scholarly journals THERMODYNAMICAL PHASES OF A REGULAR SAdS BH

2013 ◽  
Vol 22 (03) ◽  
pp. 1350010 ◽  
Author(s):  
ANAIS SMAILAGIC ◽  
EURO SPALLUCCI

This paper studies the thermodynamical stability of regular BHs in AdS5 background. We investigate off-shell free energy of the system as a function of temperature for different values of a "coupling constant" [Formula: see text], where the cosmological constant is Λ = -3/l2 and [Formula: see text] is "minimal length." The parameter [Formula: see text] admits a critical value, [Formula: see text], corresponding to the appearance of an inflexion point in the Hawking temperature. In the weak-coupling regime [Formula: see text], there are first-order phase transitions at different temperatures. Unlike the Hawking–Page case, at temperature 0 ≤ T ≤ T min the ground state is populated by "cold" near-extremal BHs instead of a pure radiation. On the other hand, for [Formula: see text], only large, thermodynamically stable BHs exist.

1993 ◽  
Vol 328 ◽  
Author(s):  
Boris E. Vugmeister ◽  
Michelle S. Malcuit ◽  
John C. Kralik ◽  
Colleen Stevens

ABSTRACTWe investigate the pretransitional behavior in laser-induced alignment of rigid rod-like polytetraflouroethylene (PTFE) suspensions. Using a laser-induced birefringence experiment, we measure both the orientational order parameter and the orientational relaxation time. We find that both increase as the volume fraction of colloidal particles approaches the critical value for the isotropic-nematic phase transition. Experimental results are compared with theory which takes into account the possibility of a first-order phase transition induced by a laser electric field.


2013 ◽  
Vol 28 (28) ◽  
pp. 1350140 ◽  
Author(s):  
WUNG-HONG HUANG

We use the matching method to investigate the first-order phase transition in holographic superconductor and superfluid. We first use the simple holographic superconductor model to describe the matching method and mention how to see the first-order phase transition. Next, we study the holographic superconductor with Stückelberg term and see that the analytic results indicate the existence of first-order phase transition. Finally, we study the holographic superfluid and show that the first-order phase transition can be found for some values of parameters. We determine the critical value analytically and compare it with the previous numerical result.


2019 ◽  
Vol 34 (15) ◽  
pp. 1950073
Author(s):  
Vo Quoc Phong ◽  
Minh Anh Nguyen

Our analysis shows that SM-like electroweak phase transition (EWPT) in the [Formula: see text] (2-2-1) model is a first-order phase transition at the 200 GeV scale (the SM scale). Its strength [Formula: see text] is about 1–2.7 and the masses of new gauge bosons are larger than 1.7 TeV when the second VEV is larger than 535 GeV in a three-stage EWPT scenario and the coupling constant of [Formula: see text] group must be larger than 2. Therefore, this first-order EWPT can be used to fix VEVs and the coupling constant of the gauge group in electroweak models.


1993 ◽  
Vol 08 (22) ◽  
pp. 2117-2123 ◽  
Author(s):  
T. INAGAKI ◽  
T. MUTA ◽  
S.D. ODINTSOV

The phase structure of Nambu-Jona-Lasinio model with N-component fermions in curved space-time is studied in the leading order of the 1/N expansion. The effective potential for composite operator [Formula: see text] is calculated by using the normal coordinate expansion in the Schwinger proper-time method. The existence of the first order phase transition caused by the change of the space-time curvature is confirmed and the dynamical mass of the fermion is calculated as a simultaneous function of the curvature and the four-fermion coupling constant. The phase diagram in the curvature and the coupling constant is obtained.


2012 ◽  
Vol 27 (21) ◽  
pp. 1250116 ◽  
Author(s):  
M. BORDAG ◽  
V. DEMCHIK ◽  
A. GULOV ◽  
V. SKALOZUB

The temperature induced phase transition is investigated in the one-component scalar field ϕ4 model on the lattice. Using the GPU cluster a huge amount of Monte Carlo simulation data is collected for a wide interval of coupling values. This gives a possibility to determine the low bound on the coupling constant λ0 when the transition happens and investigate its type. We found that for the values of λ close to this bound a weak-first-order phase transition takes place. It converts into a second-order one with the increase of λ. A comparison with the results obtained in analytic and numeric calculations by other authors is given.


1989 ◽  
Vol 44 (3) ◽  
pp. 296-306 ◽  
Author(s):  
M. Somer ◽  
W. Hönle ◽  
H. G. von Schnering

Cs3As7, a compound with cage-like As73- anions, has been prepared from the elements in sealed quartz ampoules at 820 K. The ruby-red compound undergoes a first order phase transition at 640 K and is obtained as microcrystalline samples. The structure of the low-temperature α-modification is not known, but β-Cs3As7 belongs to the plastically crystalline β-Rb3P7 type of structure (F m 3̄ m , a (673 K) = 1169,2(1) pm). Cs3As7 melts under its own vapour pressure at 1061 K, and is easily soluble in liquid ammonia. From those solutions ruby red crystals of Cs3(NH3)As7 precipitate. In dynamical vacuum NH3 is evaporated in the region of 300 to 520 K, resulting in Cs3As7. Cs3(NH3)As7 crystallizes in the space group P21/a (a = 2759.0(12) pm, b = 744.1(3) pm, c = 751.5(3) pm, β = 90.16(5)°; Z = 4). The structure is closely related to the plastically crystalline β-Rb3P7 type structure (Li3Bi variant). The heptaarsanortricyclene anion is coordinated by cesium atoms, connecting the anions to a three dimensional arrangement. The anion exhibits a differentiation of As - As bond lengths typical for ionic nortricyclenes (d(basis) = 251.2 pm; d(basis-bridge) = 235.5 pm; d(bridge-bridgehead) = 240.1 pm). The distances Cs to As are in the range 372 to 401 pm. The cesium atoms are surrounded by three resp. four As atoms and the NH3 molecules. The FIR and Raman spectra are given for different temperatures as well as of an en-solution of Cs3(NH3)As7. The valence vibrations of NH3 are found at 3175 (A1) and 3320 cm-1 (E ). The fundamental vibrations of the three-membered ring of different heteronortricyclenes with P and As are compared and yield a correlation factor χ = 0.57(1) for the observed frequencies between P3 and As3. The band gaps EG are determined from the diffuse reflexion at 2.14 eV for Cs3(NH3)As7 and 2.00 eV for Cs3As7.


2007 ◽  
Vol 18 (07) ◽  
pp. 1107-1117
Author(s):  
FATIH YAŞAR

Monte Carlo simulations using the recently proposed Wang–Landau algorithm are performed to the q = 8 state Potts model in two dimension with various degrees of randomness. We systematically studied the effect of quenched bond randomness to system which has first-order phase transition. All simulations and measurements were done from pure case r = 1 to r = 0.4. Physical quantities such as energy density and ground-state entropy were evaluated at all temperatures. We have also obtained probability distributions of energy to monitor softening of transitions. It appears quite feasible to simulate spin systems with quenched bond randomness by Wang–Landau algorithm.


2013 ◽  
Vol 27 (15) ◽  
pp. 1362037
Author(s):  
MIN-CHUL CHA

We have studied the ground state properties of hard-core bosons in a two-leg optical ladder in the presence of uniform and staggered frustrations due to an artificial gauge field. By calculating the ground state via the Lanczos method, we find first-order phase transitions tuned by the staggered gauge field between the Meissner and the vortex states. The momentum distributions show that the Meissner state has edge and staggered currents, while the vortex states have vortex-solid or vortex-glass phases in the presence of a staggered field.


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