538 research outputs found

    Walking, Weak first-order transitions, and Complex CFTs II. Two-dimensional Potts model at Q>4Q>4

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    We study complex CFTs describing fixed points of the two-dimensional QQ-state Potts model with Q>4Q>4. Their existence is closely related to the weak first-order phase transition and walking RG behavior present in the real Potts model at Q>4Q>4. The Potts model, apart from its own significance, serves as an ideal playground for testing this very general relation. Cluster formulation provides nonperturbative definition for a continuous range of parameter QQ, while Coulomb gas description and connection to minimal models provide some conformal data of the complex CFTs. We use one and two-loop conformal perturbation theory around complex CFTs to compute various properties of the real walking RG flow. These properties, such as drifting scaling dimensions, appear to be common features of the QFTs with walking RG flows, and can serve as a smoking gun for detecting walking in Monte Carlo simulations. The complex CFTs discussed in this work are perfectly well defined, and can in principle be seen in Monte Carlo simulations with complexified coupling constants. In particular, we predict a pair of S5S_5-symmetric complex CFTs with central charges c≈1.138±0.021ic\approx 1.138 \pm 0.021 i describing the fixed points of a 5-state dilute Potts model with complexified temperature and vacancy fugacity.Comment: 34 pages, 13 figures. v2: refs added; v3 refs added, typos corrected, presentation of several arguments clarifie

    Walking, Weak first-order transitions, and Complex CFTs

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    We discuss walking behavior in gauge theories and weak first-order phase transitions in statistical physics. Despite appearing in very different systems (QCD below the conformal window, the Potts model, deconfined criticality) these two phenomena both imply approximate scale invariance in a range of energies and have the same RG interpretation: a flow passing between pairs of fixed point at complex coupling. We discuss what distinguishes a real theory from a complex theory and call these fixed points complex CFTs. By using conformal perturbation theory we show how observables of the walking theory are computable by perturbing the complex CFTs. This paper discusses the general mechanism while a companion paper [1] will treat a specific and computable example: the two-dimensional Q-state Potts model with Q > 4. Concerning walking in 4d gauge theories, we also comment on the (un)likelihood of the light pseudo-dilaton, and on non-minimal scenarios of the conformal window termination.Comment: 38 pages, added reference

    Non-gaussianity of the critical 3d Ising model

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    We discuss the 4pt function of the critical 3d Ising model, extracted from recent conformal bootstrap results. We focus on the non-gaussianity Q - the ratio of the 4pt function to its gaussian part given by three Wick contractions. This ratio reveals significant non-gaussianity of the critical fluctuations. The bootstrap results are consistent with a rigorous inequality due to Lebowitz and Aizenman, which limits Q to lie between 1/3 and 1.Comment: 10 pages, 6 figures; v2: refs added; v3: refs updated, published version; v4: acknowledgement adde

    A scaling theory for the long-range to short-range crossover and an infrared duality

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    We study the second-order phase transition in the dd-dimensional Ising model with long-range interactions decreasing as a power of the distance 1/rd+s1/r^{d+s}. For ss below some known value s∗s_*, the transition is described by a conformal field theory without a local stress tensor operator, with critical exponents varying continuously as functions of ss. At s=s∗s=s_*, the phase transition crosses over to the short-range universality class. While the location s∗s_* of this crossover has been known for 40 years, its physics has not been fully understood, the main difficulty being that the standard description of the long-range critical point is strongly coupled at the crossover. In this paper we propose another field-theoretic description which, on the contrary, is weakly coupled near the crossover. We use this description to clarify the nature of the crossover and make predictions about the critical exponents. That the same long-range critical point can be reached from two different UV descriptions provides a new example of infrared duality.Comment: 57pp, detailed version of arXiv:1703.03430, v2: misprints corrected, v3: refs and discussion of log corrections at the crossover added, v4: published version plus extra comments in appendix A,B and an acknowledgement, v5: published version plus extra comments in appendix A,B and an acknowledgement (replacing the wrong tex file of v4

    Conformal Invariance in the Long-Range Ising Model

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    We consider the question of conformal invariance of the long-range Ising model at the critical point. The continuum description is given in terms of a nonlocal field theory, and the absence of a stress tensor invalidates all of the standard arguments for the enhancement of scale invariance to conformal invariance. We however show that several correlation functions, computed to second order in the epsilon expansion, are nontrivially consistent with conformal invariance. We proceed to give a proof of conformal invariance to all orders in the epsilon expansion, based on the description of the long-range Ising model as a defect theory in an auxiliary higher-dimensional space. A detailed review of conformal invariance in the d-dimensional short-range Ising model is also included and may be of independent interest.Comment: 52pp; V2: refs added; V3: ref added, published versio

