Tunable Plasmonic Chirality Revealed by Helical Heteterostructure Metamaterials
Ufuk Kilic
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04/05/2021
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In this study, by using the glancing angle deposition technique, subsequent and repeated depositions of silicon(Si) and silver(Ag) lead to nanometer-dimension sub-chiral segments, and thus, we successfully fabricated spatially coherent, highly porous, super lattice-type helical heterostructure thin films. We theoretically and experimentally investigate the chiro-optical properties of this new type of plasmonic metamaterials via finite element modeling calculations and Mueller matrix spectroscopic ellipsometry method, respectively. The systematic changes in the morphology of helical structures by incorporating the plasmonic subsegments reveal an extra-ordinary chiro-optical response with fine spectral tunability over the entire visible spectral range into the ultra-violet.
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- [00:00:01.440]Hi I am Ufuk. I am one of PhD. Students
- [00:00:03.742]who is working under the supervision of
- [00:00:05.912]Prof. Mathias Schubert
- [00:00:07.122]and It is an honor for me to give a
- [00:00:08.948]poster presentation in the research
- [00:00:10.878]fair. The title of my talk is Tunable
- [00:00:12.840]Plasmonic Chirality Reveled
- [00:00:14.540]by Helical Heterostructure
- [00:00:15.960]Metamaterials
- [00:00:16.920]but before getting into further
- [00:00:18.480]details about my topic.
- [00:00:19.960]Let me give a brief introduction on the
- [00:00:21.887]big picture in "Our Message" Section.
- [00:00:23.756]Chirality or handedness
- [00:00:24.867]is one of the most intriguing
- [00:00:26.307]inherent properties of an
- [00:00:27.637]object which cannot be made
- [00:00:28.993]super-imposable on its mirror image by
- [00:00:31.183]simple symmetry operations.
- [00:00:32.514]In nature, however, due to
- [00:00:34.245]the large-scale mismatch between
- [00:00:35.825]the wavelength of circular polarized
- [00:00:37.692]light and the size of chiral molecules
- [00:00:39.552]or crystals a weak chiral light-matter
- [00:00:41.359]interaction results in small
- [00:00:42.739]Circular Dichroism values for
- [00:00:44.418]especially visible light range.
- [00:00:46.008]With exceptional light-manipulating
- [00:00:48.292]capabilities, artificially engineered
- [00:00:50.182]nano structures so called metametarials
- [00:00:52.527]are envisioned as
- [00:00:54.487]enhancement platform.
- [00:00:56.587]In this work, our goal is
- [00:00:57.979]to use GLAD technique,
- [00:00:59.269]in order to fabricate plasmonic helical
- [00:01:01.615]heterostructures and experimentally
- [00:01:04.227]obtain their pure chiroptical responses
- [00:01:06.337]via Mueller matrix spectroscopic
- [00:01:07.897]ellipsometry technique.
- [00:01:09.510]Additionally, we plan to perform
- [00:01:11.290]finite element simulations
- [00:01:12.940]that provide physical insights to
- [00:01:14.826]understand the presented
- [00:01:16.486]strong chiral response.
- [00:01:17.888]The picture on the left is
- [00:01:19.441]a custom built ultra-high vacuum
- [00:01:21.490]GLAD from our lab which employs
- [00:01:23.670]an electron beam evaporation technique
- [00:01:26.123]to produce particle flux which impinges
- [00:01:28.473]upon the sample substrate at oblique
- [00:01:31.766]angle of incidence and thus their
- [00:01:33.810]dynamic self-shadowing ability
- [00:01:35.852]leads us to grow various 3D
- [00:01:37.721]nano morphologies such as
- [00:01:39.555]pillar, helix, spiral, zigzags etc.
