Response of strontium titanate to ion and electron irradiation

Zhang, Yongfeng; Lian, Jie; Zhu, Zihua; Bennett, Wendy D.; Saraf, Laxmikant V.; Rausch, J; Hendricks, Catherine A.; Ewing, Rodney C.; Weber, William J.

doi:10.1016/j.jnucmat.2009.02.014

Cited by 86 publications

(61 citation statements)

References 47 publications

Supporting

Mentioning

Contrasting

Order By: Relevance

“…Experimental phization dose at room temperature is below 2 dpa [12,14,16]. In our present study, no amorphous is observed in irradiated SrTiO 3 even at 5 dpa.…”

Section: Resultscontrasting

confidence: 43%

“…The potential materials for immobilization of nuclear waste must be able to endure extreme radiation environment associated with α-decay of the actinides and β-decay of the fission products. In the previous studies, several research groups have performed ion beam irradiations on SrTiO 3 to study its radiation tolerance [12][13][14][15][16]. An irradiation-induced crystalline to amorphous phase transformation was observed on SrTiO 3 , and quantitatively studies on the critical dose and temperature for amorphization were already reported [12,14,16].…”

Section: +mentioning

confidence: 99%

“…200 keV He + ions were implanted at normal incident using a fluence rate of 2×10 16 ions/m 2 to fluences of 2 × 10 21 ions/m 2 . The Stopping and Range of Ions in Matter (SRIM) program [17] was used to estimate the displacement damage in ion irradiated SrTiO 3 and Sr 3 Ti 2 O 7 .…”

Section: +mentioning

confidence: 99%

See 2 more Smart Citations

Irradiation study on Sr_n+1Ti_nO_3n+1 Ruddlesden‐Popper phases synthesized by hot‐forging

Tang

Fuierer

Dickens

et al. 2013

Phys. Status Solidi C

View full text Add to dashboard Cite

The hot‐forging technique was used to obtain both the n = 2 (Sr3Ti2O7) and n = ∞ (SrTiO3) members of Ruddlesden‐Popper phase Srn+1TinO3n+1. Pure phase and high density (>95% theoretical) materials were achieved using this technique. These polycrystalline samples were irradiated with 200 keV He ions to a fluence of 2×1021 ion/m2 (corresponding to a peak dose at 5 dpa) at room temperature to study radiation damage effects. Microstructural investigation on pristine and irradiated samples was performed using grazing incidence X‐ray diffraction (GIXRD) and transmission electron microscopy (TEM). Three phenomena are revealed upon comparing prisXtine versus irradiated samples. First, both compounds interplanar lattice spacings increased after irradiation. Second, peak broadening possibly suggests incredibly small grain due to irradiation. Third, experiment results revealed an amorphization in the irradiated Sr3Ti2O7, while no amorphization was observed in irradiated SrTiO3. (© 2013 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)

show abstract

“…Experimental phization dose at room temperature is below 2 dpa [12,14,16]. In our present study, no amorphous is observed in irradiated SrTiO 3 even at 5 dpa.…”

Section: Resultscontrasting

confidence: 43%

Section: +mentioning

confidence: 99%

See 1 more Smart Citation

Irradiation study on Sr_n+1Ti_nO_3n+1 Ruddlesden‐Popper phases synthesized by hot‐forging

Tang

Fuierer

Dickens

et al. 2013

Phys. Status Solidi C

View full text Add to dashboard Cite

show abstract

“…The small shift of damage profile of ϳ5% resulting from relatively lower stopping power of channeled He ions has been observed in slightly damaged SrTiO 3 . 54 Since this study mainly focuses on heavily damaged SiC samples, such channeling effects on the He stopping power will be ignored.…”

Section: He Stopping In Sicmentioning

confidence: 99%

“…54 The corresponding damage peak at ϳ55 nm was determined experimentally. The SRIM predicted damage peak is at 39 nm, much shallower than the experimental results with a difference close to 29%.…”

Section: Stopping Of Slow Heavy Ions In Srtio 3 Gan and Alnmentioning

confidence: 99%

Damage profile and ion distribution of slow heavy ions in compounds

Zhang¹,

Bae²,

Sun³

et al. 2009

Journal of Applied Physics

View full text Add to dashboard Cite

Slow heavy ions inevitably produce a significant concentration of defects and lattice disorder in solids during their slowing-down process via ion-solid interactions. For irradiation effects research and many industrial applications, atomic defect production, ion range, and doping concentration are commonly estimated by the stopping and range of ions in matter (SRIM) code. In this study, ion-induced damage and projectile ranges of low energy Au ions in SiC are determined using complementary ion beam and microscopy techniques. Considerable errors in both disorder profile and ion range predicted by the SRIM code indicate an overestimation of the electronic stopping power, by a factor of 2 in most cases, in the energy region up to 25 keV/nucleon. Such large discrepancies are also observed for slow heavy ions, including Pt, Au, and Pb ions, in other compound materials, such as GaN, AlN, and SrTiO3. Due to the importance of these materials for advanced device and nuclear applications, better electronic stopping cross section predictions, based on a reciprocity principle developed by Sigmund, is suggested with fitting parameters for possible improvement.

show abstract

Models for the Description of Track Formation

Dufour

Toulemonde

2016

Springer Series in Surface Sciences

View full text Add to dashboard Cite

Response of strontium titanate to ion and electron irradiation

Cited by 86 publications

References 47 publications

Irradiation study on Sr_n+1Ti_nO_3n+1 Ruddlesden‐Popper phases synthesized by hot‐forging

Irradiation study on Sr_n+1Ti_nO_3n+1 Ruddlesden‐Popper phases synthesized by hot‐forging

Damage profile and ion distribution of slow heavy ions in compounds

Models for the Description of Track Formation

Contact Info

Product

Resources

About

Response of strontium titanate to ion and electron irradiation

Cited by 86 publications

References 47 publications

Irradiation study on Srn+1TinO3n+1 Ruddlesden‐Popper phases synthesized by hot‐forging

Irradiation study on Srn+1TinO3n+1 Ruddlesden‐Popper phases synthesized by hot‐forging

Damage profile and ion distribution of slow heavy ions in compounds

Models for the Description of Track Formation

Contact Info

Product

Resources

About

Irradiation study on Sr_n+1Ti_nO_3n+1 Ruddlesden‐Popper phases synthesized by hot‐forging

Irradiation study on Sr_n+1Ti_nO_3n+1 Ruddlesden‐Popper phases synthesized by hot‐forging