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张书雯

银虫 (小有名气)

[交流] 【求助】关于pseudogap的问题

我是化学出身的,想请教物理方面的高手,pseudogap是什么意思哦?最好能用比较通俗的语言解释一下,我更容易理解,呵呵

[ Last edited by ddx-k on 2008-12-14 at 20:00 ]
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supersolid226

铁杆木虫 (正式写手)


zt970831(金币+1,VIP+0):谢谢您的交流:)
如果你有韩汝珊《高温超导物理》,里面有很详细的psudogap的图象,你可以参考

[ Last edited by supersolid226 on 2008-3-27 at 16:56 ]
4楼2008-03-27 16:54:33
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gaoky2008

木虫 (著名写手)

★ ★
zt970831(金币+2,VIP+0):谢谢:)
Pseudogap
From Wikipedia, the free encyclopedia
A pseudogap is a term from the field of high-temperature superconductivity which describes an energy (normally near the Fermi energy) which has very few states associated with it. This is very similar to a 'gap', which is an energy that has no allowed states. Such gaps open up, for example, when electrons interact with the lattice.

Interestingly only certain electrons `see' this gap. The gap, which should be associated with an insulating state, only exists for electrons travelling parallel to the copper-oxygen bonds. Electrons travelling at 45 degrees to this bond can move freely throughout the crystal. The Fermi surface therefore consists of Fermi Arcs forming pockets centred on the corner of the Brillouin zone. In the pseudogap phase these arcs gradually disappear as the temperature is lowered until only four points on the diagonals of the Brillouin zone remain ungapped.

On one hand, this could indicate a completely new electronic phase which consumes available states, leaving only a few to pair up and superconduct. On the other hand, the similarity between this partial gap and that in the superconducting state could indicate that the pseudogap results from preformed cooper pairs.


Mechanism
The origin of the pseudogap is controversial and still subject to debate in the condensed matter community. Two main interpretations are emerging:

1. The scenario of preformed pairs In this scenario, electrons form pairs at a temperature T* that can be much larger than the critical temperature Tc where superconductivity appears. T* of the order of 300K have been measured in underdoped cuprates where Tc is about 80k. The superconductivity does not appear at T* because large phase fluctuations of the pairing field cannot order at this temperature. The pseudogap is then produced by non coherent fluctuations of the pairing field.

2. The scenario of a non superconducting related pseudogap In this class of scenarios, many different origins have been put forward: like the formation of electronic stripes, antiferromagnetic ordering, exotic order parameter competing with superconductivity.


A pseudogap can be seen with several different experimental methods. One of the first observations was in specific heat measurements of YBa2Cu3O6+x by Loram et al.[1] The pseudogap is also apparent in ARPES (Angle Resolved Photoemission Spectroscopy) data, which can measure the density of states of the electrons in a material.


References
^J. W. Loram, K. A. Mirza, J. R. Cooper, and W. Y. Liang (1993). "Electronic specific heat of YBa2Cu3O6+x'' from 1.8 to 300 K".Physical Review Letters71 (11): 1740-1743. doi:10.1103/PhysRevLett.71.1740.
Emery et al. Physical Review B, Vol 56, Page 6120 (1997)
Kyle McElroy, Nature Physics, Vol 2, Page 441 (2006)

External links
pseudogap in non-superconducting materials:http://www.physorg.com/news10505.html
白天看paper,打瞌睡;晚上看paper,睡得香。
2楼2008-03-26 16:59:01
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张书雯

银虫 (小有名气)

呵呵,很难,我要好好理解一下才行.隔行如隔山,这话真的不错.不过还是非常感谢哦,非常非常感谢.
3楼2008-03-26 20:32:12
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gaoky2008

木虫 (著名写手)

赝隙又称正常态能隙。一般在铜氧化合物高温超导体的弱掺杂区中,正常态(非超导态)T*温度以下就形成了电子配对,但未发展成长程序相干的cooper对系统,只在温度低至Tc时这些cooper电子对间才有位相相干,发生超导凝聚,进入超导态。因此,常温下只显现出赝带隙。高温超导体不同于BCS超导体,对的形成和对间位相相干时的超导凝聚是分两步不同时在不同温度下产生的。也有人称正常态电子间的这种配对为“预配对”。

你说的elecreons from pairs at a temperature T*指正常温度下未发生位相相干的电子对中的电子,配对的电子未被打开。
至于electronic stripes的问题,我跟你一样不是很懂。不过我记得好像是电荷有序里面的问题,那种条纹是否指在晶格尺度的电荷和自旋等周期分布,类似反铁磁系统之类的?

高温超导里面的问题很多,我不是做这方面的,说得不一定对,多包涵。赝隙的详细介绍你可以看看李正中的《固体理论》第七章最后一节,或者楼上提到的韩汝珊《高温超导物理》;electronic stripes方面的你找几篇电荷有序的paper看看,里面可能会提到,你可以由此挖出原始文献。

[ Last edited by gaoky2008 on 2008-3-28 at 19:59 ]
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5楼2008-03-28 19:57:37
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