Quick Search:
Prog. Theor. Phys. Vol. 115 No. 1 (2006) pp. 217-228
Planar Dominance in Non-Commutative Field Theories at Infinite External Momentum
Tadayuki Konagaya1,* and
Jun Nishimura1,2,**
1Department of Particle and Nuclear Physics,
The Graduate University for Advanced Studies (Sokendai),
Tsukuba 305-0801, Japan
2High Energy Accelerator Research Organization (KEK),
Tsukuba 305-0801, Japan
(Received September 16, 2005)
Abstract:
In the perturbative expansion of field theories on a
non-commutative geometry, it is known that planar diagrams dominate when
the non-commutativity parameter θ goes to infinity.
We investigate whether this “planar dominance” occurs also in the case that
θ is finite, but the external momentum goes to infinity instead.
While this holds trivially at the one-loop level, it is not obvious
at the two-loop level, in particular in the presence of UV divergences.
We perform explicit two-loop calculations
in the six-dimensional φ3 theory and confirm
that nonplanar diagrams after renormalization do vanish in this limit.
URL :
http://ptp.ipap.jp/link?PTP/115/217/
DOI : 10.1143/PTP.115.217
References:
-
H. S. Snyder, Phys. Rev. 71 (1947), 38[APS].
A. Connes, Noncommutative geometry (Academic Press, 1990).
-
S. Doplicher, K. Fredenhagen and J. E. Roberts, Commun. Math. Phys. 172 (1995), 187[CrossRef];
hep-th/0303037[e-print arXiv].
-
N. Seiberg and E. Witten, J. High Energy Phys. 09 (1999), 032[CrossRef];
hep-th/9908142[e-print arXiv].
-
S. Minwalla, M. Van Raamsdonk and N. Seiberg, J. High Energy Phys. 02 (2000), 020[IoP STACKS];
hep-th/9912072[e-print arXiv].
-
S. S. Gubser and S. L. Sondhi, Nucl. Phys. B 605 (2001), 395[CrossRef];
hep-th/0006119[e-print arXiv].
- W. Bietenholz, F. Hofheinz and J. Nishimura, Nucl. Phys. B (Proc. Suppl.) 119 (2003), 941;
hep-lat/0209021[e-print arXiv]; Fortsch. Phys. 51 (2003), 745;
hep-th/0212258[e-print arXiv].
-
J. Ambjørn and S. Catterall, Phys. Lett. B 549 (2002), 253[CrossRef];
hep-lat/0209106[e-print arXiv].
X. Martin, J. High Energy Phys. 04 (2004), 077[CrossRef];
hep-th/0402230[e-print arXiv].
-
W. Bietenholz, F. Hofheinz and J. Nishimura, J. High Energy Phys. 06 (2004), 042[CrossRef];
hep-th/0404020[e-print arXiv].
-
M. Van Raamsdonk, J. High Energy Phys. 11 (2001), 006[CrossRef];
hep-th/0110093[e-print arXiv].
A. Armoni and E. Lopez, Nucl. Phys. B 632 (2002), 240[CrossRef];
hep-th/0110113[e-print arXiv].
-
W. Bietenholz, F. Hofheinz and J. Nishimura, J. High Energy Phys. 05 (2004), 047[CrossRef];
hep-th/0404179[e-print arXiv].
-
H. Aoki, N. Ishibashi, S. Iso, H. Kawai, Y. Kitazawa and T. Tada, Nucl. Phys. B 565 (2000), 176[CrossRef];
hep-th/9908141[e-print arXiv].
J. Ambjørn, Y. M. Makeenko, J. Nishimura and R. J. Szabo, J. High Energy Phys. 11 (1999), 029[CrossRef];
hep-th/9911041[e-print arXiv];
Phys. Lett. B 480 (2000), 399[CrossRef];
hep-th/0002158[e-print arXiv];
J. High Energy Phys. 05 (2000), 023[CrossRef];
hep-th/0004147[e-print arXiv].
-
T. Eguchi and H. Kawai, Phys. Rev. Lett. 48 (1982), 1063[APS].
-
A. Gonzalez-Arroyo and M. Okawa, Phys. Rev. D 27 (1983), 2397[APS].
-
N. Ishibashi, S. Iso, H. Kawai and Y. Kitazawa, Nucl. Phys. B 573 (2000), 573[CrossRef];
hep-th/9910004[e-print arXiv].
-
W. Bietenholz, F. Hofheinz and J. Nishimura, J. High Energy Phys. 09 (2002), 009[CrossRef];
hep-th/0203151[e-print arXiv].
- I. Ya. Aref'eva, D. M. Belov and A. S. Koshelev, Phys. Lett. B 476 (2002), 431;
hep-th/9912075[e-print arXiv].
A. Micu and M. M. Sheikh-Jabbari, J. High Energy Phys. 01 (2001), 025[IoP STACKS];
hep-th/0008057[e-print arXiv].
W. Huang, Phys. Lett. B 496 (2000), 206;
hep-th/0009067[e-print arXiv].
- Y. Kiem, S. Lee and J. Park, Nucl. Phys. B 594 (2001), 169;
hep-th/0008002[e-print arXiv].
Y. Kiem, S. Kim, S. Rey and H. Sato, Nucl. Phys. B 641 (2002), 256[CrossRef];
hep-th/0110066[e-print arXiv].
-
I. Chepelev and R. Roiban, J. High Energy Phys. 05 (2000), 037[CrossRef];
hep-th/9911098[e-print arXiv].