Abstract:The optical path lengths travelled by rays across a wavefront essentially determine the resulting phase front irrespective of the shape of a medium according to the principle of equal optical path. Thereupon we propose a method for the transformation between two arbitrary wavefronts by a slab, i.e. the profile of the spatial separation between the two wavefronts is taken to be transformed to a plane surface. Interestingly, for the mutual conversion between planar and curved wavefronts, the method reduce to an … Show more
“…As such, the virtual space ′ ′ OB C D is transformed into the physical one ′ ′ OA E D, resulting in a design with an irregular shape. To obtain a planar device, we have proposed an indirect transformation method (ITM) based on the principle of equal optical path length [22,23]: the profile of the spatial separation between the original and desired wavefronts is converted to a plane surface, i.e. from AE to BC, as shown in Fig.…”
Section: A General Pt Methods For the Conversion Between Two Arbitrarymentioning
confidence: 99%
“…This method does not depend on the symmetry of the PT. We follow the principle of equal optical path length [22,38] to attain a flat configuration and adopt a nonlinear CT to ensure the impedance match.…”
Section: Methods Of Pt By An Impedance-matched Nonmagnetic Slabmentioning
confidence: 99%
“…It is worth pointing out that this slab is also able to deflect an incident plane wave into a curved wave with a curvature radius −R i . This means that the phase transformer has a two-fold function common to phase devices [22,39,40]. The two functions are demonstrated in Fig.…”
Section: Application To Designing Deflector and Polarization Splittermentioning
confidence: 98%
“…Meanwhile, researchers applied TO in order to manipulate the phase to create phase transformers [18][19][20][21]. On this topic we have proposed a method of phase transformation (PT) between any two wavefronts through a compact slab [22,23]. Applying this method, the device configuration remains flat irrespective of its function.…”
Section: Introductionmentioning
confidence: 98%
“…We follow the method in Refs. [22,23] but adopt a nonlinear CT to ensure impedance matching, use a quasi-conformal CT to simplify the material parameters [35,37], and keep the dispersion relation unchanged to allow the device to become nonmagnetic [6,25]. Applying this method, a phase transformer is designed such that the wave shape and propagation direction can be changed.…”
“…As such, the virtual space ′ ′ OB C D is transformed into the physical one ′ ′ OA E D, resulting in a design with an irregular shape. To obtain a planar device, we have proposed an indirect transformation method (ITM) based on the principle of equal optical path length [22,23]: the profile of the spatial separation between the original and desired wavefronts is converted to a plane surface, i.e. from AE to BC, as shown in Fig.…”
Section: A General Pt Methods For the Conversion Between Two Arbitrarymentioning
confidence: 99%
“…This method does not depend on the symmetry of the PT. We follow the principle of equal optical path length [22,38] to attain a flat configuration and adopt a nonlinear CT to ensure the impedance match.…”
Section: Methods Of Pt By An Impedance-matched Nonmagnetic Slabmentioning
confidence: 99%
“…It is worth pointing out that this slab is also able to deflect an incident plane wave into a curved wave with a curvature radius −R i . This means that the phase transformer has a two-fold function common to phase devices [22,39,40]. The two functions are demonstrated in Fig.…”
Section: Application To Designing Deflector and Polarization Splittermentioning
confidence: 98%
“…Meanwhile, researchers applied TO in order to manipulate the phase to create phase transformers [18][19][20][21]. On this topic we have proposed a method of phase transformation (PT) between any two wavefronts through a compact slab [22,23]. Applying this method, the device configuration remains flat irrespective of its function.…”
Section: Introductionmentioning
confidence: 98%
“…We follow the method in Refs. [22,23] but adopt a nonlinear CT to ensure impedance matching, use a quasi-conformal CT to simplify the material parameters [35,37], and keep the dispersion relation unchanged to allow the device to become nonmagnetic [6,25]. Applying this method, a phase transformer is designed such that the wave shape and propagation direction can be changed.…”
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