By Konrad Schöbel

ISBN-10: 365811407X

ISBN-13: 9783658114077

ISBN-10: 3658114088

ISBN-13: 9783658114084

Konrad Schöbel goals to put the principles for a consequent algebraic geometric therapy of variable Separation, that is one of many oldest and strongest easy methods to build specific strategies for the basic equations in classical and quantum physics. the current paintings unearths a stunning algebraic geometric constitution in the back of the recognized record of separation coordinates, bringing jointly a good variety of arithmetic and mathematical physics, from the overdue nineteenth century thought of separation of variables to fashionable moduli area concept, Stasheff polytopes and operads.

"I am really inspired by means of his mastery of a number of thoughts and his skill to teach sincerely how they have interaction to supply his results.” (Jim Stasheff)

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Extra info for An Algebraic Geometric Approach to Separation of Variables

Example text

3). 2) appears only antisymmetrised in its two lower indices β and γ. To simplify computations we will thus replace the Nijenhuis torsion N α βγ in the integrability conditions by the tensor ¯ α := N βγ 1 2 K αδ ∇γ K δβ + K δβ ∇δ K αγ , α ¯α N [βγ] = N βγ . 4) this can be written as ¯ α = Sa a b b Sc c d d xa1 xa2 xc1 ∇α xb1 ∇δ xb2 ∇γ xc2 ∇δ xd1 ∇β xd2 N βγ 1 2 1 2 1 2 1 2 + Sa1 a2 b1 b2 Sc1 c2 d1 d2 xa1 xa2 xc1 ∇δ xb1 ∇β xb2 ∇δ xc2 ∇α xd1 ∇γ xd2 . 4. 5b). This can be computed from the so called hook formula.

3 Isokernel planes and integrable Killing tensors from S2 K.

23c). This finishes the proof. 3 The 2nd integrability condition The proceeding for the second integrability condition is similar. 3b): j j i ¯ δ Kδα = g¯ij S i N βγ a 2 b 1 b 2 S c 2 d 1 d 2 + S c2 b 1 b 2 S d 1 a 2 d 2 x b 1 x b 2 x d 1 ∇ δ x a 2 ∇ β x c2 ∇ γ x d 2 Se 1 e 2 f 1 f2 x e 1 x e 2 ∇ δ x f1 ∇ α x f2 . 4 and omit the terms that vanish due to the Bianchi identity: j j i ¯ δ Kδα = g¯ij g¯a2 f1 S i N βγ a2 b 1 b 2 S c 2 d 1 d 2 + S c2 b 1 b 2 S d 1 a 2 d 2 S e 1 e 2 f 1 f 2 x b 1 x b 2 x d 1 x e 1 x e 2 ∇ β x c2 ∇ γ x d 2 ∇ α x f 2 .

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