- [00:01:41.469]However, Unlike the other studies which
- [00:01:43.519]employs the GLAD to grow nano
- [00:01:45.604]structure, we proposed that during
- [00:01:47.795]the growth of nanostructure via GLAD
- [00:01:50.737]technique, altering the source material
- [00:01:53.244]from Ag to Si or vice versa, with
- [00:01:55.513]continuously rotated sample stage
- [00:01:57.691]allow for fabrication of highly ordered
- [00:01:59.807]and spatially coherent super-lattice type
- [00:02:02.307]chiral hetero-structured metamaterials.
- [00:02:04.264]Let me share the scanning electron
- [00:02:05.974]microscopy images of our fabricated
- [00:02:07.701]nano helical structures.
- [00:02:10.257]While the Top SEM images are
- [00:02:11.770]corresponding to cross section
- [00:02:14.023]and top views of all dielectric Si,
- [00:02:16.552]Bottom SEM images are corresponding to
- [00:02:18.600]the plasmonic hybrid Si-Ag
- [00:02:20.472]helical heterostructure metamaterials.
- [00:02:24.293]It is important to note that
- [00:02:26.129]the overall dimensions
- [00:02:27.726]of our fabricated structures
- [00:02:29.636]are one in a thousand of a hair thickness.
- [00:02:32.358]So we demonstrated that we can
- [00:02:34.579]successfully fabricate helical
- [00:02:36.408]heterostructures metamaterials.
- [00:02:38.518]Now, there is a need for
- [00:02:40.228]a chiro optical characterization
- [00:02:42.385]method where Mueller matrix
- [00:02:44.345]spectroscopic ellipsometry technique
- [00:02:46.225]in straight through transmission mode
- [00:02:48.055]configuration plays the key role.
- [00:02:49.756]An ellipsometer uses a light source
- [00:02:51.426]with a known polarization state
- [00:02:52.996]that interact with the sample
- [00:02:54.456]surface leads o a change in the
- [00:02:56.426]polarization state. This change
- [00:02:58.331]is recorded by the detector side
- [00:03:00.411]of the ellipsometry and stores
- [00:03:02.403]various optical properties of
- [00:03:04.338]the material of interest.
- [00:03:05.968]The optical manifestation of
- [00:03:07.738]chirality is known as Circular dichroism
- [00:03:10.231]can also be directly extracted with
- [00:03:12.371]this instrumentation and recently,
- [00:03:14.487]the chirality strength is reported
- [00:03:16.607]as the ratio of CD with total absorbance
- [00:03:20.659]which is called as dissymmetry factor
- [00:03:23.135]provides an excellent platform
- [00:03:25.064]to compare different structures.
- [00:03:28.934]Here is the spectral evolution with
- [00:03:31.879]of 4x4 Mueller matrix elements with full
- [00:03:35.482]azimuthal rotation corresponding to
- [00:03:38.426]Si helical on the left and Si-Ag helical
- [00:03:42.577]on the right. The vital information
- [00:03:45.967]here for us is stored in the
- [00:03:49.057]m_11 and m_14/m_41 elements.
- [00:03:52.309]Which are total, the differential
- [00:03:55.887]transmitted light through the films.
- [00:03:58.837]Next Let me also share our FEM modeling
- [00:04:03.003]frame work so that we can move
- [00:04:05.233]onto the results sections to show
- [00:04:07.283]the chirality performance of our
- [00:04:09.243]proposed novel helical
- [00:04:10.503]heterostructures.
- [00:04:11.503]In the FEM framework we employ
- [00:04:13.630]multiple port mechanism to excite
- [00:04:15.870]circular polarized light and detect
- [00:04:18.180]co polarized and cross polarized
- [00:04:20.360]transmitted and reflected light sources.
- [00:04:22.740]Here is the spectral evolution of
- [00:04:24.810]dissymmetry factors correspond
- [00:04:26.440]to LH and RH Si and Si-Ag
- [00:04:28.080]helical structures.
- [00:04:30.560]While Blue colored data are all dielectric
- [00:04:33.037]Si and Red colored data are
- [00:04:34.507]corresponding to the
- [00:04:35.947]plasmonic hybrid Si-Ag helical
- [00:04:37.917]heterostructure metamaterials.
