МИНИСТЕРСТВО ОБРАЗОВАНИЯ И НАУКИ

РОССИЙСКОЙ ФЕДЕРАЦИИ

Федеральное государственное бюджетное образовательное учреждение высшего профессионального образования Пермский государственный национальный исследовательский университет»

Кафедра английского языка профессиональной коммуникации Английский язык

English Reader for Students of Radiophysics

Методическая разработка

Часть 1 Составитель Бабаджан Сергей Савельевич

Английский язык . English Reader for

Students of Radiophysics/ метод. разработка /сост. С.С, Бабаджан;

. Перм. гос. ун-т. – Пермь, 2012.-Ч.1 -52с.

Данная разработка предназначена для студентов 1-2 курсов специальности «Радиофизика»

Издается по решению методической комиссии факультета современных иностранных языков и литератур Пермского государственного университета.

What are Josephson junctions? How do they work?

Leigh John Martinson

Richard Newrock, a professor of physics at the University of Cincinnati, has studied the physics of superconducting materials for 20 years. Here is his explanation.

A Josephson junction is made by sandwiching a thin layer of a nonsuperconducting material between two layers of superconducting material. The devices are named after Brian Josephson, who predicted in 1962 that pairs of superconducting electrons could “tunnel” right through the nonsuperconducting barrier from one superconductor to another. He also predicted the exact form of the current and voltage relations for the junction. Experimental work proved that he was right, and Josephson was awarded the 1973 Nobel Prize in Physics for his work.

To understand the unique and important features of Josephson junctions, it’s first necessary to understand the basic concepts and features of superconductivity. If you cool many metals and alloys to very low temperatures (within 20 degrees or less of absolute zero), a phase transition occurs. At this “critical temperature,” the metal goes from what is known as the normal state, where it has electrical resistance, to the superconducting state, where there is essentially no resistance to the flow of direct electrical current. The newer high-temperature superconductors, which are made from ceramic materials, exhibit the same behavior but at warmer temperatures.

What occurs is that the electrons in the metal become paired. Above the critical temperature, the net interaction between two electrons is repulsive. Below the critical temperature, though, the overall interaction between two electrons becomes very slightly attractive, a result of the electrons’ interaction with the ionic lattice of the metal.

This very slight attraction allows them to drop into a lower energy state, opening up an energy “gap.” Because of the energy gap and the lower energy state, electrons can move (and therefore current can flow) without being scattered by the ions of the lattice. When the ions scatter electrons, it causes electrical resistance in metals. There is no electrical resistance in a superconductor, and therefore no energy loss. There is, however, a maximum supercurrent that can flow, called the critical current. Above this critical current the material is normal. There is one other very important property: when a metal goes into the superconducting state, it expels all magnetic fields, as long as the magnetic fields are not too large.

In a Josephson junction, the nonsuperconducting barrier separating the two superconductors must be very thin. If the barrier is an insulator, it has to be on the order of 30 angstroms thick or less. If the barrier is another metal (nonsuperconducting), it can be as much as several microns thick. Until a critical current is reached, a supercurrent can flow across the barrier; electron pairs can tunnel across the barrier without any resistance. But when the critical current is exceeded, another voltage will develop across the junction. That voltage will depend on time—that is, it is an AC voltage. This in turn causes a lowering of the junction’s critical current, causing even more normal current to flow—and a larger AC voltage.

The frequency of this AC voltage is nearly 500 gigahertz (GHz) per millivolt across the junction. So, as long as the current through the junction is less than the critical current, the voltage is zero. As soon as the current exceeds the critical current, the voltage is not zero but oscillates in time. Detecting and measuring the change from one state to the other is at the heart of the many applications for Josephson junctions.

Electronic circuits can be built from Josephson junctions, especially digital logic circuitry. Many researchers are working on building ultrafast computers using Josephson logic. Josephson junctions can also be fashioned into circuits called SQUIDs—an acronym for superconducting quantum interference device. These devices are extremely sensitive and very useful in constructing extremely sensitive magnetometers and voltmeters. For example, one can make a voltmeter that can measure picovolts. That’s about 1,000 times more sensitive than other available voltmeters.

A SQUID consists of a loop with two Josephson junctions interrupting the loop. A SQUID is extremely sensitive to the total amount of magnetic field that penetrates the area of the loop—the voltage that you measure across the device is very strongly correlated to the total magnetic field around the loop.

SQUIDs are being used for research in a variety of areas. Since the brain operates electrically, one can, by sensing the magnetic fields created by neurological currents, monitor the activity of the brain—or the heart. You can also use a SQUID magnetometer for geological research, detecting remnants of past geophysical changes of the earth’s field in rocks.

Similarly, changes in the ambient magnetic field are created by submarines passing below the surface of the ocean, and the U.S. Navy is very interested in SQUIDs for submarine detection. SQUIDs are also of considerable use in the research laboratory in specially designed voltmeters, in magnetometers and susceptometers and in scanning SQUID microscopes. In this last instrument, a SQUID is scanned across the surface of a sample, and changes in magnetism at the surface of the sample produce an image.