“…The decelerated molecules are in the weak-field seeking |j, k, m, = |1, 1, 1, u quantum state, where j is the total angular momentum, k and m are respectively the projections of j onto the axis of symmetry and the laboratory field axis, and u denotes that the molecules are in the weak-field seeking upper state of the inversion doublet [38]. The slowed molecules, with a mean forward speed of approximately 26 m/s, exit the decelerator and are loaded into the electrostatic trap by removing the remainder of their forward kinetic energy using the trap electrodes as the final few stages of deceleration [39,40]. Once the molecules are brought to rest, the electrostatic trap is created by applying (typically) {+8,-8,-8,+8} kV to the electrodes, as listed from the closest to farthest position in relation to the Stark decelerator.…”