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general power∗ pahio† 2013-03-21 18:06:58 The general power z µ , where z (6= 0) and µ are arbitrary complex numbers, is defined via the complex exponential function and complex logarithm (denoted here by “log”) of the base by setting z µ := eµ log z = eµ(ln |z|+i arg z) . The number z is the base of the power z µ and µ is its exponent. Splitting the exponent µ = α+iβ in its real and imaginary parts one obtains z µ = eα ln |z|−β arg z · ei(β ln |z|+α arg z) , and thus |z µ | = eα ln |z|−β arg z , arg z µ = β ln |z|+α arg z. This shows that both the modulus and the argument of the general power are in general multivalued. The modulus is unique only if β = 0, i.e. if the exponent µ = α is real; in this case we have |z µ | = |z|µ , arg z µ = µ · arg z. Let β 6= 0. If one lets the point z go round the origin anticlockwise, arg z gets an addition 2π and hence the power z µ has been multiplied by a factor having the modulus e−2πβ 6= 1, and we may say that z µ has come to a new branch. Examples 1 1. z m , where m is a positive integer, coincides with the mth root of z. 2. 32 = e2 log 3 = e2(ln 3+2nπi) = 9(e2πi )2n = 9 ∀n ∈ Z. π π 3. ii = ei log i = ei(ln 1+ 2 i−2nπi) = e2nπ− 2 (with n = 0, ±1, ±2, . . .); all 1 these values are positive real numbers, the simplest of them is √ π ≈ e 0.20788. ∗ hGeneralPoweri created: h2013-03-21i by: hpahioi version: h36347i Privacy setting: h1i hDefinitioni h30D30i † This text is available under the Creative Commons Attribution/Share-Alike License 3.0. You can reuse this document or portions thereof only if you do so under terms that are compatible with the CC-BY-SA license. 1 4. (−1)i = e(2n+1)π (with n = 0, ±1, ±2, . . .) also are situated on the positive real axis. √ √ √ √ 5. (−1) 2 = e 2 log (−1) = e 2i(π+2nπ) = ei(2n+1)π 2 (with n = 0, ±1, ±2, . . .); all these are imaginary numbers (meaning here that their imaginary parts are distinct from 0), situated on the circumference of the unit circle such that all points of the circumference are accumulation points of the se√ quence of the powers (−1) 2 (see this entry). 6. 21−i = 2e2nπ (cos ln 2 + i sin ln 2) (with n = 0, ±1, ±2, . . .), are situated on the half line beginning from the origin with the argument ln 2 ≈ 0.69315 radians. 2