Non-commutative solitons
By Rajesh Gopakumar, Shiraz Minwalla, Andrew Strominger. 2000
392 citations recorded by the source corpus.
We nd classically stable solitons (instantons) in odd (even) dimen- sional scalar non-commutative eld theories whose scalar potential, V(), has at least two minima. These solutions are bubbles of the false vacuum whose size is set bythescaleofnoncommutativity. Ourconstructionusesthecorrespondencebetween non-commutativeelds and operators on a single particle Hilbert space. In the case of non-commutative gauge theories we note that expanding around a simple solu- tion shifts away the kinetic term and results in a purely quartic action with linearly realised gauge symmetries.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/0cd28c2facadd8944fe462f7c6e5cf9877beaba8
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Citations in the corpus
- Minimal Length Scale Scenarios for Quantum Gravity (2012, background): “Gaussian distributions are of interest not only because they are widely used field configurations, but, for example, also because they may describe solitonic solutions in a potential [137].”
- Conformal higher spin symmetries of 4D massless supermultiplets and osp(L,2M) invariant equations in generalized (super)space (2001, neutral): “ with the one-particle states of the same system [19]. (Note thatthese Fock modules are somewhat reminiscent of the modules introduced for the description of non-commutative solitons in string theory [28].) In addition to the su(2,2|N) generators, the algebra hu(2N−1,2N−1|8) contains the bilinear ge”
- A Review on Tachyon Condensation in Open String Field Theories (2001, positive): “It was shown in [101, 104] that the operator |n〉〈n| corresponds to the function (field) φn(r (2)) = 2(−1)ne− r 2 θ Ln ( 2r(2) θ ) , (6.”
- D-branes and strings as non-commutative solitons (2000, methodology): “22) represents, in the basis constructed in [17], a lump of size rk ∼ √ k, which approximates the string field configuration of an unstable D25-brane for smaller radius, and the closed string vacuum state for larger radius.”
- Noncommutative Tachyons And String Field Theory (2000, background): “Recently, solitons in scalar field theories on noncommutative spacetimes with very large noncommutativity parameter θ have been constructed in a strikingly simple way [1].”
- Half-strings, projectors and multiple D-branes (2001, result): “This situation is analogous to the one that arises in the study of non-commutative solitons [8, 9, 10, 11, 12].”
- Unstable solitons in noncommutative gauge theory (2000, background): “We find exact classical solutions which carry various kinds of fluxes but, as in [2], are not, in general, BPS (in contrast to the gauge theory solutions in [1]).”
- A Note on Background Independence in Noncommutative Gauge Theories, Matrix Model and Tachyon Condensation (2000, background): “(A connection between the matrix model and this problem was anticipated in [12,32].”
- Classical solutions in string field theory around the tachyon vacuum (2001, methodology): “(This is precisely what happens in the case of p-adic string theory [29, 30, 31], background independent open string field theory [32, 33, 34, 35, 36, 37, 38, 39, 40], as well as non-commutative solitons [41, 42, 43].”
- String Field Theory Around the Tachyon Vacuum (2000, methodology): “Support for these conjectures comes from the analysis of the world-sheet theory [1, 3, 4, 5, 6, 7, 8], cubic open string field theory [9, 10, 11, 12, 13, 14, 15, 16, 17, 19, 20, 21, 22, 23, 24], noncommutative limit of the effective field theory of the tachyon [25, 26, 27, 28, 29, 30], background in”
- Remarks on Tachyon Condensation in Superstring Field Theory (2000, result): “Exact results for tachyon condensation have also been obtained by introducing noncommutativity [16,17,18,19]; the recent results of [20] might give a closer relation between this approach and BSFT.”
- Exact Solution of Quantum Field Theory on Noncommutative Phase Spaces (2003, background): “The corresponding field configurations correspond to the standard θ = ∞ GMS solitons [40] and possess an infinite degeneracy under U(∞) rotations of the matrices X, leading to a non-trivial soliton moduli space which is an infinite-dimensional Grassmannian [41].”
- Chern–Simons theory with vector fermion matter (2011, background): “Also, it naturally appears in discussions of non-commutative field theory [48], [49], [50].”
- Phase structure of non-commutative scalar field theories (2000, background): “ar X iv :h ep -t h/ 00 W e investigate the phase structure ofnon-com m utative scalar eld theoriesand nd evidence forordered phaseswhich break translation invariance.”
- Quantum field theory on noncommutative spaces (2001, background): “table noncommutative solitons, which have no counterparts in ordinary field theory, have been constructed by representing the Weyl operator algebra on a multi-particle quantum mechanical Hilbert space [64, 65]. The noncommutative soliton field equations may then be solved by any projection operator on”
- Noncommutative field theory (2001, methodology): “This argument will obviously fail in the presence of a distinguished length scale √ θ and in fact one finds that for sufficiently large θ, stable solitons can exist in the noncommutative theory (Gopakumar, Minwalla, and Strominger 2000c).”