Bachelors Topic

PORTFOLIO · RESEARCH

BACHELOR TOPIC

Development of Metamaterial Absorber

OPTICAL METAMATERIALS · BACHELOR THESIS · ICEEE 2026

TUNABLE MULTI-FREQUENCY
OPTICAL METAMATERIAL
ABSORBER.

A geometrically scalable double split ring resonator absorber engineered for predictable multi-frequency optical absorption through controlled resonator scaling.

423 THz518 THz640 THz831 THzFDTD · CST≈100% ABSORPTION
DSRR
OPTICAL METAMATERIAL · LIVE SPECTRAL SCENEDSRR / Ag · SiO₂ · Ag
MULTI-FREQUENCY ABSORBER

Geometry becomes
light control.

Four scaled resonators. Four designed optical bands. Watch the unit cell respond as the selected resonance moves from 423 to 831 THz.

≈100%PEAK ABSORPTION
DESIGNED RESONANCES
4 RESONANCES423–831 THz3-LAYER ABSORBER
01
THE RESEARCH IDEA

Control the optical response through geometry.

The proposed absorber uses a DSRR printed above a dielectric spacer and continuous silver ground plane. The ground suppresses transmission, while the split-ring geometry produces LC resonances and confines electromagnetic energy. Instead of rebuilding the topology for every operating point, the resonator dimensions are systematically scaled to tune the response.

The study reports designed resonances at 423, 518, 640 and 831 THz, with absorption approaching unity at the target resonances.

Ag DSRR patterned resonatorSiO₂ 60 nm spacerAg GROUND 40 nm reflector
02
INTERACTIVE DSRR LAB

Scale the resonator. Move the resonance.

Select one of the four designs to see the actual dimensions reported in the thesis. The live model rescales the concentric DSRR geometry and animates incident optical energy toward the absorber.

423 THz DESIGNW 288 nm · r₁ 128 nm · r₂ 80 nm · w₁ 16 nm · g₁/s/t 32 nm
FDTD · NORMAL INCIDENCE423 THz
x
y
W · 288 nm
SPLIT GAPAg
SiO₂ · 60 nm
Ag GROUND · 40 nm
50 nm
GEOMETRIC SCALE MODEL · OPTICAL ABSORBER UNIT CELL
03
GEOMETRICAL SCALING

The dimensions behind four optical bands.

The spacer and ground thicknesses remain fixed while the lateral DSRR geometry is scaled. The 831 THz case keeps W at 288 nm while using the smaller ring dimensions reported for the high-frequency design.

Parameter423 THz518 THz640 THz831 THz
W (nm)288230.4180288
r₁ (nm)128102.48080
r₂ (nm)80645050
w₁ (nm)1612.81010
g₁ (nm)3225.62020
s (nm)3225.62020
t (nm)3225.62020
tₛ (nm)60606060
tᵍ (nm)40404040
Lateral geometry scalesSiO₂ spacer fixed · 60 nmAg ground fixed · 40 nm
04
S-PARAMETERS · ABSORPTIVITY

Four resonances. Near-unity absorption.

The simulated S-parameters verify the four designed optical operating points. With the continuous silver ground suppressing transmission, the absorber response is governed primarily by reflection: A = 1 − |S₁₁|² − |S₂₁|².

423 THz S-parameters
423 THzLow-frequency design
518 THz S-parameters
518 THzScaled DSRR response
640 THz S-parameters
640 THzHigh-frequency response
831 THz S-parameters
831 THzHighest designed resonance
ABSORPTIVITYA(ω) = 1 − |S₁₁|² − |S₂₁|²Continuous Ag ground → transmission approaches zero at the designed resonances.
05
SURFACE CURRENT

Seeing the resonance mechanism.

Surface-current concentration around the split rings reveals the resonant behavior and higher-order modes produced by coupling between the inner and outer resonators.

