Synthesis of a potential semiconductor neutron detector crystal LiGa(Se/Te)2: materials purity and compatibility effects

Lithium containing AIBIIICVI semiconductors are being considered as alternative materials for room temperature neutron detection. One of the primary challenges in growing a high quality crystal of such a material is the reactivity of lithium metal. The presence of nitrides, oxides, and a variety of alkali and alkaline earth metal impurities prevent pure synthesis and truncate crystal growth by introducing multiple nucleation centers during growth. Multiple lithium metal purification methods have been investigated which ultimately raised the metal purity to 99.996%. Multi-cycle vacuum distillation removed all but 40 ppm of metal impurities in lithium metal. LiGa(Se/Te)2 was then synthesized with the high purity lithium metal by a variety of conditions. Lithium metal reacts violently with many standard crucible materials, and thermodynamic studies were undertaken to insure that an appropriate crucible choice was made, with high purity iron and boron nitride crucibles being the least reactive practical materials. Once conditions were optimized for synthesis of the chalcopyrite, vertical Bridgman crystal growth resulted in red crystals. The optical, electronic, and thermodynamic properties were collected.

[1]  V. Petrov,et al.  Frequency doubling of CO2 laser radiation at 10.6 microm in the highly nonlinear chalcopyrite LiGaTe2. , 2007, Optics letters.

[2]  K. Kuriyama,et al.  Single‐crystal growth and characterization of LiGaSe2 , 1981 .

[3]  E. Hoffman THE SOLUBILITY OF NITROGEN AND OXYGEN IN LITHIUM AND METHODS OF LITHIUM PURIFICATION , 1960 .

[4]  I. Kityk,et al.  Several features of nonlinear optical susceptibilities of LiGaX2 (X = S, Se) ternary compounds , 2009 .

[5]  G. H. Broomfield,et al.  The purification of lithium by vacuum distillation , 1963 .

[6]  V. Petrov,et al.  LiGaTe2: A new highly nonlinear chalcopyrite optical crystal for the Mid-IR , 2005 .

[7]  Valentin Petrov,et al.  Second harmonic generation and optical parametric amplification in the mid-IR with orthorhombic biaxial crystals LiGaS2 and LiGaSe2 , 2004 .

[8]  Stephan Friedrich,et al.  Neutron detection with cryogenics and semiconductors , 2005 .

[9]  Valentin Petrov,et al.  Ternary chalcogenides LiBC2 (B = In, Ga; C = S, Se, Te) for mid-IR nonlinear optics , 2006 .

[10]  Gunnar Eriksson,et al.  FactSage thermochemical software and databases , 2002 .

[11]  P. H. Schmidt Purification of Lithium Metal by High‐Vacuum Fractional Distillation , 1966 .

[12]  Valentin Petrov,et al.  LiInSe2 nanosecond optical parametric oscillator. , 2005, Optics letters.

[13]  A. S. Poplavnoi,et al.  Lattice dynamics of chalcopyrite semiconductors LiAlTe2, LiGaTe2 and LiInTe2 , 2009 .

[14]  R. Rogers,et al.  Effect of Pressure on the Refining of Lithium by Distillation , 1951 .

[15]  W.C. Priedhorsky,et al.  Nuclear detection to prevent or defeat clandestine nuclear attack , 2005, IEEE Sensors Journal.

[16]  I. Kityk,et al.  Electronic properties of orthorhombic LiGaS2 and LiGaSe2 , 2009 .

[17]  V. Petrov,et al.  Growth and properties of LiGaX2 (X = S, Se, Te) single crystals for nonlinear optical applications in the mid‐IR , 2003 .

[18]  Alexander P. Yelisseyev,et al.  Growth of new nonlinear crystals LiMX2 (M = Al, In, Ga; X = S, Se, Te) for the mid-IR optics , 2005 .