    Discrete Chiral Symmetry and Mass Shift in Lattice Hamiltonian Approach to Schwinger Model

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    We revisit the lattice formulation of the Schwinger model using the Kogut-Susskind Hamiltonian approach with staggered fermions. This model, introduced by Banks et al., contains the mass term mlat∑n(−1)nχn†χnm_{\rm lat} \sum_{n} (-1)^{n} \chi^\dagger_n \chi_n, and setting it to zero is often assumed to provide the lattice regularization of the massless Schwinger model. We instead argue that the relation between the lattice and continuum mass parameters should be taken as mlat=m−18e2am_{\rm lat}=m- \frac 18 e^2 a. The model with m=0m=0 is shown to possess a discrete chiral symmetry that is generated by the unit lattice translation accompanied by the shift of the Ξ\theta-angle by π\pi. While the mass shift vanishes as the lattice spacing aa approaches zero, we find that including this shift greatly improves the rate of convergence to the continuum limit. We demonstrate the faster convergence using both numerical diagonalizations of finite lattice systems, as well as extrapolations of the lattice strong coupling expansions.Comment: 14 pages, 7 figures; v2 refs added, minor improvement

    Phase Diagram of the Two-Flavor Schwinger Model at Zero Temperature

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    We examine the phase structure of the two-flavor Schwinger model as a function of the Ξ\theta-angle and the two masses, m1m_1 and m2m_2. In particular, we find interesting effects at Ξ=π\theta=\pi: along the SU(2)SU(2)-invariant line m1=m2=mm_1 = m_2 = m, in the regime where mm is much smaller than the charge gg, the theory undergoes logarithmic RG flow of the Berezinskii-Kosterlitz-Thouless type. As a result, in this regime there is a non-perturbatively small mass gap ∌e−Ag2/m2\sim e^{- A g^2/m^2}. The SU(2)SU(2)-invariant line lies within a region of the phase diagram where the charge conjugation symmetry is spontaneously broken and whose boundaries we determine numerically. Our numerical results are obtained using the Hamiltonian lattice gauge formulation that includes the mass shift mlat=m−g2a/4m_\text{lat} = m- g^2 a/4 dictated by the discrete chiral symmetry.Comment: 7 pages, 3 figures; v2 minor improvements, refs adde

    Prevalence, associated factors and outcomes of pressure injuries in adult intensive care unit patients: the DecubICUs study

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    Funder: European Society of Intensive Care Medicine; doi: http://dx.doi.org/10.13039/501100013347Funder: Flemish Society for Critical Care NursesAbstract: Purpose: Intensive care unit (ICU) patients are particularly susceptible to developing pressure injuries. Epidemiologic data is however unavailable. We aimed to provide an international picture of the extent of pressure injuries and factors associated with ICU-acquired pressure injuries in adult ICU patients. Methods: International 1-day point-prevalence study; follow-up for outcome assessment until hospital discharge (maximum 12 weeks). Factors associated with ICU-acquired pressure injury and hospital mortality were assessed by generalised linear mixed-effects regression analysis. Results: Data from 13,254 patients in 1117 ICUs (90 countries) revealed 6747 pressure injuries; 3997 (59.2%) were ICU-acquired. Overall prevalence was 26.6% (95% confidence interval [CI] 25.9–27.3). ICU-acquired prevalence was 16.2% (95% CI 15.6–16.8). Sacrum (37%) and heels (19.5%) were most affected. Factors independently associated with ICU-acquired pressure injuries were older age, male sex, being underweight, emergency surgery, higher Simplified Acute Physiology Score II, Braden score 3 days, comorbidities (chronic obstructive pulmonary disease, immunodeficiency), organ support (renal replacement, mechanical ventilation on ICU admission), and being in a low or lower-middle income-economy. Gradually increasing associations with mortality were identified for increasing severity of pressure injury: stage I (odds ratio [OR] 1.5; 95% CI 1.2–1.8), stage II (OR 1.6; 95% CI 1.4–1.9), and stage III or worse (OR 2.8; 95% CI 2.3–3.3). Conclusion: Pressure injuries are common in adult ICU patients. ICU-acquired pressure injuries are associated with mainly intrinsic factors and mortality. Optimal care standards, increased awareness, appropriate resource allocation, and further research into optimal prevention are pivotal to tackle this important patient safety threat
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