TY - GEN
T1 - Localization and the canonical commutation relations
AU - Moylan, Patrick
N1 - Publisher Copyright:
© Springer Nature Singapore Pte Ltd. 2016.
Copyright:
Copyright 2018 Elsevier B.V., All rights reserved.
PY - 2016
Y1 - 2016
N2 - Let Wn (R) be the Weyl algebra of index n. We have shown that by using extension and localization, it is possible to construct homomorphisms of Wn (R) onto its image in a localization, or a quotient thereof, of U(so(2, q)), the universal enveloping algebra of so(2, q), forn depending upon q [1]. Here we treat the so(2, 1) case in complete detail. We establish an isomorphism of skew fields, specifically, D(so(2, 1)) ~ D(1,1)(R) where D1,1(R) is the fraction field of W1.1(R) ~ W1(R) ⊗ R(y) with R(y) being the ring of polynomials in the indeterminate y and D(so(2, 1)) is a certain extension of the skew field of fractions of U(so(2, 1)), which is described below. We give applications of this result to representations. In particular we are able to construct representations of W1 (R) out of representations of so (2, 1). Thus, we are able, for this lowest dimensional case, to obtain the canonical commutation relations and representations of them out of so(2, 1) symmetry. Using similar results in higher dimensions [1] we are able to construct representations of Wn(R) out of representations of so (2, q).
AB - Let Wn (R) be the Weyl algebra of index n. We have shown that by using extension and localization, it is possible to construct homomorphisms of Wn (R) onto its image in a localization, or a quotient thereof, of U(so(2, q)), the universal enveloping algebra of so(2, q), forn depending upon q [1]. Here we treat the so(2, 1) case in complete detail. We establish an isomorphism of skew fields, specifically, D(so(2, 1)) ~ D(1,1)(R) where D1,1(R) is the fraction field of W1.1(R) ~ W1(R) ⊗ R(y) with R(y) being the ring of polynomials in the indeterminate y and D(so(2, 1)) is a certain extension of the skew field of fractions of U(so(2, 1)), which is described below. We give applications of this result to representations. In particular we are able to construct representations of W1 (R) out of representations of so (2, 1). Thus, we are able, for this lowest dimensional case, to obtain the canonical commutation relations and representations of them out of so(2, 1) symmetry. Using similar results in higher dimensions [1] we are able to construct representations of Wn(R) out of representations of so (2, q).
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U2 - 10.1007/978-981-10-2636-2_30
DO - 10.1007/978-981-10-2636-2_30
M3 - Conference contribution
AN - SCOPUS:85009730035
SN - 9789811026355
T3 - Springer Proceedings in Mathematics and Statistics
SP - 423
EP - 430
BT - Lie Theory and Its Applications in Physics
A2 - Dobrev, Vladimir
PB - Springer New York LLC
T2 - Proceedings of the 11th International Workshop on Lie Theory and Its Applications in Physics, 2015
Y2 - 15 June 2015 through 21 June 2015
ER -