Better batteries for implantable medical devices

With electric vehicles, the challenge for battery makers is straightforward: make batteries that can hold more energy, so the vehicles they power can go further on each charge.

However, for companies that make rechargeable batteries for implantable medical devices – think pacemakers, cardiac defibrillators – safety trumps all else. Yes, these batteries need to last, but that lifespan cannot come at the expense of a patient’s health.

For that reason, the batteries currently used in these devices have anodes that operate at a higher voltage than ones in regular lithium-ion batteries. The anode is the component inside a battery that releases lithium ions and electrons when power is being drawn, and that takes up ions and electrons during charging. In most lithium-ion batteries, the anode is made of graphite.

“They’re amazing batteries, but the energy density is pretty small,” says Eric McCalla, an associate professor in McGill University’s Department of Chemistry. “As a result, there are some applications for which they simply don’t hold enough energy.”

McCalla and his team recently made a breakthrough that could change that. In an earlier study, the group demonstrated that adding a small amount of an element called neodymium to the anode resulted in a whopping 20% increase in the battery’s energy density. In this new study, they used the Canadian Light Source at the University of Saskatchewan to explore why such a small amount of the element could yield such a large increase in energy storage.

“What we think is happening is that when you add a small amount of these really big ions it doesn’t just disrupt the atoms around it, it disrupts atoms over a large distance,” says McCalla. The CLS’s HXMA beamline enabled them to see that the element they added disturbed the entire structure of the anode — even at such small amounts.

“They (neodymium ions) do a lot of local damage, which actually turns out to have benefit,” says McCalla. “Locally we damage the structure, but in a way that it opens up some other spots for lithium to go in and out (thereby increasing the battery’s energy density”.

In parallel to the experiments, other researchers on the team used computer modelling to calculate how much easier it is for lithium to move when the neodymium ions are nearby. “That really locked down this mechanism, where we’re able to make new sites where lithium wants to go.”

Being able to do their experiment “in situ” at the HXMA beamline was critical, says McCalla. “We had the battery running while we were running the experiment, so we didn’t have to take the cell apart and scrape the sample out and hope that it was stable in air,” he says. In previous attempts, the researchers found that the material degraded when it was removed from the battery. “Being able to do it in the battery, doing the measurement right on the beamline, that made all the difference.”

In this study, McCalla and his team were focused on increasing the amount of energy a battery can hold without compromising safety. Now they’re shifting their focus to increasing the battery lifespan. They identified some instability related to the electrolyte, which they think could impact its long-term use. “There’s definitely continued work that needs to happen, to make these commercially viable. But already the gains that we’ve made show that the energy (produced by the new type of battery) would enable new or different medical applications.”

Read more on CLS website

Unraveling the structural transformation of Li-rich materials in lithium-batteries

Lithium-Ion Batteries (LIBs) are essentials in everyday life in mobile applications as well as in hybrid/electric mobility. The extraordinary market success of this technology is forcing hard the need of LIBs with improved energy density, environmental compatibility and safety, making necessary to push this technology beyond the current state of the art. In this framework, Co-poor Lithium Rich Layered Oxides (LRLOs) are the most strategic alternative to current Co-rich layered oxide positive electrode materials thanks to the excellent combination of large specific capacity (>250 mAhg-1), high energy density (up to 900 WhKg-1), small costs and improved environmental benignity. The excellent performance of LRLOs derives from the peculiar combination of redox processes originated from the transition metals and the oxygen anions sublattice. The practical use of LRLOs is hindered by several drawbacks, such as voltage decay, capacity fading, and an irreversible capacity lost in the first cycle. These issues are related to structural rearrangements in the lattice upon cycling.

In this work, we demonstrate a new family of LRLOs with general formula Li1.2+xMn0.54Ni0.13Cox-yAl0.03O2 (0.03 ≤ x ≤ 0.08 and 0.03 ≤ y ≤ 0.05), obtained from the replacement of cobalt with lithium and aluminum and we highlight how the balancing of the metal blend can lead to improvements of the Coulombic efficiency in the first cycle, a better capacity retention and reduced voltage decay. To shed light on the complex crystal-chemistry of this class of LRLOs we studied the Co-poorest member of this homologue material series, namely Li1.28Mn0.54Ni0.13Co0.02Al0.03O2, in order to prove the structural evolution occurring upon charge/discharge in lithium cell. To these aims, electrodes have been recovered during the first cycle, the second cycle and after ten cycles of charge/discharge by de-assembling lithium cells into an Ar-filled glove box. These post mortem materials have been sealed in borosilicate capillary tubes (see Fig. 1a) and studied ex situ by X-ray powder diffraction at the MCX beamline.

Read more on the Elettra website

Image: Fig. 1b shows the potential curves vs time for the first two cycles and highlights the points, marked with A, B, C and so on, where the charge or discharge step was stopped and the materials recovered for analysis. According to the diffraction data (Fig. 1c), structural alterations of Li1.28Mn0.54Ni0.13Co0.02Al0.03O2 start with a fast broadening and a shift of the peaks suggesting a smooth lattice modification. When the cell reaches 4.8V vs Li+, a second phase can be identified. In the discharge process opposite structural transformations occur.

Copper doping improves sodium-ion battery performance

Although lithium-ion batteries currently drive the electronic world, sodium-ion batteries are gaining ground. A big plus is that sodium is more earth-abundant than lithium, which lowers costs and eases environmental and supply-chain concerns. As a result, enormous research efforts are underway to improve the energy density and cycling longevity of sodium-ion batteries.

One promising strategy to enhance energy density is to exploit additional sources of a key chemical reaction—oxidation reduction (redox)—in the battery’s cathode. In cathodes made of layered transition-metal oxides (the sodium ions move in and out from between the layers), it turns out that the oxygen component in the layers unexpectedly contributes to redox activity. Unfortunately, oxygen redox is frequently accompanied by irreversible oxygen behavior, resulting in both voltage and capacity decays.

To enhance oxygen redox reversibility, researchers doped a sodium-ion cathode material (Na0.6Mg0.3Mn0.7O2, or NMMO) with copper ions (Na0.6Mg0.15Mn0.7Cu0.15O2, or NMMCO). To understand how this affects the oxygen redox activity, they used a technique developed at Beamline 8.0.1 of the Advanced Light Source (ALS), called mapping of resonant inelastic x-ray scattering (mRIXS), to measure the effect of the copper doping at different states of charge.

“The mRIXS technique is one of the most powerful characterization tools available for detecting oxygen redox activities in battery electrodes,” said Liang Zhang, a professor at Soochow University and co-corresponding author of the published work. “With mRIXS, it’s also possible to quantify the reversibility of the oxygen redox reaction, which could greatly help us understand the oxygen evolution process during electrochemical cycling.”

Read more on the ALS website

Image: The partial substitution of Mg ions in the cathode with Cu ions, which possess similar ionic radii but distinct electronic states, led to strong Cu–O bonds (i.e., modulated transition metal (TM)–O covalency), which helped stabilize the lattice during repeated cycles. Light blue = Cu, dark green = Na, red = O, dark yellow = Mn, blue = Mg