Definition of fluorescence anisotropy Fluorescence anisotropy
the anisotropy (r) of light source defined ratio of polarized component total intensity (
i
t
{\displaystyle i_{t}}
):
r
=
i
z
−
i
y
i
x
+
i
y
+
i
z
{\displaystyle r={\frac {i_{z}-i_{y}}{i_{x}+i_{y}+i_{z}}}}
when excitation polarized along z-axis, emission fluorophore symmetric around z-axis(figure). hence statistically have
i
x
=
i
y
{\displaystyle i_{x}=i_{y}}
.
i
y
=
i
⊥
{\displaystyle i_{y}=i_{\perp }}
, ,
i
z
=
i
∥
{\displaystyle i_{z}=i_{\parallel }}
, have
r
=
i
∥
−
i
⊥
i
∥
+
2
i
⊥
=
i
∥
−
i
⊥
i
t
{\displaystyle r={\frac {i_{\parallel }-i_{\perp }}{i_{\parallel }+2i_{\perp }}}={\frac {i_{\parallel }-i_{\perp }}{i_{t}}}}
.
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