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Tin doping in Pb_1-xSn_xTaSe2: A New Take on Superconductivity

Examining how tin enhances superconductivity in Pb_1-xSn_xTaSe2 amid challenges.

K. Kumarasinghe, A. Rahman, M. Tomlinson, Y. Nakajima

― 7 min read


Tin Doping in Tin Doping in Superconductors Pb_1-xSn_xTaSe2 superconductivity. Investigating the effects of tin on
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Superconductors are like the superheroes of the material world. They can carry electricity without losing energy, making them incredibly useful for technology and science. They also have a special ability to repel magnetic fields. In this world, we recently looked at a special kind of superconductor called Pb_1-xSn_xTaSe2, which is made up of lead, tin, tantalum, and selenium. By adding tin to this mix, we can change how the material behaves, especially when it gets really cold.

What Happens When You Add Tin?

When we add a little tin (Sn) to our lead-based superconductor, something amazing happens: the temperature at which it becomes superconductive goes up to 5.1 K. That’s like getting a promotion in the world of superconductors! But hold on, there’s a catch. This tin addition also causes a lot of disorder in the material. Think of it like adding too many toppings to your pizza; it may be tasty, but it could also get a bit messy.

Specific Heat and Superconductivity

Now, let’s talk about something called specific heat. It tells us how much heat a material can hold. When we look at our tin-doped superconductor, its specific heat jump goes above a certain number (1.43) that we expect based on old theories. This means it’s showing off its strong-coupling superhero abilities, much like a superhero who only reveals their true powers at the last moment.

But when we add even more tin, the specific heat jump drops below this expected number. It’s like the superpower is taking a nap! This strange behavior can’t be explained by the regular single-gap model of superconductivity; it seems that our superconductor has two different types of conduction happening at once, like a superhero with two distinct powers.

The Role of Fermi Pockets

So, what’s the deal with these mysterious "Fermi pockets"? As we add tin, they appear in the material’s structure. Imagine them as secret hideouts for electrons, causing a change in how they interact with each other. The presence of these pockets enhances the odds of electrons teaming up to achieve superconductivity, despite the confusion from all the disorder that the tin brings. It’s kind of like how a great team can still win the game, even when things get hectic.

Noncentrosymmetric Superconductors

These superconductors are not your ordinary ones; they lack a certain symmetry, which opens up unusual properties. Noncentrosymmetric superconductors can mix different pairing types for electrons, making them even more fascinating. In our journey, we find that noncentrosymmetric superconductors can host something called Majorana states, which are like elusive particles that scientists are eager to study.

Examining Superconductivity Under Different Conditions

We examined our tin-doped superconductor using various experimental techniques, such as resistivity and specific heat measurements. These tests help us see how the material behaves at different temperatures and conditions. And guess what? The resistivity shows metallic characteristics at low temperatures, which is exactly what we want.

We used special equipment to ensure our samples were pure and unadulterated. The results of our tests showed that adding tin significantly impacts the superconducting properties of our material. It’s like discovering that a sidekick can sometimes outshine the hero!

Temperature and Resistivity Results

As we looked at how resistivity changes with temperature, we noticed that superconductivity kicks in at a certain point. When we plotted this temperature against the amount of tin, we saw a pattern. At first, adding tin caused the superconducting temperature to go up, which is fantastic news. But then, there’s a bit of a roller coaster where the rise levels off. It's like winning the jackpot and then finding out there are taxes involved!

When we measured how tin changes the specific heat at different temperatures, we found that the results vary quite a bit. For lower levels of tin, the specific heat jump is impressive, but as we add more tin, we can see it beginning to fall off, despite that strong-coupling superhero ability.

Disorder and Superconductivity: A Balancing Act

Here’s the funny thing about superconductors: while we often think of disorder as the enemy, in this case, our superconductor seems to handle it quite well! It’s as if adding tin makes the superhero more resilient to challenges. Even with a significant increase in disorder, superconductivity remains strong.

The Curious Case of the Debye Temperature

The Debye temperature is another important player in our story. It’s related to how quickly phonons (which are like sound waves in a solid) can travel through a material. Surprisingly, we found that the Debye temperature increases a bit with tin. However, the increase isn't enough to fully account for all the stirring excitement about the enhancements we're seeing in superconductivity.

This alludes to the fact that there’s likely more going on beneath the surface. It appears that the electron-phonon coupling strength may also be affected in ways we didn't fully expect.

