TY - JOUR T1 - Influence of Intense Laser Field on the Electronic Structure and Third-Harmonic Generation in Asymmetric Double Inverse Parabolic Quantum Wells TT - Asimetrik Çift Ters Parabolik Kuantum Kuyularındaki Yoğun Lazer Alanının Elektronik Yapı ve Üçüncü Harmonik Üretimi Üzerindeki Etkisi AU - Öztürk, Ozan PY - 2025 DA - September Y2 - 2025 DO - 10.47495/okufbed.1635337 JF - Osmaniye Korkut Ata Üniversitesi Fen Bilimleri Enstitüsü Dergisi JO - Osmaniye Korkut Ata University Journal of The Institute of Science and Techno PB - Osmaniye Korkut Ata Üniversitesi WT - DergiPark SN - 2687-3729 SP - 1644 EP - 1653 VL - 8 IS - 4 LA - en AB - This study explores the effects of an intense laser field (ILF) on the energy levels, electron probability distributions, and third-harmonic generation (THG) in asymmetric double inverse parabolic quantum wells (ADIPQW). The Schrödinger equation is solved using the finite element method under the effective mass approximation, incorporating ILF effects via the Floquet method. For ILF parameter α0 = 0, 2, 4, 6, and 8 nm, we analyze the modifications in potential profiles, energy differences, dipole moment matrix elements (DMME), and THG coefficients. The results indicate that increasing ILF intensity leads to shifts in energy levels and electron localization. The energy differences E₂₁, E₃₁/₂, and E₄₁/₃ show distinct trends under varying ILF, directly affecting THG resonance peak positions. The DMME product remains nearly constant at low ILF values but fluctuates significantly at higher ILF intensities, peaking at α0 = 5 nm and reaching a minimum at α0 = 7 nm. These findings highlight ILF as a tunable parameter for controlling electronic properties and nonlinear optical responses in semiconductor quantum structures. KW - Intense laser field KW - Parabolic quantum well KW - Third-harmonic generation N2 - Bu çalışma, asimetrik çift ters parabolik kuantum kuyularında (ADIPQW) yoğun lazer alanının (ILF) enerji seviyeleri, elektron olasılık dağılımları ve üçüncü harmonik üretimi (THG) üzerindeki etkilerini incelemektedir. Schrödinger denklemi, etkin kütle yaklaşımı çerçevesinde sonlu elemanlar yöntemi kullanılarak çözülmüş ve ILF etkileri Floquet yöntemi aracılığıyla modellenmiştir. ILF parametresi α0 = 0, 2, 4, 6 ve 8 nm için, potansiyel profillerindeki değişimler, enerji farkları, dipol moment matris elemanları (DMME) ve THG katsayıları analiz edilmiştir. Sonuçlar, ILF şiddetinin artmasının enerji seviyelerinde kaymalara ve elektron lokalizasyonunda değişimlere yol açtığını göstermektedir. Enerji farkları E₂₁, E₃₁/₂ ve E₄₁/₃, değişen ILF değerleri altında farklı eğilimler sergileyerek THG rezonans tepe noktalarını doğrudan etkilemektedir. 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