Skip to main content

The Importance of the Connection Between Quantum Physics and Thermodynamics

 

 

We know how quantum particles will behave theoretically when we reach absolute zero. We can explain this with the Bose-Einstein condensation. However, the laws of thermodynamics say that an infinite amount of energy and an infinite amount of time is required to go to absolute zero experimentally.

On top of that, a research team at TU Wien (Vienna) was able to develop a quantum version of the third law of thermodynamics, which, according to their newest research, describes absolute zero.

Although information theory and thermodynamics may seem quite different at first glance, they may be intertwined, according to the research team. In other words, if absolute zero can be reached, this can mean a perfect erasure of quantum data information. The only problem here is that going down to absolute zero does not seem technically possible for now.

According to Landauer's principle in information theory, a suitable minimum energy may be sufficient to erase one bit of information. Taking advantage of this situation, the researchers stated that there is no need for infinite energy or infinite time to go down to absolute zero, but they can do it with sufficient minimum energy and time, but a third factor, is complexity.

Marcus Huber who is one of the researchers"We found that quantum systems that allow the absolute ground state to be reached even at finite energy and in finite time can be described - none of us expected this. But these particular quantum systems have another important property: they are infinitely complex."

Also, according to the team, in order to perfectly erase quantum information in finite energy and in finite time and transfer a qubit to a completely pure ground state in the process, you would need an infinitely complex quantum computer that could theoretically control an infinite number of particles perfectly.

Stating that creating a quantum state compatible with high temperatures is important to prevent quantum states from breaking and becoming unusable for any technical use, the researchers also state that progress will be made thanks to the latest studies in these two areas.

Those who want to learn the details of the study can access the article from the link below.

Stay with physics. :)



Reference

Philip Taranto, Faraj Bakhshinezhad, Andreas Bluhm, Ralph Silva, Nicolai Friis, Maximilian P.E. Lock, Giuseppe Vitagliano, Felix C. Binder, Tiago Debarba, Emanuel Schwarzhans, Fabien Clivaz, Marcus Huber. Landauer Versus Nernst: What is the True Cost of Cooling a Quantum System? PRX Quantum, 2023; 4 (1) DOI: 10.1103/PRXQuantum.4.010332

Comments

Post a Comment

Popular posts from this blog

Bloch Sphere – Geometric Representation of Quantum State

    It is very difficult to visualize quantum states before our eyes. The Bloch sphere represents quantum state functions quite well. The Bloch sphere is named after physicist Felix Bloch. As you can see in the Bloch sphere figure below, it geometrically shows the pure states of two-level quantum mechanical systems. The poles of the Bloch sphere consist of bits |0⟩ and |1⟩. Classically, the point on the sphere indicates either 0 or 1. However, from a quantum mechanics point of view, quantum bits contain possibilities to be found on the entire surface of the sphere. Traditionally, the z-axis represents the |0⟩ qubit, and the z-axis the |1⟩ qubit. When the wave function in superposition is measured, the state function collapses to one of the two poles no matter where it is on the sphere. The probability of collapsing into either pole depends on which pole the vector representing the qubit is closest to. The angle θ that the vector makes with the z-axis determines this probabilit...

Statement of Bell's Inequality

 One of the most important applications of quantum mechanics is Bell's inequality. In 1965, John Stewart Bell actually thought that Einstein might be right and tried to prove it, but proved that quantum logic violated classical logic. It was a revolutionary discovery. Let's look at its mathematically simple explanation. To create the analogy, let's first write a classical inequality.   This inequality above is a classic expression. The quantum analogy of this expression represents the Bell inequality. With just one difference. Bell's inequality shows that the above equation is violated. Expressing Bell's inequality by skipping some complicated mathematical intermediates; While there is no such situation in the classical world that will violate the inequality we mentioned at the beginning, it is difficult to find a situation that does not violate this inequality in the quantum world. Reference https://www.youtube.com/watch?v=lMyWl6Pq904 https://slideplay...

Bernstein–Vazirani Algorithm

  Quantum computers currently available are not sufficient to solve every existing classical problem due to their own characteristics. This does not mean that they are inferior to classical computers, or that, on the contrary, quantum computers should give all kinds of advantages over classical computers. Popular quantum algorithms solved in quantum computers are algorithms created by taking advantage of the superposition and entanglement properties of particles. So, they are algorithms created to show the prominent features of quantum properties. Today I will talk about an enjoyable algorithm that demonstrates the efficiency and speed of these quantum features. Known as the Bernstein - Vazirani algorithm is a quantum algorithm invented by Ethan Bernstein and Umesh Vazirani in 1992. The purpose of this algorithm, which is a game, is to find a desired number. To put it more clearly, let's keep in mind a string of binary numbers, for example, 1011001. Next, let's write an algori...