Sinclair- Superconducting Transition Metal Oxides (La2CuO4 focus) Flashcards
Rules that may produce a high Tc material
Have an insulating parent phase (La2CuO4 is AFMI).
Unusual high oxidation states (Cu3+).
Linear B-O-B bonds (contain CuO2 planes).
Large amount of covalency in the bonding.
High oxidation states due to large (A-site) electropositive cations (Sr, Ba, La, Y).
Variable oxygen contents (YBa2Cu3O7-δ)
Rare earth, Bi and Y ion charges
All always +3
Favoured materials for industrial application
BiSCCO: Bi2Sr2CaCu2O8+δ (2212 or 90K phase) or
Bi2Sr2Ca2Cu3O10+δ (2223 or 110K phase)
YBCO: YBa2Cu3O7-δ (123 phase)
How to find oxidation states of Cu in YBCO
Y is +3, Ba is 2+ (x2), O is 2- (x7) makes -7.
So Cu3 needs to account for +7.
Could be 2Cu2+ and Cu3+ or 2Cu3+ and Cu+
Find which one using the crystal structure and coordination number.
In this case is 2Cu2+ and Cu3+. Tc,max seems to be when Cu2.33+ is present
Doped lanthanum cuprate
La2-xMxCuO4. M is Ca, Sr, Ba.
So the La3+ is partly replaced by M2+. To balance charge some Cu2+ oxidises to Cu3+ (d9 to d8)
Example: La3+ + Cu2+ -> Sr2+ + Cu3+
Becomes superconducting at T>23K
Structure of La2CuO4
Alternating layers of rocksalt AO with perovskite ABO3. SC resides in the perovskite blocks so have 2D superconducting planes. So perovskite block of LaCuO3 and rocksalt block of LaO. Orthorhombic units cell a=5.363, b=5.409, c=13.17Å. Have corner sharing octahedra (not regular but elongated)
What does band theory predict La2CuO4 to be?
A metal but is an insulator due to JT distortion
Energy vs density of states N(E) for pure La2CuO4
Have an empty UHB and a full LHB (Cu 3d9) as half an ellipse each separated. Extending either side of LHB is semicircular band from O (2p). This is d9 Jahn-Teller distortion
Energy vs density of states N(E) for doped La2CuO4
Same as pure La2CuO4 but at top of band from O 2p is empty and has holes until Ef before is reaches top of LHB.
Where do holes come from in doped La2CuO4?
70% holes come from Cu2+ + h+ = Cu3+
The 30% holes come from O2- + h+ = O-
AFM alignment in La2CuO4 (superexchange mechanism?)
In a linear Cu2+ - O2- - Cu2+ arrangement there is strict AFM (anti-parallel spin) alignement on adjacent Cu2+ neighbours. The Cu2+ has an outer 3(dx2-y2) orbital with one electron in. The O2- in the middle has an outer 2p orbital with two electrons (of opposite spins) in. The electron in O2- closest to a Cu2+ will cause its electron to have the opposite spin. Effect same for the Cu2+ on the other side of the O2- so the electrons in the two Cu2+ ions will have opposite spins.
Magnetic frustration caused by O- ion in doped La2CuO4
Now a hole on O so only has one outer electron with one spin. The spins of the outer electrons for Cu2+ ions either side are opposite to this but the same as each other leading to ferromagnetic (parallel spin) alignment of Cu2+ nearest neighbours
Magnetic frustration caused by oxidation to Cu3+ in doped La2CuO4
Consider Cu2+ - O2- - Cu3+ - O2- - Cu2+ line.
Central Cu has a hole. Leads to AFM alignment of next nearest neighbour Cu spins. Because O2- still have two electrons in outer orbital. Basically same case as pure La2CuO4 superexchange mechanism but leaping over the central Cu3+ ion
Tc vs x graph for doped La2CuO4 with Sr
Basically a dome with finite x intercepts. Has peak at x=0.15 which corresponds to average Cu2.15+. There is a dip just left of the full peak. Left of peak is underdoped, peak is optimum doping, right is overdoped. Under peak is SC behaviour. This behaviour with Cu2.15+ to Cu2.2+ in layered cuprates generally gives the optimised Tc. General behaviour but not understood
Where do oxidation and reduction occur in La2CuO4?
Oxidation in perovskite block Cu2+ -> Cu3+ + e-.
Reduction in rocksalt block