{'fraction_non_alphanumeric': 0.03735144312393888, 'fraction_numerical': 0.01867572156196944, 'mean_word_length': 5.555555555555555, 'pattern_counts': {'":': 0, '<': 0, '<?xml version=': 0, '>': 0, 'https://': 0, 'lorem ipsum': 0, 'www.': 0, 'xml': 0}, 'pii_count': 0, 'substrings_counts': 0, 'word_list_counts': {'cursed_substrings.json': 0, 'profanity_word_list.json': 0, 'sexual_word_list.json': 0, 'zh_pornsignals.json': 0}}
Trails of Mobile Majoranas in an Iron Chalcogenide?

The iron chalcogenide FeTe1−xSex has become a promising platform for the realization of localized Majorana zero modes (see previous commentaries [1, 2]). This material hosts bulk nodeless superconductivity [3], and surface states similar to those of 3D topological insulators [4, 5]. These traits actually imbue this material with even greater potentials. The two recommended papers report experimental evidence that FeTe1−xSex might also host dispersing 1D helical Majorana fermions on certain domain walls [6] or hinge structures [7].