In a 1969 paper, Petersen and Pendleton created a quantity called "modular momentum" to help explain the theory of this effect. Experimental confirmation of this effect was achieved by Tonomura and Osakabe while in 1999 Bachtold made measurements of how this effect could cause oscillations of resistance in carbon nanotubes. This effect was first predicted by Ehrenberg and Siday, whose names are occasionally attached to it. The textbook example of this effect is a beam of electrons being split and passing around either side of a solenoid, and then recombining with a phase difference equal to Berry's phase. FTP, name this quantum effect where charged particles are affected by the magnetic vector potential even in regi
In a 1969 paper, Petersen and Pendleton created a quantity called "modular momentum" to help explain the theory of this effect. Experimental confirmation of this effect was achieved by Tonomura and Osakabe while in 1999 Bachtold made measurements of how this effect could cause oscillations of resistance in carbon nanotubes. This effect was first predicted by Ehrenberg and Siday, whose names are occasionally attached to it. The textbook example of this effect is a beam of electrons being split and passing around either side of a solenoid, and then recombining with a phase difference equal to Berry's phase. FTP, name this quantum effect where charged particles are affected by the magnetic vector potential even in regions where the magnetic field is zero.
In a 1969 paper, Petersen and Pendleton created a quantity called "modular momentum" to help explain the theory of this effect.
Ehrenberg-Siday-Aharonov-Bohm effect (accept: Bohm-Aharonov effect)