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398                           Superconductivity



                                            Amorphous                              Paramagnetic
                                           semiconductor     Strongly correlated metal  metal


                                       Temperature



     Fig. 14.22                          Antiferromagnetic
     Generic phase diagram of the cuprate  insulator
     superconductors. The doping level is                  Superconductor
     measured relative to the insulating
     parent compound.                                        Doping level


                                   doubt that pairing is involved, and the effective charge is 2e. It is also known
                                   that the pairs are made up of electrons with opposite momenta, just as was
                                   shown in Fig. 14.3(a). Interaction of the electrons with the lattice might play a
                                   role, but it is certainly not the full story. Another possible mechanism is pairing
                                   by spin waves, as already referred to earlier in this chapter. An important ex-
                                   periment is to measure the magnetic flux in superconducting rings containing
                                   Josephson junctions. With conventional superconductors, the enclosed flux is
                                   always an integer multiple of the flux quantum. With cuprate superconductors,
                                   the enclosed flux turns out to be an odd multiple of the half-flux quantum. This
                                   is no proof for spin-wave pairing, but if pairing is by spin waves, then this is
                                   one of the conditions that must be satisfied.
                                     In what other directions could one look for a theory? One might possibly
                                   rely on the analogy between the quantum Hall effect and superconductivity
                                   in cuprates. Two-dimensional effects and sudden loss of resistance are char-
                                   acteristic to both. An attempt along such lines has been made at explaining
                                   the quantum Hall effect with a theory which treats electrons as some kind of
                                   composite bosons.
                                     Most theoreticians believe that an energy gap always exists, and for cuprate
                                   superconductors the relationship between gap energy and critical temperature
                                   is 2 (0) ≈ 6 kT c in contrast with 3.5 kT c , which we have come across for low
                                   temperature superconductors. No one entertains great hopes that a theory able
                                   to predict the critical temperatures of various compounds will be forthcoming
                                   in the near future. The theoretical interest will be sustained, however, very
                                   likely for decades. Pairing mechanisms have become popular. Neutron stars
                                   are supposed to have pairing condensations, and it is also believed that quark
                                   condensations began just one second after the Big Bang, although experimental
                                   evidence is lacking for the moment.
                                     How are these superconductors produced? Being ceramics, they were first
                                   produced by mixing, grinding, and baking of powdered reagents. Single crystal
                                   samples, as described above, greatly helped in advancing the understanding of
                                   their properties, but they are not suitable for mass applications. For devices one
                                   needs them as thin films. For high-field magnets they have to be in the form
                                   of wires. Thin films are mostly made by sputtering and pulsed laser deposi-
                                   tion (a pulsed excimer laser evaporates the material which is already available
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