Greetings weapons enthusiasts, history buffs, pirate fans, and nuclear physicists!
The Strongblade.com web log is up, and though we don't have much of interest for nuclear physicists, we will be offering quite a bit for all those other groups. Strongblade.com is, as you
may already know, one of the premiere (premier? Preemeer?premere?) websites for historical
reproductions of weapons and other fun stuff. If you're looking for reproduction swords, daggers, axes, spears, armor, helmets, flintlocks, lightsabers, sword belts (you get the point) then we highly recommend checking out our website: http://www.strongblade.com.

This blog will describe the backside of our business. Let me rephrase that... This blog will give you a glimpse into the seedy underbelly of the dark and violent sword industry. Hmm... that's not quite right either. Okay, here we go: This blog will attempt to enlighten the world with a detailed view into the workings and operations of a sword business. (That's a little better.) We'll talk about some of our trials and tribulations as well as our successes and joys. And of course, we'll give updates on things that are coming up on our website. We'll also occassionally give out discount codes and give readers access to products that have not made it on to our website yet. Readers will also be privvy to new designs that we are working on, promotions we have planned, and much much more.

So, bookmark this address and visit us often.

And now a little something for you nuclear physicists...

Holomorphic methods in analysis and mathematical physics
Brian C. Hall

This series converges uniformly to F on the compact set Ps (z) || U. Thus when
evaluating the integral on the RHS of (2.1) we may interchange the integral with
the sum. But now if we use polar coordinates with the origin at z, then (v − z)n =
. So for n > 1, the integral over Ps (z) (which is just a disk of radius s since
d = 1) give zero. So the only surviving term is the constant term F (z) , which
gives -s2

Cheers!