Diquark condensation in dense SU(2) matter

We report on a lattice study of two-color QCD with adjoint staggered fermions at high density. We find that the model has no early onset and we report on results for diquark condensation, from simulations with and without a diquark source term.Comment: Lattice2001(hightemp

Lattice Study of Dense Matter with Two Colors and Four Flavors

We present results from a simulation of SU(2) lattice gauge theory with N_f=4 flavors of Wilson fermion and non-zero quark chemical potential mu, using the same 12^3x24 lattice, bare gauge coupling, and pion mass in cut-off units as a previous study with N_f=2. The string tension for N_f=4 is found to be considerably smaller implying smoother gauge field configurations. Thermodynamic observables and order parameters for superfluidity and color deconfinement are studied, and comparisons drawn between the two theories. Results for quark density and pressure as functions of mu are qualitatively similar for N_f=2 and N_f=4; in both cases there is evidence for a phase in which baryonic matter is simultaneously degenerate and confined. Results for the stress-energy tensor, however, suggest that while N_f=2 has a regime where dilute matter is non-relativistic and weakly-interacting, N_f=4 matter is relativistic and strongly-interacting for all values of mu above onset.Comment: Horizontal axes of several figures rescaled. Version accepted for publicatio

The Three Dimensional Thirring Model for N_f=4 and N_f=6

We present Monte Carlo simulation results for the three dimensional Thirring model for numbers of fermion flavors N_f=4 and 6. For N_f=4 we find a second order chiral symmetry breaking transition at strong coupling, corresponding to an ultra-violet fixed point of the renormalisation group defining a non-trivial continuum limit. The critical exponents extracted from a fit to a model equation of state are distinct from those found for N_f=2. For N_f=6, in contrast, we present evidence for tunnelling between chirally symmetric and broken vacua at strong coupling, implying that the phase transition is first order and no continuum limit exists. The implications for the phase diagram of the model in the plane of coupling strength and N_f are briefly discussed.Comment: 29 pages, 13 figure

Mesonic Wavefunctions in the three-dimensional Gross-Neveu model

We present results from a numerical study of bound state wavefunctions in the (2+1)-dimensional Gross-Neveu model with staggered lattice fermions at both zero and nonzero temperature. Mesonic channels with varying quantum numbers are identified and analysed. In the strongly coupled chirally broken phase at T=0 the wavefunctions expose effects due to varying the interaction strength more effectively than straightforward spectroscopy. In the weakly coupled chirally restored phase information on fermion - antifermion scattering is recovered. In the hot chirally restored phase we find evidence for a screened interaction. The T=0 chirally symmetric phase is most readily distinguished from the symmetric phase at high T via the fermion dispersion relation.Comment: 18 page

Lattice Study of Anisotropic QED-3

We present results from a Monte Carlo simulation of non-compact lattice QED in 3 dimensions on a $16^3$ lattice in which an explicit anisotropy between $x$ and $y$ hopping terms has been introduced into the action. This formulation is inspired by recent formulations of anisotropic QED$_3$ as an effective theory of the non-superconducting portion of the cuprate phase diagram, with relativistic fermion degrees of freedom defined near the nodes of the gap function on the Fermi surface, and massless photon degrees of freedom reproducing the dynamics of the phase disorder of the superconducting order parameter. Using a parameter set corresponding to broken chiral symmetry in the isotropic limit, our results show that the renormalised anisotropy, defined in terms of the ratio of correlation lengths of gauge invariant bound states in the $x$ and $y$ directions, exceeds the explicit anisotropy $\kappa$ introduced in the lattice action, implying in contrast to recent analytic results that anisotropy is a relevant deformation of QED$_3$. There also appears to be a chiral symmetry restoring phase transition at $\kappa_c\simeq4.5$, implying that the pseudogap phase persists down to T=0 in the cuprate phase diagram.Comment: 24 pages, 9 figures, 3 tables. This (the published version) has the following alterations: i) An expanded discussion of the empirical aspects of HT superconductivity, ii) An updated version of Figure 4, iii) The removal of the consistency check in section 3.3.1 for reasons of brevit

