103 research outputs found

    Recombination peculiarities in doped Ge

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    Effect of Mn and Mg dopants on vacancy defect formation in ammonothermal GaN

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    We have applied positron annihilation spectroscopy to study the formation of Ga vacancy related defects in Mg and Mn doped bulk GaN crystals grown by the ammonothermal method. We show that Mn doping has little or no effect on the formation of Ga vacancies, while Mg doping strongly suppresses their formation, in spite of both dopants leading to highly resistive material. We suggest the differences are primarily due to the hydrogen-dopant interactions. Further investigations are called for to draw a detailed picture of the atomic scale phe-nomena in the synthesis of ammonothermal GaN.Peer reviewe

    SPECTROSCOPY OF DEFECTS IN NEUTRON IRRADIATED AMMONO-THERMAL GaN BY COMBINING PHOTOIONIZATION, PHOTOLUMINESCENCE AND POSITRON ANNIHILATION TECHNIQUES

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    In this work, pulsed photoionization as well as photoluminescence and positron annihilation spectroscopy were combined to detect different species of defects. The GaN crystals, grown by the ammono-thermal method, doped with Mn as well as Mg impurities and irradiated with different fluences of reactor neutrons, were examined to clarify the role of the technological and radiation defects. The evolution of the prevailing photoactive centres was examined by pulsed photoionization spectroscopy. Positron annihilation spectroscopy was applied to reveal vacancy-type defects.Peer reviewe

    Analysis of trap spectra in LEC and epitaxial GaAs

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    Different methods of trap parameter measurement are analysed. Transient photoconductivity and thermally stimulated effects were used to investigate the influence of traps in LEC SI-GaAs and high resistivity epitaxial GaAs. The peculiarities of the TSC were analysed and shown to be related to the influence of crystal micro-inhomogeneities.Comment: Invited talk, 6-th Workshop on Gallium Arsenide and Related Compounds June 22-26, 1998 Praha-Pruhonice, Czech Republi

    RD39 Status Report 2009

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    RD39 Status Report 2009. CERN RD39 Collaboration is developing super-radiation hard cryogenic silicon detectors for applications of LHC experiments and their future upgrades. The activities of RD39 Collaboration were focused in 2009 on concept of charge injected detector (CID)

    Π˜ΠΠ–Π•ΠšΠ¦Π˜ΠžΠΠΠ«Π™ ΠžΠ’Π–Π˜Π“ ΠšΠžΠœΠŸΠ›Π•ΠšΠ‘Π Π‘ΠžΠ‘Π‘Π’Π’Π•ΠΠΠžΠ• Π”Π˜ΠœΠ•Π–Π”ΠžΠ£Π—Π›Π˜Π• – ΠšΠ˜Π‘Π›ΠžΠ ΠžΠ” Π’ ΠšΠ Π•ΠœΠΠ˜Π˜ p-ВИПА

