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1
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85038324117
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An American collaboration among researchers at the University of Maryland, Louisiana State University, the University of Rochester, and Santa Clara University has been formed to design and build spherical antennas. There are also collaborations in Italy, the Netherlands, and Brazil
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An American collaboration among researchers at the University of Maryland, Louisiana State University, the University of Rochester, and Santa Clara University has been formed to design and build spherical antennas. There are also collaborations in Italy, the Netherlands, and Brazil.
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4
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Relativistic Gravity Research
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edited by E. Coccia, G. Pizzella, and F. Ronga (World Scientific, Singapore, 1995), p. 455
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First Edoardo Amaldi Conference on Gravitational Wave Experiments, Frascati, Italy, 1994
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Stevenson, T.R.1
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S. M. Merkowitz, Ph.D. thesis, Louisiana State University, 1995.
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C. H. Cook and M. Bernfeld, Radar Signals, an Introduction to Theory and Application (Artech House, Boston, 1993) [originally published by Academic, New York, 1967, 1987].
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Topics in Theoretical and Experimental Gravitation Physics
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Heffner, H.1
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J.-P. Richard, in Proceedings of the Second Marcel Grossmann Meeting on General Relativity, Trieste, 1979, edited by R. Ruffini (North-Holland, Amsterdam, 1982);
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See 15, Eq. (34), for example.
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38
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36149010109
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(1928)
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Nyquist, H.1
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40
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85038309671
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(Formula presented) is not invertible for (Formula presented) but has the same null space as (Formula presented) so Eq. (53) makes sense. Using the pseudoinverse (Formula presented) avoids difficulties 36
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(Formula presented) is not invertible for (Formula presented) but has the same null space as (Formula presented) so Eq. (53) makes sense. Using the pseudoinverse (Formula presented) avoids difficulties 36.
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42
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85038308915
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MATLAB, The MathWorks, Inc., 24 Prime Way, Natick, MA 01760
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MATLAB, The MathWorks, Inc., 24 Prime Way, Natick, MA 01760.
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43
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85038326516
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Figures 11 and 22 show the maximum and minimum of (Formula presented) over all general, elliptical, polarization states, but analysis of Eqs. (59) and (68) shows that, with identical (Formula presented)’s, the extremal values of (Formula presented) are attained for linearly polarized signals
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Figures 11 and 22 show the maximum and minimum of (Formula presented) over all general, elliptical, polarization states, but analysis of Eqs. (59) and (68) shows that, with identical (Formula presented)’s, the extremal values of (Formula presented) are attained for linearly polarized signals.
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46
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51249193175
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ACMAA8, and later, independently, A. Khintchine, Math. Ann. 19, 604 (1934);, also, G. I. Taylor, Proc. London Math. Soc. Sec. 2, 20, 196 (1920)
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N. Wiener, Acta Math. 55, 117 (1930); ACMAA8and later, independently, A. Khintchine, Math. Ann. 19, 604 (1934);also, G. I. Taylor, Proc. London Math. Soc. Sec. 2, 20, 196 (1920);
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48
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85038318824
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See 21
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See 21, Chap. 4.
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49
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85038281154
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MATHEMATICA, Wolfram Research, Inc., 100 Trade Center Drive, Champaign, IL 61820
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MATHEMATICA, Wolfram Research, Inc., 100 Trade Center Drive, Champaign, IL 61820.
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50
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85038307472
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Note that the ordinate of Fig. 9(b) in the Zhou-Michelson paper 9
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Note that the ordinate of Fig. 9(b) in the Zhou-Michelson paper 9 is mislabeled as variance when it is actually standard deviation.
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