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The isomorphous Hendrickson-Lattman coefficient A~iso~ for this
reflection for this derivative.
-2.0 * (Fp~obs~^2^ + Fh~calc~^2^ - Fph~obs~^2^)
* Fp~obs~ * cos(alphah~calc~)
A~iso~ = -----------------------------------------------
E^2^
E = (Fph~obs~ - Fp~obs~ - Fh~calc~)^2^
for centric reflections
= [(Fph~obs~ - Fp~obs~) * 2^1/2^ - Fh~calc~]^2^
for acentric reflections
Fp~obs~ = the observed structure-factor amplitude of the
native
Fph~obs~ = the observed structure-factor amplitude of the
derivative
Fh~calc~ = the calculated structure-factor amplitude
from the heavy-atom model
alphah~calc~ = the calculated phase from the heavy-atom model
This coefficient appears in the expression for the phase
probability of each isomorphous derivative:
P~i~(alpha) = exp[k + A * cos(alpha) + B * sin(alpha)
+ C * cos(2 * alpha) + D * sin(2 * alpha)]
Ref: Hendrickson, W. A. & Lattman, E. E. (1970). Acta
Cryst. B26, 136-143.