未知数据源 2024年10月02日
Dancing humans embody topological properties
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美国的高中生和科学家们利用舞蹈来阐释拓扑绝缘体的物理学原理。学生们按照科学家精心编排的舞蹈动作进行表演,这是一种有趣的科普活动,解释了拓扑现象。这项练习展示了拓扑非平凡系统的另一种模拟,这可能对研究有用。该研究的负责人,加州大学圣地亚哥分校的理论化学家 Joel Yuen-Zhou 表示,他们希望以更直观的方式向更广泛的受众解释物质的拓扑相的概念。

😊 拓扑绝缘体是一种拓扑材料,其内部是电绝缘体,但表面或边缘(取决于系统是 3D 还是 2D)导电。导电状态是由与整个系统相关的电子能带结构的特性引起的,这意味着即使系统存在缺陷或畸变,只要系统的基本拓扑结构不受干扰,它们就会持续存在。拓扑可以用咖啡杯与甜甜圈的拓扑等效性来理解,因为它们都有一个贯穿整个的孔。这与没有孔的果酱甜甜圈不同,因此它与咖啡杯没有拓扑等效性。

😇 没有导电边缘或表面状态的绝缘体是“拓扑平凡的”,并且在整个系统中都具有绝缘特性。Yuen-Zhou 解释说,为了使拓扑非平凡特性出现,系统必须能够支持波现象,并且必须有一些东西来充当凝聚态拓扑绝缘体中的磁场的作用。因此,人们在从海洋和大气流体到对映异构体分子和活性物质等各种系统中报道了拓扑绝缘体的模拟。尽管人们对拓扑特性在潜在应用中的兴趣浓厚,但它们仍然可能显得抽象和深奥。

🥰 Yuen-Zhou 与当时的博士生 Matthew Du(现就职于芝加哥大学)一起着手设计一种拓扑绝缘体的人类模拟。第一步是建立一个哈密顿量,该哈密顿量定义了二维晶格中的每个位置与其邻居和磁场的相互作用方式。然后,他们将系统的薛定谔方程公式化为一种算法,该算法在时间上的离散步骤后更新,并再现拓扑绝缘体行为的基本特征。这些特征包括:当最初在边缘被激发时,沿边缘的手性传播;对缺陷的鲁棒性;当晶格有一个孔时,沿内边缘的传播;以及绝缘体内部。

😁 然后,美国加州大学圣地亚哥分校的研究人员探索了如何将这种量子行为转化为人类行为。这是一个挑战,因为量子力学是在复数的领域中运作的,复数具有实部和虚部。幸运的是,他们能够确定导致算法每个时间步长的相互作用仅具有实数值的初始条件。这样,人类(对他们来说,虚数相互作用可能难以模拟)就可以合法地仅仅表现出实数,因为它们按步骤执行算法。这些实数值要么是 1(编排为向上挥舞旗帜),要么是 -1(向下挥舞旗帜),要么是 0(静止不动)。

🤩 研究人员随后在圣地亚哥附近橙色格伦高中的地板上创建了一个网格,蓝色或红色的线连接着相邻的方格。他们定义了这些位置之间的相互作用是平行还是反平行(也就是说,当被提示时,方格的占用者应该向相同或相反的方向挥舞旗帜,如蓝色和红色的线所示)。

High school students and scientists in the US have used dance to illustrate the physics of topological insulators. The students followed carefully choreographed instructions developed by scientists in what was a fun outreach activity that explained topological phenomena. The exercise demonstrates an alternative analogue for topologically nontrivial systems, which could be potentially useful for research.

“We thought that the way all of these phenomena are explained is rather contrived, and we wanted to, in some sense, democratize the notions of topological phases of matter to a broader audience,” says Joel Yuen-Zhou who is a theoretical chemist at the University of California, San Diego (UCSD). Yuen-Zhou led the research, which was done in collaboration with students and staff at Orange Glen High School near San Diego.

