Batalin-Tyutin quantization of theCPN−1model
نویسندگان
چکیده
منابع مشابه
Batalin-Tyutin Quantization of the Chiral Schwinger Model
We quantize the chiral Schwinger Model by using the Batalin-Tyutin formalism. We show that one can systematically construct the first class constraints and the desired involutive Hamiltonian, which naturally generates all secondary constraints. For a > 1, this Hamiltonian gives the gauge invariant Lagrangian including the well-known WessZumino terms, while for a = 1 the corresponding Lagrangian...
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The (2+1) dimensional nonabelian Chern-Simons theory coupled to complex scalar fields is quantized by using the Batalin-Tyutin canonical Hamiltonian method which systematically embeds second-class constraint system into first-class one. We obtain the gauge-invariant nonabelian Wess-Zumino type action in the extended phase space. ∗ E-mail address : [email protected] † E-mail address : yjpark@...
متن کاملBatalin-Tyutin quantization of the self-dual massive theory in three dimensions.
We quantize the self-dual massive theory by using the Batalin-Tyutin Hamiltonian method, which systematically embeds second class constraint system into first class one in the extended phase space by introducing the new fields. Through this analysis we obtain simultaneously the Stückelberg scalar term related to the explicit gaugebreaking effect and the new type of Wess-Zumino action related to...
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In this Letter we have proposed a point particle model that generates a noncommutative three-space, with the coordinate brackets being Lie algebraic in nature, in particular isomorphic to the angular momentum algebra. The work is in the spirit of our earlier works in this connection, i.e. PLB 618 (2005)243 and PLB 623 (2005)251, where the κ-Minkowski form of noncomutative spacetime was consider...
متن کاملSOGANG-HEP 196/95 May 1995 Batalin-Tyutin Quantization of the Chiral Schwinger Model
We quantize the chiral Schwinger Model by using the Batalin-Tyutin formalism. We show that one can systematically construct the rst class constraints and the desired involutive Hamiltonian, which naturally generates all secondary constraints. For a > 1, this Hamiltonian gives the gauge invariant Lagrangian including the well-known WessZumino terms, while for a = 1 the corresponding Lagrangian h...
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ژورنال
عنوان ژورنال: Physical Review D
سال: 1994
ISSN: 0556-2821
DOI: 10.1103/physrevd.49.1996