In accordance with the purpose(s) of the present disclosure, as embodied and broadly described herein, the disclosure, in one aspect, relates to compound Bi-poor perovskite crystals, methods for making the same, and ionizing and other electromagnetic radiation detectors constructed using the Bi-poor perovskite crystals. The Bi-poor perovskite crystals can be synthesized using melt-based growth methods and solution-based growth methods and contain no toxic heavy metals such as lead, cadmium, thallium, or mercury. Devices fabricated from the crystals maintain acceptable levels of performance over time. In some aspects, post-growth annealing can be used to improve the properties, including, but not limited to, room temperature resistivity and response to radiation.

In accordance with the purpose(s) of the present disclosure, as embodied and broadly described herein, the disclosure, in one aspect, relates to compound Bi-poor perovskite crystals, methods for making the same, and ionizing and other electromagnetic radiation detectors constructed using the Bi-poor perovskite crystals. The Bi-poor perovskite crystals can be synthesized using melt-based growth methods and solution-based growth methods and contain no toxic heavy metals such as lead, cadmium, thallium, or mercury. Devices fabricated from the crystals maintain acceptable levels of performance over time. In some aspects, post-growth annealing can be used to improve the properties, including, but not limited to, room temperature resistivity and response to radiation.

The present invention provides for a composition comprising an inorganic scintillator comprising an optionally lanthanide-doped cesium barium halide, useful for detecting nuclear material.

The present invention provides for a composition comprising an inorganic scintillator comprising an optionally lanthanide-doped cesium barium halide, useful for detecting nuclear material.

Embodiments relate to methods of forming a halide perovskite crystal. The method involves dispersing a halide perovskite material exhibiting a perovskite crystallographic lattice into a solution. The solution can include amine and a volatile solvent. The method involves forming a metastable intermediate state via amine molecules inserting into the perovskite crystallographic lattice. The method involves transitioning the perovskite material to a photo-sensitive phase via escape of the amine molecules from the perovskite crystallographic lattice. The method involves transitioning the metastable intermediate state to a halide perovskite crystal film.

Embodiments relate to methods of forming a halide perovskite crystal. The method involves dispersing a halide perovskite material exhibiting a perovskite crystallographic lattice into a solution. The solution can include amine and a volatile solvent. The method involves forming a metastable intermediate state via amine molecules inserting into the perovskite crystallographic lattice. The method involves transitioning the perovskite material to a photo-sensitive phase via escape of the amine molecules from the perovskite crystallographic lattice. The method involves transitioning the metastable intermediate state to a halide perovskite crystal film.

Inorganic halides (e.g., inorganic halide scintillators) of the general formula A.sub.3B.sub.2X.sub.9, including inorganic halides comprising thallium monovalent cations and/or combinations of different halides, are described. Radiation detectors including the inorganic halide scintillators and methods of using the detectors to detect high energy radiation are also described. In some cases, the scintillators can include a gadolinium cation, a boron cation, a lithium cation, a chloride ion, or combinations thereof and the scintillator can be used to detect neutrons.

Inorganic halides (e.g., inorganic halide scintillators) of the general formula A.sub.3B.sub.2X.sub.9, including inorganic halides comprising thallium monovalent cations and/or combinations of different halides, are described. Radiation detectors including the inorganic halide scintillators and methods of using the detectors to detect high energy radiation are also described. In some cases, the scintillators can include a gadolinium cation, a boron cation, a lithium cation, a chloride ion, or combinations thereof and the scintillator can be used to detect neutrons.

[Object] To provide a single-crystal fiber production equipment and a single-crystal fiber production method that do not at all require high precision control necessary for a conventional single-crystal production equipment, can very easily maintain a stable steady state for a long time, and can stably produce a long single crystal fiber having a length of several hundreds of meters or more. [Solution] The single-crystal fiber production equipment is used to produce a single crystal fiber by irradiating an upper surface of a raw material rod with a laser beam within a chamber to form a melt, immersing a seed single crystal in the melt, and pulling the seed single crystal upward. The single-crystal fiber production equipment includes: a laser light source that emits the laser beam as a collimated beam; a pulling device configured to be upward and downward movable in a vertical direction with the seed single crystal held thereby; and a flat reflector that reflects the laser beam such that the reflected laser beam is incident vertically on the upper surface of the raw material rod. The upper surface of the raw material rod is irradiated with the laser beam such that the melt has a donut-shaped temperature distribution.

[Object] To provide a single-crystal fiber production equipment and a single-crystal fiber production method that do not at all require high precision control necessary for a conventional single-crystal production equipment, can very easily maintain a stable steady state for a long time, and can stably produce a long single crystal fiber having a length of several hundreds of meters or more. [Solution] The single-crystal fiber production equipment is used to produce a single crystal fiber by irradiating an upper surface of a raw material rod with a laser beam within a chamber to form a melt, immersing a seed single crystal in the melt, and pulling the seed single crystal upward. The single-crystal fiber production equipment includes: a laser light source that emits the laser beam as a collimated beam; a pulling device configured to be upward and downward movable in a vertical direction with the seed single crystal held thereby; and a flat reflector that reflects the laser beam such that the reflected laser beam is incident vertically on the upper surface of the raw material rod. The upper surface of the raw material rod is irradiated with the laser beam such that the melt has a donut-shaped temperature distribution.