High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements


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Andrei Mourachkine. Innbundet Fri frakt! Om boka. Avbryt Send e-post.

By the end of next week it will be in every course of graduate lectures. Les mer. Om boka "The Frontiers of Knowhledge to coin a phrase are always on the move. Within the month there will be a clamour to have it in the undergraduate c- riculum. The challenge is to charge the solenoid with a simple mechanism and control the discharge of very little amounts of energy, for their use, at a time. Leakage should be avoided at all times [ 18 , 19 , 20 ]. A A house or a set of houses electrically powered conventionally could be powered with a superconducting reservoir of energy, kind of a cylinder as if it were a dynamo or a car alternator, B a sealed SC solenoid storing thousands of KWTTS of usable electrical energy [18, 19, 20], C a levitating magnet on top of a SC disc, and D a levitated train running on a bed of air because it has been levitated as the magnet at the left [21, 22].

A prototype is shown in Figure 1D and follows the same principle of the levitated magnet Figure 1C. Several countries are developing real-scale prototypes, and engineering problems are being faced one by one [ 21 , 22 ]. The above applications rely on just two properties of superconductors, namely, the Meissner effect and the transport of electrical current with no resistance.

The problem of interfacing with the conventional conductors that connect to machines, motors, etc. The technique of resonator measurements at Mcyc. In contrast to the behaviour of superconductors in static fields, a finite resistance is present at all temperatures, tending as the absolute zero is approached to a very low value, which is probably zero for mercury but not for tin.

Since then, spectacular discoveries and applications of superconductivity have been at work for decades in different areas of engineering, high-energy particle physics and microwave technology, communications, and scientific and medical nuclear magnetic resonance equipment [ 23 , 24 , 25 , 26 , 27 ].

At radio frequency and microwave range, SC has found applications in areas such as satellite communications, particle accelerators, microwave technology applied to precision instruments, and metrology and qubit formation [ 26 , 27 ]. In particular, high-energy physics laboratories use both, SC solenoids and electromagnetic cavities [ 28 , 29 ]. In one case, the production of dc strong magnetic fields, in the other high electric field at GHz is required. Superconducting niobium cavities, the heart of linear accelerators: more specifically, to discover, experimentally, new elementary particles, or to investigate what are they made of, it is necessary to smash them against other high-energy particles.

The electron-positron colliders [ 30 ] need to work with particles at very high kinetic energy; hence their velocity must be as high as possible. This part is the heart of the accelerating process and is supported by other fundamental parts as is the liquid helium bath to keep the temperature at 4.

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A simplified diagram of a superconducting microwave cavity in a helium bath with microwave coupling and a passing particle beam. A the red oval encloses the heart of the accelerating process, B a niobium-based 1. The photo in Figure 3 shows the work on a tandem of four superconducting cavities to mount detectors, and so on, inside a clean room. The conversion of energy from the electromagnetic to the charged particle acceleration is the highest technologically possible at present [ 29 , 30 ].

Accelerating charged particles in open space can disperse, and they cannot, by far, reach the concentrated fields and intensities that can be tailored inside SC cavities as the ones shown in Figure 2. The heart of the accelerating process is inside the superconducting cavity and inside it, in the red oval. The central piece in a linear particle accelerator is a tandem of these SC accelerating microwave cavities Figure 2B.

Working to protect the Q of superconducting cavities. The actual and the potential applications, just briefly mentioned here, are a sample of many propositions that are treated at length in Refs. The world of applications is so vast and promising that pushes the field of discovering new superconducting materials at higher and higher temperatures.

The comparison with other well-known temperatures in the world, placed on the vertical axes at the right, is illustrative. SC comprises a large family of materials with a wide range of complex properties, behaviors, and types. They are classified in different ways: conventional, non-conventional, type I, type II, gapless, s-wave, d-wave, and so forth. To understand more precisely the interactions of superconductors with microwaves, we, next, highlight seven of the most fundamental characteristics of superconductors.

Superconducting critical temperature, Tc: a superconductor becomes so below a critical temperature, Tc. The superconducting state is ordered, and so, it is destroyed by thermal agitation energy, k B T. But, as temperature is lowered, the thermal energy goes down and the atomic and molecular giggling becomes quitter, and the superconducting state produced by the pairing of electrons is not so disturbed by the thermal energy k B T below k B Tc. The formation of Cooper pairs. The ordering consists of the forming of electron-bound pairs, called Cooper pairs, by means of an attractive interaction mediated by the lattice vibrations phonons that overcomes the Coulomb repulsion that experience these electrons.

Figure 5 depicts in an exaggerated manner the lattice distortion when the couple of electrons move through this part of the material.

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Through the vibrations of the lattice, these two electrons form a bound system with zero linear momentum p and zero spin, a singlet Cooper pair. A lattice of atoms is distorted by the passage motion of two electrons, possibly tracing time reversal trajectories [42].

Boaz Almog "levitates" a superconductor

The center of mass does not move and the pair is in a singlet state. The passing electrons attract the positive-charged nuclei of the lattice, causing a slight ripple in its wake. The Ginzburg-Landau equations [ 43 ] predicted two new characteristic lengths in a superconductor.

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Thus this theory characterized all superconductors by two length scales. It was previously introduced by the London brothers in their London theory [ 6 ].

Expressed in terms of the parameters of Ginzburg-Landau model, it is. The penetration depth sets the exponential law according to which an external magnetic field decays inside the superconductor. Zero electrical resistance. Supercurrents, Js, of Cooper pairs. Losses and heating. When these Cooper pairs move in the material, they do so in phase with the lattice vibrations, and no scattering of electron pairs occurs and no electrical resistance develops, and very importantly, no dissipation of energy develops due to this charge transport see blue portion of the temperature axis and coupled blue dots Cooper pairs in Figure 6A and B.

In contrast, when single conduction electrons move in a normal metal or in YBaCuO perovskites, at temperatures above Tc red portion and red single dots in Figure 6A and B , they scatter many times from the nuclei, imperfections, impurities. The material develops Joule heat, and for high currents hundreds to thousands of amperes , the metal can even melt. Meissner effect: magnetic fields get expelled.

When a superconductor is placed in an external magnetic field, or a material becomes SC in the presence of such external magnetic field, the SC material expels the magnetic field from its interior, as shown in Figure 7A. Irrespective of the state and history of the material prior to the superconducting state, once in it, all magnetic lines of the external magnetic field get EXPELLED from its interior. This experimental result was discovered by Meissner and Ochsenfeld in and is known as the Meissner effect. By comparison, a perfect conductor is penetrated by the magnetic field lines irrespective of the temperature.

Above Tc, the material behaves as a normal conductor, and so, the magnetic field lines go through it. Type I superconductor, one critical magnetic field. Type II superconductors.

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Two critical magnetic fields, Hc1 and Hc2. The mixed state. But not all superconductors are of the first kind. For fields above Hc1, the SC of the second kind admits the entrance of magnetic field lines but in an ordered and quantized manner. These lines define approximate cylinders that can be bent and twisted.

High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements
High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements
High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements
High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements
High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements
High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements
High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements
High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements
High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements High-temperature superconductivity in cuprates : the nonlinear mechanism and tunneling measurements

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