1 / 22

Comparison of X-Ray Diffraction Patterns of La2CuO4 from Various Crystals at Room Temperature

This study presents a comprehensive analysis of the X-ray diffraction patterns observed in different crystalline forms of La2CuO4. Conducted at room temperature, the patterns were collected from various layers (0.00 to 1.00) of LSCO crystals, highlighting the influence of layer thickness on diffraction characteristics. Understanding these distinctions is crucial for advancing material science and optimizing the properties of La2CuO4 in technological applications. The results provide valuable insights into crystallography and solid-state physics.

Télécharger la présentation

Comparison of X-Ray Diffraction Patterns of La2CuO4 from Various Crystals at Room Temperature

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. Comparison of X-ray diffraction patterns of La2CuO4+dfrom different crystals at room temperature Pia Jensen

  2. (h,k,0.00)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  3. (h,k,0.05)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  4. (h,k,0.10)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  5. (h,k,0.15)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  6. (h,k,0.20)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  7. (h,k,0.25)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  8. (h,k,0.30)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  9. (h,k,0.35)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  10. (h,k,0.40)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  11. (h,k,0.45)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  12. (h,k,0.50)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  13. (h,k,0.55)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  14. (h,k,0.60)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  15. (h,k,0.65)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  16. (h,k,0.70)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  17. (h,k,0.75)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  18. (h,k,0.80)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  19. (h,k,0.85)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  20. (h,k,0.90)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  21. (h,k,0.95)-layer LSCO_01_long LSCO_03_long LSCO_07_long

  22. (h,k,1.00)-layer LSCO_01_long LSCO_03_long LSCO_07_long

More Related