Nov 10, 2009

WHAT IS HIDDEN BEHIND THE PSEUDO-GAP?

Contact: Claude Chapelier

Fig. 1: Temperature dependence of the tunnelling density of states in a thin film of disordered TiN. Unlike bulk TiN, a large pseudo-gap is observed above T_{c}.

One of the main characteristics of high critical temperature superconductors is the existence of an abnormally small density of electronic states at the Fermi level, in the normal state. We have just witnessed similar behaviour in a conventional, albeit very disordered, superconductor.

The existence of a gap in the density of electronic states and its disappearance at the transition temperature T_{c} (see inset) has been widely confirmed in experiments performed on numerous superconductors until the discovery of high critical temperature superconductors. In these so-called HTC materials, a large depression in the density of states is still observed above T_{c, up to a temperature T* of the order of room temperature. This anomaly is coined pseudo-gap.}

Arguments about the pseudo-gap

For more than 20 years physicists have been convinced that the key to understanding HTCs lies behind this pseudo-gap. Two opinions clash over this issue. One opinion claims that the pseudo-gap is a precursor state of superconductivity, in which electrons start to dynamically pair without forming a superfluid state. This model is backed by the observation that the superconducting gap below T_{c} turns smoothly into the pseudo-gap above T_{c}. Conversely, the other opinion states that the pseudo-gap competes with superconductivity and that it is the signature of a hidden order that remains to be discovered. This claim is based on the fact that by under-doping HTC materials, their resistivity increases, leading to a vanishingly small T_{c} but a higher T*. This situation suggests probing the density of states of conventional superconductors that are highly disordered, and therefore highly resistive, in the normal state.

Fig. 2: Tunnelling conductance in the normal state at V = 0 (dotted line in Fig. 1) versus the logarithm of the reduced temperature. For each of the three TiN films, linear behaviour is obtained without any adjustable parameter.

**Arguments about the pseudo-gap**

For more than 20 years physicists have been convinced that the key to understanding HTCs lies behind this pseudo-gap. Two opinions clash over this issue. One opinion claims that the pseudo-gap is a precursor state of superconductivity, in which electrons start to dynamically pair without forming a superfluid state. This model is backed by the observation that the superconducting gap below Tc turns smoothly into the pseudo-gap above T_{c}. Conversely, the other opinion states that the pseudo-gap competes with superconductivity and that it is the signature of a hidden order that remains to be discovered. This claim is based on the fact that by under-doping HTC materials, their resistivity increases, leading to a vanishingly small Tc but a higher T*. This situation suggests probing the density of states of conventional superconductors that are highly disordered, and therefore highly resistive, in the normal state.

**Highly disordered TiN films to decide of the winner**

We measure the local density of electronic states through the conductance of the tunnel junction formed between a Scanning Tunnelling Microscope tip and the sample surface. If the sample is superconducting, we access its gap and possibly the thermal dependence of this gap. We have measured three 5 nm-thick TiN films which differ by their degrees of disorder. Unlike bulk TiN whose gap closes at T_{c} (see inset), these films exhibit a pseudo-gap that persists up to 14 T_{c} (see Fig. 1). This is the first observation of a pseudo-gap in a conventional superconductor, and no hidden order can be reasonably invoked to explain it. The challenge consists in proving that we are dealing with superconducting fluctuations and not another physical phenomenon, such as dynamical Coulomb blockade. With this purpose in mind, let us plot the evolution of the density of states at the Fermi level as a function of the logarithm of the reduced temperature ε = ln(T/T_{c}). A linear behaviour as a function of ln(ε) is a signature of the presence of Cooper pairs above T_{c} , according to a theory which accounts for the order parameter fluctuations close to T_{c}. We have checked this behaviour for the three films investigated, as shown in Fig. 2. For each of them, Tc was independently determined through resistivity measurements. If another value of T_{c} is arbitrarily chosen, the linear behaviour in Fig. 2 is immediately lost: this is a dramatic illustration of the validity of this experimental signature.

**The end of a mystery**

The dynamical Cooper pairing above T_{c} is a general phenomenon in superconducting transitions. However, it is often restricted to a temperature range which is so narrow that it is experimentally out of reach. In our case, the fluctuations are enhanced by the strong disorder and the closeness to the superconducting-insulating transition. Does it mean the end of the HTC mystery? This is not certain, because the order parameter symmetry of these superconductors is different, and things become more complicated.

Further reading: B. Sacepe et al., Physical Review Letters 101 (2008) 157006; B. Sacepe et al., arXiv:0906.1193

**Superconductivity and density of states**

When a superconducting state sets in, the electrons form pairs (the so-called Cooper pairs) which are able to carry superfluid current. The onset of these pairs decreases the number of available states for single electrons, opening a gap in the normal electron density of state. This gap, which appears at the Fermi level, is about 2Delta wide, i.e., on the order of 1 milli-electronvolt for usual superconductors having a superconducting transition temperature of a few kelvins. The states that disappear are transferred to the edge of the forbidden region, and so-called coherence peaks appear in the density of state at +-Δ on each side of the Fermi energy. The amplitude Δ is at maximum at T = 0, decreases when the temperature increases, and vanishes precisely at T_{c} in bulk materials. Above T_{c}, the metal is normal with a constant density of states.

Last update : 02/20 2014 (967)

• Institut Nanosciences et Cryogénie • Service de Physique Statistique, Magnétisme et Supraconductivité • Statistical Physics, Magnetism and Superconductivity