Capacitance spectroscopy of electro nic states at the SiO2/n-Si interface in MOS structures irradiated with helium ions

Al/SiO 2 / n -Si/Al MOS structures fabricated on (100) wafers of single-crystal n -type silicon grown with the Czochralski method were studied. The electrical resistivity of silicon was 4.5 Ohm · cm at room temperature. The thickness of the SiO 2 layer thermally formed in dry oxygen was 420 nm. The thickness of the aluminum layer deposited on top of SiO 2 was 0.7 µm. The area of aluminum metallization was 1.85 × 1.85 mm 2 . At a room temperature, the structures were irradiated with helium ions (kinetic energy of an ion was 5 MeV). The radiation fluence ranged from 10 10 to 10 13 cm −2 . According to calculations performed in the SRIM program, the average projective range of the helium ion in the structure was ≈ 24 µm. The impedance modulus Z and the phase shift angle φ between the current and voltage were measured in the frequency range from 20 Hz to 2 MHz using an E4980A LCR meter. The signal amplitude was 40 mV. The constant bias voltage U varied from −40 to 40 V. The MOS structures were kept in the dark at a room temperature. The DLTS spectra were recorded using CE-7C capacitance spectrometer in the temperature range of 80–300 K. The voltage pulses for filling traps U p with c -band electrons and the voltage of emission U e of electrons from traps to c -band of n -Si varied in the range from −0.5 to −9 V. The pulse duration for filling traps with electrons was t p = 0.75 ms, and the pulse duration for emission of electrons from traps was t e = 20 ms. It was found that for the Al/SiO 2 / n -Si/Al structures irradiated with helium ions with fluences of ≤10 12 cm −2 , the dependence of the capacitance on the frequency in the depletion mode is determined by the recharging of the surface electron states at the SiO 2 / n -Si interface. It was shown that in the initial structures for fast (recharging time <1 µs) surface states, the dependence of the energy density of states N ss on the potential energy e ψ of an electron in n -Si near the SiO 2 / n -Si interface has its maximum at e ψ ≈ E F – 0.1 eV (here e is the elementary charge, ψ is the electric potential, E F is the Fermi energy level). After irradiation with helium ions with a fluence of 10 12 cm −2 , this maximum shifts towards lower energies down to e ψ ≈ E F – 0.2 eV. In the irradiated structures, a second maximum appears on the N ss ( e ψ) dependence in the region of e ψ > 0. For an irradiation fluence of 10 12 cm −2 , the maximum is located at e ψ ≈ E F + 0.1 eV. The possibility of studying surface states with the DLTS spectroscopy method in the selected energy range by varying the emission voltage U e at a constant value of the filling voltage U p and/or varying the filling voltage U p at a constant value of the emission voltage U e is shown.

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Journal
Proceedings of the National Academy of Sciences of Belarus Physics and Mathematics Series
Published
2025-03-26
DOI
https://doi.org/10.29235/1561-2430-2025-61-1-34-46
Primary Topic
Silicon and Solar Cell Technologies
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article
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article

Capacitance spectroscopy of electro nic states at the SiO2/n-Si interface in MOS structures irradiated with helium ions

S. V. Shpakovski, N. A. Poklonski, Н. И. Горбачук, K. A. Ermakova
Proceedings of the National Academy of Sciences of Belarus Physics and Mathematics Series
Silicon and Solar Cell Technologies
article

Capacitance spectroscopy of electro nic states at the SiO2/n-Si interface in MOS structures irradiated with helium ions

S. V. Shpakovski, N. A. Poklonski, Н. И. Горбачук, K. A. Ermakova
article en

Abstract

Al/SiO 2 / n -Si/Al MOS structures fabricated on (100) wafers of single-crystal n -type silicon grown with the Czochralski method were studied. The electrical resistivity of silicon was 4.5 Ohm · cm at room temperature. The thickness of the SiO 2 layer thermally formed in dry oxygen was 420 nm. The thickness of the aluminum layer deposited on top of SiO 2 was 0.7 µm. The area of aluminum metallization was 1.85 × 1.85 mm 2 . At a room temperature, the structures were irradiated with helium ions (kinetic energy of an ion was 5 MeV). The radiation fluence ranged from 10 10 to 10 13 cm −2 . According to calculations performed in the SRIM program, the average projective range of the helium ion in the structure was ≈ 24 µm. The impedance modulus Z and the phase shift angle φ between the current and voltage were measured in the frequency range from 20 Hz to 2 MHz using an E4980A LCR meter. The signal amplitude was 40 mV. The constant bias voltage U varied from −40 to 40 V. The MOS structures were kept in the dark at a room temperature. The DLTS spectra were recorded using CE-7C capacitance spectrometer in the temperature range of 80–300 K. The voltage pulses for filling traps U p with c -band electrons and the voltage of emission U e of electrons from traps to c -band of n -Si varied in the range from −0.5 to −9 V. The pulse duration for filling traps with electrons was t p = 0.75 ms, and the pulse duration for emission of electrons from traps was t e = 20 ms. It was found that for the Al/SiO 2 / n -Si/Al structures irradiated with helium ions with fluences of ≤10 12 cm −2 , the dependence of the capacitance on the frequency in the depletion mode is determined by the recharging of the surface electron states at the SiO 2 / n -Si interface. It was shown that in the initial structures for fast (recharging time <1 µs) surface states, the dependence of the energy density of states N ss on the potential energy e ψ of an electron in n -Si near the SiO 2 / n -Si interface has its maximum at e ψ ≈ E F – 0.1 eV (here e is the elementary charge, ψ is the electric potential, E F is the Fermi energy level). After irradiation with helium ions with a fluence of 10 12 cm −2 , this maximum shifts towards lower energies down to e ψ ≈ E F – 0.2 eV. In the irradiated structures, a second maximum appears on the N ss ( e ψ) dependence in the region of e ψ > 0. For an irradiation fluence of 10 12 cm −2 , the maximum is located at e ψ ≈ E F + 0.1 eV. The possibility of studying surface states with the DLTS spectroscopy method in the selected energy range by varying the emission voltage U e at a constant value of the filling voltage U p and/or varying the filling voltage U p at a constant value of the emission voltage U e is shown.

Proceedings of the National Academy of Sciences of Belarus Physics and Mathematics SeriesVol. 61(1)
Belarusian State University (BY), Integral Consulting (United States) (US)
Openalex Percentile: Top 95%
Silicon and Solar Cell Technologies
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