Comment on ‘‘Universal scaling function for domain growth in the Glauber-Ising chain’’

1992 ◽  
Vol 46 (21) ◽  
pp. 14261-14262 ◽  
Author(s):  
Stephen J. Cornell ◽  
Michel Droz
Keyword(s):  
Scaling Function ◽  
Domain Growth ◽  
Ising Chain ◽  
Universal Scaling ◽  
Universal Scaling Function

Universal scaling function for domain growth in the Glauber-Ising chain

1992 ◽  
Vol 45 (14) ◽  
pp. 8131-8133 ◽  
Author(s):  
Zhifang Lin ◽  
Xiaomin Wang ◽  
Ruibao Tao
Keyword(s):  
Scaling Function ◽  
Domain Growth ◽  
Ising Chain ◽  
Universal Scaling ◽  
Universal Scaling Function

A universal scaling function for hadron-hadron interactions

1980 ◽  
Vol 55 (4) ◽  
pp. 417-436 ◽  
Author(s):  
A. D’Innocenzo ◽  
G. Ingrosso ◽  
P. Rotelli
Keyword(s):  
Scaling Function ◽  
Universal Scaling ◽  
Universal Scaling Function

EXOTIC CARBON SYSTEMS IN TWO-NEUTRON HALO THREE-BODY MODELS

2011 ◽  
Vol 20 (supp01) ◽  
pp. 254-262
Author(s):  
LAURO TOMIO ◽  
ANTONIO DELFINO ◽  
TOBIAS FREDERICO ◽  
M. R. HADIZADEH ◽  
M. T. YAMASHITA ◽  
...  
Keyword(s):  
Halo Nucleus ◽  
Scaling Function ◽  
Neutron Halo ◽  
Mass Ratio ◽  
Weakly Bound ◽  
Universal Scaling ◽  
Body Model ◽  
Zero Range ◽  
Three Body ◽  
Universal Scaling Function

The general properties of exotic carbon systems, considered as a core with a two-neutron (n - n) halo, are described within a renormalized zero-range three-body model. In particular, it is addressed the cases with a core of 18C and 20C. In such a three-body framework, 20C has a bound subsystem (19C), whereas 22C has a Borromean structure with all subsystems unbound. 22C is also known as the heaviest carbon halo nucleus discovered. The spatial distributions of such weakly-bound three-body systems are studied in terms of a universal scaling function, which depends on the mass ratio of the particles, as well as on the nature of the subsystems.

An Extended Cahn-Hilliard Model for Interfaces with Cubic Anisotropy

2001 ◽  
Vol 701 ◽  
Author(s):  
T.A. Abinandanan ◽  
F. Haider
Keyword(s):  
Interfacial Energy ◽  
Scaling Function ◽  
Two Dimensions ◽  
One Dimensional ◽  
Universal Scaling ◽  
Main Effect ◽  
The One ◽  
Universal Scaling Function ◽  
Particle Shapes ◽  
Cubic Anisotropy

ABSTRACTFor studying systems with a cubic anisotropy in interfacial energy σ, we extend the Cahn-Hilliard model by including in it a fourth rank term, which leads to an additional linear term in the evolution equation for the compositioneld. It also leads to an orientation-dependent effective fourth rank coeffcient γ(hkl) in the governing equation for the one-dimensional composition prole across a planar interface. The main effect of a non-negative γ(hkl) is to increase both σ and interfacial width w, each of which, upon suitable scaling, is related to γ(hkl) through a universal scaling function. The anisotropy in the interfacial energy can be large enough to give rise to corners in the Wul. shapes in two dimensions. In particles of finite sizes, the corners get rounded, and their shapes tend towards the Wul. shape with increasing particle size. In the study of unmixing of concentrated alloys, the anisotropy not only leads to non-spherical particle shapes, but also to strongly elongated morphologies.

scholarly journals Universal scaling for the quantum Ising chain with a classical impurity

2017 ◽  
Vol 96 (15) ◽  
Author(s):  
Tony J. G. Apollaro ◽  
Gianluca Francica ◽  
Domenico Giuliano ◽  
Giovanni Falcone ◽  
G. Massimo Palma ◽  
...  
Keyword(s):  
Ising Chain ◽  
Universal Scaling
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