“…Throughout the years, massive efforts have been directed towards improving detection limits by achieving long interaction pathlengths. Prominent examples include the use of conventional multipass gas cells [1][2][3][4], sophisticated high-finesse cavities [5][6][7][8], gas-filled holey fibers [9][10][11], integrating spheres [12][13][14], and diffusive reflectors [15,16]. Despite this rich flora of approaches, there is a continuous struggle to reduce size, gas volume, cost and alignment complexity.…”