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AFMLF.rst

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AFMLF

.. index:: AFMLF

Description

A pair of frequencies for aligned Anti-ferrormagnetic magnetism in Longitudinal Fields.

A(t)  = \frac{A_0}{2}((1-a_1)+a_1\cos(\omega_1t+\phi))+(1-a_2)+a_2\cos(\omega_2t+\phi))

where,

a_1 =\frac{(f_a\sin\theta)^2}{(f_b+f_a\cos\theta)^2+(f_a\sin\theta)^2} ,

a_2 =\frac{(f_a\sin\theta)^2}{((f_b-f_a\cos\theta)^2+(f_a\sin\theta)^2)} ,

\omega_1 = 2\pi\sqrt{f_a^2+f_b^2+2f_af_b\cos\theta} ,

\omega_2 = 2\pi\sqrt{f_a^2+f_b^2-2f_af_b\cos\theta} ,

f_a is the ZF frequency (MHz),

f_b = 0.01355 B for B is the applied field,

\theta is the angle of internal field w.r.t. to applied field,

and \phi is the phase.

.. plot::

   from mantid.simpleapi import FunctionWrapper
   import matplotlib.pyplot as plt
   import numpy as np
   x = np.arange(0.1,16,0.1)
   y = FunctionWrapper("AFMLF")
   fig, ax=plt.subplots()
   ax.plot(x, y(x))
   ax.set_xlabel('t($\mu$s)')
   ax.set_ylabel('A(t)')



.. attributes::


.. properties::

References

[1] F.L. Pratt, Physica B 289-290, 710 (2000).

.. categories::


.. sourcelink::