- [00:04:40.465]It is apparent that the incorporation
- [00:04:42.665]of plasmonic Ag nanoparticles
- [00:04:45.035]not only enhance the chirality
- [00:04:47.115]strength but also leads
- [00:04:48.975]to the emergence of a new peak in
- [00:04:50.835]the spectra. Notably, the near
- [00:04:52.845]symmetric response of LH and RH
- [00:04:56.025]helical structures are clearly
- [00:04:57.605]demonstrating the handedness
- [00:04:59.065]effect on dissymmetry factor.
- [00:05:02.125]Here we would like to perform a
- [00:05:04.695]compressive Mueller matrix SE
- [00:05:06.725]based chiro-optical analysis to
- [00:05:09.325]unravel the tunability of the chiral
- [00:05:12.005]response possessed by
- [00:05:14.565]our novel helical structures.
- [00:05:17.095]We first studied the effect of
- [00:05:19.025]number of turns on the chirality
- [00:05:21.140]response using all-dielectric samples
- [00:05:23.620]which is summarized into the left
- [00:05:25.605]section of panel and clearly observed
- [00:05:28.175]extremely large broad band chirality.
- [00:05:31.606]Most importantly we approached
- [00:05:33.795]the maximum limit g-factor value
- [00:05:35.995]with 4 turns of Si helical structure
- [00:05:37.865]which is to the best of our knowledge
- [00:05:40.215]is the highest ever reported chirality.
- [00:05:42.445]In middle panel we incorporate
- [00:05:45.265]a single Ag subsegment per turn
- [00:05:48.465]in our helical structure and
- [00:05:50.285]we study the effect of number of turns
- [00:05:52.365]on the chiral response.
- [00:05:54.085]we observed that due to metallic losses
- [00:05:56.245]the chirality response (g-factor
- [00:05:57.825]extrema) reduces after 2 turns.
- [00:05:59.755]However, in these two systematic
- [00:06:01.295]studies (left and mid panels)
- [00:06:02.775]based on number of turns,
- [00:06:04.175]the spectral tunability was weak
- [00:06:06.165]as a function number of turns.
- [00:06:08.265]In third panel we performed
- [00:06:10.155]another systematic study
- [00:06:11.865]which employs helical structures
- [00:06:13.905]with fixed number of turns
- [00:06:15.775]but the number of Ag helical subsegments
- [00:06:18.325]is increased and hence we successfully
- [00:06:20.765]obtained spectrally tunable large
- [00:06:22.825]and broadband chiral response.
- [00:06:24.815]We wanted to perform FEM simulations
- [00:06:27.375]to obtain further insights of
- [00:06:29.385]the main driving mechanism of
- [00:06:31.445]this spectral tenability.
- [00:06:33.695]As it is seen from Figure,
- [00:06:35.325]3D color density plot of electric
- [00:06:38.115]field enhancement shows that
- [00:06:39.465]the light is extremely
- [00:06:41.075]confined at the metal-dielectric
- [00:06:43.535]interfaces which is attributed
- [00:06:45.215]to the localized surface plasmon
- [00:06:46.845]resonance effect.
- [00:06:48.915]As a complementary study,
- [00:06:50.805]we further theoretically studied
- [00:06:52.460]the influence of the rate of
- [00:06:54.200]Silver content on the dissymmetry factor
- [00:06:56.330]spectra and we observe that
- [00:06:58.150]the incorporation of further
- [00:07:00.010]Silver content will results in
- [00:07:01.910]unprecedented tunability
- [00:07:03.800]of chirality response.
- [00:07:05.306]In order to observe the asymmetric
- [00:07:07.516]behavior of changes in
- [00:07:08.896]electric and magnetic fields
- [00:07:10.606]we plotted the 2D color density plots
- [00:07:12.576]on a cut slice depicted as red hatches
- [00:07:14.846]in the schematic on the
- [00:07:21.879]left-hand side of SEM images
- [00:07:24.589]of isolated helical structures.
