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1
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B. Lin, M C. Shih, T M. Bohanon, G E. Ice and P. Dutta, Phys. Rev. Lett.65, 191 (1990).
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(1990)
Phys. Rev. Lett.
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Lin, B.1
Shih, M.C.2
Bohanon, T.M.3
Ice, G.E.4
Dutta, P.5
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2
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K. Kjaer, J. Als-Nielsen, C A. Helm, P. Tippman-Krayer and H. Mohwald, J. Phys. Chem.93, 3200 (1989).
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Kjaer, K.1
Als-Nielsen, J.2
Helm, C.A.3
Tippman-Krayer, P.4
Mohwald, H.5
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4
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0000423531
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M C. Shih, T M. Bohanon, J M. Mikrut, P. Zschack and P. Dutta, Phys. Rev. A45, 5734 (1992).
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(1992)
Phys. Rev. A
, vol.45
, pp. 5734
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Shih, M.C.1
Bohanon, T.M.2
Mikrut, J.M.3
Zschack, P.4
Dutta, P.5
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5
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0001144613
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R M. Kenn, C. Bohm, A M. Bibo, I R. Peterson, H. Mohwald, J. Als-Nielsen and K. Kjaer, J. Phys. Chem.95, 2092 (1991).
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Kenn, R.M.1
Bohm, C.2
Bibo, A.M.3
Peterson, I.R.4
Mohwald, H.5
Als-Nielsen, J.6
Kjaer, K.7
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6
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0026932969
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T M. Bohanon, A M. Lee, J B. Ketterson and P. Dutta, Langmuir8, 2497 (1992).
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(1992)
Langmuir
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, pp. 2497
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Bohanon, T.M.1
Lee, A.M.2
Ketterson, J.B.3
Dutta, P.4
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8
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0011749344
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H. Eyring
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W. J. Moore, Jr., and H. Eyring, J. Chem. Phys.6, 391 (1938).
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Moore, W.J.1
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9
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4243086841
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T M. Bohanon, J. Mikrut, B M. Abraham, J B. Ketterson, S. Jacobson, L. Flosenzier, J. Torkelson and P. Dutta, Rev. Sci. Instrum.63, 1822 (1992).
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(1992)
Rev. Sci. Instrum.
, vol.63
, pp. 1822
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Bohanon, T.M.1
Mikrut, J.2
Abraham, B.M.3
Ketterson, J.B.4
Jacobson, S.5
Flosenzier, L.6
Torkelson, J.7
Dutta, P.8
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11
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36449008698
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T M. Bohanon, B M. Abraham, P. Dutta and J B. Ketterson, Rev. Sci. Instrum.62, 2959 (1991).
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Bohanon, T.M.1
Abraham, B.M.2
Dutta, P.3
Ketterson, J.B.4
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12
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85035195195
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We note that F. Behroozi and co-workers (unpublished) have recently shown that the detection scheme of Bohanon, can be greatly improved upon by digitizing the entire time-dependent phase-modulated wave form and fitting it to the standard Bessel function expansion
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We note that F. Behroozi and co-workers (unpublished) have recently shown that the detection scheme of Bohanon can be greatly improved upon by digitizing the entire time-dependent phase-modulated wave form and fitting it to the standard Bessel function expansion.
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13
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85035206942
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The modification of the instrument to function as a torsion pendulum is due to J. Condon and it is sometimes referred to as a Condon balance. (See J. Condon, thesis, Northwestern University
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The magnet was part of a Weston recording galvanometer marketed in the 1950s. The modification of the instrument to function as a torsion pendulum is due to J. Condon and it is sometimes referred to as a Condon balance. (See J. Condon, thesis, Northwestern University, 1962.)
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(1950)
1962.)
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16
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0008763137
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R. Piazza, T. Bellini, V. Degiorgio, R E. Goldstein, S. Leibler and R. Lipowsky, Phys. Rev. B38, 7223 (1988).
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(1988)
Phys. Rev. B
, vol.38
, pp. 7223
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Piazza, R.1
Bellini, T.2
Degiorgio, V.3
Goldstein, R.E.4
Leibler, S.5
Lipowsky, R.6
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20
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5244221149
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R G. Palmer, D L. Stein, E. Abrahams and P W. Anderson, Phys. Rev. Lett.53, 958 (1984).
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(1984)
Phys. Rev. Lett.
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, pp. 958
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Palmer, R.G.1
Stein, D.L.2
Abrahams, E.3
Anderson, P.W.4
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22
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85035245803
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For an interesting discussion of relaxation phenomena, we recommend the article by H. Scher, M. F. Shlesinger, and J. T. Bender, Phys. Today, (1), 26 (1996)
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For an interesting discussion of relaxation phenomena, we recommend the article by H. Scher, M. F. Shlesinger, and J. T. Bender, Phys. Today 49 (1), 26 (1996).
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23
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0002237761
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See the article by H. Fraunfelder and P. G. Wolyner, Phys. Today, (2), 58 (1994). Confirming the temperature dependence of this model requires the availability of uninterrupted data over a sufficiently large range to determine the exponent associated with the relaxation behavior. However, in our case, the many phase transitions preclude a direct test of the model
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See the article by H. Fraunfelder and P. G. Wolyner, Phys. Today 47 (2), 58 (1994). Confirming the temperature dependence of this model requires the availability of uninterrupted data over a sufficiently large range to determine the exponent associated with the relaxation behavior. However, in our case, the many phase transitions preclude a direct test of the model.
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