Surface current at 423 THz
423 THzFundamental response
Surface current near 618 THz
≈618 THzHigher-order mode
Surface current at 767 THz
767 THzHigher-order mode
06
PHYSICAL INTERPRETATION

Why the DSRR absorbs optical energy.

The response is produced by the interaction of the patterned silver resonator, dielectric spacer and metallic ground. At resonance, the split rings concentrate electric fields and drive strong surface currents, while the grounded stack suppresses transmission and enables impedance matching to free space.

E

Field localization

The ring gaps behave as strongly capacitive regions, concentrating the incident electric field around the discontinuities.

J

Resonant currents

Coupled currents circulate around the inner and outer silver rings, creating the resonant electromagnetic response seen in the surface-current maps.

Z

Impedance matching

At the designed resonance, the effective absorber impedance approaches free-space impedance, minimizing reflected optical power.

A

Energy absorption

The continuous Ag ground makes transmission negligible; when reflection is simultaneously minimized, incident energy is trapped and dissipated in the structure.

T ≈ 0  →  A ≈ 1 − |S₁₁|²Ground-backed absorber at resonance
07
FROM BLACKBODY SPECTRUM TO UAV ENERGY

Absorb. Control. Harvest. Power the flight.

The broader research direction is to use engineered optical absorption as the front end of an energy-harvesting architecture. Tunable metamaterial resonances can target selected portions of thermal radiation, providing a path toward concentrating useful absorbed energy and delivering it to a conversion stage for wireless UAV charging concepts.

≈λ
Blackbody radiationBroad thermal spectrum incident on the receiving structure.
DSRR
Spectral selectionGeometry places resonances at selected optical frequencies.
A→1
Near-unity absorptionReflection is reduced while the ground suppresses transmission.
⇢
Energy routingAbsorbed energy becomes the input to the harvesting / conversion stage.
UAV
Wireless charging goalResearch vision: support UAV energy delivery without landing.

Multi-band optical receiver

The four designed resonances demonstrate how a common DSRR topology can be geometrically tuned across a wide optical range.

In-flight charging concept

The absorber is the electromagnetic front end; practical charging additionally requires energy conversion, power conditioning, beam/routing architecture and system-level efficiency engineering.

ENERGY DELIVERY · CONCEPT
08
RESEARCH → APPLICATION

From optical resonance to an energy-delivery architecture.

The absorber is the electromagnetic front end of a larger system. The research path begins with spectral capture, then moves through conversion and power conditioning before energy can be delivered to an airborne platform.

01CAPTUREBlackbody spectrum

Broadband optical energy reaches the engineered receiving surface.

02SELECTDSRR resonance

Scaled split-ring geometry selects designed bands from 423 to 831 THz.

03ABSORBA → 1

Ground-backed resonance suppresses transmission and minimizes reflection.

04CONVERTPower stage

Captured electromagnetic energy must be converted and conditioned for useful delivery.

05DELIVERUAV in flight

The system-level vision is energy delivery to an airborne platform without landing.

RESEARCH VISIONENGINEER THE SPECTRUM → CAPTURE THE ENERGY → POWER THE FLIGHT
09
ICEEE 2026 · ANTALYA, TÜRKİYE
27—29 APRIL · 2026
IEEE Turkey SectionIEEE CO-SPONSORED RESEARCH MILESTONE

The thesis moved from simulation to the international research stage.

My bachelor-thesis work on the development of a tunable multi-frequency optical metamaterial absorber was presented in Antalya during the 13th International Conference on Electrical and Electronics Engineering.

BACHELOR THESIS SUPERVISIONProf. Abdelmegid AllamGerman University in Cairo
13THICEEE2026
ANTALYATÜRKİYE
CONFERENCE13th ICEEE 2026
LOCATIONAntalya, Türkiye
DATESApril 27–29, 2026
RESEARCHOptical Metamaterial Absorber
CONFERENCE STORY · PRESENTATION · CERTIFICATE · PAPER → next archive section
10
WIDEBAND EVOLUTION · COUPLED DSRRs

Four resonators.
One engineered window.

