The Casimir stress on a D-dimensional sphere (the stress on a sphere is equal to the Casimir force per unit area multiplied by the area of the sphere) due to the confinement of a massless scalar field is computed as a function of D, where D is a continuous variable that ranges from -{∞} to {∞}. The dependence of the stress on the dimension is obtained using a simple and straightforward Green's function technique. We find that the Casimir stress vanishes as D{→}+{∞} (D is a noneven integer) and also vanishes when D is a negative even integer. The stress has simple poles at positive even integer values of D.
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Bender et al. (1994) studied this question.
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