They were talking about places to run and bike, and he told her where he lived and what his jogging route was, and she said that her bike had been stolen from the basement of her building, and when he asked her where she lived she told him, more or less nonchalantly, and he drank his diet soda and looked out the window, or into it, perhaps, at their faint reflections paired on the glass.
The end result is a fragmented reality of mirrored reflections paired with the continuous loop of yourself in the crowd projected onto the clothing, which you then want to record as a selfie.
And "Circle" was an elegant success, its drifting melody seamlessly paired with a reflection on romantic continuity.
Each country is paired with a reflection on a single strategy, from punishment to its alternatives: South Africa's is truth and reconciliation; Brazil's is solitary confinement; Uganda's and Jamaica's are arts education.
Rabinow's technique of report and reflection in paired volumes, of course, was set with his first two books, an ethnographic monograph and the recently-reissued Reflections on Fieldwork in Morocco (2007).
The relabelling serves to map each landmark to the corresponding one after the transformation: for the reflection, each paired landmark is mapped to its equivalent on the opposite side and each median landmark is mapped to itself (for the identity, every landmark is mapped to itself).
For reflection, there are paired and unpaired landmarks.
Differences between the observed intensities of Friedel pairs of reflections can be modelled following equation (1) with where.
Differences and quotients can be defined using Friedel pairs of reflections and applied in refinement to enable absolute structure to be determined precisely even for light atom crystal structures.
The ability to achieve a low standard uncertainty for the Flack parameter depends in part on the resonant scattering effects having sufficient magnitude to lead to measurably different intensities for Friedel pairs of reflections with indices h and.
As in the case of hf = hm = 0, each cell is symmetrical in reflecting over both the midpoint of the x-axis, s 1 f = (1 − h f ) / 2, and that of the y-axis, s 1 m = (1 − h m ) / 2. The limiting variance is symmetrical with respect to source population (Equation 54), and this pair of reflections corresponds to an exchange of source populations.
