Using the concept and tools of fractional calculus, we introduce a definition for "fractional-order" multipoles of electric-charge densities, and we show that as far as their scalar potential distributions are concerned, such fractional-order multipoles effectively behave as "intermediate" sources bridging the gap between the cases of integer-order point multipoles such as point monopoles, point dipoles, point quadrupoles, etc. This technique, which involves fractional differentiation or integration of the Dirac delta function, provides a tool for formulating an electric source distribution whose potential functions can be obtained by using fractional differentiation or integration of potentials of integer-order point-multipoles of lower or higher orders. As illustrative examples, the cases of three-dimensional (point source) and two-dimensional (line source) problems in electrostatics are treated in detail, and an extension to the time-harmonic case is also addressed. In the three-dimensional electrostatic example, we suggest an electric-charge distribution which can be regarded as an "intermediate" case between cases of the electric-point monopole (point charge) and the electric-point dipole (point dipole), and we present its electrostatic potential which behaves as r/sup -(1+/spl alpha/)/P/sub /spl alpha//(-cos/spl theta/) where 0</spl alpha/<1 and P/sub /spl alpha//(/spl middot/) is the Legendre function of noninteger degree /spl alpha/, thus denoting this charge distribution as a fractional 2/sup /spl alpha//-pole. At the two limiting cases of /spl alpha/=0 and /spl alpha/=1, this fractional 2/sup /spl alpha//-pole becomes the standard point monopole and point dipole, respectively. A corresponding intermediate fractional-order multipole is also given for the two-dimensional electrostatic case. Potential applications of this treatment to the image method in electrostatic problems are briefly mentioned. Physical insights and interpretation for such fractional-order 2/sup /spl alpha//-poles are also given.
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