- [00:07:26.477]It is obvious that asymmetric
- [00:07:28.287]electric and magnetic field changes
- [00:07:30.697]are the main driving mechanism
- [00:07:32.787]of this extreme chirality for the
- [00:07:34.747]all-dielectric Si helical structures case
- [00:07:37.890]however for the case Si-Ag helical
- [00:07:40.548]structure the plasmonic resonance
- [00:07:42.848]effect also plays a fundamental role.
- [00:07:45.188]and the electric and magnetic
- [00:07:47.128]field changes
- [00:07:48.548]are having the higher values in
- [00:07:50.618]the close vicinity of Ag subsegments.
- [00:07:52.928]Last but not least we also showed
- [00:07:55.088]the color of transmitted light
- [00:07:56.938]as the matrix of three slice pie
- [00:07:58.898]chart infographic to demonstrate
- [00:08:01.098]the spectral tunability of
- [00:08:02.798]the presented helical heterostructure.
- [00:08:05.028]Here we show this matrix as a function
- [00:08:07.388]of number of Ag sub-segments and
- [00:08:09.428]the number of turns, and we observed that
- [00:08:13.091]the color is switched from deep blue
- [00:08:15.361]to light green as the number of
- [00:08:17.301]Ag subsegments is increased
- [00:08:19.171]from 0 to 10. However, when
- [00:08:21.141]we look at the transmitted light colors
- [00:08:23.141]as a function of Ag ratio-per turn
- [00:08:25.341]and the number of turns,
- [00:08:27.211]the increase in the Ag content
- [00:08:28.991]from 0 to 50 percent color is changing
- [00:08:31.061]from deep blue to pink which is also
- [00:08:33.031]key exhibition of extreme
- [00:08:34.604]spectral tunability of giant
- [00:08:36.584]chiral response revealed
- [00:08:38.674]by novel all dielectric and hybrid
- [00:08:40.954]plasmonic Si-Ag helical
- [00:08:42.454]heterostructure metamaterials.
- [00:08:44.464]In conclusion,
- [00:08:45.584]We presented GLAD based fabrication
- [00:08:47.924]technique which enables the
- [00:08:49.934]creation of new hybrid plasmonic helical
- [00:08:52.214]heterostructure metamaterials
- [00:08:53.764]with multiple turns
- [00:08:55.304]We experimentally demonstrated
- [00:08:57.404]and theoretically verified
- [00:08:59.284]Spectrally tunable
- [00:09:00.604]Extremely large Broadband
- [00:09:02.354]chiroptical response by
- [00:09:03.664]nanohelical metamaterials.
- [00:09:04.954]The reported new designs of
- [00:09:06.364]all dielectric and dielectric-metallic
- [00:09:08.554]plasmonic metamaterials permit
- [00:09:10.714]one of the largest and broadest ever
- [00:09:12.694]measured chiral dissymmetry factor
- [00:09:14.824]achieved by a large scale
- [00:09:16.114]nanophotonic structure
- [00:09:17.425]The strong circular dichroism of the
- [00:09:19.695]presented bottom-up fabricated
- [00:09:21.285]optical metamaterials can be
- [00:09:23.035]tuned by varying their dimensions
- [00:09:25.135]and proportions between their dielectric
- [00:09:27.415]and plasmonic helical subsections
- [00:09:29.425]The currently demonstrated
- [00:09:30.985]ultrathin optical metamaterials
- [00:09:32.905]are expected to provide
- [00:09:34.375]a substantial
- [00:09:35.375]boost to the developing field of
- [00:09:37.375]chiroptics biological and quantum
- [00:09:41.669]sensing fields.
- [00:09:42.989]Here are Acknowledgements
- [00:09:44.829]and Thank you very much for attention.
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