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| Tags: gravitational, polarisation, wave |
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#11
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zigoteau:
Q_xx = p_x p_x - (1/3)p^2 or, since there are only 5 independent components, it can be written in terms of a traceless operator with 5 components, Q_+/-2 = (1/2)(Q_xx - Q_yy +/- 2i Q_xy) Q+/-1 = (1/2)(Q_xz - iQ_yz) Q_0 = sqrt(1/3)[Q_zz - (1/2)(Q_xx + Q_yy)] Oscillations in the xy-plane only, are the linerar combinations above, that contain only Q_xx, Qyy and Q_xy, i.e., Q_+/-2. You don't seem to be saying the same thing. It is perhaps tangential to sense. Bilge, it is not clear why Q_0 should not be symmetrical in x, y and z. I defined the z-axis, i.e., p_z = p cos(\theta) as the longitudinal direction. Q_0 might look more familar if you write out the components: Q_zz + (1/2)[Q_xx + Q_yy] = (p_z)^2 - (1/3)p^2 - (1/2) [(p_x)^2 + (p_y)^2 - (2/3)p^2] Since p^2 = (p_x)^2 + (p_y)^2 + (p_z)^2, p^2 - (p_z)^2 = (p_x)^2 + (p_y)^2 and you have, Q_0 = (p_z)^2 - (1/3)p^2 - (1/2) [p^2 - (p_z)^2 - (2/3)p^2] (3/2) (p_z)^2 - (1/2)p^2 = (1/2) [3 cos^2(\theta) - 1] p^2 which apart from a normalization, is Y_20 x p^2. (I also have the normalization wrong on Q_0. it should be sqrt(2/3)). Tom, distances between which points? This is presumably connected to the metric tensor. Since you give different answers while both referring to MTW (which I do not have) I deduce that the subject is not discussed explicitly anywhere in that textbook, and that this is just a tactic by both of you to blind me with science and shut me up. Or could either or both of you give page numbers? Actually, I didn't refer to MTW. I just wrote down a quadrupole tensor with the components written in terms of the projections along one of the axes. That was basically what you had asked. I seem to remember something about elements of tensor space which map into each other under the operation of the set of rotations. Is there a connection to spherical harmonics and the total angular momentum quantum number l? Am I getting warm? Yes, since in particular, the Q_m are the components of Y_lm for l = 2. |
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#12
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