Towards Stirling engine using an optically confined particle subjected to asymmetric temperature profile

• Published in: arXiv.org
• Main Authors: Nalupurackal, Gokul, Muruga Lokesh, Sarangi Suresh, Srestha Roy, Chakraborty, Snigdhadev, Goswami, Jayesh, Pal, Arnab, Roy, Basudev
• Format: Paper Journal Article
• Language: English
• Published: Ithaca Cornell University Library, arXiv.org 27.06.2023
• Subjects: Absorptivity; Asymmetry; Heat engines; Physics - Chemical Physics; Physics - Optics; Physics - Soft Condensed Matter; Physics - Statistical Mechanics; Stiffness; Stirling engines; Temperature profiles
• ISSN: 2331-8422
• DOI: 10.48550/arxiv.2306.15236

The realization of microscopic heat engines has gained a surge of research interest in statistical physics, soft matter, and biological physics. A typical microscopic heat engine employs a colloidal particle trapped in a confining potential, which is modulated in time to mimic the cycle operations. Here, we use a lanthanide-doped upconverting particle (UCP) suspended in a passive aqueous bath, which is highly absorptive at 975 nm and converts NIR photons to visible, as the working substance of the engine. When a single UCP is optically trapped with a 975 nm laser, it behaves like an active particle by executing motion subjected to an asymmetric temperature profile along the direction of propagation of the laser. The strong absorption of 975 nm light by the particle introduces a temperature gradient and results in significant thermophoretic diffusion along the temperature gradient. However, the activity of the particle vanishes when the trapping wavelength is switched to 1064 nm. We carefully regulate the wavelength-dependent activity of the particle to engineer all four cycles of a Stirling engine by using a combination of 1064 nm and 975 nm wavelengths. Since the motion of the particle is stochastic, the work done on the particle due to the stiffness modulation per cycle is random. We provide statistical estimation for this work averaged over 5 cycles which can be extended towards several cycles to make a Stirling engine. Our experiment proposes a robust set-up to systematically harness temperature which is a crucial factor behind building microscopic engines.