Two Gravity-Wave Detectors: A Comparison

نویسندگان

  • J. Weber
  • J. A. Tyson
  • S. W. Hawking
چکیده

*Work supported by the U. S. Atomic Energy Commission under contract with Union Carbide Corporation. )Present address: Department of Physics and Astronomy, Vanderbilt University, Nashville, Tenn. 37203. J. Rainwater, Phys. Bev. 79, 432 (1950). J. M. Blatt and V. F. Weisskopf, Theoretical Nuclear Physics (Wiley, New York, 1952). K. Kumar, Phys. Rev. C 1, 369 (1970). A. Bohr, Kgl. Dan. Vidensk. Selsk. , Mat. -Fys. Medd. 26, No. 14 (1952); A. Bohr and B.R. Mottelson, Kgl. Dan. Vidensk. Selsk. , Mat. -Fys. Medd. 27, No. 16 (1953); B. R. Mottelson, in The Many Body Browed, edited by J. Percus (Wiley, New York, 1958). G. Ripka, in Advances in Nuclear Physics, edited by M. Baranger and E. Vogt (Plenum, New York1,968), Vol. I, p. 183. The two-body operator defined by Eqs. (1) and (2) is similar to that of the separable, quadrupole-quadrupole interaction. However, .the two would be identical only if the nuclear mass and charge distributions were identical. We follow the conventions of A. de-Shalit and I. Tal-. mi, Nuclear Shell Theory (Academic, New York, 1963) for the tensor and scalar products of irreducible tensors (except for some obvious change of notation). de-Shalit and Talmi, Bef. 7. K. Alder and A. Winther, Coulomb Excitation (Academic, New York, 1966). I. A, Fraser et al. , Phys. Rev. Lett, 23, 1047, 1051 (1969); R. G. Stokstad, private communication of compilation of the results of several experiments fthese matrix elements can be found in Table I of K. Kumar, Phys. Bev. Lett. 26, 269 (1971)]. Kumar, Bef. 10. ' P. H. Stelson and L. Grodzins, Nucl. Data 1, 21 (1965).

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تاریخ انتشار 2011