We demonstrate passive mode-locking and single pulse generation in a fibre laser with a record-setting cavity length of 25 km. Substantial increase in the pulse round trip duration leads to ultra-low repetition rate of 8.097 kHz and the pulse energy of 3.7 µJ.PACS numbers: 42.55. Wd, 42.60.Fc, 42.60.Da, 42.60.By Nowadays, lasers have become ubiquitous devices equally important in fundamental science, engineering technologies and in a range of practical applications. In the last decade there has been a revolutionary progress in laser science fuelled by advances in high-power systems, ultra-short pulse lasers and oscillators with high pulse energy. The progress was driven by a variety of new important applications that these advanced laser systems can open-up. This expansion has been facilitated by continuous advances in material science, achievements in technology and by the improvement in our understanding of the fundamental laser principles and physical effects underlying the operation and performance of new types of lasers. In particular, laser designs based on new physical concepts offer opportunities for creating systems with non-incremental changes of performance characteristics leading to disruptive progress. In this work we outline a new direction in development of pulsed lasers, by demonstrating a dramatic increase of the cavity length for modelocking fibre lasers to a record 25 km which corresponds to the cavity optical length of 37.05 km. Our result provides insight in design possibilities which may allow for non-incremental progress in laser technology by pulse energy up-scaling using very long cavities.The length of the resonator is, indeed, an important design parameter in mode-locked laser being responsible for repetition rate of generated pulses and their per-pulse energy. Higher per-pulse energy p E of the output in mode-locked lasers (at the same average power ave P of radiation) may be achieved by direct extension of the laser cavity, since(c is the speed of light, n-refractive index) -pulse energy is directly proportional to cavity length L and round trip time R T , while the repetition rate is inversely proportional to the resonator length. For a range of laser applications in material processing a high pulse energy or respectively high peak intensity is required. Different techniques such as Q-switching, cavity dumping and optical amplification are currently used to generate high energy pulses. One of the important physical and technical challenges in laser science is to achieve high pulse energy in mode-locked lasers to provide tools for a variety of applications ranging from material processing to advanced bio-medical imaging. Compared to Q-switching and cavity dumping techniques, mode-locked lasers allow a post-compression of output pulses, making possible generation of ultrashort optical pulses with high energy.Drastic increase of the laser cavity can be implemented using a fibre waveguide. In the case of CW fibre lasers, it has been recently demonstrated that resolvable reso...