We study Josephson junctions based on inversion-asymmetric but time-reversal symmetric Weyl semimetals under the influence of Zeeman fields. We find that, due to distinct spin textures, the Weyl nodes of opposite chirality respond differently to an external magnetic field. Remarkably, a Zeeman field perpendicular to the junction direction results in a phase shift of opposite sign in the current-phase relations of opposite chirality. This leads to a finite chirality Josephson current (CJC) even in the absence of a phase difference across the junction. This feature could allow for applications in chiralitytronics. In the long junction and zero temperature limit, the CJC embodies a novel quantum anomaly of Goldstone bosons at π phase difference which is associated with a Z2 symmetry at low energies. It can be detected experimentally via an anomalous Fraunhofer pattern.Introduction.-Weyl semimetals (WSMs) have recently attracted intensive interest thanks to their realization in a number of materials [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16] and to their novel physics associated with Weyl nodes [17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33]. The Weyl nodes appear in pairs that carry opposite chirality [34] in the absence of time-reversal or inversion symmetry. Chirality is thus a defining emergent property of electrons in WSMs. The possibility to probe and manipulate chirality is one of the most intriguing aspects of WSMs. Recently, chirality-dependent physics has been discussed in various contexts [35][36][37].Josephson junctions provide a complementary method to probe the electronic properties of a particular material. They are the basic building blocks for superconducting electronics with applications ranging from electronic magnetometers to quantum computation [38][39][40][41]. Hence, it is of fundamental interest to study Josephson junctions based on WSMs. To date, most experimentally relevant WSMs preserve time-reversal symmetry but break inversion symmetry [5][6][7][8][9][10][11][12][13][14][15][16]. In these materials, s-wave superconductivity couples electrons of the same chirality [42,43]. Thus, chirality remains a well-defined property in those Josephson junctions. Hence, we could think about using chirality as a resource for electronics, just as spin in spintronics. We coin this idea chiralitytronics. Recently, Josephson junctions based on Dirac semimetals have been fabricated [44][45][46]. By similar methods, it is feasible to also investigate Josephson junctions based on WSMs. Previous theoretical work [47][48][49][50][51] instead focused on either the inversion-symmetric case or the surface states where chirality is no longer a good quantum number [42,52].In this Letter, we focus on Josephson junctions to study the interplay of Zeeman fields, s-wave superconductivity, and chirality in inversion-asymmetric WSMs. We find that the Weyl nodes of opposite chirality display distinct spin textures. Thus, they respond differently to an external magnetic field. As a result, a ...