11,807 research outputs found

    Anxiety reduction via brief intervention in dentally anxious patients : a randomized controlled trial

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    Aim: To compare the degree of anxiety reduction in dentally anxious patients attending a Dental Access Centre where the dentist did or did not receive the patients’ assessment of dental anxiety. Methods: Patients attending two Dental Access Centres in England, completed the Modified Dental Anxiety Scale (MDAS). Those that scored high completed a state anxiety questionnaire (STAI-S) and were randomized into three groups (n=182) to test the hypothesis that patients sharing assessment information about their dental anxiety to members of the dental team has beneficial effects on their state anxiety. Group 1 were controls (n=60), Group 2 gave their MDAS to the receptionist who passed it onto the dentist unknown to the patient (n=62) and Group 3 handed their MDAS to the dentist (n=60). After their appointment they repeated the STAI-S. Results and conclusion: Patients in Group 3 were less anxious (by more than STAI-S 3 scale units) on leaving the surgery than those from the other groups especially if they entered into a discussion with the dentist about their concerns (by more than 5 scale units). Brief assessment of dental anxiety shared by the patient with the dentist collaboratively has the potential to reduce anxiety on completion of the appointment. Dental anxiety is common, has a multifactorial aetiology, and is far from being homogenous, as individuals seem to differ in the origins, age of onset and manifestations of their dental fears (Locker et al., 2001b); (Milgrom et al., 1988). Previous negative experiences are a major factor in the development of dental anxiety (Kleinknect et al., 1973); (Bernstein et al., 1979); (de Jongh et al., 1995); (Locker et al., 1999); (Ost and Hugdahl, 1985). For some individuals, their fear of dentistry may be associated with concurrent anxiety disorders, or more general psychopathology (Locker, 2003); (Locker et al., 2001a).PreprintPeer reviewe

    Exotic tensor gauge theory and duality

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    Gauge fields in exotic representations of the Lorentz group in D dimensions - i.e. ones which are tensors of mixed symmetry corresponding to Young tableaux with arbitrary numbers of rows and columns - naturally arise through massive string modes and in dualising gravity and other theories in higher dimensions. We generalise the formalism of differential forms to allow the discussion of arbitrary gauge fields. We present the gauge symmetries, field strengths, field equations and actions for the free theory, and construct the various dual theories. In particular, we discuss linearised gravity in arbitrary dimensions, and its two dual forms.Comment: 28 pages, LaTeX, references added, minor change

    New Gauged N=8, D=4 Supergravities

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    New gaugings of four dimensional N=8 supergravity are constructed, including one which has a Minkowski space vacuum that preserves N=2 supersymmetry and in which the gauge group is broken to SU(3)xU(1)2SU(3)xU(1)^2. Previous gaugings used the form of the ungauged action which is invariant under a rigid SL(8,R)SL(8,R) symmetry and promoted a 28-dimensional subgroup (SO(8),SO(p,8−p)SO(8),SO(p,8-p) or the non-semi-simple contraction CSO(p,q,8−p−q)CSO(p,q,8-p-q)) to a local gauge group. Here, a dual form of the ungauged action is used which is invariant under SU∗(8)SU^*(8) instead of SL(8,R)SL(8,R) and new theories are obtained by gauging 28-dimensional subgroups of SU∗(8)SU^*(8). The gauge groups are non-semi-simple and are different real forms of the CSO(2p,8−2p)CSO(2p,8-2p) groups, denoted CSO∗(2p,8−2p)CSO^*(2p,8-2p), and the new theories have a rigid SU(2) symmetry. The five dimensional gauged N=8 supergravities are dimensionally reduced to D=4. The D=5,SO(p,6−p)D=5,SO(p,6-p) gauge theories reduce, after a duality transformation, to the D=4,CSO(p,6−p,2)D=4,CSO(p,6-p,2) gauging while the SO∗(6)SO^*(6) gauge theory reduces to the D=4,CSO∗(6,2)D=4, CSO^*(6,2) gauge theory. The new theories are related to the old ones via an analytic continuation. The non-semi-simple gaugings can be dualised to forms with different gauge groups.Comment: 33 pages. Reference adde

    A Geometry for Non-Geometric String Backgrounds

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    A geometric string solution has background fields in overlapping coordinate patches related by diffeomorphisms and gauge transformations, while for a non-geometric background this is generalised to allow transition functions involving duality transformations. Non-geometric string backgrounds arise from T-duals and mirrors of flux compactifications, from reductions with duality twists and from asymmetric orbifolds. Strings in ` T-fold' backgrounds with a local nn-torus fibration and T-duality transition functions in O(n,n;Z)O(n,n;\Z) are formulated in an enlarged space with a T2nT^{2n} fibration which is geometric, with spacetime emerging locally from a choice of a TnT^n submanifold of each T2nT^{2n} fibre, so that it is a subspace or brane embedded in the enlarged space. T-duality acts by changing to a different TnT^n subspace of T2nT^{2n}. For a geometric background, the local choices of TnT^n fit together to give a spacetime which is a TnT^n bundle, while for non-geometric string backgrounds they do not fit together to form a manifold. In such cases spacetime geometry only makes sense locally, and the global structure involves the doubled geometry. For open strings, generalised D-branes wrap a TnT^n subspace of each T2nT^{2n} fibre and the physical D-brane is the part of the part of the physical space lying in the generalised D-brane subspace.Comment: 28 Pages. Minor change

    Macroscopic Phase Coherence of Defective Vortex Lattices in Two Dimensions

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    The superfluid density is calculated theoretically for incompressible vortex lattices in two dimensions that have isolated dislocations quenched in by a random arrangement of pinned vortices. The latter are assumed to be sparse and to be fixed to material defects. It is shown that the pinned vortices act to confine a single dislocation of the vortex lattice along its glide plane. Plastic creep of the two-dimensional vortex lattice is thereby impeded, and macroscopic phase coherence results at low temperature in the limit of a dilute concentration of quenched-in dislocations.Comment: 18 pages, 1 figure, 1 table, new title, submitted to Physical Review

    Frame-like Geometry of Double Field Theory

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    We relate two formulations of the recently constructed double field theory to a frame-like geometrical formalism developed by Siegel. A self-contained presentation of this formalism is given, including a discussion of the constraints and its solutions, and of the resulting Riemann tensor, Ricci tensor and curvature scalar. This curvature scalar can be used to define an action, and it is shown that this action is equivalent to that of double field theory.Comment: 35 pages, v2: minor corrections, to appear in J. Phys.

    Metal honeycomb to porous wireform substrate diffusion bond evaluation

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    Two nondestructive techniques were used to evaluate diffusion bond quality between a metal foil honeycomb and porous wireform substrate. The two techniques, cryographics and acousto-ultrasonics, are complementary in revealing variations of bond integrity and quality in shroud segments from an experimental aircraft turbine engine
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