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Nuclear Emulsions as Characterized in Overview of Photographic Emulsions. Tadaaki Tani (Frontier Res. Labs, FUJIFILM) Introduction Large grains for color negative films Small grains for OPERA Very small grains for Dark Matter Detection
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Nuclear Emulsions as Characterized in Overview of Photographic Emulsions Tadaaki Tani (Frontier Res. Labs, FUJIFILM) • Introduction • Large grains for color negative films • Small grains for OPERA • Very small grains for Dark Matter Detection 3rd Intern. Workshop on Nuclear Emulsion Techniques, Jan. 2008, Nagoya
ゼラチン水溶液 AgNO3 + KX → AgX + KNO3 in an aqueous gelatin solution
Sens ∝ Abs×Eff Abs ∝ Vol ∝ d3 Competition→ >2 L. i. centers Ⅲ Ⅱ Ⅰ
Ⅲ Ⅱ Ⅰ ←Efficiency of latent image formation
Nuclear Emulsions as Characterized in Overview of Photographic Emulsions Tadaaki Tani (Frontier Res. Labs, FUJIFILM) • Introduction • Large grains for color negative films • Small grains for OPERA • Very small grains for Dark Matter Detection 3rd Intern. Workshop on Nuclear Emulsion Techniques, Jan. 2008, Nagoya
Nuclear Emulsions as Characterized in Overview of Photographic Emulsions Tadaaki Tani (Frontier Res. Labs, FUJIFILM) • Introduction • Large grains for color negative films • Small grains for OPERA • Very small grains for Dark Matter Detection 3rd Intern. Workshop on Nuclear Emulsion Techniques, Jan. 2008, Nagoya
Cubic AgBr (0.15μm, S + Au) Babcock & James (1976)
→1 1 (Ag2; Reduction sensitization center) →2
Microwave photoconductivity measurement recombination e- trap trapping
(Carriers; positive holes) (Carriers; electrons)
Electron-trapping Hole-trapping By electron-trapping Ag2 By hole-trapping Ag2 T. Tani et al. (1999)
Nuclear Emulsions as Characterized in Overview of Photographic Emulsions Tadaaki Tani (Frontier Res. Labs, FUJIFILM) • Introduction • Large grains for color negative films • Small grains for OPERA • Very small grains for Dark Matter Detection 3rd Intern. Workshop on Nuclear Emulsion Techniques, Jan. 2008, Nagoya
X-ray diffraction pattern of Cubic AgBr grains A・・・150 nm C・・・ 96 nm E・・・ 62 nm H・・・ 50 nm Scherrer’s equation Dhkl = Kλ/βcosθ Miyake, Tani & Nittono (2000)
B B A A
Indirect transition Direct transition
on 0.2μm AgBr on 0.2μm AgBr recombination recombination Microwave photoconductivity measurement trapping e- trap E = I×t E = I×t RRecomb = [e-]×[h+] should increase withdecreasing grain size
Challenging and interesting subjects on very small grains (VSG) of silver halide • Formation & stabilization of VSG • Precise size measurement of VSG • Quantum size effect of light absorption • Ballistic carrier transport in VSG • Enhanced recombination in VSG • Very small number of sensitization centers and impurity ions in each VSG • Very small fraction of fogged grains in VSG • Size dependence of sensitivity of VSG