Masteries · Jason GlowneyArithmoí Book 1

Masteries

1.1.12 Complex Powers and Logarithms

It may seem odd to con­sid­er rais­ing a number to an imag­i­nary power, but it is pos­si­ble to use the al­ge­bra­ic prop­er­ties of the nat­ur­al log­a­rithm and ex­po­nents. We can recall the fol­low­ing prop­er­ties for x∈ℝx\in \mathbb{R},

eln⁡(x)=x,\begin{array}{r} e^{\ln(x)} = x, \end{array}
(1.1.54)
ln⁡(ex)=x,\begin{array}{r} \ln\left( e^{x} \right) = x, \end{array}
(1.1.55)
ln⁡(ax)=xln(a).\begin{array}{r} \ln\left( a^{x} \right) = xln(a). \end{array}
(1.1.56)

For com­plex num­bers, ex­po­nen­ti­a­tion can be more easily de­ter­mined by using the com­plex polar form of (a+ib)(a + ib)

(a+ib)=|a+ib|ei∙arg⁡(a+ib).\begin{array}{r} (a + ib) = |a + ib|e^{i \bullet \arg(a + ib)}. \end{array}
(1.1.57)

We can state that (a+ib)=z(a + ib) = z, to recast the ex­pres­sion above, as

|z|ei∙arg⁡(z)→reiθ,\begin{array}{r} |z|e^{i \bullet \arg(z)} \rightarrow re^{i\theta}, \end{array}
(1.1.58)

where |z||z|is the mod­u­lus. We can now define w=u∙v=reiθw = u \bullet v = re^{i\theta}, and find

w=reiθ=eln⁡(r)eiθ=eln⁡(r)+iθ→u=eln⁡(r) and v=eiθ.\begin{array}{r} w = re^{i\theta} = e^{\ln(r)}e^{i\theta} = e^{\ln(r) + i\theta} \rightarrow u = e^{\ln(r)}\ and\ v = e^{i\theta}. \end{array}
(1.1.59)

The prin­ci­pal so­lu­tion for the log­a­rithm w∈ℂw\in \mathbb{C}, can now be stated as

ln⁡(w)=ln⁡(r)+iθ,\begin{array}{r} \ln(w) = \ln(r) + i\theta, \end{array}
(1.1.60)

where we are taking a branch cut for θ,\theta,on the in­ter­val (−π,π]( - \pi,\pi\rbrack, since any in­te­ger mul­ti­ple of 2π2\pi could be added to θ\theta, re­sult­ing in a point in the same lo­ca­tion. Now, we ex­am­ine cal­cu­lat­ing com­plex num­bers raised to com­plex powers. For w,z∈ℂw,z\in \mathbb{C}, and z=(c+id),z = (c + id),the number wzw^{z}, can be ex­pressed by the fol­low­ing

wz=ez∙ln⁡(w)=ez∙(ln⁡(r)+iθ),\begin{array}{r} w^{z} = e^{z \bullet \ln(w)} = e^{z \bullet \left( \ln(r) + i\theta \right)}, \end{array}
(1.1.61)

which ex­pands to

wz=rce−dθei(d∙ln⁡(r)+cθ).\begin{array}{r} w^{z} = r^{c}e^{- d\theta}e^{i\left( d \bullet \ln(r) + c\theta \right)}. \end{array}
(1.1.62)

Taking the simple ex­am­ple eiθe^{i\theta}, a rep­re­sen­ta­tion of the uni­tary group UU, we raise eiθe^{i\theta} to the imag­i­nary power −iϕ- i\phi, find­ing that

(eiθ) −iϕ=e−iϕ(iθ)=eϕ∙θ.\begin{array}{r} ({e^{i\theta})\ }^{- i\phi} = e^{- i\phi(i\theta)} = e^{\phi \bullet \theta}. \end{array}
(1.1.63)

So, in essence, we have raised the U(1)U(1) group to a neg­a­tive imag­i­nary power, trans­form­ing U(1)U(1) into a real ex­po­nen­tial series com­posed of hy­per­bol­ic trigono­met­ric func­tions.