 로고    scopus 로고
    • hep-ph/9804275
    • For a recent discussion and further references see N. Uraltsev, hep-ph/9804275.
    • Uraltsev, N.1
  • 27
    • 85037192424 scopus 로고    scopus 로고
    • Our result in Eq. (17) is about an order of magnitude smaller than a similar calculation in Ref
    • Our result in Eq. (17) is about an order of magnitude smaller than a similar calculation in Ref. 13.
  • 28
    • 0000088737 scopus 로고
    • Muonium annihilation was originally estimated in B. Pontecorvo, Zh. Eksp. Teor. Fiz. 33, 549 (1958) [Sov. Phys. JETP 6, 429 (1958)].
    • (1958) Sov. Phys. JETP , vol.6 , pp. 429
    • Pontecorvo, B.1
  • 29
    • 85037210062 scopus 로고    scopus 로고
    • The singlet component of muonium does not decay into (Formula presented) due to helicity suppression. The triplet decay rate can be obtained by multiplying Eq. (17) by 4/3
    • The singlet component of muonium does not decay into (Formula presented) due to helicity suppression. The triplet decay rate can be obtained by multiplying Eq. (17) by 4/3.
  • 30
    • 33744671582 scopus 로고
    • P.-J. Li, Z.-Q. Tan, and C.-E. Wu, J. Phys. G 14, 525 (1988).
    • (1988) J. Phys. G , vol.14 , pp. 525
  • 38
    • 85037211548 scopus 로고    scopus 로고
    • The expansion is analytic because the final decay state is far from any threshold. Bound state effects on the low energy (Formula presented) spectrum modify the total decay rate at (Formula presented) and can, therefore, be ignored in this analysis
    • The expansion is analytic because the final decay state is far from any threshold. Bound state effects on the low energy (Formula presented) spectrum modify the total decay rate at (Formula presented) and can, therefore, be ignored in this analysis.
  • 39
    • 85037238409 scopus 로고    scopus 로고
    • The right-hand side of the normalization condition would be the electromagnetic form factor of muonium at zero momentum transfer if the electron had no electric charge, and provided that the potential is instantaneous [which is true up to (Formula presented) corrections which we ignore]. Charge conservation or gauge invariance demands that this form factor equal unity
    • The right-hand side of the normalization condition would be the electromagnetic form factor of muonium at zero momentum transfer if the electron had no electric charge, and provided that the potential is instantaneous [which is true up to (Formula presented) corrections which we ignore]. Charge conservation or gauge invariance demands that this form factor equal unity.


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