The broadband stage is not four cards. It is one electromagnetic system: scaled DSRRs are progressively combined until their resonant modes interact, crowd the spectrum and form a wider absorption region.

COUPLED SYSTEM4× DSRRMAXIMUM MODE INTERACTION
01
ISOLATED RESPONSEEstablish the resonance.

A single scaled DSRR defines the starting optical mode.

02
MODE SPLITTINGIntroduce coupling.

A second resonator creates electromagnetic interaction and additional modes.

03
SPECTRAL CROWDINGIncrease mode density.

More scaled resonators reduce the spectral spacing between neighboring peaks.

04
WIDEBAND STATEMerge the optical window.

The four-cell configuration produces the strongest interaction and widest absorption region.

ISOLATED RESONANCESCOUPLING → OVERLAP → WIDEBANDABSORPTION WINDOW
INCREASING RESONANCE DENSITY
RESULTS / 02
11
CST RESULTS LAB · SIMULATION EVIDENCE

Read the resonance.
Then read the physics.

Switch between the designed optical bands. The laboratory pairs the reflection response with the corresponding current interpretation so the result reads like engineering evidence—not an image gallery.

REFLECTION RESPONSE · CST/FDTD423 THz
CST reflection response
DESIGNED RESONANCENEAR-UNITY ABSORPTION
ICEEE / 2026
12
ICEEE 2026 · ANTALYA · RESEARCH MILESTONE
27—29 APRIL 2026 · PAPER B4194

The simulation left the lab.
It became a conference paper.

The bachelor-thesis work on geometrically scaled DSRRs was carried from CST/FDTD simulation to an international presentation in Antalya. The official invitation, presentation certificate and paper form the research record.

13TH ICEEEANTALYA, TÜRKİYE4 DESIGNED RESONANCES
INTERNATIONAL CONFERENCEICEEE2026ANTALYA · TÜRKİYE
B4194423→518→640→831 THzGEOMETRICALLY SCALED DSRR · FDTD/CST · NEAR-UNITY ABSORPTION
THESIS / ARCHIVE
13
RESEARCH ARCHIVE · BACHELOR THESIS

The complete research, preserved as a document.

From the first DSRR scaling study to the multi-resonance absorber, the final thesis records the simulation methodology, optical response, surface-current interpretation and the progression toward broadband energy harvesting.

Development of Metamaterial Absorber bachelor thesis coverOPEN THESIS ↗
GUC · BACHELOR THESIS · JUNE 2026

Development of
Metamaterial Absorber

AUTHORMazin N. Desouky
SUPERVISORProf. Dr. A. M. M. A. Allam
FIELDOptical Metamaterials · DSRR

The thesis demonstrates geometrical tuning from 423 to 831 THz with near-unity absorption, then extends the concept to coupled multi-cell resonators for wider spectral coverage.

423 THz518 THz640 THz831 THzWIDEBAND
FINALE / 2026
14
THE RESEARCH JOURNEY · 2026

One thesis.
Six engineering moves.

From a subwavelength resonator to an international conference record, each stage answered a different engineering question.

01CONCEPTAbsorb light

Start with a ground-backed metamaterial absorber.

02MODELBuild in CST

Ag / SiO₂ / Ag unit cell with FDTD analysis.

03TUNEScale geometry

423 · 518 · 640 · 831 THz.

04EXPLAINRead currents

Interpret localization, coupling and higher modes.

05EXPANDCouple DSRRs

Increase resonance density toward a broader window.

06PRESENTICEEE Antalya

Move the work from thesis to international stage.

DSRR
DEVELOPMENT OF METAMATERIAL ABSORBER

Engineer the geometry.
Control the spectrum.

Optical metamaterials · electromagnetic simulation · frequency-selective absorption · energy-harvesting research.