27.09.2014 Views

PDF (double-sided) - Physics Department, UCSB - University of ...

PDF (double-sided) - Physics Department, UCSB - University of ...

PDF (double-sided) - Physics Department, UCSB - University of ...

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

other states using a classical excitation, one needs to change the spacing <strong>of</strong> the<br />

energy levels, i.e. introduce a non-linearity into the potential. In general it is very<br />

straightforward to make circuits behave in a non-linear fashion. In fact, almost all<br />

circuits will show some kind <strong>of</strong> non-linear behavior if they are driven hard enough.<br />

The problem here is to build a circuit that does so with only a single photon <strong>of</strong><br />

energy. Luckily, nature provides a way to achieve just that: The Josephson tunnel<br />

junction [Josephson, 1962].<br />

2.2.2 Josephson Tunnel Junctions<br />

A Josephson tunnel junction is formed every time a superconducting lead is<br />

interrupted by a thin barrier through which electrons can tunnel. The tunneling<br />

provides a weak link between the two superconducting regions and allows the wave<br />

functions <strong>of</strong> the superconducting order parameter on the two sides to interfere.<br />

This leads to very interesting electrical characteristics <strong>of</strong> the junction that are<br />

captured by the “Josephson Relations”, named after Brian Josephson who received<br />

the Nobel Prize in 1973 for predicting them:<br />

V (t) = Φ 0<br />

2π<br />

d<br />

δ(t) (2.8)<br />

dt<br />

I(t) = I c sin δ(t) (2.9)<br />

22

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!