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Perfect Chirality with imperfect polarisation
Optics · Submitted 24 Sep 2021
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim However, there is no need to restrict engineered systems to circular dipoles and with an appropriate choice of dipole unidirectional emission is possible for any elliptical polarization.
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The abstract, sentence by sentence
Unidirectional (chiral) emission of light from a circular dipole emitter into a waveguide is only possible at points of perfect circular polarisation (C points), with elliptical polarisations yielding a lower directional contrast. However, there is no need to restrict engineered systems to circular dipoles and with an appropriate choice of dipole unidirectional emission is possible for any elliptical polarization. Using elliptical dipoles, rather than circular, typically increases the size of the area suitable for chiral interactions (in an exemplary mode by a factor $\sim 30$), while simultaneously increasing coupling efficiencies. We propose illustrative schemes to engineer the necessary elliptical transitions in both atomic systems and quantum dots.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Unidirectional (chiral) emission of light from a circular dipole emitter into a waveguide is only possible at points of perfect circular polarisation (C points), with elliptical polarisations yielding a lower directional contrast. | background 1.00 | 0.11 | 0.09 | asserted 0.98 |
| s1 | However, there is no need to restrict engineered systems to circular dipoles and with an appropriate choice of dipole unidirectional emission is possible for any elliptical polarization. | contribution 0.47 | 0.36 | 0.68 | asserted 0.60 |
| s2 | Using elliptical dipoles, rather than circular, typically increases the size of the area suitable for chiral interactions (in an exemplary mode by a factor $\sim 30$), while simultaneously increasing coupling efficiencies. | result 0.93 | 0.60 | 0.34 | asserted 0.87 |
| s3 | We propose illustrative schemes to engineer the necessary elliptical transitions in both atomic systems and quantum dots. | contribution 0.90 | 0.62 | 0.07 | hedged possibility 0.46 |
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Original abstract
Unidirectional (chiral) emission of light from a circular dipole emitter into a waveguide is only possible at points of perfect circular polarisation (C points), with elliptical polarisations yielding a lower directional contrast. However, there is no need to restrict engineered systems to circular dipoles and with an appropriate choice of dipole unidirectional emission is possible for any elliptical polarization. Using elliptical dipoles, rather than circular, typically increases the size of the area suitable for chiral interactions (in an exemplary mode by a factor $\sim 30$), while simultaneously increasing coupling efficiencies. We propose illustrative schemes to engineer the necessary elliptical transitions in both atomic systems and quantum dots.
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More generally, many interesting effects have been predicted in theoretical frameworks where particular forward/backward emission rates are assumed [ref] , rather than specifying the dipoles/polarisations that determine these rates.
Quantum memory and gates using a Lambda-type quantum emitter coupled to a chiral waveguide · Introduction · 0.89
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