By F. Pittnauer

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For m-λ = 600 nm, it w i l l r e f l e c t a high i n t e n s i t y f i r s t order λ ranging from 400 to 900 nm and a high i n t e n s i t y second order λ ranging from 200 to 450 nm. The determination of wavelengths by measurements of θ at a given φ or (φ-θ) i s only p o s s i b l e , i f the order of r e f l e x i o n i s f i x e d . r a d i a t i o n s with wavelengths λ ρ λ ^ , λ ^ , All . . are namely reflected in 1 . , 2 . , 3 . , . . order at the same a n g l e , i f λ-j = 2 · = 3 · = The overlapping of orders can be prevented by i n s e r t i n g a prism or f i l t e r s in the part of the r a y s , r e f l e c t i n g by the g r a t i n g .

The upper energy state E u can belong e i t h e r to the l a s e r a c t i v e o s c i l l a t o r or to a matrix species ( e . g . He in H e / N e - l a s e r ) , i f t h i s a u x i l i a r y resonator (gene­ r a l l y an atom or a molecule) has a metastable energy state it and i s therefore able to transmit energy in c o l l i s i o n s . The energetic separation (E ffl - E^) of the s t a t e s p a r t i c i p a t i n g d i r e c t l y in stimulated r a d i a t i o n determines the wavelength of the l a s e r radiation.

1 . 3 The corpuscular nature of the electromagnetic c r a d i a t i o n (EMR). A) Measurement and E i n s t e i n ' s explanation of the photoelectric e f f e c t . B) Vector diagram f o r the explanation of the Compton effect. matter. Each p a r t i c l e c o n s i s t s of a quantum h-v of energy (energy quantum or photon). I n a photoelectric act the e n t i r e energy of a photon i s transferred to a s i n g l e electron in the metal and when the electron leaves the surface of the metal i t w i l l have an amount of k i n e t i c energy given by [ 3 ] : m e0 2 = - max = e U h - * W =^ " ί · · W 2 1 1 0 » where W i s the work required to remove the electron from the metal (work function of the metal).

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