These quantities are components of the total structure factor, and therefore must have the same units as the overall structure factor.

The definition of a structure factor is the ratio between the scattered amplitude from some "structure" of interest and the amplitude scattered by a single electron. The "structure" can be an atom, a protein, or even an entire crystal. In this way, we separate the contribution of the molecular structure from all the other "factors" of scattering (like polarization and Lorentz factors). This definition heralds back to Hartree (1925) Philos. Mag. 50, 289-306, which was the first time the term "structure factor" appeared in the English literature. Although Debye & Scherrer (1918) Physik. Zeit. 19, 474-483 probably deserve credit for coining the term (in German), something very similar to a structure factor (without the modern name) appeared as a variable "f" in Darwin's original paper on scattering theory: Darwin, C. G. (1914) Philos. Mag. 27, 315-333. It was immediately after measuring the resolution dependence of "f" that Debye amazingly and immediately realized that we were going to have to accept quantum theory (Debye (1915). Ann. Phys. 351, 809-823).

Anyway, the structure factor is a ratio, and therefore is technically a dimensionless quantity, but even a dimensionless quantity has a "unit" in that there is some situation where the structure factor is equal to unity (1.0). This "unit" is when the object of interest scatters "just as much" as one of Thomson's classical electrons would (Thomson, (1906); Woolfson, (1997) Ch. 2). So, it is convenient to describe structure factors in terms of how many electrons it would take to produce the same signal. Hence, the "unit" of structure factor is the "electron", but probably better denoted as the "electron equivalent" to avoid the present confusion. For example, the "F" values calculated by SFALL or REFMAC have units of "electron equivalents per unit cell". Again, a dimensionless quantity, but far more informative when the unit is spelled out. Abbreviations are great, but not when taken to the point where they introduce ambiguity.

I see nothing wrong with using a particle or other physical object as a "unit" as long as the meaning is made clear. After all, until recently the unit of "meter" was a metal stick they had in France. And the "unit" of mass is still a lump of metal which weighs exactly 1.0 kg. This object is slowly oxidizing, and that means that the mass of everything else in the universe is actually decreasing (by definition). Which could perhaps account for recent observations that the expansion rate of the universe is accelerating (Riess et al. (1998) Astro. J. 116, 1009).

I'm sure Ian and Mark will have more to say about this...

-James Holton
MAD Scientist


Tim Gruene wrote:
Dear all,

I just stumbled across the question about what is the unit of f' and f''.  The
first couple of hits from ixquick.com claim it was e^-. Since e^- is not a unit
but symbolises an elemtary particle (of which fractions are considered
non-existent), I was wondering whether the unit of f, f', and f'' is actually e
(a positive charge!) and the value of f^0 of Fe at its K-edge was actually 26e
or -26e - see e.g. Table 1 in
http://www.ccp4.ac.uk/courses/proceedings/1997/j_smith/main.html

Cheers, Tim

--
Tim Gruene
Institut fuer anorganische Chemie
Tammannstr. 4
D-37077 Goettingen

GPG Key ID = A46BEE1A

Reply via email to