Phase transition and Critical phenomena Youjin Deng

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1 Phase transition and Critical phenomena Youjin Deng 09.11.28

2 Phenomenological Introduction
Chapter 1 Phenomenological Introduction

3 1, States of Matter

4 固体是物质存在的一种状态。与液体和气体相比，固体有固定的体积和形状，质地也较坚硬。
一般来说，一个物体要达到一定的大小才能被称为固体，但对这个大小没有明确的规定。一般来说固体是宏观物体，除一些特殊的低温物理学的现象如超导现象、超液现象外固体作为一个整体不显示量子力学的现象。 [编辑] 特性 固体有三种特性： 固体里的粒子是紧紧相扣，不易进行运动。 固体是固定在物质里一个特定的空间。 当有外力对物质施加作用时，固体以上型态会被扭曲，引致永久性变形。 尽管任何固体都会有热能量，粒子间可以相互震动，此粒子运动却相对不那么剧烈，并不轻易靠感觉来观察。 通过其组成部分之间的相互作用，固体的特性可以与组成它的粒子的特性有很大的区别。 固体可以分为晶体和非晶体。 [编辑] 纪录 世界上最轻的固体乃气凝胶。最轻的气凝胶密度只有1.9 mg/cm³ 至 1.9 kg/m³ (约相等于水的1/530)。

5 液体： 没有确定的形状，但有一定体积，具有移动与转动等运动性。
特性： 没有确定形状，是流动的，往往受容器影响。容器是什么形状，注入液体，液体就呈什么形状。 具有一定体积。液体的体积在压力及温度不变的环境下，是固定不变的。 很难被压缩。

6 气体：气体与液体一样是流体：它可以流动，可变形。与液体不同的是气体可以被压缩。假如没有限制（容器或力场）的话，气体可以扩散，其体积不受限制，没有固定。气态物质的原子或分子相互之间可以自由运动。气态物质的原子或分子的动能比较高。 理想气体为假想的气体。其特性为： 气体分子间无作用力 气体分子本身不占有体积 气体分子与容器器壁间发生完全弹性碰撞

7 等离子体：物质的第四态，是由电子、离子等带电粒子及中性粒子组成的混合气体。
宏观上表现出准中性，即正负离子的数目基本相等，整体上呈现电中性，但在小尺度上具有明显的电磁性质。等离子体还具有明显的集体效应，带点粒子之间的相互作用是长程库仑作用，单个带点粒子的运动状态受到其它许多带电粒子的影响，又可以产生电磁场，影响其它粒子的运动。 等离子体存在广泛： 受控核聚变、空间等离子体、等离子体天体、低温等离子体等等。

8 To From Solid Liquid Gas Plasma
The transitions between the solid, liquid, and gaseous phases of a single component, due to the effects of temperature and/or pressure: To From Solid Liquid Gas Plasma Solid-Solid Transformation Melting/ Fusion Sublimation N/A Freezing Boiling/ Evaporation Deposition Condensation Ionization Recombination/Deionization

9 2, Examples Figure 1. A typical phase diagram. The dotted line gives the anomalous behavior of water

10 Figure 2. The phase transition to QGP is conceptually similar to the phase transition from ice to water and to water vapour which occurs when heat is provided to the system.

11 Figure 3. A small piece of rapidly melting argon ice simultaneously shows the transitions from solid to liquid to gas.

12 Fig. 10. Phase transition between paramagnet and ferromagnet

13 Fig. 11 A solid structure

14 Collapse phase transition in polymer system

15 Figure 4. Velocity-distribution data of a gas of rubidium atoms, confirming the discovery of a new phase of matter, the Bose-Einstein condensate.

16 Figure 5. Bose-Einstein condensation
Figure 5. Bose-Einstein condensation. From left to right this frequency is decreased and the atomic ensemble undergoes the transition from a thermal cloud to a pure Bose-Einstein condensate.

17 Figure 6. Phase Transition between Superfluid and Mott Insulator
Figure 6. Phase Transition between Superfluid and Mott Insulator. Left: High contrast interference pattern in the superfluid regime; Right: Quantum phase transition to the Mott Insulator regime with no phase coherence

18 Figure 7. From left to right: High contrast interference pattern in the superfluid regime; Quantum phase transition to the Mott Insulator regime with no phase coherence; Restored coherence after the transition back into the superfluid regime

19 Fig. 8 Dispersion relation in a model Fermi system

20 Fig. 9 Schematic phase diagrams. Left: a three-component Fermi system.
Right: a doped system

21 Fig. 10 Two schematic diagrams for quantum phase transitions

22 Fig. 11. Occurrence of topological Motts insulator

23 Fig. 11 Phase transition in earth system

24 Figure 8. Timeline of the universe

25 Fig. 9 Cooling rapidly through a phase transition leaves behind so-called topological defects, such as the "knots" in this liquid crystal that has been cooled into a colorful phase. The Universe also cooled rapidly, and experiments with a superconductor support a theory of topological defect formation in the cosmos—PRL (2006).

26 Cosmological Phase Transition
In Big Bang cosmology, reionization is the process that reionized the matter in the universe after the "dark ages." It is the second of two major phase changes of hydrogen gas in the universe. The universe is currently ionized, in this sense. The first phase change was recombination, which occurred at a redshift z = 1100 (400,000 years after the Big Bang), due to the cooling of the universe to the point where the rate of combination of an electron and proton to form neutral hydrogen was higher than the ionization rate of hydrogen. The second phase change occurred once objects started to form in the early universe energetic enough to ionize neutral hydrogen.

27 Symmetry-breaking phase transitions play an important role in cosmology. It has been speculated that, in the hot early universe, the vacuum (i.e. the various quantum fields that fill space) possessed a large number of symmetries. As the universe expanded and cooled, the vacuum underwent a series of symmetry-breaking phase transitions. I.e., the electroweak transition broke the SU(2)×U(1) symmetry of the electroweak field into the U(1) symmetry of the present-day electro- magnetic field. This transition is important to understand the asymmetry between the amount of matter and antimatter in the present-day universe.

28 Fig. 12. Virus propagation

29 Fig. 13. Phase transitions between different patterns
in non-equilibrium systems

30 “Phase Transitions” are important

31 continue

32 Continue

33 A phase transition is a natural physical process
A phase transition is a natural physical process. It has the characteristic of taking a given medium with given properties and transforming some or all of that medium, into a new medium with new properties. Phase transitions occur frequently and are found everywhere in the natural world.

34 In thermodynamics, a phase transition is the transformation of a thermodynamic system from one phase to another. At a phase transition point, physical properties may undergo abrupt change: for instance, the volume of the two phases may be vastly different as is illustrated by the boiling of liquid water to form steam.

35 Goal of Statistical Physics
Understand Macroscopic Properties of Matter from Microscopic Behavior 1), Microscopic Behavior: Newtonian Mechanics or Quantum Mechanics 2), From Micro-Macro: Statistical Distribution (Boltzmann, Fermi-Dirac, Bose-Einstein) 物含妙理总勘寻