SC in CuO Layers: Evidence & Experiments

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Discussion Overview

The discussion revolves around the evidence and experiments that suggest superconductivity (SC) resides in the copper oxide (CuO) layers of high-temperature superconductors (HTSC). Participants explore various experimental observations and theoretical implications related to this topic, including the anisotropic behavior of materials, angle-resolved photoemission spectroscopy (ARPES), and the role of CuO planes versus other structural components.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants note that the idea of SC residing in the CuO layers is still controversial, although many in the community believe it to be true based on various observations.
  • Evidence for SC in CuO layers includes the highly two-dimensional nature of the superconductors, indicated by significant anisotropy in resistivity measurements.
  • ARPES measurements reportedly show an anisotropic superconducting gap that aligns with the band structure crossing the Fermi surface on the CuO plane, along with split-band effects in dual-layer CuO compounds.
  • There is a suggestion that the transition temperature (Tc) increases with the number of CuO planes per unit cell.
  • Some participants argue that the ability to modify compounds between CuO planes without affecting superconductivity implies those planes act primarily as charge reservoirs rather than being integral to the SC phenomenon.
  • Questions arise regarding whether ARPES is a bulk measurement and requests for references on the technique are made.
  • One participant shares a journal entry discussing photoemission spectroscopy and its relevance to studying superconductors, emphasizing the photon picture of light in the theory of photoemission.
  • Another participant clarifies that the Timusk and Statt paper discusses the pseudogap state, which includes various experimental observations, with ARPES being one aspect, and notes the distinction between the pseudogap and bilayer split bands in different doping regimes.

Areas of Agreement / Disagreement

Participants express differing views on the evidence for SC residing in CuO layers, with some supporting this idea based on multiple observations while others highlight the ongoing controversy and lack of a singular convincing proof. The discussion remains unresolved regarding the definitive role of CuO layers versus other components in superconductivity.

Contextual Notes

Limitations include the dependence on specific experimental setups and the varying interpretations of results, particularly concerning the pseudogap state and its implications for understanding superconductivity in CuO layers.

nbo10
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What kinda experiments prodive evidence that SC resides in the CuO layers? Off hand I can't think of how any experiments that I'm familiar with could distinguish if the CuO or another plane where SC. Thanks
 
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nbo10 said:
What kinda experiments prodive evidence that SC resides in the CuO layers? Off hand I can't think of how any experiments that I'm familiar with could distinguish if the CuO or another plane where SC. Thanks

First of all, in some camps, this is still a controversial idea. But the community as a whole are convinced that the CuO planes are where all the actions are taking place. There is no single one convincing proof that this is occurring. Rather, it comes from several different observations.

1. We establish that the superconductor is highly 2D. This can be seen from the huge anisotropy in the resistivity of the material, where the c-axis resistivity can be several orders of magnitude greater than the ab-plane resistivity.

2. ARPES measurements see the opening of the anisotropic superconducting gap consistent with where the band crosses the Fermi surface on the CuO plane. Furthermore, we see the split-bands effects from the bonding-antibonding bands in high-Tc compounds with a dual-layer CuO planes per unit cell.

3. Tc seems to increase when there's more CuO planes per unit cell.

4. But the most convincing evidence is the fact that we can practically change the compounds in between the CuO planes and still superconductivity. This seems to indicate that the planes in between the CuO planes are simply "spacers" that act as charge reservoir and plays no significant role in superconductivity.

Zz.
 
ZapperZ said:
2. ARPES measurements see the opening of the anisotropic superconducting gap consistent with where the band crosses the Fermi surface on the CuO plane. Furthermore, we see the split-bands effects from the bonding-antibonding bands in high-Tc compounds with a dual-layer CuO planes per unit cell.
Zz.

Thanks for the response ZapperZ. Is ARPES a bulk measurement? Do you have any quick reference on ARPES? If not I can do a literature serach.

ZapperZ, would you mind if I PM a few questions that are HTSC related? Thanks
 
There's a review article by Timusk and Statt that explains ARPES measurements. You can download the pre-print from http://physwww.physics.mcmaster.ca/timusk/.

The pseudogap in high-temperature superconductors: an experimental survey, T. Timusk and B. Statt, Rep. Prog. Phys. 62, 61-122, (1999).
 
nbo10 said:
Thanks for the response ZapperZ. Is ARPES a bulk measurement? Do you have any quick reference on ARPES? If not I can do a literature serach.

ZapperZ, would you mind if I PM a few questions that are HTSC related? Thanks

I'll be tacky and mention that I have an entry in my Journal on Photoemission:

[10-17-2004 08:40 PM] - Photoemission Spectroscopy

Here are the references in that entry:

"The progress in this experimental technique evolved rather spectacularly after the discovery of the high-Tc superconductors. Having the 2D layers of copper-oxide planes where most of the superconducting effects are thought to occur, these made them a natural candidate to be studied by photoemission, especially using a technique called angle-resolved photoemission. The avatar that I am using came from such an experiment done on a highly overdoped Bi2212, a high-Tc superconductor.

It is imperative to point out that ALL of the theory of photoemission, including those applied in the study of materials that we are now using in modern electronics, make use of ONLY the photon picture of light. There have been NO other alternative formulation of light to account for the experimental observations of photoemission spectroscopies. NONE.

There are two very good reviews of the usage of the photoemission technique on superconductors. The identical technique is also used on other materials.

http://arxiv.org/abs/cond-mat/0209476
http://arxiv.org/abs/cond-mat/0208504 "

You can PM me, but unless it has something to do with private info, I'd rather discuss the physics on here. At the very least, someone with more info, or a more accurate one, can come in and contribute.

Zz.
 
Last edited:
Gokul43201 said:
There's a review article by Timusk and Statt that explains ARPES measurements. You can download the pre-print from http://physwww.physics.mcmaster.ca/timusk/.

The pseudogap in high-temperature superconductors: an experimental survey, T. Timusk and B. Statt, Rep. Prog. Phys. 62, 61-122, (1999).

Note that the Timusk paper is more of a survey of the pseudogap state. So this includes a whole bunch of experimental observations, with ARPES being just a part of it. Furthermore, you don't get to see the bilayer split bands in the pseudogap state, since the pseudogap came from the optimally and underdoped compounds. The bilayer split bands (one of the evidence that argues for the CuO planes being responsible for superconductivity) are most apparent in the overdoped regime of the phase diagram. In this regime, there are no discernable pseudogap.

Zz.
 

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