53,228 research outputs found
Variant supercurrent multiplets
In N = 1 rigid supersymmetric theories, there exist three standard
realizations of the supercurrent multiplet corresponding to the (i) old
minimal, (ii) new minimal and (iii) non-minimal off-shell formulations for N =
1 supergravity. Recently, Komargodski and Seiberg in arXiv:1002.2228 put
forward a new supercurrent and proved its consistency, although in the past it
was believed not to exist. In this paper, three new variant supercurrent
multiplets are proposed. Implications for supergravity-matter systems are
discussed.Comment: 11 pages; V2: minor changes in sect. 3; V3: published version; V4:
typos in eq. (2.3) corrected; V5: comments and references adde
Non-gravitational exceptional supermultiplets
We examine non-gravitational minimal supermultiplets which are based on the
tensor gauge fields appearing as matter fields in exceptional generalised
geometry. When possible, off-shell multiplets are given. The fields in the
multiplets describe non-gravitational parts of the internal dynamics of
compactifications of M-theory. In flat backgrounds, they enjoy a global
U-duality symmetry, but also provide multiplets with a possibility of coupling
to a generalised exceptional geometry.Comment: 11 pp., plain te
Scalar-Induced Compactifications in Higher Dimensional Supergravities
We discuss compactifications of higher dimensional supergravities which are
induced by scalars. In particular, we consider vector multiplets coupled to the
supergravity multiplet in the case of D=9, 8 and D=7 minimal supergravities.
These vector multiplets contain scalars, which parametrize coset spaces of the
general form SO(10-D,n)/SO(10-D)xSO(n), where n is the number of vector
multiplets. We discuss the compactification of the supergravity theory to D-2
dimensons, which is induced by non-trivial vacuum scalar field configurations.
There are singular and non-singular solutions, which preserve half of the
supersymmetries.Comment: 25 pages, JHEP
Anomaly cancellation in D=4, N=1 orientifolds and linear/chiral multiplet duality
It has been proposed that gauge and Kaehler anomalies in four-dimensional
type IIB orientifolds are cancelled by a generalized Green-Schwarz mechanism
involving exchange of twisted RR-fields. We explain how this can be understood
using the well-known duality between linear and chiral multiplets. We find that
all the twisted fields associated to the N=1 sectors and some of the fields
associated to the N=2 sectors reside in linear multiplets. But there are no
linear multiplets associated to order-two twists. Only the linear multiplets
contribute to anomaly cancellation. This suffices to cancel all U(1) anomalies.
In the case of Kaehler symmetries the complete SL(2,R) can be restored at the
quantum level for all planes that are not fixed by an order-two twist.Comment: 30 pages, Latex; v2: misprints correcte
New Couplings of Six-Dimensional Supergravity
We describe the couplings of six-dimensional supergravity, which contain a
self-dual tensor multiplet, to anti-self-dual tensor matter multiplets,
vector multiplets and hypermultiplets. The scalar fields of the
tensor multiplets form a coset , while the scalars in the
hypermultiplets form quaternionic K\"ahler symmetric spaces, the generic
example being . The gauging of the compact
subgroup is also described. These results generalize
previous ones in the literature on matter couplings of supergravity in
six dimensions.Comment: 24 pages, latex, no figure
SO(10) unification in noncommutative geometry revisited
We investigate the SO(10)-unification model in a Lie algebraic formulation of
noncommutative geometry. The SO(10)-symmetry is broken by a 45-Higgs and the
Majorana mass term for the right neutrinos (126-Higgs) to the standard model
structure group. We study the case that the fermion masses are as general as
possible, which leads to two 10-multiplets, four 120-multiplets and two
additional 126-multiplets of Higgs fields. This Higgs structure differs
considerably from the two Higgs multiplets 16 \otimes 16^* and 16^c \otimes
16^* used by Chamseddine and Fr\"ohlich. We find the usual tree-level
predictions of noncommutative geometry m_W=(1/2)m_t, \sin^2\theta_W=(3/8) and
g_2=g_3 as well as m_H \leq m_t.Comment: 25 pages, LaTeX 2e. v2: typos corrected and footnote on
Super-Kamiokande results adde
Conformal Partial Wave Expansions for N=4 Chiral Four Point Functions
The conformal partial wave analysis of four point functions of half BPS
operators belonging to the SU(4) [0,p,0] representation is undertaken for
p=2,3,4. Using the results of N=4 superconformal Ward identities the
contributions from protected short and semi-short multiplets are identified in
terms of the free field theory. In the large N limit contributions
corresponding to long multiplets with twist up to 2p-2 are absent. The
anomalous dimensions for twist two singlet multiplets are found to order g^4
and agree with other perturbative calculations. Results for twist four and six
are also found.Comment: 53 pages, uses harvmac, includes 1 figure, version 2 some corrections
and minor extensions, version 3 some further corrections, version 4 as to be
publishe
Effects of heavy modes on vacuum stability in supersymmetric theories
We study the effects induced by heavy fields on the masses of light fields in
supersymmetric theories, under the assumption that the heavy mass scale is much
higher than the supersymmetry breaking scale. We show that the square-masses of
light scalar fields can get two different types of significant corrections when
a heavy multiplet is integrated out. The first is an indirect level-repulsion
effect, which may arise from heavy chiral multiplets and is always negative.
The second is a direct coupling contribution, which may arise from heavy vector
multiplets and can have any sign. We then apply these results to the sGoldstino
mass and study the implications for the vacuum metastability condition. We find
that the correction from heavy chiral multiplets is always negative and tends
to compromise vacuum metastability, whereas the contribution from heavy vector
multiplets is always positive and tends on the contrary to reinforce it. These
two effects are controlled respectively by Yukawa couplings and gauge charges,
which mix one heavy and two light fields respectively in the superpotential and
the Kahler potential. Finally we also comment on similar effects induced in
soft scalar masses when the heavy multiplets couple both to the visible and the
hidden sector.Comment: LaTex, 24 pages, no figures; v2 some comments and references adde
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