Related Experiment Video
Updated: Dec 17, 2025

10:36
Advanced Experimental Methods for Low-temperature Magnetotransport Measurement of Novel Materials
Published on: January 21, 2016
10.9K
Magnetotransport in atomic-size bismuth contacts
Hans-Fridtjof Pernau1, Torsten Pietsch, Elke Scheer
1Now at Fraunhofer IPM, Heidenhofstraße 8, 79110 Freiburg.
Summary
We observed atomic-scale bismuth contacts exhibiting unique electrical conductance. These findings reveal a transition in electron transport behavior as contact size decreases.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Nanotechnology
Background:
- Atomic-size contacts are crucial for understanding quantum transport phenomena.
- Bismuth (Bi) possesses a long Fermi wavelength, making it suitable for studying quantum effects in constrictions.
Purpose of the Study:
- To investigate low-temperature electrical transport properties of atomic-scale bismuth contacts.
- To explore the transition from diffusive to ballistic and ultra-quantum transport regimes.
Main Methods:
- Fabrication of atomic-size bismuth contacts using the mechanically controlled break-junction technique at low temperatures.
- Measurement of electrical conductance and magneto-transport behavior across a range of contact sizes.
- Analysis of conductance histograms and magnetic field dependence.
Main Results:
- Stable bismuth contacts with conductance values at fractions of the conductance quantum (G0 = 2e^2/h) were observed.
- Two preferred conductance scales were identified: ~0.015 G0 (single-atom Bi contact) and ~0.15 G0.
- Rich magneto-transport behavior, including conductance fluctuations in small contacts and Shubnikov-de Haas oscillations in larger contacts, was detected.
- A transition from diffusive to ballistic and ultra-quantum transport regimes was inferred with decreasing contact size.
Conclusions:
- Atomic-scale bismuth contacts exhibit distinct quantum transport phenomena.
- The observed conductance scales and magneto-transport behavior are consistent with theoretical predictions for quantum transport in nanocontacts.
- Contact size plays a critical role in governing electron transport regimes, from diffusive to ultra-quantum.
Related Concept Videos
Diamagnetism
2.9K
Materials consisting of paired electrons have zero net magnetic moments. However, when these materials are placed under an external magnetic field, the moments opposite to the field are induced. Such materials are called diamagnets. Diamagnetism is the response of the diamagnets when placed in an external magnetic field.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
2.9K
Magnetostatic Boundary Conditions
1.5K
An electric field suffers a discontinuity at a surface charge. Similarly, a magnetic field is discontinuous at a surface current. The perpendicular component of a magnetic field is continuous across the interface of two magnetic mediums. In contrast, its parallel component, perpendicular to the current, is discontinuous by the amount equal to the product of the vacuum permeability and the surface current. Like the scalar potential in electrostatics, the vector potential is also continuous...
1.5K
Magnetic Susceptibility and Permeability
2.1K
In linear magnetic materials, like paramagnets and diamagnets, magnetization is proportional to the magnetic field intensity. The constant of proportionality, a dimensionless number, is called magnetic susceptibility. The value of the susceptibility depends on the type of material.
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
2.1K
Magnetic Fields
7.0K
A moving charge or a current creates a magnetic field in the surrounding space, in addition to its electric field. The magnetic field exerts a force on any other moving charge or current that is present in the field. Like an electric field, the magnetic field is also a vector field. At any position, the direction of the magnetic field is defined as the direction in which the north pole of a compass needle points.
A magnetic field is defined by the force that a charged particle experiences...
A magnetic field is defined by the force that a charged particle experiences...
7.0K
Paramagnetism
2.9K
Paramagnets are materials with unpaired electrons that possess a finite magnetic moment. In the absence of a magnetic field, these moments are randomly oriented, and thus the net moment is zero. Under an external field, a torque acting on the moments tends to align them along the field's direction. However, the random thermal motion of electrons produces a torque opposite to the external field and tries to disorient the moments. These two competing effects align only a few moments along the...
2.9K
Metal-Semiconductor Junctions
772
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
772

