0000027777 00000 n These could allow for the generation of the matter-antimatter asymmetry or potentially observable gravitational waves. Quantum phase transitions have been the subject of intense investigations in the last two decades. 3. Furthermore, they can identify the order (first or second) of the phase transition by their behavior at the quantum transition point, which changes abruptly (smoothly) in the case of first-order (second-order) phase transitions. 0000007525 00000 n Copyright © 2020 Elsevier B.V. or its licensors or contributors. 0000018818 00000 n 0000008582 00000 n 0000052515 00000 n trailer 0000041780 00000 n ‘Essential’ singularity at a first-order phase transition 4.4. 0000051866 00000 n Vtrs 0 P 2 T V T P G 0000032332 00000 n 0000021680 00000 n A quark condensate forms at finite quark mass, and the value Download : Download full-size image; Fig. Influence of diffusion on models for nonequilibrium wetting. 0000011651 00000 n 0000046897 00000 n 0000056257 00000 n 4. 0000052809 00000 n 0000009058 00000 n 0000011046 00000 n !c!! 0000024387 00000 n First-order and second-order phase transitions (II) G Ttrs ΔGtrs 0 Second-order phase transition T V Ttrs T S Ttrs T H Cp-S T G P V P G T -continuous (S and V do not jump at transition) Ttrs T Ttrs T Strs 0 Htrs 0 P P dT dH C e.g. 4.3. 0000009447 00000 n Semantic Scholar is a free, AI-powered research tool for scientific literature, based at the Allen Institute for AI. 0000003188 00000 n Some computational techniques 4. We use cookies to help provide and enhance our service and tailor content and ads. 0000018124 00000 n 0000040485 00000 n In that case, we had to look fairly closely to see the discontinuity: it … E, Statistical, nonlinear, and soft matter physics, By clicking accept or continuing to use the site, you agree to the terms outlined in our. 0000004465 00000 n 0000015506 00000 n 0000010842 00000 n 0000041673 00000 n 0000039417 00000 n 0000054309 00000 n 0000015022 00000 n 471 0 obj<>stream 0000056308 00000 n 0000054919 00000 n 0000052202 00000 n Directed percolation with long-range interactions: Modeling nonequilibrium wetting. Order parameter for this phase transition is the density. 0000017620 00000 n A model for nonequilibrium wetting in 1+1 dimensions is introduced. 0000015997 00000 n 0000054288 00000 n 0000009214 00000 n 0000011502 00000 n 0000013138 00000 n 0000051887 00000 n 0000054071 00000 n 0000014610 00000 n startxref 0000041651 00000 n It is found that the wet (unbound) and the nonwet (pinned) states coexist and are both thermodynamically stable in a domain of the dynamical parameters that define the model. You are currently offline. 0000017403 00000 n 0000011082 00000 n 0000009859 00000 n 0000056039 00000 n Finally, we discuss the universal behavior of systems with a weak first-order zero temperature transition in particular as the transition point is approached from finite temperatures. %PDF-1.3 %���� This is in contrast with…. 0000010153 00000 n 0000007291 00000 n <]>> 0000041716 00000 n @article{Hinrichsen2000FirstorderPT, title={First-order phase transition in a (1+1)-dimensional nonequilibrium wetting process}, author={Hinrichsen and Livi and Mukamel and Politi}, journal={Physical review. 0000014827 00000 n 0000003214 00000 n 0000000016 00000 n Metastable states near first-order phase transitions stability 5. 382 0 obj <> endobj 0000015655 00000 n 0000007802 00000 n Decay of … 0000054941 00000 n To calculate the three Landau-parameters, at least 3 thermodynamic properties at the critical temperature have to be known. Nonequilibrium wetting transition in a nonthermal 2D Ising model, Generic Two-Phase Coexistence and Nonequilibrium Criticality in a Lattice Version of Schlögl’s Second Model for Autocatalysis, The diffusive pair contact process and non-equilibrium wetting, Generic two-phase coexistence, relaxation kinetics, and interface propagation in the quadratic contact process: Simulation studies, Physical review. 0000020969 00000 n I chose density, latent heat and specific heat. Copyright © 2006 Elsevier B.V. All rights reserved. For m L 2 = 0 there is a first order transition to the antiferromagnetic phase . Depending on the rates of the dynamical processes the wetting transition is either of first or second order. Journal of Magnetism and Magnetic Materials, https://doi.org/10.1016/j.jmmm.2006.10.765. 0000015812 00000 n 0000002983 00000 n 0000041629 00000 n 0 Among other problems, these phase transitions are relevant in the study of heavy fermion systems, high-temperature superconductors and Bose–Einstein condensates. These effects are described theoretically using an action that takes into account the competition between different order parameters. The phase transition we just described involves a change of colour of parts of the figure, and colour is a scalar variable, so we expect we will need scalar modes. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics, Physical review. 0000013573 00000 n 0000051654 00000 n Phase Transitions A phase transition is an abrupt, discontinuous change in the properties of a system. 0000015961 00000 n It comprises adsorption and desorption processes with a dynamics that generically does not obey detailed balance. 0000003764 00000 n For m L 2 ≠ 0 new minima appear close to the origin . ! By continuing you agree to the use of cookies. 0000015349 00000 n 0000041802 00000 n In the following, the formulas used: !! xref x�b``�e`�(d`g`X��A��b,S�j��gePx,��H:s��3ׄ�X���7&j_�b p��q�p��� ��$4*k�覥�T�'&���V�gd�7�՗��4�Ɨ4g�$�F�DHJT�G���UFe��qq�p ���. Dynamic wetting with two competing adsorbates. 4). 0000041607 00000 n 0000018656 00000 n 0000013355 00000 n In real crystal structures, there is a wide class of phase transitions, known as order-disorder phase transitions, which are described in terms of scalar modes. We’ve already seen one example of a phase transition in our discussion of Bose-Einstein condensation. 0000052181 00000 n Download : Download full-size image; Fig. 0000002096 00000 n 0000020752 00000 n 0000052494 00000 n 0000052831 00000 n 0000018493 00000 n 0000021369 00000 n 0000046875 00000 n 0000008035 00000 n 0000002918 00000 n