Topological insulators are a type of topological material where the bulk is an electrical  insulator but the surface or edges (depending on whether the system is 3D or 2D) conducts electricity. The conducting states arise due to a characteristic of the electronic band structure associated with the system as a whole, which means they persist despite defects or distortions in the system so long as the fundamental topology of the system is undisturbed. Topology can be understood in terms of a coffee mug being topologically equivalent to a ring doughnut, because they both have a hole all the way through. This is unlike a jam doughnut which does not have a hole and is therefore not topologically equivalent to a coffee mug.

Insulators without the conducting edge or surface states are “topologically trivial” and have insulating properties throughout. Yuen-Zhou explains that for topologically nontrivial properties to emerge, the system must be able to support wave phenomena and have something that fulfils the role of a magnetic field in condensed matter topological insulators. As such, analogues of topological insulators have been reported in systems ranging from oceanic and atmospheric fluids to enantiomeric molecules and active matter. Nonetheless, and despite the interest in topological properties for potential applications, they can still seem abstract and arcane.

Human analogue

Yuen-Zhou set about devising a human analogue of a topological insulator with then PhD student Matthew Du, who is now at the University of Chicago. The first step was to establish a Hamiltonian that defines how each site in a 2D lattice interacts with its neighbours and a magnetic field. They then formulated the Schrödinger equation of the system as an algorithm that updates after discrete steps in time and reproduces essential features of topological insulator behaviour. These are chiral propagation around the edges when initially excited at an edge; robustness to defects; propagation around the inside edge when the lattice has a hole in it; and an insulating bulk.

The USCD researchers then explored how this quantum behaviour could be translated into human behaviour. This was a challenge because quantum mechanics operates in the realm of complex numbers that have real and an imaginary components. Fortunately, they were able to identify initial conditions that lead to only real number values for the interactions at each time step of the algorithm. That way the humans, for whom imaginary interactions might be hard to simulate, could legitimately manifest only real numbers as they step through the algorithm. These real values were either one (choreographed as waving flags up), minus one (waving flags down) or zero (standing still).

“The structure isn’t actually specific just to the model that we focus on,” explains Du. “There’s actually a whole class of these kinds of models, and we demonstrate this for another example – actually a more famous model – the Haldane model, which has a honeycomb lattice.”

The researchers then created a grid on a floor at Orange Glen High School, with lines in blue or red joining neighbouring squares. They defined whether the interaction between those sites was parallel or antiparallel (that is, whether the occupants of the squares should wave the flags in the same or opposite direction to each other when prompted).

Commander and caller

A “commander” acts as the initial excitation that starts things off. This is prompted by someone who is not part of the 2D lattice, whom the researchers liken to a caller in line, square or contra dancing. The caller then prompts the commander to come to a standstill, at which point all those who have their flags waving determine if they have a “match”, that is, if they are dancing in kind or opposite to their neighbours as designated by the blue and red lines. Those with a match then stop moving, after which the “commander” or excitation moves to the one site where there is no such match.

Yuen-Zhou and Du taught the choreography to second and third year high school students. The result was that excitations propagated around the edge of the lattice, but bulk excitations fizzled out. There was also a resistance to “defects”.

“The main point about topological properties is that they are characterized by mathematics that are insensitive to many details,” says Yuen-Zhou. “While we choreograph the dance, even if there are imperfections and the students mess up, the dance remains and there is the flow of the dance along the edges of the group of people.”

The researchers were excited about showing that even a system as familiar as a group of people could provide an analogue of a topological material, since so far these properties have been “restricted to very highly engineered systems or very exotic materials,” as Yuen-Zhou points out.

“The mapping of a wave function to real numbers then to human movements clearly indicates the thought process of the researchers to make it more meaningful to students as an outreach activity,” says Shanti Pise, a principal technical officer at the Indian Institute of Science, Education and Research in Pune. She was not involved in this research project but specializes in using dance to teach mathematical ideas. “I think this unique integration of wave physics and dance would also give a direction to many researchers, teachers and the general audience to think, experiment and share their ideas!”

The research is described in Science Advances.

The post Dancing humans embody topological properties appeared first on Physics World.

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拓扑绝缘体 舞蹈 物理学 科普
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