Non-Compact QED_3 with N_f=1 and N_f=4

We present numerical results for non-compact three-dimensional QED for numbers of flavors N_f=1 and N_f=4.In particular, we address the issue of whether chiral symmetry is spontaneously broken in the continuum limit, and obtain a positive answer for N_f=1, with a dimensionless condensate estimated to be beta^2 ~= O(10^-3), implying that the critical number of flavors N_fc>1. We also compare the N_f=1 and N_f=4 models by analysing the transition from strong to weak coupling behaviour using an equation of state based on a continuous phase transition. While some qualitative differences emerge, it appears difficult to determine whether N_f=4 lies above or below N_fc.Comment: 19 pages, 10 figure

Breast and prostate cancer survivor responses to group exercise and supportive group psychotherapy

This study qualitatively examined an 8 week group exercise and counseling intervention for breast and prostate cancer survivors. Groups exercised 3 days per week, 50 minutes per session, performing moderate intensity aerobic and resistance training. Groups also underwent 90 minute supportive group psychotherapy sessions once per week. Survivors discussed their experiences in focus groups post intervention. Transcripts were analyzed using interpretative phenomenological analysis. Survivors described how exercise facilitated counseling by creating mutual aid and trust, and counseling helped participants with self-identity, sexuality, and returning to normalcy. When possible, counselors and fitness professionals should create partnerships to optimally support cancer survivors

Numerical Portrait of a Relativistic Thin Film BCS Superfluid

We present results of numerical simulations of the 2+1d Nambu - Jona-Lasinio model with a non-zero baryon chemical potential mu including the effects of a diquark source term. Diquark condensates, susceptibilities and masses are measured as functions of source strength j. The results suggest that diquark condensation does not take place in the high density phase mu>mu_c, but rather that the condensate scales non-analytically with j implying a line of critical points and long range phase coherence. Analogies are drawn with the low temperature phase of the 2d XY model. The spectrum of the spin-1/2 sector is also studied yielding the quasiparticle dispersion relation. There is no evidence for a non-zero gap; rather the results are characteristic of a normal Fermi liquid with Fermi velocity less than that of light. We conclude that the high density phase of the model describes a relativistic gapless thin film BCS superfluid.Comment: 37 pages, 16 figure

Access to Secondary and Tertiary Education for All Refugees: Steps and Challenges to Overcome

During situations of displacement, access for refugee youth to secondary educational initiatives is limited at best. However, upon the return of refugees, the national structure of their home country is most often weak and unstable. To ensure the economic, social, and political development of a society that has been severely affected by conflict or disaster, it is imperative that there be a youth population of capable, productive, and educated citizens who may provide an exit strategy from the situation. Future leaders must therefore be given the opportunity to promote the development both of themselves personally, and of their national structures, through learning—notably, secondary, vocational, and tertiary education. This paper underscores the need for and gaps in the provision of secondary educational initiatives, highlighting the many challenges involved in improving refugee youth access to both secondary and vocational education, and highlighting the issues that must be considered by policy and decision makers in order to facilitate and support such access.Pendant les situations de déplacement forcé, l’accès à l’éducation secondaire des jeunes réfugiés est réduit au maximum. Cependant, à partir du moment où ils peuvent retourner à leurs pays d’origine, son structure est en général affaiblit et instable. Afin d’assurer le développement économique, social et politique d’une société qui a été sévèrement troublée par un conflit ou catastrophe, il est impératif de compter sur une jeunesse compétente, éduquée et responsable d’un point de vue civique, et capable de créer et de soutenir une stratégie de sortie aux situations du passé. Les leaders de demain doivent avoir l’opportunité de se développer individuellement, mais également de développer leurs structures nationales, à travers l’éducation, notamment secondaire, professionnelle et tertiaire. Cet article souligne les besoins et les écarts existants en ce qui concerne la provision d’initiatives dans le domaine de l’éducation secondaire, remarquant les divers défis aux-quels il faut faire face pour améliorer l’accès des jeunes réfugiés à l’éducation post-primaire (secondaire et professionnelle), et par voie de conséquence à l’éducation tertiaire. En outre, il souligne également les sujets qui devraient être considérés par les autorités politiques et décisionnaires compétentes afin de faciliter et soutenir ledit accès