1999
DOI: 10.1002/(sici)1521-396x(199912)176:2<1025::aid-pssa1025>3.0.co;2-0
|View full text |Cite
|
Sign up to set email alerts
|

Hall Effect in YBa2Cu3Ox Thin Films and Contact Misalignment

Abstract: The sign of the Hall effect provides critical transport information both for the normal state and superconducting state of High Temperature Superconductors. For Hall effect measurements in thin films, a contact misalignment of only a few micrometers produces a significant longitudinal voltage in addition to the transverse Hall voltage. This misalignment voltage is usually cancelled by reversing the current and magnetic field. However problems may arise for normal state transport in anisotropic materials and vo… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

2009
2009
2009
2009

Publication Types

Select...
1

Relationship

0
1

Authors

Journals

citations
Cited by 1 publication
(1 citation statement)
references
References 8 publications
0
1
0
Order By: Relevance
“…The temperature and field dependences of the Hall resistivity q xy were measured with a Physical Properties Measurement System (PPMS) using DC current density of %150 A=cm 2 in magnetic fields up to 8 T applied along the c-axis of the films. Longitudinal misalignment of the Hall voltage contacts was almost negligible, however we have taken it into account by measuring the transverse voltage with magnetic field in the þz and Àz directions giving [20]. The Hall voltage is obtained in the form V H ðTÞ ¼ ðV Bþ À V BÀ Þ=2.…”
Section: Methodsmentioning
confidence: 99%
“…The temperature and field dependences of the Hall resistivity q xy were measured with a Physical Properties Measurement System (PPMS) using DC current density of %150 A=cm 2 in magnetic fields up to 8 T applied along the c-axis of the films. Longitudinal misalignment of the Hall voltage contacts was almost negligible, however we have taken it into account by measuring the transverse voltage with magnetic field in the þz and Àz directions giving [20]. The Hall voltage is obtained in the form V H ðTÞ ¼ ðV Bþ À V BÀ Þ=2.…”
Section: Methodsmentioning
confidence: 99%