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    With the use of deep level transient spectroscopy (DLTS) the effect of injection of minority charge carriers (electrons) on an annealing rate of self di-interstitial – oxygen (I2O) complex in silicon has been studied. The complex has been formed by irradiation of epitaxial boron-doped n+–p diode structures with alpha-particles at room temperature. It has been shown that the disappearance of this complex at room temperature begins at a direct current density of ~1.5 A/cm2. This characteristic current density has been found for 10 WΒ·cm p-type silicon when the total radiation defect density was less than 15 % of the initial boron concentration, a divalent hole trap with energy levels of Ev + 0.43 eV and Ev + 0.54 eV has been found to appear as a result of recombination-enhanced annealing of the I2O. When the I2O complex is annealed thermally, the concurrent appearance of an electron trap with an energy level of Ec – 0.35 eV has been observed. It has been shown that the divalent hole trap represents a metastable configuration (BH-configuration) of the bistable defect, whereas the electron trap is stab le in the p-Si configuration (ME-configuration). From the comparison of DLTS signals related to different defect configurations it is found that the ME-configuration of this bistable defect can be characterized as a center with negative correlation energy. It has been shown that the injection-stimulated processes make it very difficult to obtain reliable data on the formation kinetics of the bistable defect in the BH-configuration when studying the thermal annealing of the I2O complex.ΠœΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ нСстационарной спСктроскопии Π³Π»ΡƒΠ±ΠΎΠΊΠΈΡ… ΡƒΡ€ΠΎΠ²Π½Π΅ΠΉ (DLTS) с использованиСм n+–p-структур исслСдовано влияниС ΠΈΠ½ΠΆΠ΅ΠΊΡ†ΠΈΠΈ нСосновных носитСлСй заряда (элСктронов) Π½Π° ΠΎΡ‚ΠΆΠΈΠ³ комплСкса собствСнноС Π΄ΠΈΠΌΠ΅ΠΆΠ΄ΠΎΡƒΠ·Π»ΠΈΠ΅ – кислород (I2O) Π² ΠΊΡ€Π΅ΠΌΠ½ΠΈΠΈ, ΠΎΠ±Π»ΡƒΡ‡Π΅Π½Π½ΠΎΠΌ Π°Π»ΡŒΡ„Π°-частицами. Показано, Ρ‡Ρ‚ΠΎ Π² Π»Π΅Π³ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠΌ Π±ΠΎΡ€ΠΎΠΌ ΠΊΡ€Π΅ΠΌΠ½ΠΈΠΈ, ΠΈΠΌΠ΅ΡŽΡ‰Π΅ΠΌ ΡƒΠ΄Π΅Π»ΡŒΠ½ΠΎΠ΅ сопротивлСниС 10 Ом·см, ΠΈΠ½ΠΆΠ΅ΠΊΡ†ΠΈΠΎΠ½Π½ΠΎ-стимулированный ΠΎΡ‚ΠΆΠΈΠ³ этого комплСкса ΠΏΡ€ΠΈ ΠΊΠΎΠΌΠ½Π°Ρ‚Π½ΠΎΠΉ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π΅ начинаСтся ΠΏΡ€ΠΈ плотности прямого Ρ‚ΠΎΠΊΠ° ~1,5 А/см2. ΠŸΡ€ΠΈ этом суммарная концСнтрация Ρ€Π°Π΄ΠΈΠ°Ρ†ΠΈΠΎΠ½Π½Ρ‹Ρ… Π΄Π΅Ρ„Π΅ΠΊΡ‚ΠΎΠ² Π½Π΅ ΠΏΡ€Π΅Π²Ρ‹ΡˆΠ°Π»Π° 15 % ΠΎΡ‚ Π½Π°Ρ‡Π°Π»ΡŒΠ½ΠΎΠΉ ΠΊΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†ΠΈΠΈ Π±ΠΎΡ€Π°. Π’ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π΅ ΠΈΠ½ΠΆΠ΅ΠΊΡ†ΠΈΠΎΠ½Π½ΠΎ-стимулированного ΠΎΡ‚ΠΆΠΈΠ³Π° I2O образуСтся двухвалСнтная дырочная Π»ΠΎΠ²ΡƒΡˆΠΊΠ° с уровнями Ev + 0,43 эВ ΠΈ Ev + 0,54 эВ. УстановлСно, Ρ‡Ρ‚ΠΎ Π² ΠΊΡ€Π΅ΠΌΠ½ΠΈΠΈ Ρ€-Ρ‚ΠΈΠΏΠ° проводимости эта Π»ΠΎΠ²ΡƒΡˆΠΊΠ° соотвСтствуСт эмиссии Π΄Ρ‹Ρ€ΠΎΠΊ ΠΌΠ΅Ρ‚Π°ΡΡ‚Π°Π±ΠΈΠ»ΡŒΠ½ΠΎΠΉ ΠΊΠΎΠ½Ρ„ΠΈΠ³ΡƒΡ€Π°Ρ†ΠΈΠ΅ΠΉ Π±ΠΈΡΡ‚Π°Π±ΠΈΠ»ΡŒΠ½ΠΎΠ³ΠΎ Π΄Π΅Ρ„Π΅ΠΊΡ‚Π° (BH-конфигурация). Π’ основной ΠΊΠΎΠ½Ρ„ΠΈΠ³ΡƒΡ€Π°Ρ†ΠΈΠΈ (ME-конфигурация) этот Π±ΠΈΡΡ‚Π°Π±ΠΈΠ»ΡŒΠ½Ρ‹ΠΉ Π΄Π΅Ρ„Π΅ΠΊΡ‚ проявляСт сСбя ΠΊΠ°ΠΊ элСктронная Π»ΠΎΠ²ΡƒΡˆΠΊΠ° с ΡƒΡ€ΠΎΠ²Π½Π΅ΠΌ Ec – 0,35 эВ. На основании Π΄Π°Π½Π½Ρ‹Ρ… ΠΎΠ± ΠΎΡ‚Π½ΠΎΡˆΠ΅Π½ΠΈΠΈ Π°ΠΌΠΏΠ»ΠΈΡ‚ΡƒΠ΄ сигнала DLTS Π±ΠΈΡΡ‚Π°Π±ΠΈΠ»ΡŒΠ½ΠΎΠ³ΠΎ Π΄Π΅Ρ„Π΅ΠΊΡ‚Π° Π² Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… конфигурациях сдСлан Π²Ρ‹Π²ΠΎΠ΄, Ρ‡Ρ‚ΠΎ Π² ME-ΠΊΠΎΠ½Ρ„ΠΈΠ³ΡƒΡ€Π°Ρ†ΠΈΠΈ ΠΎΠ½ Π²Π΅Π΄Π΅Ρ‚ сСбя ΠΊΠ°ΠΊ Ρ†Π΅Π½Ρ‚Ρ€ с ΠΎΡ‚Ρ€ΠΈΡ†Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ коррСляционной энСргиСй. Показано, Ρ‡Ρ‚ΠΎ Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ ΠΈΠ½ΠΆΠ΅ΠΊΡ†ΠΈΠΎΠ½Π½ΠΎ-стимулированных процСс- сов сущСствСнно затрудняСт ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½ΠΈΠ΅ достовСрных Π΄Π°Π½Π½Ρ‹Ρ… ΠΎ ΠΊΠΈΠ½Π΅Ρ‚ΠΈΠΊΠ΅ образования Π±ΠΈΡΡ‚Π°Π±ΠΈΠ»ΡŒΠ½ΠΎΠ³ΠΎ Π΄Π΅Ρ„Π΅ΠΊΡ‚Π° Π² BH-ΠΊΠΎΠ½Ρ„ΠΈΠ³ΡƒΡ€Π°Ρ†ΠΈΠΈ ΠΏΡ€ΠΈ исслСдовании тСрмичСского ΠΎΡ‚ΠΆΠΈΠ³Π° комплСкса собствСнноС Π΄ΠΈΠΌΠ΅ΠΆΠ΄ΠΎΡƒΠ·Π»ΠΈΠ΅ – кислород
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