Specific Heat Measurements and the Two-Gap Model

When we examined the specific heat in more detail, the results led us to believe that something more complex than a single-gap superconducting state was at play. We introduced the two-gap model, which seems to provide a better explanation for our findings. This model highlights that there are different contributions to the superconductivity based on the electronic structure of the material.

As we dug deeper into the specifics, we found the superconducting gap amplitudes changing with the level of tin doping. The behavior of the specific heat jumps matched our theoretical calculations from the two-gap model, strongly suggesting that the Sn doping creates complex interactions that enhance the superconducting state.

The Battle of the Models: Single-Gap vs. Two-Gap

As we continued our research, we realized that our original single-gap model wasn’t cutting it. It simply could not explain the peculiar behavior we observed in the doped samples. That’s when we turned to the two-gap model and found it to be far more successful in describing the specific heat jumps we measured.

In essence, it seems like our tin-doped superconductor is involved in a bit of a duel. The two-gap model fits our observations, whereas the single-gap model struggles to keep up. It's like watching a classic battle between old traditions and new innovations!

The Multiband Effect

Let’s not forget the multiband effect that came into play with the Sn doping. We suspect that this effect is the real game-changer in our superconductor. The idea is that as we add tin, new electronic states become available, which allows for enhanced electron-phonon interactions.

These interactions are crucial because they help facilitate the pairing of electrons, which is essential for superconductivity to occur. So, while adding tin creates chaos, it also opens up new avenues for enhancing superconductive abilities.

Resilience Against Disorder

What’s remarkable is that despite the significant increase in disorder due to tin doping, superconductivity remains strong. This goes against the grain of how we usually think about disorder adversely affecting superconductors. Instead, our findings indicate that Pb_1-xSn_xTaSe2 is resilient in the face of disorder. It’s like our superconductor just put on a pair of glasses and decided to keep going!

Why This Matters

Understanding how tin impacts the superconductivity of this material not only helps us learn about this specific compound but could also have broader implications for how we approach superconductors in general. If we can figure out how to harness these effects, we could develop better materials for everything from quantum computing to better power transmission systems.

Final Thoughts

In summary, our exploration of the Pb_1-xSn_xTaSe2 superconductor has revealed a complex interplay of factors that influence its superconducting abilities. We’ve seen how adding tin can enhance its temperature transition, how disorder plays a surprisingly supportive role, and how the two-gap model offers a better explanation for our findings.

As we keep digging into the world of superconductors, we’re left with the exciting potential that new materials and doping strategies might lead to even more incredible superconducting properties in the future. So, stay tuned because the next chapter in superconductor research is just around the corner, and it might just be as thrilling as a superhero movie!

Original Source

Title: Enhancement of the superconducting transition temperature due to multiband effect in the topological nodal-line semimetal Pb$_{1-x}$Sn$_{x}$TaSe$_{2}$

Abstract: We report a systematic study of the normal-state and superconducting properties of single crystal Pb$_{1-x}$Sn$_{x}$TaSe$_{2}$ $(0\leq x \leq 0.23)$. Sn doping enhances the superconducting temperature $T_{c}$ up to 5.1 K, while also significantly increasing impurity scattering in the crystals. For $x=0$, the specific heat jump at $T_{c}$ exceeds the Bardeen-Cooper-Schrieffer (BCS) weak-coupling value of 1.43, indicating the realization of strong-coupling superconductivity in PbTaSe$_{2}$. In contrast, substituting Pb with Sn lowers the specific heat jump at $T_{c}$ below the BSC value of 1.43, which cannot be explained by a single-gap model. Rather, the observed specific heat of Sn-doped PbTaSe$_{2}$ is reproduced by a two-gap model. Our observations suggest that additional Fermi pockets appear due to a reduction of the spin-orbit gap with Sn doping, and the multiband effect arising from these emergent Fermi pockets enhances the effective electron-phonon coupling strength, leading to the increase in $T_{c}$.

Authors: K. Kumarasinghe, A. Rahman, M. Tomlinson, Y. Nakajima

Last Update: 2024-11-29 00:00:00

Language: English

Source URL: https://arxiv.org/abs/2411.19932

Source PDF: https://arxiv.org/pdf/2411.19932

Licence: https://creativecommons.org/licenses/by/4.0/

Changes: This summary was created with assistance from AI and may have inaccuracies. For accurate information, please refer to the original source documents linked here.

Thank you to arxiv for use of its open access interoperability.

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