Related Experiment Video
Updated: Jan 22, 2026
![Measuring the Spin-Lattice Relaxation Magnetic Field Dependence of Hyperpolarized [1-13C]pyruvate](/_next/image?url=https%3A%2F%2Fcloudfront.jove.com%2FCDNSource%2Fteasers%2F59399.jpg&w=3840&q=50)
11:57
Measuring the Spin-Lattice Relaxation Magnetic Field Dependence of Hyperpolarized [1-13C]pyruvate
Published on: September 13, 2019
7.0K
Vortex lattice instability at the nanoscale in a parallel magnetic field
Gaia Grimaldi1, Antonio Leo1,2, Francesco Avitabile2
1CNR SPIN, Salerno, Italy.
Nanotechnology
|July 18, 2019
Summary
Superconducting vortex lattice instability was studied in ultra-thin NbN and NbTiN films. An unusual "flying birds" feature appeared in a parallel magnetic field, relevant for nanostructure applications.
Area of Science:
- Condensed Matter Physics
- Materials Science
Background:
- Vortex lattice instability in superconductors occurs at high vortex velocities, leading to a sudden transition to the normal state.
- Understanding nanoscale effects is crucial for advanced superconducting device applications.
Purpose of the Study:
- To experimentally investigate the influence of nanoscale geometry on vortex lattice instability in ultra-thin superconducting films.
- To examine the effect of magnetic field orientation on vortex lattice instability.
- To compare critical currents and instability currents in different configurations.
Main Methods:
- Fabrication of submicron bridges from ultra-thin films (few nanometers) of Niobium Nitride (NbN) and Niobium Titanium Nitride (NbTiN).
- Experimental measurements of critical currents (Ic) and instability currents (I*) under magnetic fields applied parallel and perpendicular to the c-axis.
- Analysis of the magnetic field dependence of current switching behavior.
Main Results:
- Vortex lattice instability was observed in both NbN and NbTiN ultra-thin films, irrespective of the magnetic field orientation.
- An unusual 'flying birds' feature was identified in the parallel magnetic field configuration, where the ratio I*/Ic approached 1.
- The ultra-thin film geometry with in-plane magnetic fields mimics nanoscale bridge narrowing.
Conclusions:
- The study demonstrates that nanoscale effects significantly influence vortex lattice instability in superconductors.
- The 'flying birds' feature in the parallel field configuration offers potential for practical applications in superconducting nanostructures.
- Scaling down film thickness and orienting the magnetic field in-plane are key strategies for controlling vortex dynamics in nanodevices.
Related Concept Videos
Lattice Centering and Coordination Number
11.4K
The structure of a crystalline solid, whether a metal or not, is best described by considering its simplest repeating unit, which is referred to as its unit cell. The unit cell consists of lattice points that represent the locations of atoms or ions. The entire structure then consists of this unit cell repeating in three dimensions. The three different types of unit cells present in the cubic lattice are illustrated in Figure 1.
Types of Unit Cells
Imagine taking a large number of identical...
Types of Unit Cells
Imagine taking a large number of identical...
11.4K
Magnetic Fields
7.1K
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...
7.1K
Magnetic Force Between Two Parallel Currents
4.5K
Two long, straight, and parallel current-carrying conductors exert a force of equal magnitude on one another. The direction of the force depends on the current direction in the conductors.
The force exerted by the magnetic field due to the first conductor over a finite length of the second conductor is given as the product of the current in the second conductor and the vector product of the length vector along the current element and the field due to the first conductor. According to the...
The force exerted by the magnetic field due to the first conductor over a finite length of the second conductor is given as the product of the current in the second conductor and the vector product of the length vector along the current element and the field due to the first conductor. According to the...
4.5K
Electric Field of Parallel Conducting Plates
1.6K
Gauss' law relates the electric flux through a closed surface to the net charge enclosed by that surface. Gauss's law can be applied to find the electric field and the charge enclosed in a region depending on its charge distribution.
Consider a cross-section of a thin, infinite conducting plate having a positive charge. For such a large thin plate, as the thickness of the plate tends to zero, the positive charges lie on the plate's two large faces. Without an external electric field, the...
Consider a cross-section of a thin, infinite conducting plate having a positive charge. For such a large thin plate, as the thickness of the plate tends to zero, the positive charges lie on the plate's two large faces. Without an external electric field, the...
1.6K
Magnetic Field of a Solenoid
5.7K
A solenoid is a conducting wire coated with an insulating material, wound tightly in the form of a helical coil. The magnetic field due to a solenoid is the vector sum of the magnetic fields due to its individual turns. Therefore, for an ideal solenoid, the magnetic field within the solenoid is directly proportional to the number of turns per unit length and the current. Conversely, the magnetic field outside the solenoid is zero.
Consider a solenoid with 100 turns wrapped around a cylinder of...
Consider a solenoid with 100 turns wrapped around a cylinder of...
5.7K
Magnetic Field Lines
5.5K
The representation of magnetic fields by magnetic field lines is very useful in visualizing the strength and direction of the magnetic field. Each of the magnetic field lines forms a closed loop. The field lines emerge from the north pole (N), loop around to the south pole (S), and continue through the bar magnet back to the north pole.
Magnetic field lines follow several hard-and-fast rules:
Magnetic field lines follow several hard-and-fast rules:
5.5K

