Phase singularities are locations where light is twisted like a corkscrew, with positive or negative topological charge, depending on the twisting direction. Among the multitude of singularities arising in random wave fields, some of them can be found at the same location, but only when they exhibit opposite topological charge, which results in their mutual annihilation. New pairs can be created as well. With near-field experiments supported by theory and numerical simulations we study persistence and pairing statistics of phase singularities in random optical fields as a function of the excitation wavelength. We demonstrate how such entities can encrypt fundamental properties of the random fields in which they arise.A wide variety of physical systems exhibit vortices: locations around which an observable rotates while being undetermined in the middle [1][2][3][4][5][6][7][8][9]. It is exceptionally fascinating when the properties and evolution of such singular entities can comprehensively describe complex phenomena such as the Kosterlitz-Thouless transition [10]. But vortices are not a peculiarity of superconductors: light's phase swirls around optical vortices, where it is singular [11]. A multitude of these phase singularities arises in random optical fields, one half swirling in opposite direction to the other, so that they can approach respectively to an arbitrarily small distance [12][13][14][15][16]. It is by letting them move that one can observe creation and/or annihilation of such pairs [17][18][19][20][21][22].With near-field experiments we track phase singularities in a random optical field from birth to death. We map the singularities' trajectories at varying the excitation wavelength, and quantitatively determine properties such as their persistence in the field and the correspondence between creation and annihilation partner of a singularity, known as lifelong fidelity [23]. We observe two populations of singularities, neatly differentiated by their typical persistence in the varying wave field: short-lived pairs that are predominantly faithful to their creation partner, and a more promiscuous population.To generate optical random waves we couple monochromatic light (λ 0 ∼ 1550 nm) into a photonic crystal chaotic cavity realized in a silicon-on-insulator platform (Fig. 1a) [24]. We map the optical field inside the cavity with near-field microscopy, resolving amplitude, phase and polarization of such in-plane complex electric field (E x , E y ) [25][26][27]. Figure 1 presents a typical example of our measurements of amplitude and phase of E x . The optical field inside the cavity can be thought of as a random superposition of light waves [28] with transverse electric (TE) polarization [15]. Only the behavior of E x is presented here, without loss of generality as it is representative of the behavior of all in-plane field components [15]. Figure 1b represents a full-size measurement: a square map 17 µm × 17 µm with a pixel size of about 17 nm. In this map we distinguish a multitude of dark and brigh...