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Space-Time Noncommutative Field Theories And Unitarity
High Energy Physics - Theory · Submitted 14 May 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Field theories with space-time noncommutativity do not have a unitary S-matrix.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
We study the perturbative unitarity of noncommutative scalar field theories. Field theories with space-time noncommutativity do not have a unitary S-matrix. Field theories with only space noncommutativity are perturbatively unitary. This can be understood from string theory, since space noncommutative field theories describe a low energy limit of string theory in a background magnetic field. On the other hand, there is no regime in which space-time noncommutative field theory is an appropriate description of string theory. Whenever space-time noncommutative field theory becomes relevant massive open string states cannot be neglected.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study the perturbative unitarity of noncommutative scalar field theories. | contribution 1.00 | 0.91 | 0.05 | unclear 0.70 |
| s1 | Field theories with space-time noncommutativity do not have a unitary S-matrix. | result 1.00 | 0.62 | 0.76 | asserted 1.00 |
| s2 | Field theories with only space noncommutativity are perturbatively unitary. | result 1.00 | 0.64 | 0.21 | asserted 1.00 |
| s3 | This can be understood from string theory, since space noncommutative field theories describe a low energy limit of string theory in a background magnetic field. | interpretation 0.99 | 0.14 | 0.05 | asserted 0.89 |
| s4 | On the other hand, there is no regime in which space-time noncommutative field theory is an appropriate description of string theory. | interpretation 0.62 | 0.52 | 0.15 | asserted 1.00 |
| s5 | Whenever space-time noncommutative field theory becomes relevant massive open string states cannot be neglected. | interpretation 0.64 | 0.49 | 0.13 | asserted 1.00 |
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The paper
Original abstract
We study the perturbative unitarity of noncommutative scalar field theories. Field theories with space-time noncommutativity do not have a unitary S-matrix. Field theories with only space noncommutativity are perturbatively unitary. This can be understood from string theory, since space noncommutative field theories describe a low energy limit of string theory in a background magnetic field. On the other hand, there is no regime in which space-time noncommutative field theory is an appropriate description of string theory. Whenever space-time noncommutative field theory becomes relevant massive open string states cannot be neglected.
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References
How later papers used it
68 later papers cite it
4 later papers by other authors are listed below: 4 cited it as support.
Cites it as support 4 of 7 papers with this label
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Used this paper's result that nonzero θ^0i makes a noncommutative theory nonunitary to choose θ to lie in the (1, 2) plane without loss of generality.
Photon-neutrino interaction in theta-exact covariant noncommutative model: Phenomenology and Quantum properties* (2011) · 0.95 · paraphrased: the licence does not allow quoting
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To circumvent potential unitarity issues associated with time-space or time-time non-commutativity [ref] , we restrict our analysis to the case of purely space-space non-commutativity.
Constraining non-commutative geometry with W/Z+jet production at the LHC (2025) · W/Z+jet phenomenology in NC geometry · 0.97
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Chose the limit θ^0i = 0 since this paper shows the unitarity of the theory is violated for θ^0i ≠ 0.
Singlet scalar dark matter in the non-commutative space-time: a viable hypothesis to explain the gamma-ray excess in the galactic center (2020) · 0.97 · paraphrased: the licence does not allow quoting
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In this work, we assume space-space non-commutativity, i.e., $Θ^i0 = 0$, motivated by unitarity considerations [ref] , and without loss of generality, we set $Θ^21 = Θ$ and $Θ^13 = Θ^23 = 0$.
Transverse momentum and rapidity distributions of top quarks in pair and single top quark production within the non-commutative standard model at the LHC (2024) · Top-Antitop Quark Production in the NC-SM · 0.99
How the literature uses it
64 arXiv papers cite this in 81 sentences
Papers whose main result relates to this one's
States a conflicting result 1 paper
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This S-matrix is manifestly unitary.
Unitarity in space-time noncommutative field theories · 0.99
Papers citing it · 63 sentences without a confident label
Cites it as support 5 papers
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In fact it was shown in [ref] that in this case the modified Feynman rules lead to a violation of unitarity.
Dispersion relations in quantum electrodynamics on the noncommutative Minkowski space · Introduction · 0.96
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To circumvent potential unitarity issues associated with time-space or time-time non-commutativity [ref] , we restrict our analysis to the case of purely space-space non-commutativity.
Constraining non-commutative geometry with W/Z+jet production at the LHC · W/Z+jet phenomenology in NC geometry · 0.97
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Since the unitarity of the theory is violated for $θ^0i≠0$ [ref] , the limit $θ^0i= 0$ is chosen.
Singlet scalar dark matter in the non-commutative space-time: a viable hypothesis to explain the gamma-ray excess in the galactic center · THE NCST THEORY · 0.97
Cites it as background 12 papers
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We have three types of space-time noncommutativity [ref] : (i) The pure space-space (spacelike) NC, where $c_i0=0$; $c_ij≠0, ∀i,j=1,2,3$, makes unitary safe theory, (ii) the pure time-space (timelike) NC, with $c_i0≠0$; $c_ij=0, ∀i,j=1,2,3$, makes unitarity breaking theory, (iii) the so called lightlike noncommutativity satisfying $E^2_θ=B^2_θ$ and $E_θ ·B_θ=0$, where the $c_0i$ elements are defined by the direction of the background $E_θ=1/Λ_NC^2( c_01, c_02, c_03)$ field, while the $c_ij$ coefficients are defined by the direction of the $B_θ=1/Λ_NC^2 (c_23, -c_13, c_12)$ field, produces unitary safe NCQED theory.
Remarks on Compton forward scattering singularity in the NCQED · Compton scattering in the NCQED and collinear singularity · 0.80
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The former case, discussed in Eq. [ref], encodes non-commutativity among space and time coordinates, namely $θ_0i≠0$, while the latter case, in Eq. [ref], corresponds to selecting $θ_0i=0$, ensuring unitarity of the $θ$-Poincaré models [ref] .
Strongest atomic physics bounds on Non-Commutative Quantum Gravity Models · Introduction · 0.81
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We remark that noncommutative field theories typically contain infinitely many time derivatives in their actions, which may lead to apparent violations of unitarity [ref] and causality [ref] .
Exponentially Long Evaporation of Noncommutative Black Hole · Introduction · 0.84
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