1 / 5

Hebel-Slicther Coherence Peak

Hebel-Slicther Coherence Peak. L. C. Hebel and C. P. Slichter, Phys. Rev. 113 , 1504 (1959). Type II Coherence Effects. Y. Masuda and A. G. Redfield Phys. Rev. 125 , 159 (1962). 1/T 1. T c. Temperature. Absence of Type II Coherence Effects in Cuprates.

jponder
Download Presentation

Hebel-Slicther Coherence Peak

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Hebel-Slicther Coherence Peak L. C. Hebel and C. P. Slichter, Phys. Rev. 113, 1504 (1959). Type II Coherence Effects Y. Masuda and A. G. Redfield Phys. Rev. 125, 159 (1962) 1/T1 Tc Temperature

  2. Absence of Type II Coherence Effects in Cuprates Y. Kitaoka, et al., J. Phys. Soc. Japan 57, 30 (1988) Reasons for absence of coherence effects in high-Tc cuprates Gap anisotropy Spin fluctuations (not QPs) dominate spin relaxation Clean limit electrodynamics (suppresses “coherence peak”) d s N(E) N(E) E E The absence of “coherence effects” does not rule out a BCS-like description of the cuprates K. Holczer, et al., Phys. Rev. Lett. 67, 152 (1991)

  3. D. M. Ginsburg and M. Tinkham, Phys. Rev. 118, 990 (1960) Type II Coherence Effects R. E. Glover and M. Tinkham, Phys. Rev. 104, 844 (1956)

  4. L. H. Palmer and M. Tinkham, Phys. Rev. 165, 588 (1968)

  5. Type I Coherence Effects Ultrasonic Attenuation R. W. Morse and H. V. Bohm, Phys. Rev. 108, 1094 (1957)

More Related