Room-Temperature Superconductors 28, 29 and 30
Via 5b Metals


27 August 2015
Superconductors.ORG

        Superconductors.ORG herein reports the discovery of room-temperature superconductors number 28, 29 and 30. These three materials all feature the F212C copper-chain structure shown below left. However, unlike the Zr19A prototype announced in July 2015, they all have a Group 5b metal in the anion (the "Light" region of the structure). 5b metals typically have a +5 preferred oxidation state.

        The chemical formulas of these compounds are TaBa9Cu10O20+, NbBa9Cu10O20+ and VBa9Cu10O20+. All three were confirmed by sharp transitions observed in direct resistance and magnetization tests performed on low volume fraction (VF) samples. At page top resistance shifts can be seen occurring above 40C, 41C and 54C respectively1,2. (Note that some plots on this page are heating and some are cooling.)


        The below magnetization tests show Meissner transitions of 5 to 8 milliGauss near the same critical transition temperatures (Tc) as the resistance tests. (Up is more magnetic. Down is more diamagnetic. The straight lines drawn through the noise represent the average of the data points.)


         



        These discoveries expand the universe of elements from which room-temperature copper-oxide superconductors can be synthesized. While the best performing materials were previously limited to having an anion with a +4 oxidation state, +5 now appears equally viable. These discoveries also make it possible to quantify the influence of planar weight ratio (PWR) directly with dielectric constant (K). Since tantalum and niobium have similar chemical properties and transition temperatures, it can be deduced that a 2-to-1 PWR increase will produce the same Tc improvement as a 10-to-1 Kappa increase. This is because the weight disadvantage of using tantalum is completely offset by the higher Kappa of Ta-Cu-O versus Nb-O. The below graph illustrates the correlation between PWR and Tc, as well as confirms the strong influence that dielectric constant has in promoting Tc. A tantalum-copper-oxide anion will produce a much higher transition temperature at the same PWR.

        In order to maximize formation of the F212C structure, These compounds were synthesized using the layer cake method, as shown below. The pellet had approximately 100 interference layers. And, even using this layering technique, the volume fraction is low, requiring very sensitive test equipment.

        Stoichiometric ratios of the below chemicals were used for the ODD layers:

BaCO3   99.95%   (Alfa Aesar) (decomposes to BaO during calcination, releasing the carbon as CO2)
CuO   99.995%   (Alfa Aesar)  

       ...and the below for the EVEN layers.

BaCuO   99.9%   (Alfa Aesar)  
Ta2O5   99.993%   or   Nb2O5   99.5%   or   V2O5   99.6%   (Alfa Aesar)  

       The chemical precursors were pelletized at 60,000 PSI and calcined for various periods3 and then sintered for 9 hours at 880C. Lastly the pellet was annealed for 10+ hours at 500C in flowing O2. Temperature was determined using an Omega type "T" thermocouple and precision OP77 DC amplifier. The magnetometer employed twin Honeywell SS94A1F Hall-effect sensors with a tandem sensitivity of 50 mv/Gauss.


FOR A LIST of all 30 room-temperature superconductors, click HERE.

RESEARCH NOTE: The copper-oxides are strongly hygroscopic. All tests should be performed immediately after annealing.

RE-PUBLICATION NOTICE: Elsevier Publishing, dba Elsevier Science, as well as Morris Communications, both print and broadcast divisions, are specifically prohibited from re-publishing any part of this news story.


E. Joe Eck
2015 Superconductors.ORG
All rights reserved.

1. Testing temperatures are believed accurate within ± 0.5 degrees C.
2. All three of these compounds were multi-phasic. The strongest transition
     was deemed to be the stoichiometric phase.
3. Calcination temperatures and durations can be provided upon request.



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